Velocity 4-vector
define the u_4 vector note the differentiation with respect to ds.
u=(u_t, u_x, u_y, u_z) = (cdt/ds, dx/ds, dy/ds, dz/ds) note that by its definition the 4-velocity is dimensionless like beta=v/c
take the u^2 = u_t^2-u_x^2-u_y^2-u_z^2 = [ (cdt)^2- dx^2-dy^2-dz^2]/ ds^2 = ds^2/ds^2 = 1
express ds^2=gamma^(-2) c^2 dt^2
> (c^2dt^2)/(ds^2)
gamma^(2)
then the u_t component above is cdt/ds= sqrt(c^2dt^2/ds^2) = sqrt (gamma^2)
=> u_t
gamma
everybody should reproduce the above
and then u_4 =( gamma, v/c gamma)
Momentum 4-vector
newtonian
P =m
v where v=3-velocity
Define 4-momentum as follows
P_j= m_0 * u_j * c where u_j is the the famous 4-velocity (i.e. j runs 0(time) , 1(x), 2(y), 3(z))
then the 3-momentum using the 3-velocity (v_a) can be expressed as
P_a=m_0 * u_a * c = m_0 * (gamma v_a/c ) * c (taking the 3-velocity from above)
= m_0 * gamma * v_a this should be equal to
P=m
v (newton) because it is the 3-component part of the 4-vector
=> m
m_0 * gamma (this says that the total mass of the moving particle is bigger than its rest mass m_0)
the temporal component of the momentum 4-vector as we defined above is
P_t= m_0 * u_t * c =
m_0 * gamma * c =
m*c
from the Taylor expanded mass we had m*c^2=m_0*c^2+KE and we said the total energy of the moving particle is
E_tot=m*c^2 =
m c* * c = P_t *c
> P_t
E_tot/c ==>
the temporal component of the momentum is the total energy divided by c
So now we look for the direct relation between E_tot, and P_j
P_j = (P_t,
P) =>
P_j^2 P_t^2- P^2 = (E_tot/c)^2- P^2 ==>
(m_0 * u_j c)^2*
= (E_tot/c)^2- P^2 ==> (u_j^2=1 from the 4-velocity)
m_0^2 *c^2 = E_tot^2/c^2 - P^2 ==>
E_tot= +- sqrt(m0^2*c^4+P^2c^2)
-- Main.smaria - 2011-01-21