1 pharos university mech 253 fluid mechanics ii lecture # 5 inviscid flows
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Pharos UniversityMECH 253 FLUID
MECHANICS II
Lecture # 5 INVISCID FLOWS
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1 Inviscid Flow Inviscid flow implies that the viscous effect is
negligible. This occurs in the flow domain away from a solid boundary outside the boundary layer at Re.
The flows are governed by Euler Equations
where , v, and p can be functions of r and t .
gvvv
pt
)(
0)(
vt
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7.1 Inviscid Flow On the other hand, if flows are steady but
compressible, the governing equation becomes
where can be a function of r
For compressible flows, the state equation is needed; then, we will require the equation for temperature T also.
gvv p)(
0)( v
RTp
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7.1 Inviscid Flow
Compressible inviscid flows usually belong to the scope of aerodynamics of high speed flight of aircraft. Here we consider only incompressible inviscid flows.
For incompressible flow, the governing equations reduce to
where = constant.
gvvv
pt
)(
0 v
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7.1 Inviscid Flow For steady incompressible flow, the governing eqt reduce further to
where = constant. The equation of motion can be rewrited into
Take the scalar products with dr and integrate from a reference at along an arbitrary streamline =C , leads to
since
)(2
)v( 2
vv
zgp
gvv p)(
0 v
constant22
v 22
gz
vpgz
p
Calong0)d( rvvr
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7.1 Inviscid Flow If the constant (total energy per unit mass) is the same for
all streamlines, the path of the integral can be arbitrary, and in the flow domain except inside boundary
layers.
Finally, the governing equations for inviscid, irrotational steady flow are
Since is the vorticity , flows with are called irrotational flows.
0 v
0 v
0 v
vω 0 v
constant2
v2
gzp
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7.1 Inviscid Flow
Note that the velocity and pressure fields are decoupled. Hence, we can solve the velocity field from the continuity and vorticity equations. Then the pressure field is determined by Bernoulli equation.
A velocity potential exists for irrotational flow, such that,
and irrotationality is automatically satisfied.
v
0 v
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7.1 Inviscid Flow
The continuity equation becomes
which is also known as the Laplace equation.
Every potential satisfy this equation. Flows with the existence of potential functions satisfying the Laplace equation are called potential flow.
02
2
2
2
2
22
zyx
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7.1 Inviscid Flow The linearity of the governing equation for the flow fields
implies that different potential flows can be superposed.
If 1 and 2 are two potential flows, the sum =(1+2) also constitutes a potential flow. We have
However, the pressure cannot be superposed due to the nonlinearity in the Bernoulli equation, i.e.
21 vvv 2121 )(
21 ppp
Potential FlowsIntegral Equations Irrotational Flow Flow Potential Conservation of Mass
Laplace Equation
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If restricted to steady two dimensional potential flow, then the governing equations become
E.g. potential flow past a circular cylinder with D/L <<1 is a 2D potential flow near the middle of the cylinder, where both w component and /z0.
7.2 2D Potential Flows
L
D
U
x
y
z
0
y
v
x
uv
0
ky
u
x
vv
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The 2-D velocity potential function gives
and then the continuity equation becomes
The pressure distribution can be determined by the Bernoulli equation,
where p is the dynamic pressure
7.2 2D Potential Flows
xu
yv
02
2
2
22
yx
constant)( 2221 vup
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7.2 2D Potential Flows For 2D potential flows, a stream function (x,y) can also be
defined together with (x,y). In Cartisian coordinates,
where continuity equation is automatically satisfied, and irrotationality leads to the Laplace equation,
Both Laplace equations are satisfied for a 2D potential flow
02
2
2
22
yx
02
2
2
2
yx
02
2
2
2
yx
yu
xv
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7.2 Two-Dimensional Potential Flows For two-dimensional flows, become:
In a Cartesian coordinate system
In a Cylindrical coordinate system
v
y
,x
v,ujiv vu and
r,
rv,ur iiv vu rr and
Taking into account:
xv
yu
,
0
0
yxyxy
v
x
u
y
v
x
u
Continuity equation
Irrotational Flow Approximation
For 2D flows, we can also use the stream function Recall the definition of stream function for planar (x-y)
flows
Since vorticity is zero,
This proves that the Laplace equation holds for the stream function and the velocity potential
Cylindrical coordinate system
In cylindrical coordinates (r , q ,z ) with 0 /-axisymmetric case
Taking into account:
zrv
rru
1
,1
01111
)()(
0)()(
zrzrrzrr
rzrr
vr
vr
z
ur
r
rv
z
rur
rv
z
ru
Continuity equation
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7.2 Two-Dimensional Potential Flows Therefore, there exists a stream function such that in the Cartesian coordinate system and
in the cylindrical coordinate system.
The transformation between the two coordinate systems
r
,r
v,ur
x
,y
v,u
v
u
v
u ,
v
u
v
u rr
cossin
sin-cos
cossin-
sincos
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7.2 Two-Dimensional Potential Flows The potential function and the stream function are
conjugate pair of an analytical function in complex variable analysis. The conditions:
These are the Cauchy-Riemann conditions. The analytical property implies that the constant potential line and the constant streamline are orthogonal, i.e.,
and to imply that .
xyyx
and
u,v- v,u 0
Irrotational Flow Approximation
Irrotational approximation: vorticity is negligibly small
In general, inviscid regions are also irrotational, but there are situations where inviscid flow are rotational, e.g., solid body rotation
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7.3 Simple 2-D Potential Flows
Uniform Flow
Stagnation Flow
Source (Sink)
Free Vortex
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7.3.1 Uniform Flow
)( VU,v
yU
x
xV
y
VyUx VxUy
and
and
For a uniform flow given by , we have
Therefore,
Where the arbitrary integration constants are taken to be zero at the origin.
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7.3.1 Uniform Flow This is a simple uniform flow along a single direction.
22 vuU
Elementary Planar Irrotational FlowsUniform Stream
In Cartesian coordinates
Conversion to cylindrical coordinates can be achieved using the transformation
Proof with Mathematica
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7.3.2 Stagnation Flow For a stagnation flow, . Hence,
Therefore,
2 cos22
222 rB
)yx(B
xBy
y ,
yBx
x
By,Bx v
2sin 2
2rB
Bxy
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The flow an incoming far field flow which is perpendicular to the wall, and then turn its direction near the wall
The origin is the stagnation point of the flow. The velocity is zero there.
7.3.2 Stagnation Flow
x
y
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7.3.3 Source (Sink) Consider a line source at the origin along the z-
direction. The fluid flows radially outward from (or inward toward) the origin. If m denotes the flowrate per unit length, we have (source if m is positive and sink if negative).
Therefore,
mur r 2
ru
r
rr
mu
r r
02
and
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7.3.3 Source (Sink) The integration leads to
Where again the arbitrary integration constants are taken to be zero at .
rm
ln2
2
m
1,0,r
and
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A pure radial flow either away from source or into a sink A +ve m indicates a source, and –ve m indicates a sink The magnitude of the flow decrease as 1/r z direction = into the paper. (change graphics)
7.3.3 Source (Sink)
Elementary Planar Irrotational FlowsLine Source/Sink
Potential and streamfunction are derived by observing that volume flow rate across any circle is
This gives velocity components
Elementary Planar Irrotational FlowsLine Source/Sink
Using definition of (Ur, U)
These can be integrated to give and
Equations are for a source/sinkat the originProof with Mathematica
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7.3.4 Free Vortex Consider the flow circulating around the origin
with a constant circulation . We have: where fluid moves counter clockwise if is positive and clockwise if negative.
Therefore,
ur2
rru
r
ru
r r
20 and
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7.3.4 Free Vortex
2
rln2
1,0,r
and
The integration leads to
where again the arbitrary integration constants are taken to be zero at
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The potential represents a flow swirling around origin with a constant circulation .
The magnitude of the flow decrease as 1/r.
7.3.4 Free Vortex
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7.4. Superposition of 2-D Potential Flows Because the potential and stream functions
satisfy the linear Laplace equation, the superposition of two potential flow is also a potential flow.
From this, it is possible to construct potential flows of more complex geometry.
