lecture 27: lift
DESCRIPTION
Lecture 27: Lift. Many biological devices (Biofoils) are used to create Lift. How do these work?. chord section analysis…. (normal to U). total force. (normal to wing). lift. angle of attack = a. (parallel to U). drag. wing velocity = U. First, some definitions…. wing section,c - PowerPoint PPT PresentationTRANSCRIPT
Lecture 27: Lift
Many biological devices (Biofoils) are used to create Lift.How do these work?
First, some definitions…
wing section,c(chord)
totalforce(normal to wing)
drag
lift(normal to U)
(parallel to U)
chord section analysis….
wingvelocity = U
angle ofattack =
winglength, R wing
area, S
Two ways to derive lift:1) mass deflection
totalforce
U
air deflecteddownward by wing
USUmUForce dtd ~)(
Surface area, S
)(Re,
221
fC
SUCForce
total
total
Pressure always acts normal to the surface of an object.Therefore, this mass deflection force acts roughly perpendicular to surface of biofoil.
1) Massdeflection
totalforce
drag
lift
U
air deflecteddownward by wing
Surface area, S
221 SUCForce total
Lift and drag are defined ascomponents perpendicularand parallel to direction of motion.
viscoustotaldrag
totallift
drag
lift
CCC
CC
SUCDrag
SUCLift
sin
cos
221
221
RoboFly
amplitude · length2
frequency · viscosityReynolds number =
reduced frequency =forward velocity
length · angular velocity
dimensionless scaling parameters
totalforce
-9 0 9 18 27 36 45 54 63 72 81 90
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
tota
l for
ce c
oeff
icie
ntC
T
angle of attack (degs)
-9 0 9 18 27 36 45 54 63 72 81 90
-60
-40
-20
0
20
40
60
80
10090o
tota
l for
ce o
rien
tati
on
degs
angle of attack (degs)
CL
CD
Fs
0 15 30 45 60 75 90
0
1
2
3
4
CT
angle of attack ()
CT = 3.5 sin
0 15 30 45 60 75 90
0
1
2
3
4
CD
angle of attack ()
CD = CT sin
0 15 30 45 60 75 90
0
1
2
3
angle of attack ()
CL = CT cos
CL
{viscous
drag
CT sin
CT
CT cos
totalforce
drag
lift
U
Surface area, S
~
sinsin
cossin
221
221
k
CkC
kC
SUCDrag
SUCLift
viscousdrag
lift
drag
lift
-9 0 9 18 27 36 45 54 63 72 81 90-0.5
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
angle of attack (degs)
forc
e co
effi
cien
ts
CL
CD
Polar plot of lift and drag:
0 1 2 3 4-1
0
1
2
3
drag coefficient
lift
coe
ffic
ient
=-9
=-9
=22.5
=45
=90
highestlift:drag ratio
U
Flow is tangentialat trailing edge
Flow separatesat leading edge
2. Circulation
Law of continuity applies to streamline
fluid travels fasterover to of biofoil
U
Difference in velocityacross surface is equivalent
to net circular flow around biofoil = Circulation,
dSUmathematically:
dA
Kutta-Joukowski Theorem:
UtLif (lift per unit span) Uc
C
URSUC
L
L
/221
combine withpreviousdefinition: R=biofoil length
c= biofoil width
Consider 2D biofoil starting from rest:
=0
=0
startingvortex
boundvortex
Required byKelvin’s Law
Consider 3D biofoil starting from rest:
startingvortex
tipvortex
boundvortex
Downward flowthrough centerof vortex ring
Circulation, , is constantalong vortex ring
Helmholtz’ Law requires that a vortex filament cannot end abruptly:
How is structure of vortex ring related to lift on biofoil?
Circulation, Area = A
forward velocity, U
Ring momentum =mass flux through
ring=A
Force = d/dt (A)
= d/dt(A)
= R U
Force/R = U = Kutta-Joukwski
R
Therefore, elongation of vortex ring is manifestation of force on biofoil.
Three important descriptors of fluid motion:
2. vorticity, (x,y)
1. velocity, u(x,y)
u(x,y)
ux
uy
x
y
uxyx
uy
3. circulation,
Fslap = m U / t
where m is bolus of accelerated water, moving atvelocity, u
impulse (F x t) = mass x velocity
Fstroke = A /t
Momentum of vortex ring A
= circulation
A