- A37°C.
- B62°C.
- C99°C.
- D124°C.
- 99°C.
Explanation:
Thermal capacity = Mass × Specific heat = m × s
Explanation:
Second law puts limitation on the efficiency of a heat engine and on the coefficient of performance of a refrigerator. Heat engine cannot have efficiency equal to 1 and a refrigerator cannot have infinite value of coefficient of performance.
$\frac52\text{R}$
Explanation:
Here, T1 = T, W = 6R
$\gamma=\frac{\text{C}_\text{P}}{\text{C}_\text{V}}=\frac53,\text{T}_2=?$
In and adiabatic process,
$\text{W}=\frac{\text{R}(\text{T}_2-\text{T}_1}{1-\gamma}$
$\text{6R}=\frac{\text{R}(\text{T}_2-\text{T}_1)}{1-\frac53}$
$\text{T}_2-\text{T}=6\Big(-\frac23\Big)=-4$
$\text{T}_2-\text{(T}-4)\text{K}$
$\alpha=\frac{\text{Q}_2}{\text{W}}$
Explanation:
For reversible engine, according to Carnot, efficiency is maximum.
Explanation:
During melting of ice, volume decreases. Therefore, positive work is done on the system by the atmosphere. Also heat spent in melting increases the internal energy of ice-water system.
Explanation:
Coefficient of performance of refrigerator is,
$\frac{\text{Q}_2}{\text{W}}=\frac{\text{T}_2}{\text{T}_1-\text{T}_2}$
When the door of a running refrigerator inside a room is left open, T2 → T1. Coefficient of performance increases. Q2 increases.
Therefore, heat energy given to the room increases. Hence the room will be warmed up gradually.
Explanation:
If two systems are in thermal equilibrium with each other, it means their temperatures must be same. Masses may be equal or unequal.
Explanation:
580 × 103 Calories are needed to convert 1kg H2O into steam.
1cal will producer sweat $=\frac{1}{580\times10^{3}}$
14.5 × 103cal will producer sweat $=\frac{14.5\times10^3}{580\times10^3}$
$=\frac{145}{5800}\text{kg }\text{per}\text{minute}=0.25\text{kg }\text{per}\text{minute}$
Explanation:
Key concept: Reversible process: A reversible process is one which can be reversed in such a way that all changes occurring in the direct process are exactly repeated in the opposite order and inverse sense and no change is left in any of the bodies taking part in the process or in the surroundings.
The conditions for reversibility are:
Irreversible process: Any process which is not reversible exactly is an irreversible process. All natural processes such as conduction, radiation, radioactive decay etc. are irreversible. All practical processes such as free expansion, Joule-Thomson expansion, electrical heating of a wire are also irreversible.