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P. R. Naren

School of Chemical & Biotechnology

SASTRA Deemed to be University

Thanjavur 613401

E-mail:

[email protected]

at

One Week

National Workshop on Advances in Computational Mechanics

School of Mechanical Engineering

SASTRA Deemed to be University

Thanjavur 613401

(2)

Outline

Conservation equations and control volume

Eulerian and Lagrangian framework

Integral form of conservation equation

FVM approach

Steady state diffusion equation in 1D

Convective term

(3)

Governing Equations

Conservation of mass

Conservation of momentum

Conservation of energy

Concept of CV

*

m

lim

  

 



(4)

Framework

Eulerian

Fixed reference

Infinitesimally small

control volume

Differential form

Lagrangian

Moving reference

Finite control volume

Integral form

Gross behaviour

(5)

Advection

i

V

N

T

P

i

V

N

T

P

i

u

N

T

P

i i

u

u

N

N

T

T

P

 

  

 

 

x

P

i

m

u A

P m u

Q mC T

N

 

P

i

1

u

C T

x

P

m

P

u

Q

C T

N

 



 



 



(6)

Generic Transport Equation

Transport equation for a quantity

f

Accumulation + Net outflow = Net Diffusion + Net source

 

div( V )

div

grad

S

t

f

 f

 f 

f 



Equation

Specific quantity

f

per unit mass)

S

f

Mass balance

1

0

0

Momentum

balance

u

m

g

Energy balance

C

p

T

k

-D

H

R

UA

D

T

Species balance i

x

i

D

r

i

P

(7)

Mass Balance

Mass

d i v (

)

0

t

 

U

 

u

 

v

w

0

t

x

y

z

 

 

 

 

(8)

Momentum Balance

Navier Stokes

M

D

div

div

S

Dt

U

p

 

Mx

u

p

div( u )

div

grad u S

t

x

 

 -

m

U

Navier

(9)

Numerical Techniques

Finite Difference

Finite Element

Finite Volume

(10)
(11)
(12)

Illustration: 1D heat Conduction

Steady state 1D heat conduction in a solid rod with ends kept at fixed temp

Model Formulation

Axisymmetric

q

L >> D

Radial variation ignored

No heat loss thro’ surrounding

Governing equation

BC: z = 0 T = T

A

; z = L T = T

B

with constant thermo-physical properties

T

A

T

B

L

T

A

T

B

d

d T

0

d z

d z

axisymmetric

(13)

Solution to Heat Conduction in Rod

Analytical Solution

Continuous

Numerical solution

Finite Difference

Solution at discrete points

Affected by

D

z

T

A

T

B

T

A

T

B

T

A

T

B

Finite Diff

Grids

Soln

B

A

A

T

T

T

T

z

L

-

i 1

i

i 1

1

A

T

2 T

T

0

i

2 to N 1

T

T

-

(14)
(15)

Issues with Finite Difference

Solution discrete vs. governing equation continuous

Treatment of local source terms

Discontinuities in solution

(16)

Integral Form of Conservation Equation

 

S

x

dx

d

dx

d

u

dx

d

f

f

f

 

f

f

f

f

div

u

div

grad

S

t

f

u

div

grad

f

S

f

div

x

d

u d

d

d

d

S d

d x

d x

d x

f

D  D  D 

f

 f

 

 

Gau

b

x

d

u S. d x

d

d

S. d x

S

S.d x

d x

d x

d x

f

f

 f

For steady state flow

For 1D flow

(17)

Integral Form of Momentum Equation

(18)

FVM Approach for Heat Conduction

Computational domain for

heat conduction in rod

Temperature at node is

average of CV around the

node

Boundary nodes

Internal nodes

T

A

T

B

T

A

T

B

(19)

S

x

dx

d

dx

d

u

dx

d

f

f

f

dV

S

dV

dx

d

dx

d

dV

u

dx

d

V x V

V

D f D

D

f

f

P

E

W

w

e

s

n

S

N

Finite Volume Formulation

 

f

f

f

f

S

grad

div

u

div

t

f

u

div

grad

f

S

f

(20)

Some Mathematics !!

Taylor Series

(21)

P

E

W

w

e

s

n

S

N

Finite Volume Formulation . . .

dV

S

dV

dx

d

dx

d

dV

u

dx

d

V x V

V

D f D

D

f

f

 

e

w

V

u

u

dV

u

dx

d

f

f

-

f

D

 

 

u

u

2

u

u

2

u

u

W E

P W

P E

f

-f

f

f

-f

f

(22)

P

E

Finite Volume Formulation . . .

(23)

Finite Volume Formulation

P

E

W

w

e

s

n

S

N

f

f

f

f

a

a

s

a

P

P

W

W

E

E

f

f

f

f

f

f

a

a

a

a

s

a

P

P

W

W

E

E

N

N

S

S

dV

S

dV

dx

d

dx

d

dV

u

dx

d

V

x

V

V

D

f

D

D

f

(24)

   

e

w

V

p

p

dV

x

p

-

-

D

 

2

p

p

2

p

p

2

p

p

W

E

W

P

P

E

-

-

P

E

W

w

e

s

n

S

N

Difficulty in pressure term discretization

Checker board

Solution?

Suhas V Patankar

(25)

Summary

Finite volume

Solution represent average over the region NOT a point

solution

Finite volume approach applied to Integral form of

Conservation equation

Discretization of diffusion and advective terms

How to get values of advected quantities at face

f

e

f

w

?

Other alternatives

(26)

Resources

Chung T. J. (2002)

Computational Fluid Dynamics

. Cambridge University Press

Date A. W. (2005).

Introduction to Computational Fluid Dynamics

. Cambridge University Press

Fox, R. O. (2003)

Computational Models for Turbulent Reacting Flows

. Cambridge University

Press

Hoffmann K. A. and Chiang S. T. (2000).

Computational Fluid Dynamics

Vol1, 2 and 3.

Engineering Education System, Kansas, USA.

John F. W., Anderson, J.D. (1996)

Computational Fluid Dynamics: An Introduction

Springer

Patankar, S. (1980)

Numerical Heat Transfer and Fluid Flow

. Taylor and Francis

Ranade, V.V. (2002).

Computational Flow Modeling for Chemical Reactor Engineering

,

Academic Press, New York.

(27)

Web Resources

http://www.cfd-online.com

http://en.wikipedia.org/wiki/Computational_fluid_dynamics

http://www.cfdreview.com/

https://confluence.cornell.edu/display/SIMULATION/FLUENT

+Learning+Modules

http://weblab.open.ac.uk/firstflight/forces/#

NPTEL

(28)

Gratitude

Dr. Vivek V. Ranade – My Mentor Guide and Teacher

iFMg - Research group at NCL, Pune

Audience

(29)

THANK YOU

A person who never made a

mistake never tried anything new

- Albert Einstein

(30)
(31)
(32)
(33)

dV

(34)
(35)
(36)
(37)
(38)

I,J I 1,J

J , i J ,

i

u

au

p

p

a

-

-

dV

y

u

y

dV

x

u

x

dV

x

p

dV

y

vu

dv

x

uu

V V

V V

V

D D

D D

D





m

m

-

Referensi

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