ExamGOAL
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47
Subjective

Represent the potential energy/enthalpy change in the following processes graphically.

(a) Throwing a stone from the ground to roof.

(b) $\frac{1}{2} \mathrm{H}_2(\mathrm{~g})+\frac{1}{2} \mathrm{Cl}_2(\mathrm{~g}) \rightleftharpoons \mathrm{HCl}(\mathrm{g}) \Delta_r H^{\mathrm{s}}=-92.32 \mathrm{~kJ} \mathrm{~mol}^{-1}$

In which of the processes potential energy/enthalpy change is contributing factor to the spontaneity?

Explanation

Representation of potential energy/enthalpy change in the following processes

(a) Throwing a stone from the ground to roof.

(b) $\frac{1}{2} \mathrm{H}_2(g)+\frac{1}{2} \mathrm{Cl}_2(g) \rightleftharpoons \mathrm{HCl}(g) ; \Delta_r H^s=-92.32 \mathrm{~kJ} \mathrm{~mol}^{-1}$

Energy increases in (a) and it decreases in (b) process. Hence, in process (b), enthalpy change is the contributing factor to the spontaneity.

48
Subjective

Enthalpy diagram for a particular reaction is given in figure. Is it possible to decide spontaneity of a reaction from given diagram. Explain.

Explanation

No, enthalpy is one of the contributing factors in deciding spontaneity but it is not the only factor. Another contributory factor, entropy factor has also to be taken into consideration.

49
Subjective

1.0 mol of a monoatomic ideal gas is expanded from state (1) to state (2) as shown in figure. Calculate the work done for the expansion of gas from state (1) to state (2) at 298 K .

Explanation

The given diagram represent that the process is carried out in infinite steps, hence it is isothermal reversible expansion of the ideal gas from pressure 2.0 atm to 1.0 atm 298 K .

$$\begin{aligned} & W=-2.303 n R T \log \frac{p_1}{p_2} \\ & W=-2.303 \times 1 \mathrm{~mol} \times 8.314 \mathrm{JK}^{-1} \mathrm{~mol}^{-1} \times 298 \mathrm{Klog} 2 \quad \left(\because \frac{p_1}{p_2}=\frac{2}{1}\right)\\ & W=-2.303 \times 1 \times 8.314 \times 298 \times 0.3010 \mathrm{~J} \\ & W=-1717.46 \mathrm{~J} \end{aligned}$$

50
Subjective

An ideal gas is allowed to expand against a constant pressure of 2 bar from 10 L to 50 L in one step. Calculate the amount of work done by the gas. If the same expansion were carried out reversibly, will the work done be higher or lower than the earlier case? (Given that, 1 L bar = 100 J )

Explanation

In the first case, as the expansion is against constant external pressure

$$\begin{aligned} W & =-p_{\text {ext }}\left(V_2-V_1\right)=-2 \text { bar } \times(50-10) \mathrm{L} \\ & =-80 \mathrm{~L} \text { bar } \quad \text{(1L bar = 100 J)}\\ & =-80 \times 100 \mathrm{~J} \\ & =-8 \mathrm{~kJ} \end{aligned}$$

If the given expansion was carried out reversibly, the internal pressure of the gas should be greater than the external pressure at every stage. Hence, the work done will be more.

51
Subjective

Match the following.

List I List II
A. Adiabatic process 1. Heat
B. Isolated system 2. At constant volume
C. Isothermal change 3. First law of thermodynamics
D. Path function 4. No exchange of energy and matter
E. State function 5. No transfer of heat
F. $$\Delta U=q$$ 6. Constant temperature
G. Law of conservation of energy 7. Internal energy
H. Reversible process 8. $$p_{ext=0}$$
I. Free expansion 9. At constant pressure
J. $$\Delta H=q$$ 10. Infinitely slow process which proceeds through a series of equilibrium states.
K. Intensive property 11. Entropy
L. Extensive property 12. Pressure
13. Specific heat

Explanation

$$\begin{aligned} &\begin{aligned} & \text { I. } \rightarrow(8) \quad \text { J. } \rightarrow(9) \quad \text { K. } \rightarrow(1,12,13) \quad \text { L. } \rightarrow(7,11) \end{aligned}\\ &\text { I. } \rightarrow(8) \quad \text { J. } \rightarrow(9) \quad \text { K. } \rightarrow(1,12,13) \quad \text { L. } \rightarrow(7,11) \end{aligned}$$

Correct matching can be done as

A. Adiabatic process No transfer of heat
B. Isolated system No exchange of energy and matter
C. Isothermal change Constant temperature
D. Path function Heat
E. State function Internal energy
Entropy
Pressure
F. $$\Delta U=q$$ At constant volume
G. Law of conservation of energy First law of thermodynamics
H. Reversible process Infinitely slow process which proceeds through a series of equilibrium states
I. Free expansion $$p_{ext}=0$$
J. $$\Delta H=q$$ At constant pressure
K. Intensive property Heat
Pressure
Specific heat
L. Extensive property Internal energy
Entropy