Source and Sink Doublet Source in Uniform Stream 2-D Rankine Ovals Flows Around a Circular Cylinder
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7.4.1 Source and Sink Consider a source of m at (-a, 0) and a sink of m at (a, 0)
For a point P with polar coordinate of (r, ). If the polar coordinate from (-a,0) to P is and from (a, 0) to P is
Then the stream function and potential function obtained by superposition are given by:
11 ,r
22 ,r
1212 lnln22
rrm
, m
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7.4.1 Source and Sink
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7.4.1 Source and Sink Hence,
Since
We have
12
1212 tantan1
tantantan
2tan
m
22
sin22tan
ar
ar
m
ar
r
ar
r
cos
sintan
cos
sintan 12 and
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7.4.1 Source and Sink We have
By
Therefore,
22
1- sin2tan
2 ar
arm
cos2cossin
cos2cossin22222
1
222222
arararrr
arararrr
cos2
cos2ln
2 22
22
arar
ararm
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7.4.1 Source and Sink The velocity component are:
sin2
sin
sin2
sin
2
cos2
cos
cos2
cos
2
2222
2222
arar
r
arar
rmv
arar
ar
arar
armu
Elementary Planar Irrotational FlowsDoublet
A doublet is a combination of a line sink and source of equal magnitude
Source
Sink
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7.4.1 Source and Sink
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7.4.2 Doublet The doublet occurs when a source and a sink
of the same strength are collocated the same location, say at the origin.
This can be obtained by placing a source at (-a,0) and a sink of equal strength at (a,0) and then letting a 0, and m , with ma keeping constant, say 2am=M
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7.4.2 Doublet For source of m at (-a,0) and sink of m at (a,0)
Under these limiting conditions of a0, m , we have
cos2
cos2
cos2lnlim
sin2sin2tanlim
22
22
0a
221-
0a
r
a
arar
arar
r
a
ar
ar
and ar
arm
22
1- sin2tan
2
cos2
cos2ln
2 22
22
arar
ararm
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7.4.2 Doublet Therefore, as a0 and m with 2am=M
The corresponding velocity components are
r
M
2
cosand
r
M
2
sin
22
sin
r
Mu
and 22
cos
r
Mun
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7.4.2 Doublet
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7.4.3 Source in Uniform Stream
Assuming the uniform flow U is in x-direction and the source of m at(0,0), the velocity potential and stream function of the superposed potential flow become:
2sin
2
ln2
cosln2
mUr
mUy
rm
Urrm
Ux
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7.4.3 Source in Uniform Stream
2m
ψ 2m
ψ
0ψ
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7.4.3 Source in Uniform Stream The velocity components are:
A stagnation point occurs at
Therefore, the streamline passing through the
stagnation point when .
The maximum height of the curve is
sin2
cos Ur
ur
mU
rur
and
U
mrs
2
and
Urm
ss 2
2
ms
and as r U
mrh 0
2sin
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7.4.3 Source in Uniform Stream
For underground flows in an aquifer of constant thickness, the flow through porous media are potential flows.
An injection well at the origin than act as a point source and the underground flow can be regarded as a uniform flow.
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7.4.4 2-D Rankine Ovals The 2D Rankine ovals are the results of the
superposition of equal strength sink and source at x=a and –a with a uniform flow in x-direction.
Hence,
12
12
2sin
lnln2
cos
mUr
rrm
Ur
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7.4.4 2-D Rankine Ovals Equivalently,
22
1
22
22
sin2tan
2sin
cos2
cos2ln
2cos
ar
armUr
arar
ararmUr
sin2
sin
sin2
sin
2
cos2
cos
cos2
cos
2
2222
2222
arar
r
arar
rmv
arar
ar
arar
armu
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7.4.4 2-D Rankine Ovals The stagnation points occur at
where with corresponding .
0
12
1
2
1
2
s
ss
y
Ua
m
a
xa
U
max
i.e., ,
0v 0s
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7.4.4 2-D Rankine Ovals The maximum height of the Rankine oval is
located at when ,i.e.,
which can only be solved numerically.
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,r 0 s
a
r
m
Ua
a
r
a
r
ar
armUr
o0
2tan1
2
1
02
tan2
2
0
220
010
or
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7.4.4 2-D Rankine Ovals
rs
ro
ro
rs
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7.4.5 Flows Around a Circular Cylinder
Steady Cylinder
Rotating Cylinder
Lift Force
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7.4.5.1 Steady Cylinder Flow around a steady circular cylinder is the
limiting case of a Rankine oval when a0.
