0

I have the equations defined as follows: $$ \begin{align} \frac{dX}{dt}&=f(X,U), \\ U(t)&=g(X)+\xi_t, \end{align} $$ where $\xi_t$ is a Gaussian white noise, $f(X,U)$ and $g(X)$ are such functions as one could rewrite the first equation by substituting the second equation in it as follows: $$ \frac{dX}{dt}=\psi(X)+\sigma \xi_t. $$ It's possible to apply the Euler-Maruyama scheme to solve the differential equation only as we can write down its Ito's form: $$ dX=\psi(X)dt+\sigma dW. $$ The numeric scheme for a differential equation would be $$ X(t_{n+1})=X(t_n)+\psi(X(t_n))\Delta t+ \sigma \sqrt{\Delta t} \hat{\xi},\quad \hat{\xi}\in N(0,1). $$ But how to compute the algebraic variable $U(t_{n+1})$ on the same time step? The problem is the random variable $\hat{\xi}$ somehow depends on $\xi_t$.

0 Answers0