by g.f1. avlt · 2019-04-29 · euranee against structural failure. _ an . iaportant phase of the...
TRANSCRIPT
t as 0
~
by Gf1 Avlt y ~ ea-s becaus~ tte~ re~-t proml
~xr1~srial thstand tl~
n t of the- middots1l~r a110ls ~et-ro -usi-on
d i2proved ria l s a~ still ~-ired to i~~rovebut
ce tin ogteraticm at hi$~rrfo
the rurboj et as ~xplained d sr
reali h1~b~r thrust and the turbopro~ll~r sectlins J fici~nc7 and pow~r
_ratJres a~ inc~ased 1ven i f these b~tVr
_ ter1ampls are not he pOll~rplan t t Jra~ at hizher
peratures these t-ria1s Will 1nc~ase s~rvce Efe and r~liaoi1i ty
arrr c t the present t the alloys in the j~t-~r ~ncine bull
can apr oxi tel y 15000 7a~nhei t 1 r r~seamprch
in this field th~ operatin or UleS~ ~~ra13 can roa~1middot1 be exshy
any of these allo-Js 1fe~ ~eve10~C b-j indus trJtlnded a f~ hLld~d
~ria1s bullp 0 t~~ on H~t- e3i
y of the 1erials now in use -ere d~7~10~d dlil t1 2 war by
cookbook metbo1s and a Ert of the researcn on lCltl1aiS
is d1~cted towartls an understadin of hOW tM3~ 2tcrials licr so that
ents basd on Lndallenta1 factcrs aff~ctr tr~ o-o- ra tion of
~r1als can b lJilde Uos t of the suo~r alloys ~ l arPe lalti ti~s of
scarce ~ria1s such as cobalt and co1UJ~lWl In tile case of a f utx-e
these less a lundant ca~r--a1s 11 lose
ampa
rected reOlcL use o these sca~A~ terials
~J
- 2 shybull
tho~ 57 rtich b~ r~sista~ce to te3 ra-~ ext~Ies can
An ~~ple of thipaSQ is bv the lSe of ma~rials tbat (an ~ cooea
+_ nAv7 ri bull rTlctaticn i~ Iis sh
ampis ar~al w~c fahLcated to
s you can see tbe oxy-ac etl~n~ fla=Je has h~atedIgt nave 0 ~rcen t porosit7
~ now ~ir~ct ~~ ai~ str~a~ ~~t~ a n~a1er or holethe block to a ~d ~ L
A
38 of an nch in dia1~~r thit has ooen 1illed into ti1c blocl bull
orcsi ty in tr~ bloc~ will liSr3 and conllct t~ air streaa in suct a
~r as efecti~ ccolin
c~ral3l ~ s can e readi faorcated Wit1 al~cs t atr des
e of )or os a~-als i s tia t of
s trerth is
ro~le ~ is also ~d~r in~st~~ticn bull
oOtai~i-1( hi~h ~orosi vj hil~ retainl hi
c )1 ~on ~l tshy
i t is natural to turn t rials lavi1
f r )sitr
a1ts aes i ners
in
~ Vt -rj hir~st ltelting oil ts bull hese aaterials ar~ hih-meltL1~-fOIf
tal such a s tlmgsten and ao17odem and the oT1ies nitri~s carbi des
ani bO~ce3 0 ll~ tdl ~is latter grOU ar~ c~l1~d c~ra ~c~ bull
teJ~ra tre scale along the top 0 this oa~l has on i t sClll~ 0 r UlII
i th 1rhic ~ 1 ir
res~ctive red
or t~ ~ry
of tn ra tutlS t
stress calliti
crart we can see in
~
~
~
~
bull
- J shy
aJPraxiJlaUily 24000 F These c~raric terials bein cClls -je r~d run fr
this paint uprar d to carbide at 7JX)deg
In o r to illustrate raphi~ally soe fa~ tors 12t nt-r in the J
perfOlllaIlce of materials I have hre a Sii1Jla~d mt~el se~~nt on whch
thre~ turbine blades bull fi r s t on~ 5 abrica ted r (]]l a typi cal
hi~h-teaperatilre al loy the s econd one is a pure c~ralic terial and t~
third one is a tal-bon~ed cera~c t eria l which p- have te~d a cer best c inatl oos ot pure ceraric Jrials for high- tezperature use in
turbines ve be~ 1evelo~d by the at i cnal eau ~ ~ ds middotmder
ccntract to the bull e now pass the wheel se=l~ t h=ough the oxy- ace t yl ene torches which are set to operate at apprCixila tltly 27X)deg - As 0 1 can s~e
~rature allCTJ olade has gt~en ~l~i ~ilc the ~eaic and cerara l
blamp are un ged ceraal blade however gtoss es s es -_~a thr lec-anical
shock parti cularl y at ele7ated teIper atues e _et a c onten t
er~ls -J ccns ide to oe sui tabl e for sanr hih- teJgte rature
aDDlicati provided that the craic and ~tal ccnstit~nts aT be
ded s~ccess fally tensive bvesti~tions are IDc iTa here to 1ete ri1e
the Cas ie factors affectinz the bonding a=d s~t-e s t1~ we t tng of the laquo
cerazric and th tal Toois such as elctrCfl- ifra~ticn irs tr-nn~s Le
1CTftd to de the na t ure of the la eS eYistin on the siTface of the
rticles cit e up the cera=al otoicro-ra-hs a I cbtaind
at opt ical gnificatims up to 15)) diaeters to stu7 the rti cles and
the er in which they oond ieraD4ls are relatively nw terlals but
~middot lr-a thev have shOllD eJcellen t Iva ted te shy pera tUIs d we shall c Jill to inv~sti~ate he as rapmiddotdly as possille
~
laquo
~
lt
~
-
~Cials rct have 2sirable_higt- te_ Ie c~s
10 4 used ~caU8~ hav~ Cor - c_ onatioo properti~s
In cr~r to v~r -hs isa
a ti1s d~veb~d wi fu plusmn~ inac al a5ss tance ani Imd~rrotec~ive c~ra=ic
t~~ s~nsors~i 0 tee IvS~ ~I ati 7Ial ~~au ~
f the orote~ti thus aifcrd is Ll the nezt de=O-tsta~on ~~ we
to ~~ has cen ivn ilave two cars f
rot-=~tiV~ c ir n tho a JPlca ton 0 --a~e ~i~zng
~ a~ lIi L
1~ 1P- notic~ ta t th~ bc~ ~a t has not ~~n s
r sLlts the caials rOlf il ~ ~ccain~ porJS ard ~S~~ its str~nmiddot-
The oth~r bar as lOll will see la~r has r~taine s shdpe and has su~ red
no apparent loss in str~n~th
_rtlJ~lr L h~~~rtt a~va ~e in ce=-aic and c~ra-a -verials s J-er
1 s ~-r tie s ~rial9 or hi7h- te3prature applcatioos haV
s~ci~ic 6a7it s r~pounding to 8 er alicJ he o ~r hand have
spe~i~i~ Era~ite s ralging ro~ 2 to 5 and are in~ ~~=iate with
speci ic =-ra~~izs tl n ce rr- to 7 TIris r ~T 7S in two VJI7
desiraSl e e~e~t3 First th~ e of cer ltllCS or era-als wcJlc r edu=e
~th~ r - all f e aircraft propulsi31 S7Sve ~cor ~ or
appli cati ons wtore he s ss is d~ t~ned i C~- tr -al o~e or
Axalpl tllbin~ ~lad~s th~ stss Will ~ lm~ ~~or t~ l~ --n-rr r t~rials
middot t is thlS not n~c~ssar- or t -tra l to Je ~1~ as hi~
stresss be ~rial can siad oJ cccause its s~ _i ~ht r tio is
hih
ro
~
~
- gt shy
~ ~arlr a rtP-pts to lSe c~ral cs lI~ ~ari9~ ~ ~ Oor t~Ilal
s~ ~~~~~r i e s 0 ~~~s~ ~tera~s l thol~ ES e c~~ot elual th~
~
ad __ S10c prc~~rt~s o ~ I s las i r07~Il-JS ~a1 dd d ve ~~nt~~Ci~
in the ~~ ~21 s~ ~i ~~~~~ tie 9 ~ c~ rcLics or exa b the ~1l-1n nm
a se nver5OS ~ zi~c ~ ~ ~ u~ S lp~eSS~ ~ ~7 D r r a i1itions of
-J ~~ 3 a~s =J-ov~~ ~~~r7z1 soc~ C ~t~ s -c ci- strate J
in e-is l_r rae c~ a~ 55 at ) )~p ~ ~~ ar lsn~hin~ W~ notic~
t ~ac s~~ter illus at~ t~~t ~~v~ ~~~~~l
shy r -)~r -= s can re Ecmiddoted in cara- i c a ~als ac -a arial ~
~~~~ c ~s -~7al sX I r~3 isa1ce ar =- 5 t~e ~3e c t t ha t 1ie
r~ _r~st ~a ~ ~~~
~ ~ f_ ~iatv__ 0 -_ s ~ En ii ~i lt hshy ~-r sap s 7~ ~
- - ___ r r- _J _ _ C1 ~ oJ c J ~ ~ is a ~- ~lj O~ 2middot1a w t- the n~1J
~~iU~3 r~ ~~3~ -lt J ~ a ~w -a~rial _n-3 a~ _ isola- a
~ L~~3-~l- s-t~ ~d ~1~n~ - r ts w~c ~~l~ _ ~n a ~~~a~d ro
~~~~~c =a~~~als -es~ rs 3~ ot ngc~ssail- d~v~ 10~i to t~ Oint
-middot~h~re -~~ 1till ~_ sta~ 1gt1 ~ ~1 2 L1 ~ ~ra~O middotJJt th~r 10 indicat~
lt h~ f~~s i lt middot ~ ~~~~~in- ~~rts fro c ~ a ~~ ~ ~ -~ 15 - LlJ ~n~ral
i- -_ - shyOv~ __ -L_ fa ~ ~~ ~a~~ tr= _ _ ~ t~s - cc s~s -~ C3stin 7
s~-ri -j C ~3 _= ~1- 3~ ~s 1~1 ~ _ e lasi - la-e
~~~-lt 3O ~ r~~ ~2 pl i _ - ~s a~ =-1 this -- ~-~ ~ 2~e _~tho shy ziss o~ ~~ ~ 1 -~~ -a t rJ 2r O O~ a~j s l~r-alte r
~ l_5 S1OW1 ~~ rJ tis th lL _- o~ aMcatin~e
__ J t a - i3 a ~ )ir -- )l bull -~ - -rs~ C~ ~~iallj7 ~ir~ ~te-
lr i~i - ~n- f=~ ish ~~~in~ ~-s rl middot -Lpl icates tal
- a l cO3~~~~tlJ ~aciliti~5 c~ ~aailr a7~labl~
~ I
- 6 shy
sla Yaae8 turbotrupsrcbarger buck-ta an I-ul tshOllll ell ~
1 er __ in th1a
III ccmclaiCD we are iJlTe8t1gating the oasic soects of ratP-rials or
in aircraft iDclul alloys cellbics an1 + terial a comiddot
biDatiCD of _tal8 and ceramics called ceraaals
t
bull
~
1
1~
I
8S VIBRAlIOH EIFIElT PCR FIRS ~mUAL nSPPpoundTIO
October 8 9 and 10 1947 by S S Manson
DnROWCTICN
In an aircraft engine ~ 19bt st be combined with abeomte inshy
euranee against structural failure _ An iaportant phase of the research at
e IMA is therefore the determination of the criteria for structural
failure and a search for the _tllOds tomiddot increase the life of an engine while
the S8IIe tille reducing its weight and increasing its eftic1enC7 and power
output This phase of the research is known as stress and Vibration I
all l1A1t r ks to those aspects of the research relating to turbine
disks and turbine and coaresBor blades
TtRBIIE DIS
In turbine disks we are ccncerned with t major stress problelll8 The
irst of these 18 ria cracking which ico~n in disks in which the blades
are welded to the wheel It has been found that in such disks cracks occur
at the bases between the blades after periods ot operation Dch shorter than
bulluld ordinarily be c)osidered the reasonable Ute o t~ wheel Analytical
research has linked these cracks with high thelllal stresses due to hot -
operation plastic low that results froJ the high therDa1 stresses and a
tr~ss concentration inherent at the ba~e of tmiddothe blades Here is the apshy
p-ox1ate length of the cracks present of the blades of the disk
n the disk was removed froa service It was considered that this was a
dapgeroll8 length he Gna1rtical research indicated that it wuld be possible
to ~opagate the cracks bJ the ap l1cation ot successive heating and cooling I
cycles and here are BOI8 of the rcpagated cracks obtained by such crcles
ot tbeJlOtent1a1 eolutlol18 indicated by t~e analysis is the raval ot
Cf3
-- - --- shy
- 2 shy
bull
the stress concentration ~ drilling II holes at the bases ot the blades (
Pere are some cf the holes that were drilled prior to the aplicat ion of tne
heating cyc les and it will be seen that very few cracks propagated beyond
the holes The Derit of this type of solution has yet to be further tested
and we are building large spin ~its mere disks such as these will be able
to be tested under conditions of full speed and temperature gradient These
ts will also be used to middottest the cerit of a number of other indicated
lutions
