The basic form is dXt=μt dt+σt dWtdX_t = \mu_t\,dt + \sigma_t\,dW_t, where μt\mu_t is the drift and σt\sigma_t is the coefficient of the dWtdW_t term. If μt\mu_t and σt\sigma_t are constants, X is Brownian motion with drift, Xt=μt+σWtX_t = \mu t + \sigma W_t. Geometric Brownian motion corresponds to μt=μSt\mu_t = \mu S_t and σt=σSt\sigma_t = \sigma S_t.

The equation takes on its meaning when it is written in integral form. The integral of the dWtdW_t term is called the Ito integral, and it requires the integrand to be determined by information up to that time. Ito's lemma is used to transform such equations.