The evolution immediately after the measurement occurs according to the Schrödinger equation, but now with a known initial state. In general, in order to be able to "repeat" a measurement you have to prepare the state again.
For example, say I have a particle in a harmonic oscillator potential prepared in the state
$$|\psi\rangle = \frac{1}{\sqrt{2}}|0\rangle + \frac{1}{\sqrt{2}}|1\rangle $$
I measure its energy and find it to be $\frac{\hbar \omega}{2} $, indicating the particle was found in the $|0\rangle$ state.
Because $|0\rangle$ is an energy eigenstate, time evolution will not change it, so any subsequent measurement will continue to give the same value for the energy: $\frac{\hbar \omega}{2}$. In order to perform a "repeat" of the original measurement you have to prepare the state $|\psi\rangle$ again.