Category:Quasilinear equations and Talk:Particle Systems: Difference between pages

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A quasilinear equation is one that is linear in all but the terms involving the highest order derivatives (whether they are of fractional order or not).  See also the article for [[Quasilinear equations]]
#REDIRECT [[Talk:Interactive Particle Systems]]
 
 
For instance, the following equations are all quasilinear (and not semilinear)
 
\[u_t-\mbox{div} \left ( \frac{\nabla u}{\sqrt{1+|\nabla u|^2}}\right ) = 0 \]
 
<center> [[Mean curvature flow]] </center>
 
\[ u_t = \mbox{div} \left ( u \nabla \mathcal{K_\alpha} u\right ),\;\;\; \mathcal{K_\alpha} u = u * |x|^{-n+\alpha} \]
 
<center> [[Nonlocal porous medium equation]] </center>
 
Equations which are not quasilinear are called [[Fully nonlinear equations]], which include for instance [[Monge Ampére]] and [[Fully nonlinear integro-differential equations]]. Note that all [[Semilinear equations]] are automatically quasilinear.
 
Note: In this category are listed all equations which are quasilinear  and NOT semilinear.  Strictly speaking, all semilinear equations ought to be listed here aswell, however, as the specific methods and questions are so different in both categories (i.e. quasilinear techniques may give results for semilinear equations which are weaker when compared to the more powerful methods tailor-made for semilinear ones) we prefer to list semilinear ones in their own category only.

Latest revision as of 16:09, 13 February 2012

Pages in category "Quasilinear equations"

The following 2 pages are in this category, out of 2 total.