As the temperature increases, the heat capacity also increases. Hence, the heat capacity of the second substance is greater than the first. Let the heat capacities be \( c_1 \) and \( c_2 \) for the first and second substances, respectively, and let the common temperature be \( T \). The equation for heat transfer is:
\(mc_1 (T - 0) = mc_2 (100 - T)\)
We can simplify this equation to:
\(\frac{T}{100 - T} = \frac{c_2}{c_1} > 1\)
This implies:
\(c_2 > c_1\)
Since \( \frac{T}{100 - T} > 1 \), it follows that:
\(T > 50\)
The temperature \( T \) must be greater than 50 for the heat capacity of the second substance to be greater than the first.
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) \( J\,m^{-1}K^{-1}s^{-1} \) |
Specific heat of a solid or liquid is the amount of heat that raises the temperature of a unit mass of the solid through 1°C.
The Molar specific heat of a solid or liquid of a material is the heat that you provide to raise the temperature of one mole of solid or liquid through 1K or 1°C.
The volume of solid remains constant when heated through a small range of temperature. This is known as specific heat at a constant volume. It is denoted as CV.
The pressure of solid remains constant when heated through a small range of temperature. This is known as specific heat at constant pressure which can be denoted as CP.