In mathematics, KPP–Fisher equation (named after Andrey Kolmogorov, Ivan Petrovsky, Nikolai Piskunov and Ronald Fisher) also known as the KPP equation, Fisher equation or Fisher–KPP equation is the partial differential equation:It is a kind of reaction–diffusion system that can be used to model population growth and wave propagation.
KPP–Fisher equation belongs to the class of reaction-diffusion equations: in fact, it is one of the simplest semilinear reaction-diffusion equations, the one which has the inhomogeneous term
f(u,x,t)=ru(1-u),
which can exhibit traveling wave solutions that switch between equilibrium states given by
f(u)=0
Fisher proposed this equation in his 1937 paper The wave of advance of advantageous genes in the context of population dynamics to describe the spatial spread of an advantageous allele and explored its travelling wave solutions.[1] For every wave speed
c\geq2\sqrt{rD}
c\geq2
u(x,t)=v(x\pmct)\equivv(z),
where
stylev
\limz → -inftyv\left(z\right)=0, \limz → inftyv\left(z\right)=1.
That is, the solution switches from the equilibrium state u = 0 to the equilibrium state u = 1. No such solution exists for c < 2.[1] [2] [3] The wave shape for a given wave speed is unique. The travelling-wave solutions are stable against near-field perturbations, but not to far-field perturbations which can thicken the tail. One can prove using the comparison principle and super-solution theory that all solutions with compact initial data converge to waves with the minimum speed.
For the special wave speed
c=\pm5/\sqrt{6}
v(z)=\left(1+Cexp\left(\mp{z}/{\sqrt6}\right)\right)-2
where
C
C>0
Proof of the existence of travelling wave solutions and analysis of their properties is often done by the phase space method.
In the same year (1937) as Fisher, Kolmogorov, Petrovsky and Piskunov introduced the more general reaction-diffusion equation
\partialu | - | |
\partialt |
\partial2u | |
\partialx2 |
=F(u)
F
F(0)=F(1)=0,F'(0)=r>0
F(v)>0,F'(v)<r
0<v<1
F(u)=ru(1-u)
x
\sqrt{D}
F(u)=ru(1-uq)
q>0
q=2
The minimum speed of a KPP-type traveling wave is given by
2\sqrt{\left. | dF |
du |
\right|u=0
which differs from other type of waves, see for example ZFK-type waves.