Looking at a Franck-Hertz experimental setup, and given a potential difference such as $4.0\ V$ which is too small to excite out the first electron orbital, the electrons moving through the tube will have elastic collisions with the Hg atoms. I'm supposed to show that given some kinetic energy $E$, of a flowing electron, that the maximum recoil of a Hg atom that it hits is approximately $4Em/M$ (where $m$ is the mass of the electron, and $M$ is the mass of the Hg atom). I know to use conservation of energy, and given that the Hg atom was initially at rest, I know the electron is probably bouncing backward (so something like $2\times E-\text{sub - elec} = E\text{ - sub - hg}$). I can't seem to find where the 4 comes from. Is it the $4.0\ V$ potential difference?
I tried playing with conservation of energy formula but can't get $\frac{4Em}{M}$. (Taking lower case to be the electron and UPPER CASE TO BE THE ATOM:) [$mv^2 = MV^2 - mv^2$] so [$mv^2 = 0.5MV^2$] so [$2e = E$] but I'm supposed to find that [$E = 4Em/M$]. I know there is something I'm missing here.
P.S.: The original problem is #44 here (or as an image here) in case I'm misunderstanding something.