The second problem associ ated with disks is that of disk burstingbull
Di9k bursting has occurred in practice but one of the cajor r easons f or
studying it is the desire to reduce the weight of the lIheel a step that
increase the number of this type of failure The results ot a pre1ia1nary
investigation of disk bursting are shown on this panel Here we were studying ~
he ef fect of ductility or the amount of stretch that the _ terial is capble
of withstanding without ruptm-e Here is a disk with a VI high ductility
Characteristic of its fracture are ~he low nucber of failed pieces and the
o fact that the lane of fracture is inclined at an angle of 45 to t he thickshy
ness of the disk As we decrease the ductility the nuber of fractured
pieces increases and t he plane I)f fr acture is perpendicular to thickness
of the disk The problem requ ires consider able additional- investigation and th~ pit s t hat will be used for t he r im cracking investigations will also
be used for testineuro ge disks such as shown on the other panel in disk bursting investigationsbull
)UMiDUSCOPIC VTIIUlIO
I should like to leaTe now the subject ot turbine disks and go on to
-
if
- 3 shy
r and turbine blades In this case we are concerned with blade
V1bration Vibration is a DOYeDent back and torth or the blade which re-
Its in aGme c in critical stress and fracture of the blade I t is
treacherous type of stress condition f irst because at any one time the
rese may DOt ~ great enough to campuae fracture but over a period of time
the ac lated e cause fracture wit hout nrning It is a l so
treacberou because so little is Imom about the causes for blade vitI-ation
~ ~ It fIl17 be present in engines but not in others and in any one engine r
be Jresent under SOlIe conditions but not under others It has taken
a good deal of research to gain eYen an e ntar understanding or blade
vibration
UJt _ dsonstrate a blade in a condition or vibration - Here is a
J
blade which has vibrational characteristics quite similar to t ho se of t urshy
l bine COIltressor blades except that i t is constructed to a JlUch larger
scale tban orcl1nary blades Connected to the end of the blade is an
electronic exc iter br which can vary the excttation llIIpulses until t he
natural frequency of the blade is r eached The blade will t hen go irto a
bullcondition of vitration The vibration i s too r apid to view with t he naked
and _ therefore uae stroboscopic light to stuctr it This light flickers
on and off at apJrOx1ateq the s frequency as t he blade vi
~ therefore JUkes the blAde appear to be standing still or to vi brate slowl y-
while in reality- i t is 1brati~ verf rap~
ltI
vibration 1Ou have seen is a verf simple t~ of vibr ation At any-
point along the length of the blade the entire section r e l y moving up
and down re are other IlUcb more complicated types of vibration and 0
IS
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
- 2 shybull
tho~ 57 rtich b~ r~sista~ce to te3 ra-~ ext~Ies can
An ~~ple of thipaSQ is bv the lSe of ma~rials tbat (an ~ cooea
+_ nAv7 ri bull rTlctaticn i~ Iis sh
ampis ar~al w~c fahLcated to
s you can see tbe oxy-ac etl~n~ fla=Je has h~atedIgt nave 0 ~rcen t porosit7
~ now ~ir~ct ~~ ai~ str~a~ ~~t~ a n~a1er or holethe block to a ~d ~ L
A
38 of an nch in dia1~~r thit has ooen 1illed into ti1c blocl bull
orcsi ty in tr~ bloc~ will liSr3 and conllct t~ air streaa in suct a
~r as efecti~ ccolin
c~ral3l ~ s can e readi faorcated Wit1 al~cs t atr des
e of )or os a~-als i s tia t of
s trerth is
ro~le ~ is also ~d~r in~st~~ticn bull
oOtai~i-1( hi~h ~orosi vj hil~ retainl hi
c )1 ~on ~l tshy
i t is natural to turn t rials lavi1
f r )sitr
a1ts aes i ners
in
~ Vt -rj hir~st ltelting oil ts bull hese aaterials ar~ hih-meltL1~-fOIf
tal such a s tlmgsten and ao17odem and the oT1ies nitri~s carbi des
ani bO~ce3 0 ll~ tdl ~is latter grOU ar~ c~l1~d c~ra ~c~ bull
teJ~ra tre scale along the top 0 this oa~l has on i t sClll~ 0 r UlII
i th 1rhic ~ 1 ir
res~ctive red
or t~ ~ry
of tn ra tutlS t
stress calliti
crart we can see in
~
~
~
~
bull
- J shy
aJPraxiJlaUily 24000 F These c~raric terials bein cClls -je r~d run fr
this paint uprar d to carbide at 7JX)deg
In o r to illustrate raphi~ally soe fa~ tors 12t nt-r in the J
perfOlllaIlce of materials I have hre a Sii1Jla~d mt~el se~~nt on whch
thre~ turbine blades bull fi r s t on~ 5 abrica ted r (]]l a typi cal
hi~h-teaperatilre al loy the s econd one is a pure c~ralic terial and t~
third one is a tal-bon~ed cera~c t eria l which p- have te~d a cer best c inatl oos ot pure ceraric Jrials for high- tezperature use in
turbines ve be~ 1evelo~d by the at i cnal eau ~ ~ ds middotmder
ccntract to the bull e now pass the wheel se=l~ t h=ough the oxy- ace t yl ene torches which are set to operate at apprCixila tltly 27X)deg - As 0 1 can s~e
~rature allCTJ olade has gt~en ~l~i ~ilc the ~eaic and cerara l
blamp are un ged ceraal blade however gtoss es s es -_~a thr lec-anical
shock parti cularl y at ele7ated teIper atues e _et a c onten t
er~ls -J ccns ide to oe sui tabl e for sanr hih- teJgte rature
aDDlicati provided that the craic and ~tal ccnstit~nts aT be
ded s~ccess fally tensive bvesti~tions are IDc iTa here to 1ete ri1e
the Cas ie factors affectinz the bonding a=d s~t-e s t1~ we t tng of the laquo
cerazric and th tal Toois such as elctrCfl- ifra~ticn irs tr-nn~s Le
1CTftd to de the na t ure of the la eS eYistin on the siTface of the
rticles cit e up the cera=al otoicro-ra-hs a I cbtaind
at opt ical gnificatims up to 15)) diaeters to stu7 the rti cles and
the er in which they oond ieraD4ls are relatively nw terlals but
~middot lr-a thev have shOllD eJcellen t Iva ted te shy pera tUIs d we shall c Jill to inv~sti~ate he as rapmiddotdly as possille
~
laquo
~
lt
~
-
~Cials rct have 2sirable_higt- te_ Ie c~s
10 4 used ~caU8~ hav~ Cor - c_ onatioo properti~s
In cr~r to v~r -hs isa
a ti1s d~veb~d wi fu plusmn~ inac al a5ss tance ani Imd~rrotec~ive c~ra=ic
t~~ s~nsors~i 0 tee IvS~ ~I ati 7Ial ~~au ~
f the orote~ti thus aifcrd is Ll the nezt de=O-tsta~on ~~ we
to ~~ has cen ivn ilave two cars f
rot-=~tiV~ c ir n tho a JPlca ton 0 --a~e ~i~zng
~ a~ lIi L
1~ 1P- notic~ ta t th~ bc~ ~a t has not ~~n s
r sLlts the caials rOlf il ~ ~ccain~ porJS ard ~S~~ its str~nmiddot-
The oth~r bar as lOll will see la~r has r~taine s shdpe and has su~ red
no apparent loss in str~n~th
_rtlJ~lr L h~~~rtt a~va ~e in ce=-aic and c~ra-a -verials s J-er
1 s ~-r tie s ~rial9 or hi7h- te3prature applcatioos haV
s~ci~ic 6a7it s r~pounding to 8 er alicJ he o ~r hand have
spe~i~i~ Era~ite s ralging ro~ 2 to 5 and are in~ ~~=iate with
speci ic =-ra~~izs tl n ce rr- to 7 TIris r ~T 7S in two VJI7
desiraSl e e~e~t3 First th~ e of cer ltllCS or era-als wcJlc r edu=e
~th~ r - all f e aircraft propulsi31 S7Sve ~cor ~ or
appli cati ons wtore he s ss is d~ t~ned i C~- tr -al o~e or
Axalpl tllbin~ ~lad~s th~ stss Will ~ lm~ ~~or t~ l~ --n-rr r t~rials
middot t is thlS not n~c~ssar- or t -tra l to Je ~1~ as hi~
stresss be ~rial can siad oJ cccause its s~ _i ~ht r tio is
hih
ro
~
~
- gt shy
~ ~arlr a rtP-pts to lSe c~ral cs lI~ ~ari9~ ~ ~ Oor t~Ilal
s~ ~~~~~r i e s 0 ~~~s~ ~tera~s l thol~ ES e c~~ot elual th~
~
ad __ S10c prc~~rt~s o ~ I s las i r07~Il-JS ~a1 dd d ve ~~nt~~Ci~
in the ~~ ~21 s~ ~i ~~~~~ tie 9 ~ c~ rcLics or exa b the ~1l-1n nm
a se nver5OS ~ zi~c ~ ~ ~ u~ S lp~eSS~ ~ ~7 D r r a i1itions of
-J ~~ 3 a~s =J-ov~~ ~~~r7z1 soc~ C ~t~ s -c ci- strate J
in e-is l_r rae c~ a~ 55 at ) )~p ~ ~~ ar lsn~hin~ W~ notic~
t ~ac s~~ter illus at~ t~~t ~~v~ ~~~~~l
shy r -)~r -= s can re Ecmiddoted in cara- i c a ~als ac -a arial ~
~~~~ c ~s -~7al sX I r~3 isa1ce ar =- 5 t~e ~3e c t t ha t 1ie
r~ _r~st ~a ~ ~~~
~ ~ f_ ~iatv__ 0 -_ s ~ En ii ~i lt hshy ~-r sap s 7~ ~
- - ___ r r- _J _ _ C1 ~ oJ c J ~ ~ is a ~- ~lj O~ 2middot1a w t- the n~1J
~~iU~3 r~ ~~3~ -lt J ~ a ~w -a~rial _n-3 a~ _ isola- a
~ L~~3-~l- s-t~ ~d ~1~n~ - r ts w~c ~~l~ _ ~n a ~~~a~d ro
~~~~~c =a~~~als -es~ rs 3~ ot ngc~ssail- d~v~ 10~i to t~ Oint
-middot~h~re -~~ 1till ~_ sta~ 1gt1 ~ ~1 2 L1 ~ ~ra~O middotJJt th~r 10 indicat~
lt h~ f~~s i lt middot ~ ~~~~~in- ~~rts fro c ~ a ~~ ~ ~ -~ 15 - LlJ ~n~ral
i- -_ - shyOv~ __ -L_ fa ~ ~~ ~a~~ tr= _ _ ~ t~s - cc s~s -~ C3stin 7
s~-ri -j C ~3 _= ~1- 3~ ~s 1~1 ~ _ e lasi - la-e
~~~-lt 3O ~ r~~ ~2 pl i _ - ~s a~ =-1 this -- ~-~ ~ 2~e _~tho shy ziss o~ ~~ ~ 1 -~~ -a t rJ 2r O O~ a~j s l~r-alte r
~ l_5 S1OW1 ~~ rJ tis th lL _- o~ aMcatin~e
__ J t a - i3 a ~ )ir -- )l bull -~ - -rs~ C~ ~~iallj7 ~ir~ ~te-
lr i~i - ~n- f=~ ish ~~~in~ ~-s rl middot -Lpl icates tal
- a l cO3~~~~tlJ ~aciliti~5 c~ ~aailr a7~labl~
~ I
- 6 shy
sla Yaae8 turbotrupsrcbarger buck-ta an I-ul tshOllll ell ~
1 er __ in th1a
III ccmclaiCD we are iJlTe8t1gating the oasic soects of ratP-rials or
in aircraft iDclul alloys cellbics an1 + terial a comiddot
biDatiCD of _tal8 and ceramics called ceraaals
t
bull
~
1
1~
I
8S VIBRAlIOH EIFIElT PCR FIRS ~mUAL nSPPpoundTIO
October 8 9 and 10 1947 by S S Manson
DnROWCTICN
In an aircraft engine ~ 19bt st be combined with abeomte inshy
euranee against structural failure _ An iaportant phase of the research at
e IMA is therefore the determination of the criteria for structural
failure and a search for the _tllOds tomiddot increase the life of an engine while
the S8IIe tille reducing its weight and increasing its eftic1enC7 and power
output This phase of the research is known as stress and Vibration I
all l1A1t r ks to those aspects of the research relating to turbine
disks and turbine and coaresBor blades
