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Q. A beam of cathode rays is subjected to crossed electric $(E)$ and magnetic fields $(B)$. The fields are adjusted such that the beam is not deflected. The specific charge of the cathode rays is given by (Where $V$ is the potential difference between cathode and anode)

AIPMTAIPMT 2010Dual Nature of Radiation and Matter

Solution:

Its the electron beam is not deflected then,
$ \begin{array}{l} F _{ m }= Ee \\ Bev = Ee \\ v =\frac{ E }{ B } \end{array} $
According to the law of conservation of energy
$ \begin{array}{l} \frac{1}{2} mv ^{2}= eV \\ v =\sqrt{\frac{2 eV }{ m }} \\ \sqrt{\frac{2 eV }{ m }}=\frac{E}{ B } \\ \frac{ e }{ m }=\frac{ E ^{2}}{2 VB ^{2}} \end{array} $