We have momentum and energy operators that we can use here. The momentum operator is [tex]\hat{p}[/tex] and the energy operator is [tex]\hat{E}[/tex] where
[tex]\hat{p} = \hbar / i \frac{\partial }{\partial x}[/tex]
and
[tex]\hat{E} = i \hbar \frac{\partial }{\partial t}[/tex]
For any function [tex]g(x)[/tex] we have the expectation value as:
[tex]\langle g(x) \rangle = \int^{\infty}_{-\infty} \psi^\star (x,t) g(x) \psi (x,t)\,dx[/tex]
Then we have
[tex]\langle p \rangle = \hbar / i \int^\infty_{-\infty} \psi^\star (x,t) \frac{\partial }{\partial x} \psi (x,t)\,dx[/tex]
and
[tex]\langle E \rangle = i \hbar \int^\infty_{-\infty} \psi^\star (x,t) \frac{\partial }{\partial t} \psi (x,t)\,dx[/tex]
and also
[tex]\langle p^2 \rangle = \hbar^2 \int^\infty_{-\infty} \psi^\star (x,t) \frac{\partial^2 }{\partial x^2} \psi (x,t)\,dx[/tex]