TtRBIIE DIS
In turbine disks we are ccncerned with t major stress problelll8 The
irst of these 18 ria cracking which ico~n in disks in which the blades
are welded to the wheel It has been found that in such disks cracks occur
at the bases between the blades after periods ot operation Dch shorter than
bulluld ordinarily be c)osidered the reasonable Ute o t~ wheel Analytical
research has linked these cracks with high thelllal stresses due to hot -
operation plastic low that results froJ the high therDa1 stresses and a
tr~ss concentration inherent at the ba~e of tmiddothe blades Here is the apshy
p-ox1ate length of the cracks present of the blades of the disk
n the disk was removed froa service It was considered that this was a
dapgeroll8 length he Gna1rtical research indicated that it wuld be possible
to ~opagate the cracks bJ the ap l1cation ot successive heating and cooling I
cycles and here are BOI8 of the rcpagated cracks obtained by such crcles
ot tbeJlOtent1a1 eolutlol18 indicated by t~e analysis is the raval ot
Cf3
-- - --- shy
- 2 shy
bull
the stress concentration ~ drilling II holes at the bases ot the blades (
Pere are some cf the holes that were drilled prior to the aplicat ion of tne
heating cyc les and it will be seen that very few cracks propagated beyond
the holes The Derit of this type of solution has yet to be further tested
and we are building large spin ~its mere disks such as these will be able
to be tested under conditions of full speed and temperature gradient These
ts will also be used to middottest the cerit of a number of other indicated
lutions
The second problem associ ated with disks is that of disk burstingbull
Di9k bursting has occurred in practice but one of the cajor r easons f or
studying it is the desire to reduce the weight of the lIheel a step that
increase the number of this type of failure The results ot a pre1ia1nary
investigation of disk bursting are shown on this panel Here we were studying ~
he ef fect of ductility or the amount of stretch that the _ terial is capble
of withstanding without ruptm-e Here is a disk with a VI high ductility
Characteristic of its fracture are ~he low nucber of failed pieces and the
o fact that the lane of fracture is inclined at an angle of 45 to t he thickshy
ness of the disk As we decrease the ductility the nuber of fractured
pieces increases and t he plane I)f fr acture is perpendicular to thickness
of the disk The problem requ ires consider able additional- investigation and th~ pit s t hat will be used for t he r im cracking investigations will also
be used for testineuro ge disks such as shown on the other panel in disk bursting investigationsbull
)UMiDUSCOPIC VTIIUlIO
I should like to leaTe now the subject ot turbine disks and go on to
-
if
- 3 shy
r and turbine blades In this case we are concerned with blade
V1bration Vibration is a DOYeDent back and torth or the blade which re-
Its in aGme c in critical stress and fracture of the blade I t is
treacherous type of stress condition f irst because at any one time the
rese may DOt ~ great enough to campuae fracture but over a period of time
the ac lated e cause fracture wit hout nrning It is a l so
treacberou because so little is Imom about the causes for blade vitI-ation
~ ~ It fIl17 be present in engines but not in others and in any one engine r
be Jresent under SOlIe conditions but not under others It has taken
a good deal of research to gain eYen an e ntar understanding or blade
vibration
UJt _ dsonstrate a blade in a condition or vibration - Here is a
J
blade which has vibrational characteristics quite similar to t ho se of t urshy
l bine COIltressor blades except that i t is constructed to a JlUch larger
scale tban orcl1nary blades Connected to the end of the blade is an
electronic exc iter br which can vary the excttation llIIpulses until t he
natural frequency of the blade is r eached The blade will t hen go irto a
bullcondition of vitration The vibration i s too r apid to view with t he naked
and _ therefore uae stroboscopic light to stuctr it This light flickers
on and off at apJrOx1ateq the s frequency as t he blade vi
~ therefore JUkes the blAde appear to be standing still or to vi brate slowl y-
while in reality- i t is 1brati~ verf rap~
ltI
vibration 1Ou have seen is a verf simple t~ of vibr ation At any-
point along the length of the blade the entire section r e l y moving up
and down re are other IlUcb more complicated types of vibration and 0
IS
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
bull
- J shy
aJPraxiJlaUily 24000 F These c~raric terials bein cClls -je r~d run fr
this paint uprar d to carbide at 7JX)deg
In o r to illustrate raphi~ally soe fa~ tors 12t nt-r in the J
perfOlllaIlce of materials I have hre a Sii1Jla~d mt~el se~~nt on whch
thre~ turbine blades bull fi r s t on~ 5 abrica ted r (]]l a typi cal
hi~h-teaperatilre al loy the s econd one is a pure c~ralic terial and t~
third one is a tal-bon~ed cera~c t eria l which p- have te~d a cer best c inatl oos ot pure ceraric Jrials for high- tezperature use in
turbines ve be~ 1evelo~d by the at i cnal eau ~ ~ ds middotmder
ccntract to the bull e now pass the wheel se=l~ t h=ough the oxy- ace t yl ene torches which are set to operate at apprCixila tltly 27X)deg - As 0 1 can s~e
~rature allCTJ olade has gt~en ~l~i ~ilc the ~eaic and cerara l
blamp are un ged ceraal blade however gtoss es s es -_~a thr lec-anical
shock parti cularl y at ele7ated teIper atues e _et a c onten t
er~ls -J ccns ide to oe sui tabl e for sanr hih- teJgte rature
aDDlicati provided that the craic and ~tal ccnstit~nts aT be
ded s~ccess fally tensive bvesti~tions are IDc iTa here to 1ete ri1e
the Cas ie factors affectinz the bonding a=d s~t-e s t1~ we t tng of the laquo
cerazric and th tal Toois such as elctrCfl- ifra~ticn irs tr-nn~s Le
1CTftd to de the na t ure of the la eS eYistin on the siTface of the
rticles cit e up the cera=al otoicro-ra-hs a I cbtaind
at opt ical gnificatims up to 15)) diaeters to stu7 the rti cles and
the er in which they oond ieraD4ls are relatively nw terlals but
~middot lr-a thev have shOllD eJcellen t Iva ted te shy pera tUIs d we shall c Jill to inv~sti~ate he as rapmiddotdly as possille
~
laquo
~
lt
~
-
~Cials rct have 2sirable_higt- te_ Ie c~s
10 4 used ~caU8~ hav~ Cor - c_ onatioo properti~s
In cr~r to v~r -hs isa
a ti1s d~veb~d wi fu plusmn~ inac al a5ss tance ani Imd~rrotec~ive c~ra=ic
t~~ s~nsors~i 0 tee IvS~ ~I ati 7Ial ~~au ~
f the orote~ti thus aifcrd is Ll the nezt de=O-tsta~on ~~ we
to ~~ has cen ivn ilave two cars f
rot-=~tiV~ c ir n tho a JPlca ton 0 --a~e ~i~zng
~ a~ lIi L
1~ 1P- notic~ ta t th~ bc~ ~a t has not ~~n s
r sLlts the caials rOlf il ~ ~ccain~ porJS ard ~S~~ its str~nmiddot-
The oth~r bar as lOll will see la~r has r~taine s shdpe and has su~ red
no apparent loss in str~n~th
_rtlJ~lr L h~~~rtt a~va ~e in ce=-aic and c~ra-a -verials s J-er
1 s ~-r tie s ~rial9 or hi7h- te3prature applcatioos haV
s~ci~ic 6a7it s r~pounding to 8 er alicJ he o ~r hand have
spe~i~i~ Era~ite s ralging ro~ 2 to 5 and are in~ ~~=iate with
speci ic =-ra~~izs tl n ce rr- to 7 TIris r ~T 7S in two VJI7
desiraSl e e~e~t3 First th~ e of cer ltllCS or era-als wcJlc r edu=e
~th~ r - all f e aircraft propulsi31 S7Sve ~cor ~ or
appli cati ons wtore he s ss is d~ t~ned i C~- tr -al o~e or
Axalpl tllbin~ ~lad~s th~ stss Will ~ lm~ ~~or t~ l~ --n-rr r t~rials
middot t is thlS not n~c~ssar- or t -tra l to Je ~1~ as hi~
stresss be ~rial can siad oJ cccause its s~ _i ~ht r tio is
hih
ro
~
~
- gt shy
~ ~arlr a rtP-pts to lSe c~ral cs lI~ ~ari9~ ~ ~ Oor t~Ilal
s~ ~~~~~r i e s 0 ~~~s~ ~tera~s l thol~ ES e c~~ot elual th~
~
ad __ S10c prc~~rt~s o ~ I s las i r07~Il-JS ~a1 dd d ve ~~nt~~Ci~
in the ~~ ~21 s~ ~i ~~~~~ tie 9 ~ c~ rcLics or exa b the ~1l-1n nm
a se nver5OS ~ zi~c ~ ~ ~ u~ S lp~eSS~ ~ ~7 D r r a i1itions of
-J ~~ 3 a~s =J-ov~~ ~~~r7z1 soc~ C ~t~ s -c ci- strate J
in e-is l_r rae c~ a~ 55 at ) )~p ~ ~~ ar lsn~hin~ W~ notic~
t ~ac s~~ter illus at~ t~~t ~~v~ ~~~~~l
shy r -)~r -= s can re Ecmiddoted in cara- i c a ~als ac -a arial ~
~~~~ c ~s -~7al sX I r~3 isa1ce ar =- 5 t~e ~3e c t t ha t 1ie
r~ _r~st ~a ~ ~~~
~ ~ f_ ~iatv__ 0 -_ s ~ En ii ~i lt hshy ~-r sap s 7~ ~
- - ___ r r- _J _ _ C1 ~ oJ c J ~ ~ is a ~- ~lj O~ 2middot1a w t- the n~1J
~~iU~3 r~ ~~3~ -lt J ~ a ~w -a~rial _n-3 a~ _ isola- a
~ L~~3-~l- s-t~ ~d ~1~n~ - r ts w~c ~~l~ _ ~n a ~~~a~d ro
~~~~~c =a~~~als -es~ rs 3~ ot ngc~ssail- d~v~ 10~i to t~ Oint
-middot~h~re -~~ 1till ~_ sta~ 1gt1 ~ ~1 2 L1 ~ ~ra~O middotJJt th~r 10 indicat~
lt h~ f~~s i lt middot ~ ~~~~~in- ~~rts fro c ~ a ~~ ~ ~ -~ 15 - LlJ ~n~ral
i- -_ - shyOv~ __ -L_ fa ~ ~~ ~a~~ tr= _ _ ~ t~s - cc s~s -~ C3stin 7
s~-ri -j C ~3 _= ~1- 3~ ~s 1~1 ~ _ e lasi - la-e
~~~-lt 3O ~ r~~ ~2 pl i _ - ~s a~ =-1 this -- ~-~ ~ 2~e _~tho shy ziss o~ ~~ ~ 1 -~~ -a t rJ 2r O O~ a~j s l~r-alte r
~ l_5 S1OW1 ~~ rJ tis th lL _- o~ aMcatin~e
__ J t a - i3 a ~ )ir -- )l bull -~ - -rs~ C~ ~~iallj7 ~ir~ ~te-
lr i~i - ~n- f=~ ish ~~~in~ ~-s rl middot -Lpl icates tal
- a l cO3~~~~tlJ ~aciliti~5 c~ ~aailr a7~labl~
~ I
- 6 shy
sla Yaae8 turbotrupsrcbarger buck-ta an I-ul tshOllll ell ~
1 er __ in th1a
III ccmclaiCD we are iJlTe8t1gating the oasic soects of ratP-rials or
in aircraft iDclul alloys cellbics an1 + terial a comiddot
biDatiCD of _tal8 and ceramics called ceraaals
t
bull
~
1
1~
I
8S VIBRAlIOH EIFIElT PCR FIRS ~mUAL nSPPpoundTIO
October 8 9 and 10 1947 by S S Manson
DnROWCTICN
In an aircraft engine ~ 19bt st be combined with abeomte inshy
