bhsmith said:
Ah ok, I'm really trying to understand this.
I would have P(total)= sqrt(E(total)^2 - m(total)^2)
This equation doesn't hold in general. For each particle we have
E_i^2 - |\vec{p}_i c|^2 = (m_i c^2)^2 ,
but
\left( \sum_i E_i \right)^2 - \left|\sum_i\vec{p_i} c\right|^2 \neq \left( \sum_i m_i c^2\right)^2,
What is true is that
\left( \sum_i E_i \right)^2 - \left|\sum_i\vec{p_i} c\right|^2 = \left( \sum_i E'_i \right)^2 - \left|\sum_i\vec{p'}_i c\right|^2.
where initial quantities are on the LHS and the primed quantities on the RHS are from the final state. This equation just follows from energy and momentum conservation.
But shouldn't i already know the final momentum because it should be equal to the momentum before the collision.
But Ptotal=P'total=P'(photon)+P'(proton) and the same thing goes for energy.
But so would if the speed for the photon is still the speed of light and that should be equal to Energy since it's massless then that would give me P(photon)=0... because P=mv(gamma) and mass is zero. I am so confused.
P=mv(gamma) is not valid for a photon exactly because the photon is massless. Let the initial photon momentum be \vec{k}. The relation to the wavelength is through the magnitude
| \vec{k}| = \frac{h}{\lambda}.
You will also need to find a convenient way to parametrize the directions of the particles to solve the problem.
The energy-momentum relation for the photon is
E_{\tex{photon}}^2 - |\vec{k} c|^2 = 0,
which is consistent with the relation
E_{\tex{photon}} = h f,
where f is the frequency of the photon.