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{{Other uses|Pitchfork (disambiguation)}}
In [[bifurcation theory]], a field within [[mathematics]], a '''pitchfork bifurcation''' is a particular type of local bifurcation. Pitchfork bifurcations, like [[Hopf bifurcation]]s have two types - supercritical or subcritical.
 
In continuous dynamical systems described by [[Ordinary differential equation|ODEs]]&mdash;i.e. flows&mdash;pitchfork bifurcations occur generically in systems with [[symmetry in mathematics|symmetry]].
 
==Supercritical case==
[[Image:Pitchfork bifurcation supercritical.svg|180px|right|thumb|Supercritical case: solid lines represent stable points, while dotted line
represents unstable one.]]
The [[normal form (bifurcation theory)|normal form]] of the supercritical pitchfork bifurcation is
:<math> \frac{dx}{dt}=rx-x^3. </math>
For negative values of <math>r</math>, there is one stable equilibrium at <math>x = 0</math>. For <math>r>0</math> there is an unstable equilibrium at <math>x = 0</math>, and two stable equilibria at <math>x = \pm\sqrt{r}</math>.
 
==Subcritical case==
[[Image:Pitchfork bifurcation subcritical.svg|180px|right|thumb|Subcritical case: solid line represents stable point, while dotted lines
represent unstable ones.]]
The [[normal form (bifurcation theory)|normal form]] for the subcritical case is
:<math> \frac{dx}{dt}=rx+x^3. </math>
In this case, for <math>r<0</math> the equilibrium at <math>x=0</math> is stable, and there are two unstable equilbria at <math>x = \pm \sqrt{-r}</math>. For <math>r>0</math> the equilibrium at <math>x=0</math> is unstable.
 
==Formal definition==
An ODE
:<math> \dot{x}=f(x,r)\,</math>
described by a one parameter function <math>f(x, r)</math> with <math> r \in \Bbb{R}</math> satisfying:
:<math> -f(x, r) = f(-x, r)\,\,</math><!-- the \,\, is to force no-hinting in the antialiasing mode of pngtex - please do not remove it! -->&nbsp; (f is an [[odd function]]),
 
:<math>
\begin{array}{lll}
\displaystyle\frac{\part f}{\part x}(0, r_{o}) = 0 , &
\displaystyle\frac{\part^2 f}{\part x^2}(0, r_{o}) = 0, &
\displaystyle\frac{\part^3 f}{\part x^3}(0, r_{o}) \neq 0,
\\[12pt]
\displaystyle\frac{\part f}{\part r}(0, r_{o}) = 0, &
\displaystyle\frac{\part^2 f}{\part r \part x}(0, r_{o}) \neq 0.
\end{array}
</math>
 
has a '''pitchfork bifurcation''' at <math>(x, r) = (0, r_{o})</math>. The form of the pitchfork is given
by the sign of the third derivative:
 
:<math> \frac{\part^3 f}{\part x^3}(0, r_{o})
\left\{
  \begin{matrix}
    < 0, & \mathrm{supercritical} \\
    > 0, & \mathrm{subcritical}
  \end{matrix}
\right.\,\,
</math><!-- the \,\, is to force no-hinting in the antialiasing mode of pngtex - please do not remove it! -->
 
==References==
*Steven Strogatz, "Non-linear Dynamics and Chaos: With applications to Physics, Biology, Chemistry and Engineering", Perseus Books, 2000.
*S. Wiggins, "Introduction to Applied Nonlinear Dynamical Systems and Chaos", Springer-Verlag, 1990.
 
== See also ==
 
* [[Bifurcation theory]]
* [[Bifurcation diagram]]
 
[[Category:Bifurcation theory]]

Revision as of 18:47, 31 January 2014

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my site; wellness [continue reading this..] In bifurcation theory, a field within mathematics, a pitchfork bifurcation is a particular type of local bifurcation. Pitchfork bifurcations, like Hopf bifurcations have two types - supercritical or subcritical.

In continuous dynamical systems described by ODEs—i.e. flows—pitchfork bifurcations occur generically in systems with symmetry.

Supercritical case

Supercritical case: solid lines represent stable points, while dotted line represents unstable one.

The normal form of the supercritical pitchfork bifurcation is

For negative values of , there is one stable equilibrium at . For there is an unstable equilibrium at , and two stable equilibria at .

Subcritical case

Subcritical case: solid line represents stable point, while dotted lines represent unstable ones.

The normal form for the subcritical case is

In this case, for the equilibrium at is stable, and there are two unstable equilbria at . For the equilibrium at is unstable.

Formal definition

An ODE

described by a one parameter function with satisfying:

  (f is an odd function),

has a pitchfork bifurcation at . The form of the pitchfork is given by the sign of the third derivative:

References

  • Steven Strogatz, "Non-linear Dynamics and Chaos: With applications to Physics, Biology, Chemistry and Engineering", Perseus Books, 2000.
  • S. Wiggins, "Introduction to Applied Nonlinear Dynamical Systems and Chaos", Springer-Verlag, 1990.

See also