euranee against structural failure _ An iaportant phase of the research at
e IMA is therefore the determination of the criteria for structural
failure and a search for the _tllOds tomiddot increase the life of an engine while
the S8IIe tille reducing its weight and increasing its eftic1enC7 and power
output This phase of the research is known as stress and Vibration I
all l1A1t r ks to those aspects of the research relating to turbine
disks and turbine and coaresBor blades
TtRBIIE DIS
In turbine disks we are ccncerned with t major stress problelll8 The
irst of these 18 ria cracking which ico~n in disks in which the blades
are welded to the wheel It has been found that in such disks cracks occur
at the bases between the blades after periods ot operation Dch shorter than
bulluld ordinarily be c)osidered the reasonable Ute o t~ wheel Analytical
research has linked these cracks with high thelllal stresses due to hot -
operation plastic low that results froJ the high therDa1 stresses and a
tr~ss concentration inherent at the ba~e of tmiddothe blades Here is the apshy
p-ox1ate length of the cracks present of the blades of the disk
n the disk was removed froa service It was considered that this was a
dapgeroll8 length he Gna1rtical research indicated that it wuld be possible
to ~opagate the cracks bJ the ap l1cation ot successive heating and cooling I
cycles and here are BOI8 of the rcpagated cracks obtained by such crcles
ot tbeJlOtent1a1 eolutlol18 indicated by t~e analysis is the raval ot
Cf3
-- - --- shy
- 2 shy
bull
the stress concentration ~ drilling II holes at the bases ot the blades (
Pere are some cf the holes that were drilled prior to the aplicat ion of tne
heating cyc les and it will be seen that very few cracks propagated beyond
the holes The Derit of this type of solution has yet to be further tested
and we are building large spin ~its mere disks such as these will be able
to be tested under conditions of full speed and temperature gradient These
ts will also be used to middottest the cerit of a number of other indicated
lutions
The second problem associ ated with disks is that of disk burstingbull
Di9k bursting has occurred in practice but one of the cajor r easons f or
studying it is the desire to reduce the weight of the lIheel a step that
increase the number of this type of failure The results ot a pre1ia1nary
investigation of disk bursting are shown on this panel Here we were studying ~
he ef fect of ductility or the amount of stretch that the _ terial is capble
of withstanding without ruptm-e Here is a disk with a VI high ductility
Characteristic of its fracture are ~he low nucber of failed pieces and the
o fact that the lane of fracture is inclined at an angle of 45 to t he thickshy
ness of the disk As we decrease the ductility the nuber of fractured
pieces increases and t he plane I)f fr acture is perpendicular to thickness
of the disk The problem requ ires consider able additional- investigation and th~ pit s t hat will be used for t he r im cracking investigations will also
be used for testineuro ge disks such as shown on the other panel in disk bursting investigationsbull
)UMiDUSCOPIC VTIIUlIO
I should like to leaTe now the subject ot turbine disks and go on to
-
if
- 3 shy
r and turbine blades In this case we are concerned with blade
V1bration Vibration is a DOYeDent back and torth or the blade which re-
Its in aGme c in critical stress and fracture of the blade I t is
treacherous type of stress condition f irst because at any one time the
rese may DOt ~ great enough to campuae fracture but over a period of time
the ac lated e cause fracture wit hout nrning It is a l so
treacberou because so little is Imom about the causes for blade vitI-ation
~ ~ It fIl17 be present in engines but not in others and in any one engine r
be Jresent under SOlIe conditions but not under others It has taken
a good deal of research to gain eYen an e ntar understanding or blade
vibration
UJt _ dsonstrate a blade in a condition or vibration - Here is a
J
blade which has vibrational characteristics quite similar to t ho se of t urshy
l bine COIltressor blades except that i t is constructed to a JlUch larger
scale tban orcl1nary blades Connected to the end of the blade is an
electronic exc iter br which can vary the excttation llIIpulses until t he
natural frequency of the blade is r eached The blade will t hen go irto a
bullcondition of vitration The vibration i s too r apid to view with t he naked
and _ therefore uae stroboscopic light to stuctr it This light flickers
on and off at apJrOx1ateq the s frequency as t he blade vi
~ therefore JUkes the blAde appear to be standing still or to vi brate slowl y-
while in reality- i t is 1brati~ verf rap~
ltI
vibration 1Ou have seen is a verf simple t~ of vibr ation At any-
point along the length of the blade the entire section r e l y moving up
and down re are other IlUcb more complicated types of vibration and 0
IS
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
laquo
~
lt
~
-
~Cials rct have 2sirable_higt- te_ Ie c~s
10 4 used ~caU8~ hav~ Cor - c_ onatioo properti~s
In cr~r to v~r -hs isa
a ti1s d~veb~d wi fu plusmn~ inac al a5ss tance ani Imd~rrotec~ive c~ra=ic
t~~ s~nsors~i 0 tee IvS~ ~I ati 7Ial ~~au ~
f the orote~ti thus aifcrd is Ll the nezt de=O-tsta~on ~~ we
to ~~ has cen ivn ilave two cars f
rot-=~tiV~ c ir n tho a JPlca ton 0 --a~e ~i~zng
~ a~ lIi L
1~ 1P- notic~ ta t th~ bc~ ~a t has not ~~n s
r sLlts the caials rOlf il ~ ~ccain~ porJS ard ~S~~ its str~nmiddot-
The oth~r bar as lOll will see la~r has r~taine s shdpe and has su~ red
no apparent loss in str~n~th
_rtlJ~lr L h~~~rtt a~va ~e in ce=-aic and c~ra-a -verials s J-er
1 s ~-r tie s ~rial9 or hi7h- te3prature applcatioos haV
s~ci~ic 6a7it s r~pounding to 8 er alicJ he o ~r hand have
spe~i~i~ Era~ite s ralging ro~ 2 to 5 and are in~ ~~=iate with
speci ic =-ra~~izs tl n ce rr- to 7 TIris r ~T 7S in two VJI7
desiraSl e e~e~t3 First th~ e of cer ltllCS or era-als wcJlc r edu=e
~th~ r - all f e aircraft propulsi31 S7Sve ~cor ~ or
appli cati ons wtore he s ss is d~ t~ned i C~- tr -al o~e or
Axalpl tllbin~ ~lad~s th~ stss Will ~ lm~ ~~or t~ l~ --n-rr r t~rials
middot t is thlS not n~c~ssar- or t -tra l to Je ~1~ as hi~
stresss be ~rial can siad oJ cccause its s~ _i ~ht r tio is
hih
ro
~
~
- gt shy
~ ~arlr a rtP-pts to lSe c~ral cs lI~ ~ari9~ ~ ~ Oor t~Ilal
s~ ~~~~~r i e s 0 ~~~s~ ~tera~s l thol~ ES e c~~ot elual th~
~
ad __ S10c prc~~rt~s o ~ I s las i r07~Il-JS ~a1 dd d ve ~~nt~~Ci~
in the ~~ ~21 s~ ~i ~~~~~ tie 9 ~ c~ rcLics or exa b the ~1l-1n nm
a se nver5OS ~ zi~c ~ ~ ~ u~ S lp~eSS~ ~ ~7 D r r a i1itions of
-J ~~ 3 a~s =J-ov~~ ~~~r7z1 soc~ C ~t~ s -c ci- strate J
in e-is l_r rae c~ a~ 55 at ) )~p ~ ~~ ar lsn~hin~ W~ notic~
t ~ac s~~ter illus at~ t~~t ~~v~ ~~~~~l
shy r -)~r -= s can re Ecmiddoted in cara- i c a ~als ac -a arial ~
~~~~ c ~s -~7al sX I r~3 isa1ce ar =- 5 t~e ~3e c t t ha t 1ie
r~ _r~st ~a ~ ~~~
~ ~ f_ ~iatv__ 0 -_ s ~ En ii ~i lt hshy ~-r sap s 7~ ~
- - ___ r r- _J _ _ C1 ~ oJ c J ~ ~ is a ~- ~lj O~ 2middot1a w t- the n~1J
~~iU~3 r~ ~~3~ -lt J ~ a ~w -a~rial _n-3 a~ _ isola- a
~ L~~3-~l- s-t~ ~d ~1~n~ - r ts w~c ~~l~ _ ~n a ~~~a~d ro
~~~~~c =a~~~als -es~ rs 3~ ot ngc~ssail- d~v~ 10~i to t~ Oint
-middot~h~re -~~ 1till ~_ sta~ 1gt1 ~ ~1 2 L1 ~ ~ra~O middotJJt th~r 10 indicat~
lt h~ f~~s i lt middot ~ ~~~~~in- ~~rts fro c ~ a ~~ ~ ~ -~ 15 - LlJ ~n~ral
i- -_ - shyOv~ __ -L_ fa ~ ~~ ~a~~ tr= _ _ ~ t~s - cc s~s -~ C3stin 7
s~-ri -j C ~3 _= ~1- 3~ ~s 1~1 ~ _ e lasi - la-e
~~~-lt 3O ~ r~~ ~2 pl i _ - ~s a~ =-1 this -- ~-~ ~ 2~e _~tho shy ziss o~ ~~ ~ 1 -~~ -a t rJ 2r O O~ a~j s l~r-alte r
~ l_5 S1OW1 ~~ rJ tis th lL _- o~ aMcatin~e
__ J t a - i3 a ~ )ir -- )l bull -~ - -rs~ C~ ~~iallj7 ~ir~ ~te-
lr i~i - ~n- f=~ ish ~~~in~ ~-s rl middot -Lpl icates tal
- a l cO3~~~~tlJ ~aciliti~5 c~ ~aailr a7~labl~
~ I
- 6 shy
sla Yaae8 turbotrupsrcbarger buck-ta an I-ul tshOllll ell ~
1 er __ in th1a
III ccmclaiCD we are iJlTe8t1gating the oasic soects of ratP-rials or
in aircraft iDclul alloys cellbics an1 + terial a comiddot
biDatiCD of _tal8 and ceramics called ceraaals
t
bull
~
1
1~
I
8S VIBRAlIOH EIFIElT PCR FIRS ~mUAL nSPPpoundTIO
October 8 9 and 10 1947 by S S Manson
DnROWCTICN
In an aircraft engine ~ 19bt st be combined with abeomte inshy
euranee against structural failure _ An iaportant phase of the research at
e IMA is therefore the determination of the criteria for structural
failure and a search for the _tllOds tomiddot increase the life of an engine while
the S8IIe tille reducing its weight and increasing its eftic1enC7 and power
output This phase of the research is known as stress and Vibration I
all l1A1t r ks to those aspects of the research relating to turbine
disks and turbine and coaresBor blades
TtRBIIE DIS
In turbine disks we are ccncerned with t major stress problelll8 The
irst of these 18 ria cracking which ico~n in disks in which the blades
are welded to the wheel It has been found that in such disks cracks occur
at the bases between the blades after periods ot operation Dch shorter than
bulluld ordinarily be c)osidered the reasonable Ute o t~ wheel Analytical
research has linked these cracks with high thelllal stresses due to hot -
operation plastic low that results froJ the high therDa1 stresses and a
tr~ss concentration inherent at the ba~e of tmiddothe blades Here is the apshy
p-ox1ate length of the cracks present of the blades of the disk
n the disk was removed froa service It was considered that this was a
