aoe 5104 class 9 online presentations for next class: –kinematics 2 and 3 homework 4 (6 questions,...
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AOE 5104 Class 9
• Online presentations for next class:– Kinematics 2 and 3
• Homework 4 (6 questions, 2 graded, 2 recitations, worth double, due 10/2)
• No office hours this week
Kinematics
Kinematics of Velocity
The Equations of MotionDifferential Form (for a fixed volume element)
V. Dt
D
).(2)()(f
)().(2)(f
)()().(2f
31
31
31
V
V
V
z
w
zy
w
z
v
yx
w
z
u
xz
p
Dt
Dw
y
w
z
v
zy
v
yy
u
x
v
xy
p
Dt
Dv
x
w
z
u
zy
u
x
v
yx
u
xx
p
Dt
Du
z
y
x
).(2)()()().(2)(
)()().(2).()(.)(
31
31
31
221
VV
VVVf
z
ww
y
w
z
vv
x
w
z
uu
zy
w
z
vw
y
vv
y
u
x
vu
y
x
w
z
uw
y
u
x
vv
x
uu
xTkp
Dt
VeD
The Continuity equation
The Navier Stokes’ equations
The Viscous Flow Energy Equation
v
p
Dt
Dff
V
Kinematic Concepts - Velocity
1. Fluid Line. Any continuous string of fluid particles. Moves with flow. Cannot be broken. Fluid loop – closed fluid line.
2. Particle Path. Locus traced out by an individual fluid particle.
1 23
4
www.lavision.de
Kinematic Concepts - Velocity3. Streamline. A line everywhere
tangent to the velocity vector. Never cross, except at a stagnation point. No flow across a streamline.
4. Streamsurface. Surface everywhere tangent to the velocity vector. Surface made by all the streamlines passing through a fixed curve in space. No flow through a stream surface. Infinite number of stream surfaces that contain a given streamline. A streamline must appear at the intersection of two stream surfaces.
5. Streamtube. Streamsurface rolled so as to form a tube. No flow through tube wall.
-2-1.5-1-0.500
0.5
1
1.5
(z-zw)/c
a
y/c a
x/ca=1.366, t=.165, regular trip, motion (no), Chit
Flow
Francis turbine simulation ETH Zurich
http://www.cg.inf.ethz.ch/~bauer/turbo/research_gallery.html
Mathematical Description
Flow
ds
VStreamline1. Streamlines 0Vsd
2. StreamsurfacesMake up a function (x,y,z,t) so that surfaces = const. are streamsurfaces. is called a ‘streamfunction’.
1 = const.2 = const.
3. Relationship between 1 and 2• Consider a streamline that sits at the intersection of two streamsurfaces. • The two streamsurfaces must be described by two different streamfunctions, say 1 and 2
• At any point on the streamline the perpendicular to each streamsurface, and the velocity must all be normal to each other
• So, what about that mathematical relationship?
u
w
dx
dz
w
v
dz
dy
u
v
dx
dy ;;
Flow
1 = const.2 = const.
Mathematical Description
21 V
)definition(By 0.. 21 V
0. V
21DirDir V
where = (x,y,z,t) and scalar
To find we take
So,
Steady flow: = ,Incompressible flow: = 1, Unsteady flow: streamlines largely meaningless
0. V0. V
1
2
V
Example: 2D – Flow Over An Airfoil
Take z2
100
11121 zyx
kji
V
xv
yu
11 ,
y
x
z
Find consistent relations for the steamfuncitons (implicit or in terms of the velocity field).
VV
k 2
Titan
Example: Spherical Flow
Choose const.) (2 r
Flow takes place in spherical shells (no radial velocity).
rr rrrr
eee
e
sin2
11
111
sin
001sin
11
rr
rrr
r
ee
eee
V
11 1,
sin
1
rV
rV
r
eree
r
Find a set of streamfunctions.
Kinematics of Vorticity
Hermann Ludwig Ferdinand von Helmholtz (1821-1894)
Vorticity =V• 2 circumferentially averaged
angular velocity of the fluid particles • Sum of rotation rates of 2
perpendicular fluid lines• Non-zero vorticity doesn’t imply
spin .=0. Incompressible?• Direction of ?
U
y
Always true!
Can be anything compared to V that the curl produces
No spin, but a net rotation rate
Circulation
•
• Macroscopic rotation of the fluid around loop C
• Non-zero circulation doesn’t imply spin
• Connected to vorticity flux through Stokes’ theorem
• Stokes’ for a closed surface?
