Abstract
The problem of flow and heat transfer due to an infinite flat surface suddenly set into motion in an unbounded mass of viscoelastic fluid is investigated under the consideration of time-dependent temperature distribution along the plate surface. A new type of similarity solution is devised that converts the governing partial differential equations into a set of non-linear ordinary differential equations with four physical parameters, viz., viscoelastic parameter k, unsteadiness parameter \(\beta \), Eckert number E and Prandtl number Pr. These equations are then solved numerically by finite-difference method after using the perturbation technique owing to the inherent unavailability of the necessary boundary conditions for solving this type of flow problem. The influences of these parameters on this flow dynamics are graphically analysed. The present analysis discloses that both the velocity and temperature at a given location decrease with the increase of the elasticity in the fluid as well as the unsteadiness of the flow field. The analysis reveals that the elastic property of the fluids causes the back-flow inside the boundary layer after a certain value of the unsteadiness parameter depending upon the presence of elasticity in the fluids. Another important result of this study that comes from the heat transfer analysis is that the elasticity of the fluids reduces the severity of the unwanted effect of the viscous heating.
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Abbreviations
- A :
-
temporal variation of the fluid velocity and wall temperature
- C :
-
dimensionless positive constant
- \(c_p\) :
-
specific heat
- \(C_f\) :
-
skin-friction coefficient
- \(e_{ik}\) :
-
rate-of-strain tensor
- E :
-
Eckert number
- \(E_{cr}\) :
-
critical value of E
- f :
-
similarity function
- k :
-
viscoelastic parameter
- \(k_0\) :
-
viscoelastic coefficient of the fluid
- \(Nu_x\) :
-
local Nusselt number
- p :
-
fluid pressure
- Pr :
-
Prandtl number
- \(Re_x\) :
-
local Reynolds number
- t :
-
time
- \(t_{0}\) :
-
constant reference value of t
- T :
-
fluid temperature
- \(T_{0}\) :
-
constant reference value of T
- \(T_w\) :
-
wall temperature
- \(T_{\infty }\) :
-
ambient fluid temperature
- u, v :
-
velocity components along and normal to the plate surface
- U :
-
plate velocity
- \(U_0\) :
-
velocity scale
- x, y :
-
coordinates along and normal to the plate surface
- \(\beta \) :
-
unsteadiness parameter
- \(\lambda \) :
-
thermal conductivity of the fluid
- \(\delta \) :
-
shear layer thickness (depth of penetration)
- \(\eta \) :
-
dimensionless distance normal to the plate surface
- \(\eta _s\) :
-
corresponding value of \(\eta \) where the wall effect on the fluid has dropped to one percent
- \(\mu \) :
-
dynamic coefficient of viscosity
- \(\nu \) :
-
kinematic coefficient of viscosity
- \(\psi \) :
-
stream function of the fluid
- \(\rho \) :
-
density of the fluid
- \(\tau _{ij}\) :
-
stress tensor
- \(\theta \) :
-
dimensionless temperature of the fluid
- 0:
-
reference
- cr :
-
critical
- w :
-
wall
- \({\prime }\) :
-
differentiation with respect to \(\eta \)
- \({{\varvec{\dot{}}}}\) :
-
differentiation with respect to \({{\bar{t}}}\)
- \({{\varvec{\bar{}}}}\) :
-
dimensionless quantities
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Acknowledgements
The author is very thankful to the editors and referees for their constructive suggestions that essentially improved the presentation of the paper. The author would also like to thank Shreya Dholey and Anita Dholey for their kind cooperation during the work. This work has been supported by SERB (No. EMR/2016/005533) of India.
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Dholey, S. Flow due to an infinite flat plate suddenly set into motion in a viscoelastic fluid: first Stokes problem. Sādhanā 44, 118 (2019). https://doi.org/10.1007/s12046-019-1098-9
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DOI: https://doi.org/10.1007/s12046-019-1098-9