Exact solution for motion of an Oldroyd-B fluid over an infinite flat plate that applies an oscillating shear stress to the fluid
The unsteady motion of an Oldroyd-B fluid over an infinite flat plate is studied by means of the Laplace and Fourier transforms. After time t = 0, the plate applies cosine/sine oscillating shear stress to the fluid. The solutions that have been obtained are presented as a sum of steady-state and tra...
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Published in | Boundary value problems Vol. 2012; no. 1; pp. 1 - 19 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Cham
Springer International Publishing
24.04.2012
Hindawi Limited BioMed Central Ltd |
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ISSN | 1687-2770 1687-2762 1687-2770 |
DOI | 10.1186/1687-2770-2012-48 |
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Abstract | The unsteady motion of an Oldroyd-B fluid over an infinite flat plate is studied by means of the Laplace and Fourier transforms. After time
t
= 0, the plate applies cosine/sine oscillating shear stress to the fluid. The solutions that have been obtained are presented as a sum of steady-state and transient solutions and can be easily reduced to the similar solutions corresponding to Newtonian or Maxwell fluids. They describe the motion of the fluid some time after its initiation. After that time when the transients disappear, the motion is described by the steady-state solutions that are periodic in time and independent of the initial conditions. Finally, the required time to reach the steady-state is established by graphical illustrations. It is lower for cosine oscillations in comparison with sine oscillations of the shear, decreases with respect to
ω
and
λ
and increases with regard to
λ
r
.
Mathematical Subject Classification (2010):
76A05; 76A10.
PACS:
47.50.-d; 47.85.-g. |
---|---|
AbstractList | The unsteady motion of an Oldroyd-B fluid over an infinite flat plate is studied by means of the Laplace and Fourier transforms. After time
t
= 0, the plate applies cosine/sine oscillating shear stress to the fluid. The solutions that have been obtained are presented as a sum of steady-state and transient solutions and can be easily reduced to the similar solutions corresponding to Newtonian or Maxwell fluids. They describe the motion of the fluid some time after its initiation. After that time when the transients disappear, the motion is described by the steady-state solutions that are periodic in time and independent of the initial conditions. Finally, the required time to reach the steady-state is established by graphical illustrations. It is lower for cosine oscillations in comparison with sine oscillations of the shear, decreases with respect to
ω
and
λ
and increases with regard to
λ
r
.
Mathematical Subject Classification (2010):
76A05; 76A10.
PACS:
47.50.-d; 47.85.-g. The unsteady motion of an Oldroyd-B fluid over an infinite flat plate is studied by means of the Laplace and Fourier transforms. After time t = 0, the plate applies cosine/sine oscillating shear stress to the fluid. The solutions that have been obtained are presented as a sum of steady-state and transient solutions and can be easily reduced to the similar solutions corresponding to Newtonian or Maxwell fluids. They describe the motion of the fluid some time after its initiation. After that time when the transients disappear, the motion is described by the steady-state solutions that are periodic in time and independent of the initial conditions. Finally, the required time to reach the steady-state is established by graphical illustrations. It is lower for cosine oscillations in comparison with sine oscillations of the shear, decreases with respect to omega and lambda and increases with regard to lambda sub( )r Mathematical Subject Classification (2010): 76A05; 76A10. PACS: 47.50.-d; 47.85.-g. The unsteady motion of an Oldroyd-B fluid over an infinite flat plate is studied by means of the Laplace and Fourier transforms. After time t = 0, the plate applies cosine/sine oscillating shear stress to the fluid. The solutions that have been obtained are presented as a sum of steady-state and transient solutions and can be easily reduced to the similar solutions corresponding to Newtonian or Maxwell fluids. They describe the motion of the fluid some time after its initiation. After that time when the transients disappear, the motion is described by the steady-state solutions that are periodic in time and independent of the initial conditions. Finally, the required time to reach the steady-state is established by graphical illustrations. It is lower for cosine oscillations in comparison with sine oscillations of the shear, decreases with respect to ω and λ and increases with regard to λr.Mathematical Subject Classification (2010): 76A05; 76A10.PACS: 47.50.-d; 47.85.-g. The unsteady motion of an Oldroyd-B fluid over an infinite flat plate is studied by means of the Laplace and Fourier transforms. After time t = 0, the plate applies cosine/sine oscillating shear stress to the fluid. The solutions that have been obtained are presented as a sum of steady-state and transient solutions and can be easily reduced to the similar solutions corresponding to Newtonian or Maxwell fluids. They describe the motion of the fluid some time after its initiation. After that time when the transients disappear, the motion is described by the steady-state solutions that are periodic in time and independent of the initial conditions. Finally, the required time to reach the steady-state is established by graphical illustrations. It is lower for cosine oscillations in comparison with sine oscillations of the shear, decreases with respect to Ï[per thousand] and λ and increases with regard to λ ^sub r^. Mathematical Subject Classification (2010): 76A05; 76A10. PACS: 47.50.-d; 47.85.-g.[PUBLICATION ABSTRACT] |
ArticleNumber | 48 |
Author | Siddique, Imran Shahid, Nazish Rana, Mehwish |
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Cites_doi | 10.1016/0020-7462(82)90006-3 10.1007/BF01975401 10.1007/BF01177223 10.1016/S0377-0257(99)00023-3 10.1016/S0020-7462(98)00063-8 10.1115/1.2830061 10.1007/BF01595580 10.1007/BF01212645 10.1016/j.ijengsci.2004.12.009 10.1016/j.ijengsci.2006.04.010 10.1007/s00033-006-0063-8 10.1007/s11012-007-9081-7 10.1016/j.nonrwa.2010.02.004 10.1016/S0020-7462(99)00019-0 10.1016/j.cnsns.2011.05.004 10.1016/j.nonrwa.2008.10.055 10.1017/S0022112068000509 10.1007/BF01236358 10.1016/j.jnnfm.2008.02.005 10.1016/j.nucengdes.2011.11.024 10.1016/j.apm.2005.11.032 10.2478/s11534-010-0073-1 |
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Copyright | Shahid et al; licensee Springer. 2012. This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License ( ), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Springer International Publishing AG 2012 |
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Snippet | The unsteady motion of an Oldroyd-B fluid over an infinite flat plate is studied by means of the Laplace and Fourier transforms. After time
t
= 0, the plate... The unsteady motion of an Oldroyd-B fluid over an infinite flat plate is studied by means of the Laplace and Fourier transforms. After time t = 0, the plate... |
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SubjectTerms | Analysis Approximations and Expansions Boundary value problems Computational fluid dynamics Difference and Functional Equations Flat plates Fluid flow Fluids Mathematical analysis Mathematics Mathematics and Statistics Ordinary Differential Equations Oscillating Oscillations Partial Differential Equations Trigonometric functions |
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Title | Exact solution for motion of an Oldroyd-B fluid over an infinite flat plate that applies an oscillating shear stress to the fluid |
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