Let us now consider, following the usual method of treatment, the longitudinal and transversal mass of a moving electron. We write the equations ([A]) in the form
d²x
mβ² ----- = eX = eX′
dt²
d²y v
mβ² ----- = eβ (Y - --- N) = eY′
dt² c
d²z v
Let us now consider, following the usual method of treatment, the longitudinal and transversal mass of a moving electron. We write the equations ([A]) in the form
d²x
mβ² ----- = eX = eX′
dt²
d²y v
mβ² ----- = eβ (Y - --- N) = eY′
dt² c
d²z v