dapgeroll8 length he Gna1rtical research indicated that it wuld be possible
to ~opagate the cracks bJ the ap l1cation ot successive heating and cooling I
cycles and here are BOI8 of the rcpagated cracks obtained by such crcles
ot tbeJlOtent1a1 eolutlol18 indicated by t~e analysis is the raval ot
Cf3
-- - --- shy
- 2 shy
bull
the stress concentration ~ drilling II holes at the bases ot the blades (
Pere are some cf the holes that were drilled prior to the aplicat ion of tne
heating cyc les and it will be seen that very few cracks propagated beyond
the holes The Derit of this type of solution has yet to be further tested
and we are building large spin ~its mere disks such as these will be able
to be tested under conditions of full speed and temperature gradient These
ts will also be used to middottest the cerit of a number of other indicated
lutions
The second problem associ ated with disks is that of disk burstingbull
Di9k bursting has occurred in practice but one of the cajor r easons f or
studying it is the desire to reduce the weight of the lIheel a step that
increase the number of this type of failure The results ot a pre1ia1nary
investigation of disk bursting are shown on this panel Here we were studying ~
he ef fect of ductility or the amount of stretch that the _ terial is capble
of withstanding without ruptm-e Here is a disk with a VI high ductility
Characteristic of its fracture are ~he low nucber of failed pieces and the
o fact that the lane of fracture is inclined at an angle of 45 to t he thickshy
ness of the disk As we decrease the ductility the nuber of fractured
pieces increases and t he plane I)f fr acture is perpendicular to thickness
of the disk The problem requ ires consider able additional- investigation and th~ pit s t hat will be used for t he r im cracking investigations will also
be used for testineuro ge disks such as shown on the other panel in disk bursting investigationsbull
)UMiDUSCOPIC VTIIUlIO
I should like to leaTe now the subject ot turbine disks and go on to
-
if
- 3 shy
r and turbine blades In this case we are concerned with blade
V1bration Vibration is a DOYeDent back and torth or the blade which re-
Its in aGme c in critical stress and fracture of the blade I t is
treacherous type of stress condition f irst because at any one time the
rese may DOt ~ great enough to campuae fracture but over a period of time
the ac lated e cause fracture wit hout nrning It is a l so
treacberou because so little is Imom about the causes for blade vitI-ation
~ ~ It fIl17 be present in engines but not in others and in any one engine r
be Jresent under SOlIe conditions but not under others It has taken
a good deal of research to gain eYen an e ntar understanding or blade
vibration
UJt _ dsonstrate a blade in a condition or vibration - Here is a
J
blade which has vibrational characteristics quite similar to t ho se of t urshy
l bine COIltressor blades except that i t is constructed to a JlUch larger
scale tban orcl1nary blades Connected to the end of the blade is an
electronic exc iter br which can vary the excttation llIIpulses until t he
natural frequency of the blade is r eached The blade will t hen go irto a
bullcondition of vitration The vibration i s too r apid to view with t he naked
and _ therefore uae stroboscopic light to stuctr it This light flickers
on and off at apJrOx1ateq the s frequency as t he blade vi
~ therefore JUkes the blAde appear to be standing still or to vi brate slowl y-
while in reality- i t is 1brati~ verf rap~
ltI
vibration 1Ou have seen is a verf simple t~ of vibr ation At any-
point along the length of the blade the entire section r e l y moving up
and down re are other IlUcb more complicated types of vibration and 0
IS
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
~
~
- gt shy
~ ~arlr a rtP-pts to lSe c~ral cs lI~ ~ari9~ ~ ~ Oor t~Ilal
s~ ~~~~~r i e s 0 ~~~s~ ~tera~s l thol~ ES e c~~ot elual th~
~
ad __ S10c prc~~rt~s o ~ I s las i r07~Il-JS ~a1 dd d ve ~~nt~~Ci~
in the ~~ ~21 s~ ~i ~~~~~ tie 9 ~ c~ rcLics or exa b the ~1l-1n nm
a se nver5OS ~ zi~c ~ ~ ~ u~ S lp~eSS~ ~ ~7 D r r a i1itions of
-J ~~ 3 a~s =J-ov~~ ~~~r7z1 soc~ C ~t~ s -c ci- strate J
in e-is l_r rae c~ a~ 55 at ) )~p ~ ~~ ar lsn~hin~ W~ notic~
t ~ac s~~ter illus at~ t~~t ~~v~ ~~~~~l
shy r -)~r -= s can re Ecmiddoted in cara- i c a ~als ac -a arial ~
~~~~ c ~s -~7al sX I r~3 isa1ce ar =- 5 t~e ~3e c t t ha t 1ie
r~ _r~st ~a ~ ~~~
~ ~ f_ ~iatv__ 0 -_ s ~ En ii ~i lt hshy ~-r sap s 7~ ~
- - ___ r r- _J _ _ C1 ~ oJ c J ~ ~ is a ~- ~lj O~ 2middot1a w t- the n~1J
~~iU~3 r~ ~~3~ -lt J ~ a ~w -a~rial _n-3 a~ _ isola- a
~ L~~3-~l- s-t~ ~d ~1~n~ - r ts w~c ~~l~ _ ~n a ~~~a~d ro
~~~~~c =a~~~als -es~ rs 3~ ot ngc~ssail- d~v~ 10~i to t~ Oint
-middot~h~re -~~ 1till ~_ sta~ 1gt1 ~ ~1 2 L1 ~ ~ra~O middotJJt th~r 10 indicat~
lt h~ f~~s i lt middot ~ ~~~~~in- ~~rts fro c ~ a ~~ ~ ~ -~ 15 - LlJ ~n~ral
i- -_ - shyOv~ __ -L_ fa ~ ~~ ~a~~ tr= _ _ ~ t~s - cc s~s -~ C3stin 7
s~-ri -j C ~3 _= ~1- 3~ ~s 1~1 ~ _ e lasi - la-e
~~~-lt 3O ~ r~~ ~2 pl i _ - ~s a~ =-1 this -- ~-~ ~ 2~e _~tho shy ziss o~ ~~ ~ 1 -~~ -a t rJ 2r O O~ a~j s l~r-alte r
~ l_5 S1OW1 ~~ rJ tis th lL _- o~ aMcatin~e
__ J t a - i3 a ~ )ir -- )l bull -~ - -rs~ C~ ~~iallj7 ~ir~ ~te-
lr i~i - ~n- f=~ ish ~~~in~ ~-s rl middot -Lpl icates tal
- a l cO3~~~~tlJ ~aciliti~5 c~ ~aailr a7~labl~
~ I
- 6 shy
sla Yaae8 turbotrupsrcbarger buck-ta an I-ul tshOllll ell ~
1 er __ in th1a
III ccmclaiCD we are iJlTe8t1gating the oasic soects of ratP-rials or
in aircraft iDclul alloys cellbics an1 + terial a comiddot
biDatiCD of _tal8 and ceramics called ceraaals
t
bull
~
1
1~
I
8S VIBRAlIOH EIFIElT PCR FIRS ~mUAL nSPPpoundTIO
October 8 9 and 10 1947 by S S Manson
DnROWCTICN
In an aircraft engine ~ 19bt st be combined with abeomte inshy
euranee against structural failure _ An iaportant phase of the research at
e IMA is therefore the determination of the criteria for structural
failure and a search for the _tllOds tomiddot increase the life of an engine while
the S8IIe tille reducing its weight and increasing its eftic1enC7 and power
output This phase of the research is known as stress and Vibration I
all l1A1t r ks to those aspects of the research relating to turbine
disks and turbine and coaresBor blades
TtRBIIE DIS
In turbine disks we are ccncerned with t major stress problelll8 The
irst of these 18 ria cracking which ico~n in disks in which the blades
are welded to the wheel It has been found that in such disks cracks occur
at the bases between the blades after periods ot operation Dch shorter than
bulluld ordinarily be c)osidered the reasonable Ute o t~ wheel Analytical
research has linked these cracks with high thelllal stresses due to hot -
operation plastic low that results froJ the high therDa1 stresses and a
tr~ss concentration inherent at the ba~e of tmiddothe blades Here is the apshy
p-ox1ate length of the cracks present of the blades of the disk
n the disk was removed froa service It was considered that this was a
dapgeroll8 length he Gna1rtical research indicated that it wuld be possible
to ~opagate the cracks bJ the ap l1cation ot successive heating and cooling I
cycles and here are BOI8 of the rcpagated cracks obtained by such crcles
ot tbeJlOtent1a1 eolutlol18 indicated by t~e analysis is the raval ot
Cf3
-- - --- shy
- 2 shy
bull
the stress concentration ~ drilling II holes at the bases ot the blades (
Pere are some cf the holes that were drilled prior to the aplicat ion of tne
heating cyc les and it will be seen that very few cracks propagated beyond
the holes The Derit of this type of solution has yet to be further tested
and we are building large spin ~its mere disks such as these will be able
to be tested under conditions of full speed and temperature gradient These
ts will also be used to middottest the cerit of a number of other indicated
lutions
The second problem associ ated with disks is that of disk burstingbull
Di9k bursting has occurred in practice but one of the cajor r easons f or
studying it is the desire to reduce the weight of the lIheel a step that
increase the number of this type of failure The results ot a pre1ia1nary
investigation of disk bursting are shown on this panel Here we were studying ~
he ef fect of ductility or the amount of stretch that the _ terial is capble
of withstanding without ruptm-e Here is a disk with a VI high ductility
Characteristic of its fracture are ~he low nucber of failed pieces and the
o fact that the lane of fracture is inclined at an angle of 45 to t he thickshy
ness of the disk As we decrease the ductility the nuber of fractured
pieces increases and t he plane I)f fr acture is perpendicular to thickness
of the disk The problem requ ires consider able additional- investigation and th~ pit s t hat will be used for t he r im cracking investigations will also
be used for testineuro ge disks such as shown on the other panel in disk bursting investigationsbull
)UMiDUSCOPIC VTIIUlIO
I should like to leaTe now the subject ot turbine disks and go on to
-
if
- 3 shy
r and turbine blades In this case we are concerned with blade
V1bration Vibration is a DOYeDent back and torth or the blade which re-
Its in aGme c in critical stress and fracture of the blade I t is
treacherous type of stress condition f irst because at any one time the
rese may DOt ~ great enough to campuae fracture but over a period of time
the ac lated e cause fracture wit hout nrning It is a l so
treacberou because so little is Imom about the causes for blade vitI-ation
