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
In the given cycle ABCDA, the heat required for an ideal monoatomic gas will be:
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
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 :
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.