



To solve this problem, we need to understand how the temperature of the liquids in breakers A and B changes over time. The rate at which a liquid cools down depends on its mass, specific heat capacity, and the difference in temperature between the liquid and its surroundings.
Let's analyze each breaker's properties:
Both liquids are initially at the same temperature of \(60^\circ \text{C}\). Assuming the volumes are equal and the emissivity of both breakers is the same, we can use the properties of heat transfer to understand the cooling process:
The cooling rate depends on the heat capacity (mass × specific heat capacity). The heat capacity is a measure of the energy required to change the temperature of a substance. A higher heat capacity means a slower cooling rate for the same temperature difference.
We calculate the heat capacity for each liquid:
Let's simplify this analysis using ratios since the actual volumes and masses are not provided:
Given the higher specific heat of liquid B, even with its lower density, it results in a higher heat capacity compared to liquid A.
Conclusion:
Liquid B, having a higher effective heat capacity, will cool down more slowly compared to liquid A. This implies that the temperature vs. time curve for liquid B will have a gentler slope compared to that of liquid A, meaning that it retains its heat longer.
The correct graph visually represents the slower cooling rate of liquid B compared to liquid A.
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
