Search engine for discovering works of Art, research articles, and books related to Art and Culture
ShareThis
Javascript must be enabled to continue!

Modular Korteweg - de Vries equation: Riemann, cnoidal and solitary waves

View through CrossRef
<p>The review paper by Oleg Rudenko [1] suggests several examples of elastic systems with so-called modular nonlinearities. In this study we consider the modular Korteweg - de Vries (KdV) equation in the form u_t + 6 u u_x + u_{xxx} = 0. This equation is not integrable by means of the Inverse Scattering Transform in the general case, but sign-defined functions which never change the sign satisfy the integrable KdV equation, and hence possess an exact solution. Firstly, we consider the dispersionless limit of the modular KdV equation and analyze the evolution of a simple nonlinear wave (Riemann wave) and its Fourier transform including the asymptotics when the wave tends to break [2]. Then, we study the structure of travelling waves. If the waves propagate on a pedestal and do not cross the zero level u = 0, they coincide with the well-known travelling wave solutions of the classic KdV equation in the form of cnoidal and solitary waves. If the pedestal is zero, the structure of sign-varying travelling waves is expressed through Jacobi elliptic functions. The interaction of solitary waves of different polarities is studied numerically using an implicit pseudo-spectral method. The simulation has revealed the inelastic character of the collision; in the course of the interaction the solitons can alter their amplitudes (the small soliton decreases and the large one grows) and emit small-amplitude waves. The inelastic effects are most pronounced when the solitons’ amplitudes are close. When their amplitudes differ significantly, the maximum wave height which is attained during the absorb-emit interaction tends to the sum of the heights of the solitons with the polarity inherited from the large soliton, as predicted in the frameworks of different long-wave integrable models in [3, 4]. As a result of the collision the solitons may experience non-classic phase shifts as they both jump back.</p><p>[1] O.V. Rudenko. Physics – Uspekhi, Vol. 56(7), 683-690 (2013).</p><p>[2] E. Tobisch, and E. Pelinovsky. Appl. Math. Lett., Vol. 97, 1-5 (2019).</p><p>[3] A.V. Slunyaev, and E.N. Pelinovsky. Phys. Rev. Lett., Vol. 117, 214501 (2016).</p><p>[4] A. Slunyaev. Stud. Appl. Math., Vol. 142, 385-413 (2019).</p>
Title: Modular Korteweg - de Vries equation: Riemann, cnoidal and solitary waves
Description:
<p>The review paper by Oleg Rudenko [1] suggests several examples of elastic systems with so-called modular nonlinearities.
In this study we consider the modular Korteweg - de Vries (KdV) equation in the form u_t + 6 u u_x + u_{xxx} = 0.
This equation is not integrable by means of the Inverse Scattering Transform in the general case, but sign-defined functions which never change the sign satisfy the integrable KdV equation, and hence possess an exact solution.
Firstly, we consider the dispersionless limit of the modular KdV equation and analyze the evolution of a simple nonlinear wave (Riemann wave) and its Fourier transform including the asymptotics when the wave tends to break [2].
Then, we study the structure of travelling waves.
If the waves propagate on a pedestal and do not cross the zero level u = 0, they coincide with the well-known travelling wave solutions of the classic KdV equation in the form of cnoidal and solitary waves.
If the pedestal is zero, the structure of sign-varying travelling waves is expressed through Jacobi elliptic functions.
The interaction of solitary waves of different polarities is studied numerically using an implicit pseudo-spectral method.
The simulation has revealed the inelastic character of the collision; in the course of the interaction the solitons can alter their amplitudes (the small soliton decreases and the large one grows) and emit small-amplitude waves.
The inelastic effects are most pronounced when the solitons’ amplitudes are close.
When their amplitudes differ significantly, the maximum wave height which is attained during the absorb-emit interaction tends to the sum of the heights of the solitons with the polarity inherited from the large soliton, as predicted in the frameworks of different long-wave integrable models in [3, 4].
As a result of the collision the solitons may experience non-classic phase shifts as they both jump back.
</p><p>[1] O.
V.
Rudenko.
Physics – Uspekhi, Vol.
56(7), 683-690 (2013).
</p><p>[2] E.
Tobisch, and E.
Pelinovsky.
Appl.
Math.
Lett.
, Vol.
97, 1-5 (2019).
</p><p>[3] A.
V.
Slunyaev, and E.
N.
Pelinovsky.
Phys.
Rev.
Lett.
, Vol.
117, 214501 (2016).
</p><p>[4] A.
Slunyaev.
Stud.
Appl.
Math.
, Vol.
142, 385-413 (2019).
</p>.

Related Results

The Generalized Riemann Integral
The Generalized Riemann Integral
Riemann integration theory integrates functions on a bounded interval  as a Riemann sum approach (integral) where the fineness of the partitions is controlled by a number (norm) of...
Time-harmonic waves in Korteweg and nematic-Korteweg fluids
Time-harmonic waves in Korteweg and nematic-Korteweg fluids
We derive the Helmholtz–Korteweg equation, which models acoustic waves in Korteweg fluids. We further derive a nematic variant of the Helmholtz–Korteweg equation, which incorporate...
Inverse Jacobian and related topics for certain superelliptic curves
Inverse Jacobian and related topics for certain superelliptic curves
Given an elliptic curve E over the complex numbers (CC) given by y^2 = x^3 + ax + b, there exists a lattice L in CC such that the group E(CC) of complex points on E is isomorphic ...
The Origin of de Broglie Waves (Version 2.0)
The Origin of de Broglie Waves (Version 2.0)
The famous 1927 Solvay Conference was considered a turning point in the world of Physics. The scientific realists like Albert Einstein had lost and the instrumentalists like Niels ...
Ion acoustic and spin electron acoustic cnoidal waves in a spin polarized plasma with exchange effects
Ion acoustic and spin electron acoustic cnoidal waves in a spin polarized plasma with exchange effects
Separate spin evolution-quantum hydrodynamic model is employed to address the nonlinear propagation of ion acoustic wave (IAW) and spin electron acoustic wave (SEAW) in a spin pola...
Can stationary cnoidal waves explain periodic deformation bands in porous sandstone?
Can stationary cnoidal waves explain periodic deformation bands in porous sandstone?
<p>Deformation bands are sub-seismic brittle structures found in granular materials. These structures exhibit two spatial distributions: [1] non-linear decay of spaci...
Origin of De Broglie Waves
Origin of De Broglie Waves
The famous 1927 Solvay Conference was considered a turning point in the world of Physics. The scientific realists like Albert Einstein had lost and the instrumentalists like Niels ...
Statistical properties of the internal solitary wave ensemble
Statistical properties of the internal solitary wave ensemble
<p>Internal solitary wave ensembles are often observed on the ocean shelves. The long internal baroclinic tide is generated by a barotropic tide on the shelf edges, a...

Back to Top