While doing his experiment, Millikan one day observed the following charges on a single drop
$(i)$ $6.563 \times {10^{ - 19}}C$ $ (ii)$ $8.204 \times {10^{ - 19}}C$
$(iii)$ $11.50 \times {10^{ - 19}}C$ $ (iv)$ $13.13 \times {10^{ - 19}}C$
$(v)$ $16.48 \times {10^{ - 19}}C$ $ (vi)$ $18.09 \times {10^{ - 19}}C$
From this data the value of the elementary charge $(e)$ was found to be
$1.641 \times {10^{ - 19}}C$
$1.630 \times {10^{ - 19}}C$
$1.648 \times {10^{ - 19}}C$
$1.602 \times {10^{ - 19}}C$
When electron beam passes through an electric field, they gain kinetic energy. If the same beam passes through magnetic field, then
The specific charge of an electron is
In a Thomson set-up for the determination of e/m, electrons accelerated by $2.5$ $kV$ enter the region of crossed electric and magnetic fields of strengths $3.6 \times {10^4}V{m^{ - 1}}$ and $1.2 \times {10^{ - 3}}T$ respectively and go through undeflected. The measured value of $e/m$ of the electron is equal to
An oxide coated filament is useful in vacuum tubes because essentially
If an electron oscillates at a frequency of $ 1 GHz$ it gives