forwindvr - graham wind turbine talk
TRANSCRIPT
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Aerodynamics of Horizontal Axis Wind-
Turbine Rotors.
J. Michael R. Graham,
Department of Aeronautics,
Imperial College, London, UK.
Seminar: University of Oldenbur! "#. ". #$. .
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Rotor Stall %elay &Himmels'am( )ffect*
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+m dia. model of
W), rotor tested in
x /ind tunnel
settlin c0amber
&12m dia.*
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3ressure %istribution c4r 5 #.$2 &6onstant c0ord blade!
Wind Tunnel*
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3ressure %istribution c4r 5 #.7 &6onstant c0ord blade!
Wind Tunnel*
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3ressure %istribution
c4r 5 #.2 &W), blade!
Wind Tunnel*
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Sectional 8ift 6oefficients aainst Anle of Attac'
for W), Rotor 9lade &Wind Tunnel*
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ield Tests &";m Wind Harvester turbine at
Rut0erford A((leton 8aboratory*
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ield Rotor &Wind Harvester* Test
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Surface (ressure time 0istory! inboard station.
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3ressure at &a((rox.* maximum lift coefficient
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Approimate !oundar"#la"er anal"sis of Coriolis$ %orce
suggests separation depends on parameter &chord'radius(.
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3ossible
)x(lanations
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Rotor-To/er
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6ombined )x(eriment- %o/n/ind Rotor&=ational
Rene/able )nery 8ab! ,olden! 6O! USA.
Robinson! Simms! Hand and Sc0rec'*
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)ffect of To/er S0ado/ &Wa'e %efect* on %o/n/ind
Rotor9lade &Wind Tunnel! W), 9lade*
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)ffect of To/er S0ado/ &9loc'ae*! on U(/ind
Rotor9lade &Wind Tunnel! We 9lade*: 3ressure
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)ffect of To/er S0ado/ &Wa'e* on %o/n/ind
Rotor&Wind Tunnel ! W), blade*: 3ressure
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To/er S0ado/ effect &/a'e* on Stalled
%o/n/ind Rotor&Wind Tunnel! W), 9lade*
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Rotor#1o*er Interaction using an Incompressi!le
2+erset Grid Method
%rederi 3ahle &Risoe La!() Moti+ation for the pro4ect-
5 Current C%D code can onl" handle isolated rotors
5De+elopment of a C%D tool *hich can handle complete*ind tur!ine configuration *ith focus on rotor#to*er
interaction
) 2utline5/umerical Method
5/R6L 7hase 8I eperiment comparison
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2riginal C%D Code 6llip0"s9D
) Unstead" incompressi!le /a+ier#0toes sol+er) %inite +olume, pressure !ased, sol+ing for primiti+e
+aria!les u, v, wandpin general cur+ilinear
coordinates in a cell#centered arrangement
) 0UD0':UICK, 0IM7L6'7I02
) #M001, D60 &;"!rid L60(
)
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1he 2+erset Grid Method) Ideal for comple geometr",
multi#!od", mo+ing grid pro!lems) Grid around each component is
generated independentl" of others
) Allo*s grids to o+erlap ar!itraril"
) Com!ination of !od"#fitted
&cur+ilinear( and off#!od"&Cartesian( grids
) ;ole#cutting adds further
flei!ilit"
) Local grid refinement possi!le
) Use of eisting implicit structured
sol+ers maintains high efficienc"
) Can !e parallelised
) %airl" high computational cost
associated *ith search and
interpolation routines
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/R6L UA6 7hase 8I 6periment
) Conducted in /A0A Ames 9?.? m @.m
) B m diameter *ind tur!ine
)
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Computational %rame*or
) Mesh-5 Consists of t*o !od" fitted cur+ilinear
grids and three Cartesian !acgroundgrids. 1otal . M cells.
5 /acelle omitted
5 0ame farfield dimensions as /A0Atunnel.
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%lo* %ield
) Iso contours of a!solute +orticit"
)1ip and root +ortices preser+ed *ell do*nstream of tur!ine
) 8orte shedding from to*er is clearl" +isi!le
) Induction from rotor reduces aial +elocit", and modifies +orte shedding
freFuenc" on to*er. 8orte dislocation !elo* rotor due to change in
shedding freFuenc".
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1o*er Response
)1o*er response inside rotor disc appears to !e eperiencing loc#in
) 9 shedding periods per re+olution inside rotor disc- fs9.? ;
) 0hedding freFuenc" !elo* rotor disc- fs.B ;
) %reFuenc" content sho*s 97 pea *hich is the shedding freFuenc", @7 and 7
peas from !lade passage freFuenc". 8orte shedding loced#in
) Causes !lade response to !e periodic and correlated span*ise
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Conclusions and 2utloo
) 9D o+erset computations capa!le of accuratel" capturing the interaction!et*een the rotor and to*er. 6cellent agreement *ith eperiment.
) C/response largel" depends on changes in aial +elocit". CM also reflects
local changes in pressure caused !" the
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=ind 1ur!ines and
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1han "ou for "our attentionN