ch11
DESCRIPTION
structures notesTRANSCRIPT
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11. Prismatic Beam Design
Design a beam to resist
both bending and
shear loads.
Develop methods used
for designing prismaticbeams.
Determine shape of fully
stressed beams.
Design of shafts based on
both bending and torsional moments.
CHAPTER OBJECTIVES
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11. Prismatic Beam Design
CHAPTER OUTLINE
1. Basis for Beam Design
2. Prismatic Beam Design
3. *Fully tressed Beams
!. *haft Design
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11. Prismatic Beam Design
11.1 BASIS FOR BEA DESI!N
Beams are structural members designed to supportloadings perpendicular to their longitudinal a"es.
#nder load$ internal shear force and bendingmoment that vary from pt to pt along a"is of beam.
%"ial stress is ignored in design$ as it&s muchsmaller than the shear force and bending moment.
% beam designed to resist shear and bendingmoment is designed on the basis of strength.
'e use the shear and fle"ure formulae fromchapters ( and ) to design a beam$ only if the beamis homogeneous and displays linearelasticbehavior.
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11. Prismatic Beam Design
11.1 BASIS FOR BEA DESI!N
%s sho+n$ e"ternal distributed and pt loads appliedto a beam is neglected +hen +e do stress analysis.
%dvanced analysis sho+s that the ma"imum value
of such stresses are of a small percentage
compared to bending stresses. %lso$ engineers prefer
to design for bearing
loads rather than pt
loads to spread the
load more evenly.
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11. Prismatic Beam Design
-he actual bending and shear stresses must note"ceed the allo+able values specified in structural
and mechanical codes of practice.
'e need to determine the beam&s section modulus.
#sing fle"ure formula$ Mc/I$ +e have
0 is determined from the beam&s moment diagram$
and allo+able bending stress$ allo+ is specified in a
design code.
11." PRISATIC BEA DESI!N
( )1-11allow
dreq'
MS =
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11. Prismatic Beam Design
nce Sreqdis no+n$ +e can determine thedimensions of the "section of the beam.
o+ever$ for beams +ith "section consisting of
various elements 4e.g. +ideflange section5$ then
an infinite no. of +eb and flange dimensions can becomputed.
6n practice$ the engineer +ill choose a commonly
manufactured standard shape from a handboo
that satisfies S7 Sre8&d.
11." PRISATIC BEA DESI!N
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11. Prismatic Beam Design
#se symmetric "section if allo+able bending stressis the same for tension and compression.
ther+ise$ +e use an unsymmetrical "section to
resist both the largest positive and negative
moment in the span. nce beam selected$ use shear formula
allo+ VQ/Itto chec that the allo+able shear stresshas not been e"ceeded.
9"ceptional cases are +hen the material used is
+ood.
11." PRISATIC BEA DESI!N
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11. Prismatic Beam Design
11." PRISATIC BEA DESI!N
Fabricated Beams
1. Steel sections
0ost manufactured steel beams produced by rollinga hot ingot of steel till the desired shape is
produced. -he rolled shapes have properties that aretabulated in the %merican6nstitute of teel ;onstruction
4%6;5 manual. 4%ppendi" B5 'ide flange shapes defined by
their depth and +eight per unitlength.
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sections +hile the actual dimensions are smallerdue to sa+ing do+n the rough surfaces.
%ctual dimensions are to be used +hen performing
stress calculations.
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11." PRISATIC BEA DESI!N
Fabricated Beams
3. Built-up Sections
% builtup section is constructed from t+o or more
parts ?oined together to form a single unit.
Based on 98n 111$ the momentresisting capacityof such a section +ill be greatest for the greatest
moment of inertia.
-hus$ most of the material should be built furthestfrom the neutral a"is.
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11. Prismatic Beam Design
11." PRISATIC BEA DESI!N
Fabricated Beams
3. Built-up Sections
For very large loads$ +e use a deep Ishapedsection to resist the moments.
-he sections are usually+elded or bolted to
form the builtup section.
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11. Prismatic Beam Design
11." PRISATIC BEA DESI!N
Fabricated Beams
3. Built-up Sections
'ooden bo" beams are made from
ply+ood +ebs and larger boards for the
flanges. For very large spans$ glulam beams are
used. uch members are made from
several boards gluelaminated together.
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11. Prismatic Beam Design
11." PRISATIC BEA DESI!N
60P@-%>-
Beams support loadings that are applied
perpendicular to their a"es.
6f they are designed on the basis of strength$ they
must resist allo+able shear and bending stresses. -he ma"imum bending stress in the beam is
assumed to be much greater than the localiAed
stresses caused by the application of loadings on
the surface of the beam.
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11. Prismatic Beam Design
11." PRISATIC BEA DESI!N
Procedure for analysis
hear and moment diagrams
Determine the ma"imum shear and moment in
the beam. -his is often done by constructing the
beam&s shear and moment diagrams. For builtup beams$ shear and moment diagrams
are useful for identifying regions +here the shear
and moment are e"cessively large and may
re8uire additional structural reinforcement or
fasteners.
