词条 | Whitham equation |
释义 |
In mathematical physics, the Whitham equation is a non-local model for non-linear dispersive waves. [1][2][3] The equation is notated as follows : This integro-differential equation for the oscillatory variable η(x,t) is named after Gerald Whitham who introduced it as a model to study breaking of non-linear dispersive water waves in 1967.[4] Wave breaking – bounded solutions with unbounded derivatives – for the Whitham equation has recently been proven.[5] For a certain choice of the kernel K(x − ξ) it becomes the Fornberg–Whitham equation. Water wavesUsing the Fourier transform (and its inverse), with respect to the space coordinate x and in terms of the wavenumber k:
{{pad|2em}} while {{pad|2em}} with g the gravitational acceleration and h the mean water depth. The associated kernel Kww(s) is, using the inverse Fourier transform:[4] since cww is an even function of the wavenumber k.
{{pad|3em}} {{pad|3em}} with δ(s) the Dirac delta function.
{{pad|2em}} and {{pad|2em}} {{pad|2em}} with {{pad|2em}} The resulting integro-differential equation can be reduced to the partial differential equation known as the Fornberg–Whitham equation:[6] This equation is shown to allow for peakon solutions – as a model for waves of limiting height – as well as the occurrence of wave breaking (shock waves, absent in e.g. solutions of the Korteweg–de Vries equation).[6][3] Notes and referencesNotes1. ^{{harvtxt|Debnath|2005|p=364}} 2. ^{{harvtxt|Naumkin|Shishmarev|1994|p=1}} 3. ^1 {{harvtxt|Whitham|1974|pp=476–482}} 4. ^1 2 3 {{harvtxt|Whitham|1967}} 5. ^{{harvtxt|Hur|2017}} 6. ^1 2 {{harvtxt|Fornberg|Whitham|1978}} References{{ref begin}}
| publisher = Springer | isbn = 9780817643232 | last = Debnath | first = L. | title = Nonlinear Partial Differential Equations for Scientists and Engineers | year = 2005 }}
| last1 = Fetecau | first1 = R. | last2 = Levy | first2 = Doron | journal = Communications in Mathematical Sciences | issue = 2 | pages = 159–170 | title = Approximate Model Equations for Water Waves | volume = 3 | year = 2005 | doi = 10.4310/CMS.2005.v3.n2.a4 }}
| doi = 10.1098/rsta.1978.0064 | volume = 289 | issue = 1361 | pages = 373–404 | last1 = Fornberg | first1 = B. | first2 = G.B. | last2 = Whitham | author2-link = Gerald B. Whitham | title = A Numerical and Theoretical Study of Certain Nonlinear Wave Phenomena | journal = Philosophical Transactions of the Royal Society A | year = 1978 |bibcode = 1978RSPTA.289..373F | citeseerx = 10.1.1.67.6331 }}
| last = Hur | first = V.M. | title = Wave breaking in the Whitham equation | journal = Advances in Mathematics | volume = 317 | pages = 410–437 | year = 2017 | doi = 10.1016/j.aim.2017.07.006 }}
| title = The Whitham Equation as a model for surface water waves | journal = Physica D: Nonlinear Phenomena | volume = 309 | pages = 99–107 | year = 2015 | doi = 10.1016/j.physd.2015.07.010 | first1 = D. | last1 = Moldabayev | first2 = H. | last2 = Kalisch | first3 = D. | last3 = Dutykh | arxiv = 1410.8299 | bibcode = 2015PhyD..309...99M }}
| publisher = American Mathematical Society | isbn = 9780821845738 | last1 = Naumkin | first1 = P.I. | first2 = I.A. | last2 = Shishmarev | title = Nonlinear Nonlocal Equations in the Theory of Waves | year = 1994 }}
| doi = 10.1098/rspa.1967.0119 | volume = 299 | issue = 1456 | pages = 6–25 | last = Whitham | first = G.B. | author-link = Gerald B. Whitham | title = Variational methods and applications to water waves | journal = Proceedings of the Royal Society A | year = 1967 |bibcode = 1967RSPSA.299....6W }}
| first = G.B. | last = Whitham | author-link = Gerald B. Whitham | year = 1974 | title = Linear and nonlinear waves | publisher = Wiley-Interscience | isbn = 978-0-471-94090-6 | doi=10.1002/9781118032954 }}{{ref end}} 3 : Water waves|Partial differential equations|Equations of fluid dynamics |
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