To calculate the number of spectral lines emitted when a 12.5 eV electron beam bombards gaseous hydrogen, we need to consider the energy levels of the hydrogen atom.
In a hydrogen atom, electrons can occupy discrete energy levels given by:
E_n = -\frac{13.6}{n^2} \text{ eV}
where n is the principal quantum number.
Given that the electron beam energy is 12.5 eV, it can excite the hydrogen electron from the ground state (n = 1) to a higher energy level.
The energy difference between two levels is:
\Delta E = E_{n_f} - E_{n_i}
To find how high the electron can go using the given energy of 12.5 eV, we set:
12.5 = -\frac{13.6}{n^2} + (-13.6)
Solving for n:
12.5 = 13.6\left(1 - \frac{1}{n^2}\right)
\frac{12.5}{13.6} = 1 - \frac{1}{n^2}
\frac{1}{n^2} = 1 - \frac{12.5}{13.6}
\frac{1}{n^2} = \frac{1.1}{13.6} \approx 0.0809
n^2 \approx \frac{1}{0.0809} \approx 12.36
n \approx \sqrt{12.36} \approx 3.5
Since n must be an integer, the closest achievable level is n = 3.
The electron is excited to n = 3 and can transition back down to lower energy levels, emitting photons as it does. The possible transitions are:
Thus, a total of 3 spectral lines will be emitted.
The correct answer is: 3.
Match List-I with List-II.
| List-I | List-II |
| (A) Heat capacity of body | (I) \( J\,kg^{-1} \) |
| (B) Specific heat capacity of body | (II) \( J\,K^{-1} \) |
| (C) Latent heat | (III) \( J\,kg^{-1}K^{-1} \) |
| (D) Thermal conductivity | (IV) \( J\,m^{-1}K^{-1}s^{-1} \) |
In the given cycle ABCDA, the heat required for an ideal monoatomic gas will be:

The pressure of a gas changes linearly with volume from $A$ to $B$ as shown in figure If no heat is supplied to or extracted from the gas then change in the internal energy of the gas will be Is
