On Temporal instability of Electrically forced jets with nonzero basic state velocity

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ON TEMPORAL INSTABILITY OF ELECTRICALLY FORCED JETS WITH NONZERO BASIC STATE VELOCITY Sayantan Das(SD) Masters Student @ UT Pan Am Mentors :Dr . D.N. Riahi & Dr. D. Bhatta

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On Temporal instability of Electrically forced jets with nonzero basic state velocity. Sayantan Das(SD)  Masters Student @ UT Pan Am Mentors : Dr . D.N. Riahi & Dr. D. Bhatta. In other words…. What is electro-spinning?. Process of producing nano -fibers - PowerPoint PPT Presentation

Transcript of On Temporal instability of Electrically forced jets with nonzero basic state velocity

Page 1: On  Temporal instability of Electrically forced jets with nonzero basic state velocity

ON TEMPORAL INSTABILITY

OF ELECTRICALLY FORCED JETS WITH NONZERO

BASIC STATE VELOCITYSayantan Das(SD)

Masters Student @ UT Pan Am

Mentors :Dr . D.N. Riahi & Dr. D. Bhatta

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IN OTHER WORDS…

Modeling instabilities of the Electro spinning process

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WHAT IS ELECTRO -SPINNING?

Process of producing nano-fibers

http://nano.mtu.edu/Electrospinning_start.html

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QUALITY NANOFIBERS

unparalleled in their porosity, high surface areafineness and uniformity

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STABILITY?

. Here stability in terms of perturbation is considered

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IN DETAIL

Schematic Representation

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To detect and understand temporal

instabilities Parameter regime

under which Instabilities are

strong Subsequent ways

to control and eliminate such instabilities

WHY

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WE USE,ELECTRO-HYDRODYNAMIC

EQUATION mass conservation D/Dt+.u=0

(1a) momentum Du/Dt =P+.( u)+qE

(1b) charge conservation Dq/Dt+.(KE)=0

(1c) electric potential E=

(1d) D/Dt =/t+ u. - total derivative t-time variable

u-velocity vector P-pressure E -

electric field vector -electric potential q- charge

-fluid density -dynamic viscosity K-conductivity

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HOW WE MODEL?

We non- dimensionaliz

e 1(a-d)

We get four non

dimensional equation 2(a-

d)

Using perturbation technique we linearize the

PDE,s

Forming 4x4

determinant , we get the Dispersi

on relation

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THE NON DIMENSIONAL EQN

022

vh

zh

t (2a)

2

2

3

2

2

2

24

811

E

zh

zh

zh

hzz

vvtv

zvh

zhhE 2

2

32 (2c)

hz

Ehz

EzEb 42

)ln()( 22

2

(2d)

 

021 2

KEh

zhv

zh

t (2b)

  All the constant parameters are from Hohman et al 2001

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PERTURBATION TECHNIQUE

We consider (h,v, , E)= Perturbation quantities , by subscript ‘1’

Where, =()exp( )are assumed to be small in magnitude

Basic state solution , by subscript ‘b’

Linearized w.r.t. amplitude

The complex growth rate ()

k is the axial wave number

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MATHEMATICALLY We plug in (h,v, , E) in the non dimensional equation

We then get the coefficient of each dependent variable for each equations

Then we form a 4X4 Determinant of the coefficients .

Then by finding a nontrivial solution , we find the DISPERSION RELATION

DISPERSION RELATION tells us about the growth rate &frequency of the perturbations

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OUR WORK

Hohman et.al ,2001, considered the basic state velocity to be zero

We considered basic state velocity to be a non zero and a constant quantity

Considering this case we derived the DISPERSION RELATION

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DISPERSION RELATION

Where,

0322

13 TTT

KivkkT b

431

414412

21 2

22

22

b

bEKkkT

kKkiviv bb

863

2124

4214 2

222

3

kEiEkKk

T bbb

b

KEkvik b

bb

1214442

1 222

3

bb ikvKkvk

43 222

2,),(ln,89.01 2 kk

We get ,

with;

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COMPUTATIONAL

We use Matlab to produce the zeroes of the dispersion relation

In Matlab we used the inbuilt function Fzero

Fzero finds the root of a function

For growth rate we considered the real part of

For frequency we considered the imaginary part of

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RESULTS

Growth rate v/s Wave number for K*=inf ,vb=1, and variable applied field

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Growth rate v/s Wave number for K*=0,vb=1,and variable applied field

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MORE…

Growth rate v/s Wave number for K*=19.3 ,vb=1, for variable applied field

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Growth rate v/s Wave number for K*=19.3,v*=0.3,sigmab=0.1vb=1,Eb varied

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Contd….

Primary and Secondary modes with K*=19.3,sigmab=0.1,vb=1,Eb=2.9,&v*=0

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SO…• The variable applied field is stabilizing

• The finite values of either viscosity or conductivity are stabilizing

• There are two modes of instability for small values of the wavenumber

• All above results comply with Hohman et al with zero basic state velocity

• Hence,the growth rate in temporal instabilty is unaffected by the value of the basic state velocity, but significant changes are already seen in spatial instability cases.

• So is our work is of no importance ? with vb being nonzero

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NO The non zero basic state velocity significantly

affects the frequency of the perturbed state

Hence also affects the period

Which is significant for producing quality fibers

LETS SEE HOW

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FIGURE

Frequency v/s k, with K*=0,v*=0,sigmab=0.1,Eb=2.9

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Frequency v/s k, with K*=19.3,v*=0,sigmab=0.1,Eb=2.9

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HENCE

More the vb less is the frequency , hence more is the period

Presence of conductivity increases the period

As velocity of the wave is proportional to the negative frequency

As vb increases the velocity of the wave increases (Obvious)

Hence production of nanofibers will be affected

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FUTURE STUDIES…• Investigate the case for spatial instability with

non zero basic state velocity

• Investigate combined spatial and temporal instability with non zero basic state velocity

• Investigate non-linear model

• Investigate non axisymmetric case

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THANK YOU ALL…

My special thanks to Dr Bhatta, & Dr Riahi for the support and enthusiasm…..

Any questions or comments are gladly welcomed