naviers
TRANSCRIPT
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PRESENTED BY:
1NAVIER'S-STOKES EQUATION
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` Fora fluid of constant density and constant
viscosity we used equationof motion known as
Naviers-stokes equation.` In vector form:
gVP
Dt
DV!
2V
2NAVIER'S-STOKES EQUATION
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` Considera volume element,now the momentun
balance onthe element as
` Rate of accumulation = (rate of momentum in)-(rate of momentum out)+(forces actingonthe
system)
` eqn-(1)
` The velocityof fluid In cartesian form
kwjviuV !
3NAVIER'S-STOKES EQUATION
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` Considerthe fluid flowsthoughthe six facesofthe
element.First we considered that
` The fluid flowingthroughthe x-direction:
` Momentum enters at x =
` Momentum leaves at x+x =
` Similarly fory-direction:
`
Momentum enters aty =` Momentum leaves aty+y =
zyuux
(()(V
zyuuxx ((()(V
zxuu y (()(V
zxuuyy
(((
)(V
4NAVIER'S-STOKES EQUATION
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` Forz-direction:
` Momentum enters at z =` Momentum leaves at z+z =
` Now the net convective flow throughthe element:
eqn-(2)
yxuuz
(()(V
yxuuzz
((()(V
])()[(
])()[(])()[(
zzz
yyyxxx
uuuuyx
uuuuzxuuuuzy
(
((
((
((((
5NAVIER'S-STOKES EQUATION
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` Now the normal stress actingonthe element:
`
` Normal Stress actingonthe x-face:
` Normal stress at x =
` Normal stress at x+x =
` Similarlynormal stress actingony-face:
` Normal stress aty =
`
Normal stress aty+y =
zyxxx
(()(X
zyxxxx
(((
X
zxyyx
((X
zxyyyx (((X
6NAVIER'S-STOKES EQUATION
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` Forthe z-face:
` Normal stress at z =` Normal stress at z+z =
` The netnormal stress actingonthe element:
`
eqn-(3)
` The shearstressresult from the deformationof
the volume element.
yxz
zxX
yxzzzx
X
][
][][
zzzxzzx
yyyyxxxxxxxx
yx
yxzxzy
(
((
((
((((
7NAVIER'S-STOKES EQUATION
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` The fores arise due tothe system is fluid pressure
p and the gravitational force perunit massg.
` The resultantofthe forces inthe x-direction:
` eqn-(4)` Finallythe rate of accumulationof x momentum
withinthe element isx yz (u/ t)
` Substitute all the above expression inthe equationno. 1 and resulting equation divide
zyxgppzyxxxx
V
8NAVIER'S-STOKES EQUATION
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` byxyz.takingthe limit asx,y, and z
appoachesto zerogivesthe x componentofthe
equationof motion:
` eqn-(5)
xzxyxxxg
x
p
ttt
wu
t
vu
t
uu
t
u
t
VXXX
VVVV
x
x
x
x
x
x
x
x
x
x
x
x
x
x!
x
x
)(
)(
9NAVIER'S-STOKES EQUATION
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` The equation isrearranged withthe help of
equationof continuitytogive:
`
eqn-(6)` Similarequation may be derived forthe y and z
components. Addingthe three equation vectorially
gives
` eqn-(7)
xzxyxxx gzyxt
p
Dt
DuVXXXV
x
x
x
x
x
x
x
x! )(
gpDt
DV VXV ! ][
10NAVIER'S-STOKES EQUATION
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` The stress at any point is dependsonthe velocity
gradient and the rheological propertiesofthe fluids.Forthe newtonian fluids,the x-direction component
ofthe stresstensorare
` eqn-(8)
eqn-(9)
eqn-(10)
z
w
y
v
x
uV
x
v
y
u
Vx
u
yxxy
xx
x
x
x
x
x
x!
x
x
x
x!!
x
x!
)(
))(3
2(2
QXX
OQQX
11NAVIER'S-STOKES EQUATION
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` Where k= bulk viscosity
` The general equationof motion fora newtonian
fluid with varying and viscosity are exemplified by
the following equation forthe x direction:
`
` eqn(11)
xg
z
u
x
w
zx
v
y
u
y
Vx
u
x
p
Dt
Du
VQ
OQQV
xx
xx
xx
xx
xx
xx
xx
xx
!
][][
])3
2(2[
12NAVIER'S-STOKES EQUATION
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z
y
gVz
w
z
z
v
y
w
yz
v
x
w
xz
p
Dt
Dw
gz
v
y
w
z
Vy
v
y
y
u
x
v
xy
p
Dt
Dv
VOQQ
QQV
VQ
OQQ
QV
xx
xx
x
x
x
x
x
x
x
x
x
x
x
x
x
x!
xx
xx
xx
xx
xx
xx
xx
xx
xx
!
]3
22[
][][
][
]3
22[
][
13NAVIER'S-STOKES EQUATION
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` Fora fluid of constant density and constant viscosity
the equations (5) becomes
`
` eqn(14)
` eqn(15)
xx
xx
xx
xx
z
uw
y
uv
x
uu
t
uV
xg
x
p
z
u
y
u
x
u VQ xx
xx
xx
xx! )(
2
2
2
2
2
2
x
x
x
x
x
x
x
x
z
u
w
u
v
u
ut
u
V
gp
z
uuuVQ
x
x
x
x
x
x
x
x!
2
2
2
2
2
2
14NAVIER'S-STOKES EQUATION
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x
x
x
x
x
x
x
x
z
uw
y
uv
x
uu
t
wV
zg
z
p
z
w
y
w
x
wVQ
x
x
x
x
x
x
x
x!
2
2
2
2
2
2
gVpDt
DVVQV ! 2
15NAVIER'S-STOKES EQUATION
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` Unitoperationof chemical engineering-MacCabe
smith and harriott
NAVIER'S-STOKES EQUATION 16