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11." PRISATIC BEA DESI!N
Procedure for analysis
%verage normal stress
6f beam is relatively long$ it is designed by finding its
section modulus using the fle"ure formula$
Sre8&d Mma"/allo+. nce Sre8&dis determined$ the "sectional
dimensions for simple shapes can then be
computed$ since Sre8&d I/c. 6f rolledsteel sections are to be used$ several
possible values of Smay be selected from the
tables in %ppendi" B.
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11. Prismatic Beam Design
11." PRISATIC BEA DESI!N
Procedure for analysis
%verage normal stress
;hoose the one +ith the smallest "sectional area$
since it has the least +eight and is therefore the
most economical.hear stress
>ormally$ beams that are short and carry large
loads$ especially those made of +ood$ are firstdesigned to resist shear and later checed against
the allo+ablebendingstress re8uirements.
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11. Prismatic Beam Design
11." PRISATIC BEA DESI!N
Procedure for analysis
hear stress
#se the shear formula to chec to see that theallo+able shear stress is not e"ceeded
allo+CVma"Q/It.
6f the beam has a solid rectangular "section$ theshear formula becomes allo+C 1.,4Vma"/A)$98n ),$ and if the "section is a +ide flange$ it is
to assume that shear stress is constant overthe "sectional area of the beam&s +eb so that allo+C Vma"/A+eb$ +here A+ebis determined from theproduct of the beam&s depth and the +eb&sthicness.
11 P i ti B D i
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+ill only slightly increase Sre8&d. -hus$
3333' mm)10(1120mm)10(706
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11. Prismatic Beam Design
E#APLE 11.1 $SOLN%
hear stress
ince beam is a +ideflange section$ the average
shear stress +ithin the +eb +ill be considered.
ere the +eb is assumed to e"tend from the very top
to the very bottom of the beam.From %ppendi" B$ for a '1:!=$ d !,, mm$tw : mm$ thus
#se a '!(=(=.
( ) ( ) !a100!a7.24mm8mm455 N1090
3
maxa"#
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11. Prismatic Beam Design
E#APLE 11.&
aminated +ooden beam supports a uniform
distributed loading of 12 >/m. 6f the beam is to havea heightto+idth ratio of 1.,$ determine its smallest
+idth. -he allo+able bending stress is allo+ < 0Pa
and the allo+able shear stress is allo+ =.( 0Pa.>eglect the +eight of the beam.
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11. Prismatic Beam Design
E#APLE 11.& $SOLN%
hear and moment diagrams
upport reactions at Aand B
have been calculated and the
shear and moment diagrams
are sho+n.ere$ Vma" 2= >$
Mma" 1=.() >m.
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11. Prismatic Beam Design
E#APLE 11.& $SOLN%
Bending stress
%pplying the fle"ure formula yields$
%ssume that +idth is a$ then height is h 1.,a. -hus$( )
323
allow
maxdreq' m00119.0
kN/m109
mkN67.10=
==
MS
( ) ( )
( )
m147.0
m003160.0
m00119.075.0
35.1121
33
3
dreq'
==
===
a
a
a
aa
c
I
S
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11. Prismatic Beam Design
E#APLE 11.& $SOLN%
hear stress
%pplying shear formula for rectangular sections
4special case of ma" VQ/It5$ +e have
( )( ) ( ) ( )
!a60!a929.0
m147.05.1m147.0kN205.15.1 maxmax
.
A
V
>=
==
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2ote that although this result indicates that h = atx =$ it&s necessary that beam resist shear stress atthe supports$ that is$ h7 = at the supports.
b
PL
h allow
2
0 2
3
=
xL
hh
=202 2
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11. Prismatic Beam Design
hafts +ith circular "section are used in many
types of mechanical e8uipment and machinery.
-hus$ they are sub?ected to cyclic or fatigue stress$
caused by the combined bending and torsional
loads they must transmit. tress concentrations +ill
also occur due to eys$
couplings$ and sudden
transitions in its"sectional area.
'11.) SHAFT DESI!N
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11. Prismatic Beam Design
For e"ample$ +e can resolve
and replace the loads +iththeir e8uivalent components.
Bendingmoment diagrams for
the loads in each plane can bedra+n and resultant internal
moment at any section along
shaft is determined by vector
addition$ M (Mx2G Mz25.
'11.) SHAFT DESI!N
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11. Prismatic Beam Design
6n addition$ the tor8ue diagram
can also be dra+n.
Based on the diagrams$ +e
investigate certain critical
sections +here thecombination of resultant moment and
tor8ue Tcreates the +orst stress situation.
-hen $+e apply fle"ure formula using the resultant
moment on the principal a"is of inertia.
'11.) SHAFT DESI!N
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11. Prismatic Beam Design
'11.) SHAFT DESI!N
6n general$ critical element D4or C5
on the shaft is sub?ected to plane
stress as sho+n$ +here
J
Tc
I
Mc == and
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3ormally$ the "section of a beam is first designed
to resist the allo+able bending stress$ then the
allo+able shear stress is checed.
For rectangular sections$ allo+C 1., 4Vma"/A5.
For +ideflange sections$ +e use allo+C Vma"/A+eb.
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