~ ~ It fIl17 be present in engines but not in others and in any one engine r
be Jresent under SOlIe conditions but not under others It has taken
a good deal of research to gain eYen an e ntar understanding or blade
vibration
UJt _ dsonstrate a blade in a condition or vibration - Here is a
J
blade which has vibrational characteristics quite similar to t ho se of t urshy
l bine COIltressor blades except that i t is constructed to a JlUch larger
scale tban orcl1nary blades Connected to the end of the blade is an
electronic exc iter br which can vary the excttation llIIpulses until t he
natural frequency of the blade is r eached The blade will t hen go irto a
bullcondition of vitration The vibration i s too r apid to view with t he naked
and _ therefore uae stroboscopic light to stuctr it This light flickers
on and off at apJrOx1ateq the s frequency as t he blade vi
~ therefore JUkes the blAde appear to be standing still or to vi brate slowl y-
while in reality- i t is 1brati~ verf rap~
ltI
vibration 1Ou have seen is a verf simple t~ of vibr ation At any-
point along the length of the blade the entire section r e l y moving up
and down re are other IlUcb more complicated types of vibration and 0
IS
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
- 6 shy
sla Yaae8 turbotrupsrcbarger buck-ta an I-ul tshOllll ell ~
1 er __ in th1a
III ccmclaiCD we are iJlTe8t1gating the oasic soects of ratP-rials or
in aircraft iDclul alloys cellbics an1 + terial a comiddot
biDatiCD of _tal8 and ceramics called ceraaals
t
bull
~
1
1~
I
8S VIBRAlIOH EIFIElT PCR FIRS ~mUAL nSPPpoundTIO
October 8 9 and 10 1947 by S S Manson
DnROWCTICN
In an aircraft engine ~ 19bt st be combined with abeomte inshy
euranee against structural failure _ An iaportant phase of the research at
e IMA is therefore the determination of the criteria for structural
failure and a search for the _tllOds tomiddot increase the life of an engine while
the S8IIe tille reducing its weight and increasing its eftic1enC7 and power
output This phase of the research is known as stress and Vibration I
all l1A1t r ks to those aspects of the research relating to turbine
disks and turbine and coaresBor blades
TtRBIIE DIS
In turbine disks we are ccncerned with t major stress problelll8 The
irst of these 18 ria cracking which ico~n in disks in which the blades
are welded to the wheel It has been found that in such disks cracks occur
at the bases between the blades after periods ot operation Dch shorter than
bulluld ordinarily be c)osidered the reasonable Ute o t~ wheel Analytical
research has linked these cracks with high thelllal stresses due to hot -
operation plastic low that results froJ the high therDa1 stresses and a
tr~ss concentration inherent at the ba~e of tmiddothe blades Here is the apshy
p-ox1ate length of the cracks present of the blades of the disk
n the disk was removed froa service It was considered that this was a
dapgeroll8 length he Gna1rtical research indicated that it wuld be possible
to ~opagate the cracks bJ the ap l1cation ot successive heating and cooling I
cycles and here are BOI8 of the rcpagated cracks obtained by such crcles
ot tbeJlOtent1a1 eolutlol18 indicated by t~e analysis is the raval ot
Cf3
-- - --- shy
- 2 shy
bull
the stress concentration ~ drilling II holes at the bases ot the blades (
Pere are some cf the holes that were drilled prior to the aplicat ion of tne
heating cyc les and it will be seen that very few cracks propagated beyond
the holes The Derit of this type of solution has yet to be further tested
and we are building large spin ~its mere disks such as these will be able
to be tested under conditions of full speed and temperature gradient These
ts will also be used to middottest the cerit of a number of other indicated
lutions
The second problem associ ated with disks is that of disk burstingbull
Di9k bursting has occurred in practice but one of the cajor r easons f or
studying it is the desire to reduce the weight of the lIheel a step that
increase the number of this type of failure The results ot a pre1ia1nary
investigation of disk bursting are shown on this panel Here we were studying ~
he ef fect of ductility or the amount of stretch that the _ terial is capble
of withstanding without ruptm-e Here is a disk with a VI high ductility
Characteristic of its fracture are ~he low nucber of failed pieces and the
o fact that the lane of fracture is inclined at an angle of 45 to t he thickshy
ness of the disk As we decrease the ductility the nuber of fractured
pieces increases and t he plane I)f fr acture is perpendicular to thickness
of the disk The problem requ ires consider able additional- investigation and th~ pit s t hat will be used for t he r im cracking investigations will also
be used for testineuro ge disks such as shown on the other panel in disk bursting investigationsbull
)UMiDUSCOPIC VTIIUlIO
I should like to leaTe now the subject ot turbine disks and go on to
-
if
- 3 shy
r and turbine blades In this case we are concerned with blade
V1bration Vibration is a DOYeDent back and torth or the blade which re-
Its in aGme c in critical stress and fracture of the blade I t is
treacherous type of stress condition f irst because at any one time the
rese may DOt ~ great enough to campuae fracture but over a period of time
the ac lated e cause fracture wit hout nrning It is a l so
treacberou because so little is Imom about the causes for blade vitI-ation
~ ~ It fIl17 be present in engines but not in others and in any one engine r
be Jresent under SOlIe conditions but not under others It has taken
a good deal of research to gain eYen an e ntar understanding or blade
vibration
UJt _ dsonstrate a blade in a condition or vibration - Here is a
J
blade which has vibrational characteristics quite similar to t ho se of t urshy
l bine COIltressor blades except that i t is constructed to a JlUch larger
scale tban orcl1nary blades Connected to the end of the blade is an
electronic exc iter br which can vary the excttation llIIpulses until t he
natural frequency of the blade is r eached The blade will t hen go irto a
bullcondition of vitration The vibration i s too r apid to view with t he naked
and _ therefore uae stroboscopic light to stuctr it This light flickers
on and off at apJrOx1ateq the s frequency as t he blade vi
~ therefore JUkes the blAde appear to be standing still or to vi brate slowl y-
while in reality- i t is 1brati~ verf rap~
ltI
vibration 1Ou have seen is a verf simple t~ of vibr ation At any-
point along the length of the blade the entire section r e l y moving up
and down re are other IlUcb more complicated types of vibration and 0
IS
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
I
8S VIBRAlIOH EIFIElT PCR FIRS ~mUAL nSPPpoundTIO
October 8 9 and 10 1947 by S S Manson
DnROWCTICN
In an aircraft engine ~ 19bt st be combined with abeomte inshy
euranee against structural failure _ An iaportant phase of the research at
e IMA is therefore the determination of the criteria for structural
failure and a search for the _tllOds tomiddot increase the life of an engine while
the S8IIe tille reducing its weight and increasing its eftic1enC7 and power
output This phase of the research is known as stress and Vibration I
all l1A1t r ks to those aspects of the research relating to turbine
disks and turbine and coaresBor blades
TtRBIIE DIS
In turbine disks we are ccncerned with t major stress problelll8 The
irst of these 18 ria cracking which ico~n in disks in which the blades
are welded to the wheel It has been found that in such disks cracks occur
at the bases between the blades after periods ot operation Dch shorter than
bulluld ordinarily be c)osidered the reasonable Ute o t~ wheel Analytical
research has linked these cracks with high thelllal stresses due to hot -
operation plastic low that results froJ the high therDa1 stresses and a
tr~ss concentration inherent at the ba~e of tmiddothe blades Here is the apshy
p-ox1ate length of the cracks present of the blades of the disk
n the disk was removed froa service It was considered that this was a
dapgeroll8 length he Gna1rtical research indicated that it wuld be possible
to ~opagate the cracks bJ the ap l1cation ot successive heating and cooling I
cycles and here are BOI8 of the rcpagated cracks obtained by such crcles
ot tbeJlOtent1a1 eolutlol18 indicated by t~e analysis is the raval ot
Cf3
-- - --- shy
- 2 shy
bull
the stress concentration ~ drilling II holes at the bases ot the blades (
Pere are some cf the holes that were drilled prior to the aplicat ion of tne
heating cyc les and it will be seen that very few cracks propagated beyond
the holes The Derit of this type of solution has yet to be further tested
and we are building large spin ~its mere disks such as these will be able
to be tested under conditions of full speed and temperature gradient These
ts will also be used to middottest the cerit of a number of other indicated
lutions
The second problem associ ated with disks is that of disk burstingbull
Di9k bursting has occurred in practice but one of the cajor r easons f or
studying it is the desire to reduce the weight of the lIheel a step that
increase the number of this type of failure The results ot a pre1ia1nary
investigation of disk bursting are shown on this panel Here we were studying ~
he ef fect of ductility or the amount of stretch that the _ terial is capble
of withstanding without ruptm-e Here is a disk with a VI high ductility
Characteristic of its fracture are ~he low nucber of failed pieces and the