This becomes the superposition of a uniform parallel flow with a doublet in x-direction.
Under this limit and with M=2a. m=constant,
is the radius of the cylinder.
2
1
0 2
U
Mrr s
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7.4.5.1 Steady Cylinder The stream function and velocity potential
become:
The radial and circumferential velocities are:
sin12
sinsin
cos12
coscos
2
2
2
2
r
rUr
r
MUr
r
rUr
r
MUr
o
o
and
sin1cos12
20
2
20
r
rUU
r
rUU r and
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7.4.5.1 Steady Cylinder
ro
Examples of Irrotational Flows Formed by Superposition
Flow over a circular cylinder: Free stream + doublet
Assume body is = 0 (r = a) K = Va2
Examples of Irrotational Flows Formed by Superposition Velocity field can be found
by differentiating streamfunction
On the cylinder surface (r=a)
Normal velocity (Ur) is zero, Tangential velocity (U) is non-zero slip condition.
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Rotating Cylinder The potential flows for a rotating cylinder is the free vortex
flow. Therefore, the potential flow of a uniform parallel flow past a rotating cylinder at high Reynolds number is the superposition of a uniform parallel flow, a doublet and free vortex.
Hence, the stream function and the velocity potential are given by
rr
rUr
r
rUr
ln2
sin1
2cos1
2
20
2
20
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Rotating Cylinder The radial and circumferential velocities are given by
rr
rU
ru
2sin1
2
20
cos1
2
20
r
rU
rur
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Rotating Cylinder
The stagnation points occur at
From
0 ssr uu
0cos
0cos12
20
s
os
s
rr
r
rU
:B Case
:A Case
0sru
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Rotating Cylinder
2
12
22
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4sin
14
02
sin2
Urryrx
Urry
Ur
rU u
rr
oosos
osos
o
oss
os
:A Case
when exits only Solution
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Rotating Cylinder
sr real positivefor implies which
with sign :B Case
Ur
UrUrr
r
rr
rU u
s
ss
ss
1
04
2
12
000
2
20
144
02
10
1sin0cos
68
Rotating Cylinder
The stagnation points occur at
Case 1:
Case 2:
Case 3:
14 0
Ur
14 0
Ur
14 0
Ur
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Rotating Cylinder
Case 1:
14 0
Ur
2
12
0000 41
4
Urr
x
Urr
y ss
and
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Rotating Cylinder Case 2:
The two stagnation points merge to one at cylinder surface where .
14 0
Ur
00 r,y,x ss
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Rotating Cylinder Case 3:
The stagnation point occurs outside the cylinder
when where . The condition of
leads to
Therefore, as , we have
14 0
Ur
ss ry 0u2
2
12
0000
144
UrUrr
r
r
y ss
14 0
Ur
1
2 00
Urr
ys
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Rotating Cylinder
Case 3: 14 0
Ur
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Lift Force
The force per unit length of cylinder due to pressure on the cylinder surface can be obtained by integrating the surface pressure around the cylinder.
The tangential velocity along the cylinder surface is obtained by letting r=ro,
0
0 2sin2
0r
Ur
urr
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Lift Force The surface pressure as obtained from Bernoulli
equation is
where is the pressure at far away from the cylinder.
0p
22
2sin2
00
2
2
Up
rU
p
p
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Lift Force
Hence,
The force due to pressure in x and y directions are then obtained by
22
02
2
0
20 4
sin2
sin412 UrUr
Up p
2
drp drp dpFFCCyx ]sincos[ 00000 jiji sF
UdrpF drpF yx 0
2
0 00
2
0 0 sin0cos and
ji drd o sincos swhere
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Lift Force The lift on rotating bodies is called the Magnus effect. the lift force is due to the circulation around the body.
An airfoil without rotation can develop a circulation around the airfoil when Kutta condition is satisfied at the rear tip of the airfoil.
Therefore, The tangential velocity along the cylinder surface is obtained by letting r=ro:
This forms the base of aerodynamic theory of airplane.