To find the value of one vernier scale division, we will use the concept of a vernier caliper. A vernier caliper is a precision instrument used to measure length with great accuracy. It consists of a main scale and a vernier scale.
The relationship between the least count, main scale division, and vernier scale division can be expressed as:
\[ \text{Least Count (LC)} = \text{Value of 1 main scale division (MSD)} - \text{Value of 1 vernier scale division (VSD)} \]From the given data:
Substitute these values into the formula for the least count:
\[ \frac{1}{200N} = 1 - \text{VSD} \]Solving for the vernier scale division (VSD):
\[ \text{VSD} = 1 - \frac{1}{200N} \] \[ \text{VSD} = \frac{200N}{200N} - \frac{1}{200N} \] \[ \text{VSD} = \frac{200N - 1}{200N} \] \[ \text{VSD} = \frac{2N - 1}{2N} \text{ mm} \]Thus, the value of one vernier scale division is \frac{2N-1}{2N} \text{ mm}. Therefore, the correct answer is:
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
