4. 4
Vortex induced vibration (VIV) is suppressed when the splitter plate
length is large
The VIV decreases with decreasing of flexibility of splitter plate at
critical length.
The investigations on the effect of VIV using splitter plate
composed of viscoelastic material is still untouched.
To study the effect on VIV using linear viscoelastic model (standard linear
solid) of splitter plate
To perform the simulation using nonlinear viscoelastic models (Reese-
Govindjee Model)
5. Linear Viscoelastic models
5
WORK PRESENTED IN APS-I I
Maxwell Body:
Voigt Body:
Standard Linear Solid:
η E
1 0 1
d d
p q q
dt dt
1 0 1
p , 0,
q q
E
1 0 1, 1
p 0,q E q
1
1 0 1, 1
2 2
p , (1 )
E
q E q
E E
6. Study of static and dynamic behaviour of
Viscoelastic material
Validation of creep and relaxation using structure
solver (Tahoe) with derived analytical solution
Comparison of 2D Elastic and Viscoelastic splitter
plate behind cylinder
6
WORK PRESENTED IN APS-I I
7. Applications
Literature Review
Objectives of the present work
Finite Strain Viscoelastic
7
Study of Viscoelastic splitter plate behind the cylinder
2
9. • Chen et al. (2011). Analyzed the flutter . Either increasing the
structure-to-fluid ratio or decreasing dimensionless bending
stiffness ( )causes the system transits from periodic to
chaotic.
• Chen et al.(2014). Increase of either elastic or viscous component
of flag stabilizes the system.
• Tang et al. (2007) considered Kelvin-Voigt model , flutter amplitude
decreases with the increase of the material damping.
• Purohit et al. (2016). At lower flexibility forcing field of flowing field
dominates the vibration plate, as the plate stiffer plate response is
effected by elastic inertial force.
9
2 3
EI
u L
10. • The investigations of effect of flag material finite strain
viscoelastic model is scarce.
• Few studies has been done using Kelvin –Voigt model. Standard
linear solid model is very few.
• To study the stability of viscoelastic splitter plate attached behind
the cylinder.
• To study the effect on vibration amplitude with viscoelastic
parameters
10
11. Based on the multiplicative decomposition of deformation gradient into elastic and inelastic part
In thermodynamic equilibrium spring of maxwell element is relaxed , ,hence
Stress
For equilibrium and non equilibrium parts of material neo-Hookean model has been implemented
11
Second Piola-Kirchho stress tensor, 2
is strain energy density function, E Lagrangian strain tensor, C right Cauchy-Green deforformation tensor
ij
ij ij
ij ij
W W
S
E C
W
2
2 /3 2 2 2 2 2 2 2 2 2 2 2 2
1 1 2 3 2 1 2 2 3 1 3 3 1 2 3
2 2 2
1 2 3
W= ( 3) ( 1 1ln( )
4
, shear and bulk modulus, , invarients as I , ,
, , is Eigen values (principal stretch ratios) of Green deform
i
i i
k
I J J
k I J I I I I
2 2 2
1 2 3
ation tensor Cij, J=
2 2
1 2
1 1
Split of free energy, ( ) ( )
2 2
e eq neq e
E E
0
e
( )
eq
2
The ansatz, ( ) ( ), elastic right Cauchy-Green tensor (loosly speaking strain E )
eq neq e e
C C C
1
2 +2F F = , F deformation gradient of dashpot in fig
eq neq T
eq neq i i i
e
S S S
C C C
12. 12
Results
3
Free vibration of cantilever beam under time varying sinusoidal l
Vortex induced vibration of viscoelastic splitter plate behind a cy
13. 13
P1=7.125 N, P2=6.84 ( 50 nodes with 0.285 per node, p1 25, p2 24 nodes)
L=10 m , f(t) = sin(0.2t), density 10 kg/m3
Viscoelastic parameters
Kneq, Keq are bulk modulus corresponding to E2 and E1
Sneq, Seq are shear modulus for E2, E1 in N/m2
Relaxation time (sec)
A: tip (point A) vibration amplitude
Standard linear solid
2
/ E
14. cas
e
Keq Kneq Seq Sneq R.
time
A
1 2333.33 2333.33 500 500 0.1 9
2 2333.33 2333.33 500 500 1 8
3 2333.33 2333.33 500 500 2 6.6
4 2333.33 2333.33 500 500 10 4.7
5 2333.33 2333.33 500 500 100 4.5
6 2333.33 233333.33 500 50000 0.1 2.85
7 2333.33 233333.33 500 50000 1 0.3
8 2333.33 233333.33 500 50000 10 .07
9 233333.33 2333.33 50000 500 1 0.5
Variation of amplitude with relaxation time
29. For constant modulus
amplitude decreases with increase of viscosity
Steady state time decreases with decrease of viscosity
Steady state time increases with relaxation then further increasing the
relaxation time steady state time decreases
Amplitude increases with increase of relaxation time
29
30. The four dimensionless governing parameters for viscoelastic FSI are structure-to-
fuid density ratio, Young modulus (equilibrium and non equilibrium) , viscosity of
structure
Current study structure-to-fuid density ratio kept constant. Its effect also need to be
investigated.
Solving an FSI problem contrasting the behavior of hyperelastic vs. viscoelastic
solid using interaction of two splitter plates mounted on cylinders in cross flow.
As in hyperelastic vortex of one plate helps to enhance the amplitude and vice
versa. Its effect when damping is present in structure needs to be studied.
30