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<math> |
<math> |
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− | \epsilon v_t(x,t)=\epsilon^2v_{xx}(x,t)+f(v(x,t))-w(x,t)+g, |
+ | \epsilon v_t(x,t)=\epsilon^2v_{xx}(x,t)+f(v(x,t))-w(x,t)+g, |
</math> |
</math> |
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w_t(x,t)=hv(x,t)-\gamma w(x,t)+g, |
w_t(x,t)=hv(x,t)-\gamma w(x,t)+g, |
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</math> |
</math> |
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+ | |||
+ | with <math>f(v)=v(v-0.1)(1-v)</math> and initial and boundary conditions |
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+ | |||
+ | <math> |
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+ | v(x,0)=0,\quad w(x,0)=0, \quad x\in [0,1], |
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+ | </math> |
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+ | |||
+ | <math> |
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+ | v_x(0,t)=-i_0(t), \quad v_x(1,t)\quad =0, \quad t \geq 0, |
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+ | </math> |
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+ | |||
+ | where <math>\epsilon=0.015,\;h=0.5,\;\gamma=2,\;g=0.05,\;i_0(t)=5\cdot |
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+ | 10^4t^3 \exp(-15t).</math> In [1], the previous system of coupled nonlinear PDEs is spatially discretized by means of a finite difference scheme with <math>k=512 </math> nodes for each PDE. Hence, one obtains a nonlinear (cubic) system of ODEs with state dimension <math>n=1024. </math> |
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+ | |||
+ | [[File:FHN.jpg]] |
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==References== |
==References== |
Revision as of 17:37, 20 November 2012
Description
The FitzHugh-Nagumo system describes a prototype of an excitable system (e.g., a neuron).
If the external stimulus exceeds a certain threshold value, the system will exhibit a characteristic excursion in phase space, before the variables
and
relax back to their rest values. This behaviour is typical for spike generations (=short elevation of membrane voltage
) in a neuron after stimulation by an external input current.
Here, we present the setting from [1], where the equations for the dynamical system read
with and initial and boundary conditions
where In [1], the previous system of coupled nonlinear PDEs is spatially discretized by means of a finite difference scheme with
nodes for each PDE. Hence, one obtains a nonlinear (cubic) system of ODEs with state dimension
References
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