Svandp(N, T, x0, v0, a, b, omega, sigma, Step = FALSE, Output = FALSE)
Step = TRUE
ploting step by step.Output = yes
write a output to an Excel (.csv).x0
and v0
(ringed points).
Stochastic perturbations of the Van Der pol equation, and random excitations force of such systems by White noise e(t)
, with delta-type correlation functions
E(e(t)e(t+h))=sigma*deltat(h)
: $$x'' + a * x' * ( x^2 /b - 1 ) + omega^2 * x = e(t)$$
where a,omega,sigma >= 0
and b > 0
.
a=0
one obtains the stochastic harmonic oscillatorSharosc
; the amplitude of the oscillations depends on the initial conditions. By increasinga
one notes an increasingly important deformation of the oscillations and portrait of phase.b
determines the amplitude of the oscillations: when|x|, the reaction is positive and the amplitude increases. When|x|>b
it is the reverse which occurs. The amplitude is stabilized around2b
.
Spendu
stochastic pendulum, Sharosc
stochastic harmonic oscillator, Srayle
stochastic Rayleigh oscillator,
SSCPP
stochastic system with a cylindric phase plane, Sosadd
stochastic oscillator with additive noise.## a = 0, b = 0.3, omega= 2.5, sigma=0.1
Svandp(N=10000, T=100, x0=1, v0=0, a=0, b=0.3, omega=2.5, sigma=0.1)
## a = 3
Svandp(N=10000, T=100, x0=1, v0=0, a=3, b=0.3, omega=2.5, sigma=0.1)
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