From the equations (1) and (2) can be deduced the velocity,
, of the projectiles, and the ratio,
/
, of the electric charge to the corresponding mass.
The experiments of Becquerel have shown that for the β-rays of greatest intensity the ratio,
From the equations (1) and (2) can be deduced the velocity,
, of the projectiles, and the ratio,
/
, of the electric charge to the corresponding mass.
The experiments of Becquerel have shown that for the β-rays of greatest intensity the ratio,