Estimating equations: Difference between revisions
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en>Qwfp GMM is not the same as estimating equations. GMM means something more specific. |
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In [[mathematics]], the '''Euler–Poisson–Darboux'''<ref name=Zwillinger1997>{{cite book | |||
| author = Zwillinger, D. | |||
| year = 1997 | |||
| title = Handbook of Differential Equations 3rd edition | |||
| publisher = Academic Press, Boston, MA | |||
| isbn = | |||
}}</ref> equation is the [[partial differential equation]] | |||
: <math>u_{x,y}+\frac{N(u_x+u_y)}{x+y}=0. </math> | |||
This equation is named for [[Siméon Poisson]], [[Leonhard Euler]], and [[Gaston Darboux]]. It plays important role in solving the classical [[wave equation]]. | |||
== References == | |||
{{reflist}} | |||
==External links== | |||
*{{springer | title=Euler–Poisson–Darboux equation | id=E/e130050 | last=Moroşanu | first=C.}} | |||
{{DEFAULTSORT:Euler-Poisson-Darboux equation}} | |||
[[Category:Differential calculus]] | |||
[[Category:Partial differential equations]] | |||
{{mathanalysis-stub}} | |||
Revision as of 22:31, 4 December 2013
In mathematics, the Euler–Poisson–Darboux[1] equation is the partial differential equation
This equation is named for Siméon Poisson, Leonhard Euler, and Gaston Darboux. It plays important role in solving the classical wave equation.
References
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