o fact that the lane of fracture is inclined at an angle of 45 to t he thickshy
ness of the disk As we decrease the ductility the nuber of fractured
pieces increases and t he plane I)f fr acture is perpendicular to thickness
of the disk The problem requ ires consider able additional- investigation and th~ pit s t hat will be used for t he r im cracking investigations will also
be used for testineuro ge disks such as shown on the other panel in disk bursting investigationsbull
)UMiDUSCOPIC VTIIUlIO
I should like to leaTe now the subject ot turbine disks and go on to
-
if
- 3 shy
r and turbine blades In this case we are concerned with blade
V1bration Vibration is a DOYeDent back and torth or the blade which re-
Its in aGme c in critical stress and fracture of the blade I t is
treacherous type of stress condition f irst because at any one time the
rese may DOt ~ great enough to campuae fracture but over a period of time
the ac lated e cause fracture wit hout nrning It is a l so
treacberou because so little is Imom about the causes for blade vitI-ation
~ ~ It fIl17 be present in engines but not in others and in any one engine r
be Jresent under SOlIe conditions but not under others It has taken
a good deal of research to gain eYen an e ntar understanding or blade
vibration
UJt _ dsonstrate a blade in a condition or vibration - Here is a
J
blade which has vibrational characteristics quite similar to t ho se of t urshy
l bine COIltressor blades except that i t is constructed to a JlUch larger
scale tban orcl1nary blades Connected to the end of the blade is an
electronic exc iter br which can vary the excttation llIIpulses until t he
natural frequency of the blade is r eached The blade will t hen go irto a
bullcondition of vitration The vibration i s too r apid to view with t he naked
and _ therefore uae stroboscopic light to stuctr it This light flickers
on and off at apJrOx1ateq the s frequency as t he blade vi
~ therefore JUkes the blAde appear to be standing still or to vi brate slowl y-
while in reality- i t is 1brati~ verf rap~
ltI
vibration 1Ou have seen is a verf simple t~ of vibr ation At any-
point along the length of the blade the entire section r e l y moving up
and down re are other IlUcb more complicated types of vibration and 0
IS
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
8S VIBRAlIOH EIFIElT PCR FIRS ~mUAL nSPPpoundTIO
October 8 9 and 10 1947 by S S Manson
DnROWCTICN
In an aircraft engine ~ 19bt st be combined with abeomte inshy
euranee against structural failure _ An iaportant phase of the research at
e IMA is therefore the determination of the criteria for structural
failure and a search for the _tllOds tomiddot increase the life of an engine while
the S8IIe tille reducing its weight and increasing its eftic1enC7 and power
output This phase of the research is known as stress and Vibration I
all l1A1t r ks to those aspects of the research relating to turbine
disks and turbine and coaresBor blades
TtRBIIE DIS
In turbine disks we are ccncerned with t major stress problelll8 The
irst of these 18 ria cracking which ico~n in disks in which the blades
are welded to the wheel It has been found that in such disks cracks occur
at the bases between the blades after periods ot operation Dch shorter than
bulluld ordinarily be c)osidered the reasonable Ute o t~ wheel Analytical
research has linked these cracks with high thelllal stresses due to hot -
operation plastic low that results froJ the high therDa1 stresses and a
tr~ss concentration inherent at the ba~e of tmiddothe blades Here is the apshy
p-ox1ate length of the cracks present of the blades of the disk
n the disk was removed froa service It was considered that this was a
dapgeroll8 length he Gna1rtical research indicated that it wuld be possible
to ~opagate the cracks bJ the ap l1cation ot successive heating and cooling I
cycles and here are BOI8 of the rcpagated cracks obtained by such crcles
ot tbeJlOtent1a1 eolutlol18 indicated by t~e analysis is the raval ot
Cf3
-- - --- shy
- 2 shy
bull
the stress concentration ~ drilling II holes at the bases ot the blades (
Pere are some cf the holes that were drilled prior to the aplicat ion of tne
heating cyc les and it will be seen that very few cracks propagated beyond
the holes The Derit of this type of solution has yet to be further tested
and we are building large spin ~its mere disks such as these will be able
to be tested under conditions of full speed and temperature gradient These
ts will also be used to middottest the cerit of a number of other indicated
lutions
The second problem associ ated with disks is that of disk burstingbull
Di9k bursting has occurred in practice but one of the cajor r easons f or
studying it is the desire to reduce the weight of the lIheel a step that
increase the number of this type of failure The results ot a pre1ia1nary
investigation of disk bursting are shown on this panel Here we were studying ~
he ef fect of ductility or the amount of stretch that the _ terial is capble
of withstanding without ruptm-e Here is a disk with a VI high ductility
Characteristic of its fracture are ~he low nucber of failed pieces and the
o fact that the lane of fracture is inclined at an angle of 45 to t he thickshy
ness of the disk As we decrease the ductility the nuber of fractured
pieces increases and t he plane I)f fr acture is perpendicular to thickness
of the disk The problem requ ires consider able additional- investigation and th~ pit s t hat will be used for t he r im cracking investigations will also
be used for testineuro ge disks such as shown on the other panel in disk bursting investigationsbull
)UMiDUSCOPIC VTIIUlIO
I should like to leaTe now the subject ot turbine disks and go on to
-
if
- 3 shy
r and turbine blades In this case we are concerned with blade
V1bration Vibration is a DOYeDent back and torth or the blade which re-
Its in aGme c in critical stress and fracture of the blade I t is
treacherous type of stress condition f irst because at any one time the
rese may DOt ~ great enough to campuae fracture but over a period of time
the ac lated e cause fracture wit hout nrning It is a l so
treacberou because so little is Imom about the causes for blade vitI-ation
~ ~ It fIl17 be present in engines but not in others and in any one engine r
be Jresent under SOlIe conditions but not under others It has taken
a good deal of research to gain eYen an e ntar understanding or blade
vibration
UJt _ dsonstrate a blade in a condition or vibration - Here is a
J
blade which has vibrational characteristics quite similar to t ho se of t urshy
l bine COIltressor blades except that i t is constructed to a JlUch larger
scale tban orcl1nary blades Connected to the end of the blade is an
electronic exc iter br which can vary the excttation llIIpulses until t he
natural frequency of the blade is r eached The blade will t hen go irto a
bullcondition of vitration The vibration i s too r apid to view with t he naked
and _ therefore uae stroboscopic light to stuctr it This light flickers
on and off at apJrOx1ateq the s frequency as t he blade vi
~ therefore JUkes the blAde appear to be standing still or to vi brate slowl y-
while in reality- i t is 1brati~ verf rap~
ltI
vibration 1Ou have seen is a verf simple t~ of vibr ation At any-
point along the length of the blade the entire section r e l y moving up
and down re are other IlUcb more complicated types of vibration and 0
IS
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
-- - --- shy
- 2 shy
bull
the stress concentration ~ drilling II holes at the bases ot the blades (
Pere are some cf the holes that were drilled prior to the aplicat ion of tne
heating cyc les and it will be seen that very few cracks propagated beyond
the holes The Derit of this type of solution has yet to be further tested
and we are building large spin ~its mere disks such as these will be able
to be tested under conditions of full speed and temperature gradient These
ts will also be used to middottest the cerit of a number of other indicated
lutions
The second problem associ ated with disks is that of disk burstingbull
Di9k bursting has occurred in practice but one of the cajor r easons f or
studying it is the desire to reduce the weight of the lIheel a step that
increase the number of this type of failure The results ot a pre1ia1nary
investigation of disk bursting are shown on this panel Here we were studying ~
he ef fect of ductility or the amount of stretch that the _ terial is capble
of withstanding without ruptm-e Here is a disk with a VI high ductility
Characteristic of its fracture are ~he low nucber of failed pieces and the
o fact that the lane of fracture is inclined at an angle of 45 to t he thickshy
ness of the disk As we decrease the ductility the nuber of fractured
pieces increases and t he plane I)f fr acture is perpendicular to thickness
of the disk The problem requ ires consider able additional- investigation and th~ pit s t hat will be used for t he r im cracking investigations will also
be used for testineuro ge disks such as shown on the other panel in disk bursting investigationsbull
)UMiDUSCOPIC VTIIUlIO
I should like to leaTe now the subject ot turbine disks and go on to
-
if
- 3 shy
r and turbine blades In this case we are concerned with blade
V1bration Vibration is a DOYeDent back and torth or the blade which re-
Its in aGme c in critical stress and fracture of the blade I t is
treacherous type of stress condition f irst because at any one time the
rese may DOt ~ great enough to campuae fracture but over a period of time
