Stochastic Partial Differential Equations (SPDEs) are a class of mathematical equations that extend partial differential equations (PDEs) to include terms that incorporate randomness. These equations model phenomena where there is uncertainty or randomness, such as in physics, biology, finance, and engineering. The incorporation of stochastic processes makes SPDEs powerful tools for modeling systems affected by noise over space and time.
$\frac{\partial u(t, x)}{\partial t} = \mathcal{L}u(t, x) + f(u(t, x)) + \sigma(u(t, x)) \dot{W}(t, x),$
where: - $u(t, x)$ is the unknown function (e.g., temperature, concentration, or financial value), - $\mathcal{L}$ is a differential operator (e.g., the Laplacian), - $f(u(t, x))$ is a deterministic source or drift term, - $\sigma(u(t, x)) \dot{W}(t, x)$ represents the stochastic term, where $\dot{W}(t, x)$ denotes a noise process (often modeled as white noise or a more structured stochastic process).
$\frac{\partial u(t, x)}{\partial t} = \Delta u(t, x) + \dot{W}(t, x),$
where $\Delta$ is the Laplacian operator.
$\frac{\partial u(t, x)}{\partial t} = \mathcal{L}u(t, x) + f(u(t, x)) + \dot{W}(t, x).$
$\frac{\partial u(t, x)}{\partial t} = \mathcal{L}u(t, x) + f(u(t, x)) + \sigma(u(t, x)) \dot{W}(t, x).$
$\frac{\partial u(t, x)}{\partial t} = \Delta u(t, x) + \sigma(u(t, x)) \dot{W}(t, x),$
where $\Delta$ is the Laplacian and $\dot{W}(t, x)$ is a space-time white noise.
$\frac{\partial u(t, x)}{\partial t} + u(t, x) \frac{\partial u(t, x)}{\partial x} = \nu \frac{\partial^2 u(t, x)}{\partial x^2} + \sigma \dot{W}(t, x),$
where $\nu$ is the viscosity term.
$\frac{\partial u(t, x)}{\partial t} + (u(t, x) \cdot \nabla) u(t, x) = -\nabla p(t, x) + \nu \Delta u(t, x) + \sigma \dot{W}(t, x),$
where $p(t, x)$ is the pressure and $\nu$ is the kinematic viscosity.