2012
DOI: 10.1016/j.euromechflu.2012.01.016
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On the propagation of nonlinear acoustic waves in viscous and thermoviscous fluids

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Cited by 20 publications
(31 citation statements)
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“…As an illustration, consider the potential (7) with α 2 = 121/128. In this case, (18) takes the form…”
Section: T I C < T < T Ii Cmentioning
confidence: 99%
See 1 more Smart Citation
“…As an illustration, consider the potential (7) with α 2 = 121/128. In this case, (18) takes the form…”
Section: T I C < T < T Ii Cmentioning
confidence: 99%
“…The study of kinks (also known as topological solitons [13]) and domain walls in classical and quantum field theories [14,15], in theories of gravity and cosmology [16,17] and even in the nonlinear field theories of fluid * Electronic address: khare@iiserpune.ac.in † Electronic address: christov@lanl.gov ‡ Electronic address: avadh@lanl.gov mechanics [18] remains a topic of active research. Similarly, Ginzburg-Landau theories [19,20] have been very successful in explaining superconducting, superfluid and many other transitions as well as in modeling topological defects (e.g., vortices and domain walls) in a variety of functional materials, through the inclusion of the gradient of the relevant order parameter in the free energy.…”
Section: Introductionmentioning
confidence: 99%
“…differences between the traveling wave solutions of the original and the approximate equations. Here, we follow the approach in [43] and find the associated ODE of (A.1) to be…”
Section: Resultsmentioning
confidence: 99%
“…Taking the limit a 1 → 0, (4.9) reduces to 10) which is the special case of the Blackstock-Lesser-Seebass-Crighton model corresponding to classical lossless fluids; see Jordan et al (2012) and the references therein.…”
Section: (A) Bidirectional Equation Of Motionmentioning
confidence: 99%
“…If we now divide (4.9) by [1 − 2e(b − 1)f t ], which can never be zero, expand each occurrence of the reciprocal of this quantity in a binomial series (recall e 1) and then simplify and neglect terms O(e 2 ), our equation of motion becomes 11) which in the limit a 1 → 0 reduces to the lossless version of Kuznetsov's equation; again, see Jordan et al (2012) and the references therein. Because we have confined our attention to only right-running waves, let us now replace 3 the wave operator and the 'small' term (f t ) 2 in (4.11) with 2v t (v t + v x ) and (f x ) 2 , respectively.…”
Section: (B) Right-running Approximation: a Travelling Wave Solution mentioning
confidence: 99%