the ac lated e cause fracture wit hout nrning It is a l so
treacberou because so little is Imom about the causes for blade vitI-ation
~ ~ It fIl17 be present in engines but not in others and in any one engine r
be Jresent under SOlIe conditions but not under others It has taken
a good deal of research to gain eYen an e ntar understanding or blade
vibration
UJt _ dsonstrate a blade in a condition or vibration - Here is a
J
blade which has vibrational characteristics quite similar to t ho se of t urshy
l bine COIltressor blades except that i t is constructed to a JlUch larger
scale tban orcl1nary blades Connected to the end of the blade is an
electronic exc iter br which can vary the excttation llIIpulses until t he
natural frequency of the blade is r eached The blade will t hen go irto a
bullcondition of vitration The vibration i s too r apid to view with t he naked
and _ therefore uae stroboscopic light to stuctr it This light flickers
on and off at apJrOx1ateq the s frequency as t he blade vi
~ therefore JUkes the blAde appear to be standing still or to vi brate slowl y-
while in reality- i t is 1brati~ verf rap~
ltI
vibration 1Ou have seen is a verf simple t~ of vibr ation At any-
point along the length of the blade the entire section r e l y moving up
and down re are other IlUcb more complicated types of vibration and 0
IS
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
- 3 shy
r and turbine blades In this case we are concerned with blade
V1bration Vibration is a DOYeDent back and torth or the blade which re-
Its in aGme c in critical stress and fracture of the blade I t is
treacherous type of stress condition f irst because at any one time the
rese may DOt ~ great enough to campuae fracture but over a period of time
the ac lated e cause fracture wit hout nrning It is a l so
treacberou because so little is Imom about the causes for blade vitI-ation
~ ~ It fIl17 be present in engines but not in others and in any one engine r
be Jresent under SOlIe conditions but not under others It has taken
a good deal of research to gain eYen an e ntar understanding or blade
vibration
UJt _ dsonstrate a blade in a condition or vibration - Here is a
J
blade which has vibrational characteristics quite similar to t ho se of t urshy
l bine COIltressor blades except that i t is constructed to a JlUch larger
scale tban orcl1nary blades Connected to the end of the blade is an
electronic exc iter br which can vary the excttation llIIpulses until t he
natural frequency of the blade is r eached The blade will t hen go irto a
bullcondition of vitration The vibration i s too r apid to view with t he naked
and _ therefore uae stroboscopic light to stuctr it This light flickers
on and off at apJrOx1ateq the s frequency as t he blade vi
~ therefore JUkes the blAde appear to be standing still or to vi brate slowl y-
while in reality- i t is 1brati~ verf rap~
ltI
vibration 1Ou have seen is a verf simple t~ of vibr ation At any-
point along the length of the blade the entire section r e l y moving up
and down re are other IlUcb more complicated types of vibration and 0
IS
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
- h shy
of the first pob lens in the science is to categorize these yitrations This
is done h7 the use of mat we call sand patterns I ehall srinkle sand oyer
the entire blade and then vary the excitation trequenq on the blade Wltil
i t begins to vibrate in one ot its IIOre complex odes The sand particles
boWlce aroWld and naturally tend to pile up at the locations ot ainbIua vibrashy
t io Here is one jat tern I now increase the excitation trequeIlC7 until
I reach another vibr ational requenq ot the blade the sand bounces around
~ in another t)attern and again in another pattern In this way we can class itr
the vibrational characteristics of a~ blade according to t he frequen~ of
vibration and the stress condition in the bladB at anyone fr equellC7
HIGH TEJ~E STRAr~ I
The next p-obl en is to learn which types ot vibration actually do exist
in an engine For this FWpose _ e use of wire strain g~es The strain
gage consists nerely of a strand 01 resistance wire 1Ihich is cemented onto
he blade As this blade vibrates it changes minutely the elect rical reshy
sistance ot t he wire By measuring the change in electrical resistance the
amount and type ot vibration can be determined We had had a great deal ot
experience with wire-resistar1 ~
strain gages as applied to r eciprocati
ng
enpoundines When we started to study turbines we learned that the strain gages
t~at had tormerly been used were suitable tor the terlperatures of hCXLsocP F
revicusly encountered but were certainly not suitable tor the temperat ures
in the range ot 1500 o
- 180(0
F which were now ot interest After considerable
~
laquo
r esearch we learned however that by using th suitable I18terials and lOst
imjOr tant by using proper electronic c ircuits it was possible to find strain 0
gages capable ot withstanding 1500 -180( F I shoulc1 like to demonstrate
to you the operation of Slch a strain Z8gs Here 118 have a strain ~age ounted
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
- Sshy at the base on a typical turbine blade SUrrourvljng the blade is an inshy
ductlon beating coil This coil rov1des a rapidly fiuctuating magnetic
field around the gage and in 80 do~ induces eddy currents in the blade
ncb beat up to a Yery high value At the present t the blade in the
ovicinity of the gage is fairly close to ISco F Attached to the block
in ~1ch the gage is _lted is a 11 air turbine It I increase the air
preeaure the peed or the turbine ~reases and provides a mechanical ~
J
excitation mich men it reaches the natural frequency of t he bl ade
cau it to vibrate The rl~at1on of the blade is lfxiicated by the apshy
anee of a waYe on the oscillograph screen above the blade
~~ DOOBIE REFRACTlm
Yen when _ know about the presence of vibration the trequency of the
vibration and the characteristics of the vibration at the Parti cular freshy
- qulllc YtJry often we do not kD01l the source of t he excitation and therefor e
it is 1ampposs1ble to find a remedy In some cases the excitation y be
lleCban1cal as it was in this dsonstration In 80_ cases however the
Gcitatlon aerodynaaic t hat is it is due to flnctuat ion of air forces
on the bladll Ie have recently introduced the streaa1ng double retract ion bull
~ thod of flDid no into our r esearch in order to gain a better undershy
~ standing of the no phe~na that My cause vibration The equi1ll1ent for
tfi type of research consist of a ~urce of polarized light and a channel
in which a blade ccntour is suspended in a tluid consisting of bentonite clay
_ter Th~ fluid has the pecuUar Jroperty of double retraction in that
a beD of light passing through it bave one or more of its color COl1shy
PODe~S retarded 80 Uat the portion of the light that leaves the channel has
o~ that color co2lpgtnent of the entering tdte light which is not r etarded
17
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
- 6 shy
The r esult is a color pattern which rep-esents the condition of fluid no t= middot77 ~~~L~
in a very colorful and graphical manner It we turn on the equiPlent atbull
first s lowlY so that the flow around t he blade contour is stream] 1ned we
see the close adhererce of the f luid to the b lade contour Even at this
slow speed t here i s present a small amount of wiggling in the wake of the
blade and this fluct uation or f luid flow maJ produce excitation forces I
both on this b1ade and on arr blade that succeeds this b l ade It we now
increase the rate of rIow the fluid creaks away from the model a1d t he ~
flow becomes turbulent 7he exc itation force under this condition are
r e vo1ent The colCr pat tern becomes somewhat more diffuse because the
flow is so r apid that the various colors are interacting with cne another
prcducing what appears to th~ eye to be white light It 118 had been able
to use stroboscopic light as we did in the case or the vibrating blade
we would be able to see the Jrecise luctuation of the fiuid flow Unshy
fortunately stroboscopi c l ight does not project very well but we have b7
~rect observation studied the pattern of flo If we now further increase
the rate of flow the flo pattern disappears a lmost entirelJ as far as the
naked eye is concer ned but the exc itation forces are 80 vio l ent as to ake
the b lade flutter vehecently
CCUCLUSION
Gentlemen I have demonstr ated several of the t echniques that we use in
the basic r esearch of stres s a~d vibration In the last analysis however
it is necessary act ually to get into the turbine or pre ssor in order to
stuctr the existing phenomena Here we have a compressor that was 1nstruenteci
with strain gages and ru under lull operating condi tione bave l earned
from this compressor the effeets of such pbenoaena as 8I1rging and tbe IreHDCe
f(
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
-7 shy of high pressure ratio Here is a turbine which was instrumented with highshy
rature strain gages and operated under hot gas cOnditions We have
fro it the effects on the rlbration of such factors as the l1UJIber
of collbastion ch-bers )(any of the results of these tests have already
been ~b1i8bed in lac reX)rts her r esults are in Ule process of JQbshy
lication Much research raains to be done It is hoped that tliis research
will Jrovicie the necessary data to aake possible the realization of the
re efficient and powerful engines of the future
T
bull
SSM
I
1
LL
bull
LL
bull