A quantum mechanical particle of mass ‘m’ free to rotate o...
$m$ is described by a wave function $\Psi(x,t)$, where $x$ is the particle's position and $t$ is time. The wave function satisfies the Schrödinger equation:
$$i\hbar\frac{\partial \Psi}{\partial t}=-\frac{\hbar^2}{2m}\frac{\partial^2 \Psi}{\partial x^2}+V(x)\Psi$$
where $\hbar$ is the reduced Planck constant and $V(x)$ is the potential energy function.
The wave function contains all the information about the particle's position, momentum, and energy. The probability of finding the particle in a particular location $x$ is given by $|\Psi(x,t)|^2$. The expectation value of the position and momentum of the particle are given by:
$$\langle x \rangle =\int_{-\infty}^{\infty}x|\Psi(x,t)|^2dx$$
and
$$\langle p \rangle =\int_{-\infty}^{\infty}\Psi^*(x,t)\frac{\hbar}{i}\frac{\partial \Psi(x,t)}{\partial x}dx$$
respectively.
The wave function evolves in time according to the Schrödinger equation. This means that the probability distribution and expectation values of position and momentum change with time. The behavior of the wave function is subject to certain boundary conditions, such as being continuous and finite, and to the nature of the potential energy function.