examples of potential flows source flow all rights reserved by don moorcroft
DESCRIPTION
Polar coordinates Cartesian coordinatesTRANSCRIPT
02 Examples of Potential Flows
SOURCE FLOW
All rights reserved by don moorcroft
02 Examples of Potential Flows
u
SOURCE FLOW
x
yr
xu
yv
Cartesian coordinates
Potential Function
02
u
rQur
rrQur
2
01
ru
Polar coordinates
rur
r
u 1
xu
yv
Cartesian coordinates
rrQ
2
01
r
rQur 2
sincos ryrx
ry
yrx
xr
ruvu sincos
rrQ
2
01
r
cfrQ
ln
2
crf
rQ ln2
rQ
rur
2
1
0
r
u
2Q
cf
2Q
crfQ
2
For a SINK flow, Q will be negative
Stream Function
Kundu’s book p. 69
All rights reserved by don moorcroft
02 Examples of Potential FlowsIRROTATIONAL
VORTEX
02
rur
u
The circulation along any circle around the origin is a constant
edrd ˆ
constdrudu
2
0
2
0 22ddr
r
As a potential flow, it is irrotational & incompressible
011
ur
urrr
u r
011
rur
urrr
u
02
rur
u
IRROTATIONALVORTEX
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02
rur
u
IRROTATIONAL VORTEX Potential Function
0
r
ur cf
rru
21
c
2
02
rur
u
VORTEX Stream Function
rru
2
01
rur
cfr
ln
2
crf
DOUBLET (Sources and Sinks)
x
y
source sink Both have strength Q. The flow field can be obtained by combining the potential function for the sink φ2 and the source φ1. Laplace’s function is linear – linear superposition is valid.
21
2222 ln2
ln2
yxQyxQ
0, 0,
221 ln
4yxQ
222221 lnln
4
Oyx
xyxQ
Taylor expansion
221 ln
4yxQ
2
2222
12ln
4
O
yxxyxQ
2
2222
22ln
4
Oyx
xyxQSimilarly
2
22214
4
Oyx
xQ
Q
rrr
yxx
coscos
222
22 yxx
In the same way ψ2 and ψ 1 can be added because Laplace’s function is linear – linear superposition is valid.
xy
xyQ 11 tantan
2
222
11 tantan
O
yxy
xy
xy
222
2 yxyQ
22 yxy
Q
22 yxy