C
dsV.
U
y
c
CS
ddS sVnΩ ..
Open Surface Swith Perimeter CndS
0. dSS
nΩ
Net outflow of vorticity is zero
Flow Past a ‘Cookie-Tin’
Pictures are from “An Album of Fluid Motion” by Van Dyke
Side view
Top view
‘Horseshoe vortex’
Re ~ 4,000
Large Eddy Simulation Re=5000
George Constantinescu IIHR, U. Iowa
Kinematic Concepts - VorticityBoundary layer growing on flat plate
Cylinder projecting from plate
Vortex Line: A line everywhere tangent to the vorticity vector. Vortex lines may not cross. Rarely are they streamlines. Thread together axes of spin of fluid particles. Given by ds=0.
Vortex sheet: Surface formed by all the vortex lines passing through the same curve in space. No vorticity flux through a vortex sheet, i.e. .ndS=0
Vortex tube: Vortex sheet rolled so as to form a tube.
ndS
Vortex line
Vortex tube
Vortex sheet
Vortex Tube
0. S
dSnΩ
dSdS nΩnΩ ..1sec2sec
Section 1
Section 2
ndS
c
CS
ddS sVnΩ ..
Since
12
So, we call
The Vortex Tube Strength
Implications (Helmholtz’ Vortex Theorems, Part 1)
• The strength of a vortex tube (defined as the circulation around it) is constant along the tube.
• The tube, and the vortex lines from which it is composed, can therefore never end. They must extend to infinity or form loops.
• The average vorticity magnitude inside a vortex tube is inversely proportional to the cross-sectional area of the tube
But, does the vortex tube travel along with the fluid, or does it have a life of it’s own?
Fluid loop C at time t
Same fluid loop at time t+dt
Vdt
(V+dV)dt
If it moves with the fluid, then the circulation around the fluid loop shown should stay the same.
CCC Dt
Ddd
Dt
Dd
Dt
D
Dt
D sVs
VsV ...
ds
dtDt
Ddd
ss
0
sVd
Dt
D
Dt
D
C
.
Fluid loop at time t
Same fluid loop at time t+dt
Vdt
(V+dV)dt
v
p
Dt
Dff
V
C
dDt
D
Dt
Ds
V.So the rate of change of around the fluid loop is
Now, the momentum eq. tell us that
Body force per unit mass
Pressure force per unit mass
Viscous force per unit mass, say fv
CCC
ddp
dDt
Dsfssf v ...
‘Body force torque’
‘Pressure force torque’
Viscous force ‘torque’
So, in general
Body Force Torque
kf g
SC
dSd nfsf ..Stokes Theorem
For gravity 0 f
So, body force torque is zero for gravity and for any irrotational body force field
Therefore, body force torque is zero for most practical situations
Pressure Force Torque0.
1.
1
SC
dSpdp ns
If density is constant
So, pressure force torque is zero. Also true as long as = (p).
Pressure torques generated by
• Curved shocks
• Free surface / stratificationEarth ScienceandEngineeringImperialCollege UK
Shock in a CD Nozzle
Bourgoing & Benay (2005), ONERA, France Schlieren visualizationSensitive to in-plane index of ref. gradient
Viscous Force Torque• Viscous force torques are non-zero where viscous forces
are present ( e.g. Boundary layer, wakes)
• Can be really small, even in viscous regions at high Reynolds numbers since viscous force is small in that case
• The viscous force torques can then often be ignored over short time periods or distances
Implications
In the absence of body-force torques, pressure torques and viscous torques…
• the circulation around a fluid loop stays constant: Kelvin’s Circulation Theorem
• a vortex tube travels with the fluid material (as though it were part of it), or– a vortex line will remain coincident with the same fluid line– the vorticity convects with the fluid material, and doesn’t diffuse– fluid with vorticity will always have it– fluid that has no vorticity will never get it
CCC
ddp
dDt
Dsfssf v ...
‘Body force torque’
‘Pressure force torque’
Viscous force ‘torque’
Helmholtz’ Vortex Theorems, Part 2
0Dt
D
Lord William Thompson Kelvin (1824-1907)
Vorticity Transport Equation
• The kinematic condition for convection of vortex lines with fluid lines is found as follows
0dsΩDt
D
VΩΩ
.Dt
D
After a lot of math we get....