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12
Subjective

Can a system be heated and its temperature remains constant?

Explanation

Yes, this is possible when the entire heat supplied to the system is utilised in expansion. i.e., its working against the surroundings.

13
Subjective

A system goes from $P$ to $Q$ by two different paths in the $p-V$ diagram as shown in figure. Heat given to the system in path 1 is 1000 J . The work done by the system along path 1 is more than path 2 by 100 J . What is the heat exchanged by the system in path 2?

Explanation

$$ \begin{aligned} \text { For path 1, } \quad \text { Heat given } Q_1 & =+1000 \mathrm{~J} \\ \text { Work done } & =W_1 \text { (let) } \end{aligned}$$

For path 2,

Work done $$\left(W_2\right)=\left(W_1-100\right) \mathrm{J}$$

Heat given $Q_2=$ ?

$$\begin{aligned} &\text { As change in internal energy between two states for different path is same. }\\ &\begin{aligned} \therefore \quad & \Delta U =Q_1-W_1=Q_2-W_2 \\ \Rightarrow \quad & 1000-W_1 =Q_2-\left(W_1-100\right) \\ \Rightarrow \quad & Q_2 =1000-100=900 \mathrm{~J} \end{aligned} \end{aligned}$$

14
Subjective

If a refrigerator's door is kept open, will the room become cool or hot? Explain.

Explanation

If a refrigerator's door is kept open, then room will become hot, because amount of heat removed would be less than the amount of heat released in the room.

15
Subjective

Is it possible to increase the temperature of a gas without adding heat to it? Explain.

Explanation

Yes, during adiabatic compression the temperature of a gas increases while no heat is given to it.

$$\begin{aligned} \text{In adiabatic compression,}\quad & d Q=0 \\ \therefore \quad \text{From first law of thermodynamics,}\quad & d U=d Q-d W \\ & d U=-d W \end{aligned}$$

In compression work is done on the gas i.e., work done is negative.

Therefore, $$\quad d U=\text { Positive }$$

Hence, internal energy of the gas increases due to which its temperature increases.

16
Subjective

Air pressure in a car tyre increases during driving. Explain.

Explanation

During, driving, temperature of the gas increases while its volume remains constant.

So, according to Charle's law, at constant volume ($V$),

Pressure $(p) \propto$ Temperature $(T)$

Therefore, pressure of gas increases.