In Thomson's experiment, he found that the electron-to-mass (\(\frac em\)) ratio for cathode ray particles was the same regardless of the material of the electrodes or the gas inside the tube. This finding suggested that cathode rays consisted of particles (electrons) that were much lighter than atoms, which led to the conclusion that electrons were constituents of atoms and had a very high \(\frac em\) ratio compared to protons.
Therefore,
(\(\frac em\))electron >> (\(\frac em\))proton
[∴ (\(\frac em\))proton = \(\frac {1}{1837}\) (\(\frac em\))electron]
Option (A) is not correct because cathode rays are streams of electrons, not negatively charged ions.
Option (B) is not related to Thomson's experiment, as it concerns the atomic nucleus, which was not part of his investigation.
Option (D) is also not directly related to Thomson's experiment. The experiment mainly dealt with electrons and their properties, not with the effect of different gases in the discharge tube.
So, the correct option is (C): the \(\frac em\) of electrons is much greater than the \(\frac em\) of protons
The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :
A full wave rectifier circuit with diodes (\(D_1\)) and (\(D_2\)) is shown in the figure. If input supply voltage \(V_{in} = 220 \sin(100 \pi t)\) volt, then at \(t = 15\) msec: