I am not sure I understand your question clearly, but here are some ideas trying to cover as many cases as possible:
For the electron in the first Bohr orbit in the hydrogen atom:
The frequency of its rotational motion is the number of times it will rotate around the proton in one second, and it isabout
$f=6.58\times 10^{15} s^{-1}.$
In a uniform magnetic field:
For an electron that has entered a uniform magnetic field of flux density B, depending on the speed $v$ of the electron, the magnetic field can put it into a circular orbit with frequency that can be found using these two equations
$Bev=\frac{mv^2}{r}$
which is the balance equation between the magnetic and centripetal
forces, and
$v=2\pi fr$
which is from the circular motion of the electron at uniform speed $v$. These two lead to the equation
$f={\frac {Be}{2\pi m}}$.
For an electron in a piece of wire: carrying an electric current of frequency 50Hz say, it means that the electron oscillates at 50Hz (i.e. goes back and forward, and it does this 50 times per second.)
For a free electron: The frequency is of quantum mechanical nature. It relates to the the wave function of the electron
$\psi (x)=u(p)e^{i({\bf p.r}-Et)/h}$.
Note that in the above equation $E/h$ is the frequency of rotation of the phasor (the exponential part), it does not mean the electron goes back and forward so many times per second. So the larger the energy the larger the frequency of rotation of the phasor, hence of the wave function of the electron. For a relativistic electron, the energy is
$E=c\sqrt{p^2+m_o^2c^2}$
so that the frequency is given by
$f=c\sqrt{p^2+m_o^2c^2}/h$,
hence the origin of the more general part $\hbar\omega t$ of the phasor (in the wave function) representing an electron.
I hope this helps.