Chemical Thermodynamics MCQ Questions & Answers in Physical Chemistry | Chemistry
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51.
If an endothermic reaction is non-spontaneous at freezing point of water and becomes feasible at its boiling point, then
A
$$\Delta H\,is - ve,\,\Delta S\,is\, + ve$$
B
$$\Delta H\,and\,\,\Delta S\,\,both\,are\, + ve$$
TIPS/Formulae:
$$\Delta G = \Delta H - T\Delta S$$
Since $$\Delta G = \Delta H - T\Delta S$$ for an endothermic reaction,
$$\Delta H = + ve$$ and at low temperature $$\Delta S = + ve$$
Hence $$\Delta G = \left( + \right)\Delta H - T\left( + \right)\Delta S$$
and if $$T\Delta S < \Delta H$$ (at low temp)
$$\Delta G = + ve$$ (non spontaneous)
But at high temperature, reaction becomes spontaneous i.e. $$\Delta G = - ve.$$
because at higher temperature $$T\Delta S > \Delta H.$$
52.
Standard enthalpy and standard entropy changes for the oxidation of ammonia at $$298\,K$$ are $$ - 382.64\,kJ\,mo{l^{ - 1}}$$ and $$ - 145.6\,J{K^{ - 1}}mo{l^{ - 1}},$$ respectively. Standard Gibbs energy change for the same reaction at $$298\,K$$ is
53.
$${H_2}$$ gas is mixed with air at $${25^ \circ }C$$ under a pressure of 1 atmosphere and exploded in a closed vessel. The heat of the reaction, $${H_{2\left( g \right)}} + \frac{1}{2}{O_{2\left( g \right)}} \to {H_2}{O_{\left( \nu \right)}}$$ at constant volume, $$\Delta {U_{298\,K}} = - 240.60\,kJ\,mo{l^{ - 1}}$$ and $${C_V}$$ values for $${H_2}O$$ vapour and $${N_2}$$ in the temperature range $$298\,K$$ and $$3200\,K$$ are $$39.06\,J{K^{ - 1}}\,mo{l^{ - 1}}$$ and $$26.40\,J{K^{ - 1}}\,mo{l^{ - 1}}$$ respectively. The explosion temperature under adiabatic conditions is ( Given : $${n_{{N_2}}} = 2$$ )
A
$$2900\,K$$
B
$${2900^ \circ }C$$
C
$$2917\,K$$
D
$${3000^ \circ }C$$
Answer :
$$2917\,K$$
If the process is carried out adiabatically and isochorically,
$$\eqalign{
& \Delta U = \Delta {U_{{\text{heating}}}} + \Delta {U_{298\,K}} = 0\,\,{\text{or}}\,\,\Delta {U_{{\text{heating}}}} = - \Delta {U_{298\,K}} \cr
& \,\,\,\,\,\,\,\,\,\,\, = \int\limits_{298\,K}^{{T_f}} {n\sum {{C_\nu }dT} = + 240.60\,kJ\,mo{l^{ - 1}}} \cr
& \sum {n{C_\nu } = n \cdot {C_{\nu \left( {{H_2}{O_{\left( v \right)}}} \right)}} + n{C_{\nu \left( {{N_{2\left( g \right)}}} \right)}}} \cr
& \,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, = \left( {39.06 + 2 \times 26.40} \right) \cr
& \,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, = 91.86\,J{K^{ - 1}}\,mo{l^{ - 1}} \cr} $$
by using the value of $$\sum {n{C_\nu }} $$ in the above equation
$$\eqalign{
& \left( {91.86} \right)\left( {{T_f} - 298} \right) = 240600\,J\,mo{l^{ - 1}} \cr
& {T_f} - 298 = \frac{{240600}}{{91.86}} = 2619\,K \cr
& {T_f} = 2619 + 298 = 2917\,K \cr} $$
54.
The enthalpy of vapourization of liquid is $$30\,kJ\,mo{l^{ - 1}}$$ and entropy of vapourization is $$75\,J\,mo{l^{ - 1}}K.$$ The boiling point of the liquid at 1 atm is
55.
The species which by definition has zero standard molar enthalpy of formation at $$298\,K$$ is
A
$$B{r_2}\left( g \right)$$
B
$$C{l_2}\left( g \right)$$
C
$${H_2}O\left( g \right)$$
D
$$C{H_4}\left( g \right)$$
Answer :
$$C{l_2}\left( g \right)$$
The species in its elemental form has zero standard molar enthalpy of formation at $$298\,K.$$ At $$298\,K,C{l_2}$$ is gas while $$B{r_2}$$ is liquid.
56.
Boron can undergo the following reactions with the given enthalpy changes :
$$\eqalign{
& 2B\left( s \right) + \frac{3}{2}{O_2}\left( g \right) \to {B_2}{O_3}\left( s \right);\,\Delta H = - 1260\,kJ \cr
& 2B\left( s \right) + 3{H_2}\left( g \right) \to {B_2}{H_6}\left( g \right);\,\Delta H = 30\,kJ \cr} $$
Assume no other reactions are occurring.
If in a container ( operating at constant pressure ) which is isolated from the surrounding, mixture of $${H_2}$$ (gas) and $${O_2}$$ (gas) are passed over excess of $$B(s),$$ then calculate the molar ratio $$\left( {{O_2}:{H_2}} \right)$$ so that temperature of the container do not change :
A
15 : 3
B
42 : 1
C
1 : 42
D
1 : 84
Answer :
1 : 84
No. of moles of $${O_2}$$ required to supplied $$30\,kJ$$ heat to second reaction
$$\eqalign{
& = \frac{{30}}{{1260}} \times \frac{3}{2} = \frac{1}{{28}} \cr
& {n_{{O_2}}}:{n_{{H_2}}} = \frac{1}{{28}}:3\,\,\,{\text{or}}\,\,1:84 \cr} $$
57.
An ideal gas in a thermally insulated vessel at internal pressure $$ = {P_1},$$ volume $$ = {V_1}$$ and absolute temperature $$ = {T_1}$$ expands irreversibly against zero external pressure, as shown in the diagram. The final internal pressure, volume and absolute temperature of gas are $${P_2},{V_2}$$ and $${T_2},$$ respectively. For this expansion,
A
$$q = 0$$
B
$${T_2} = {T_1}$$
C
$${P_2}{V_2} = {P_1}{V_1}$$
D
$${\text{all of these}}$$
Answer :
$${\text{all of these}}$$
Since vessel is thermally insulated, i.e., the process is adiabatic hence, $$q = 0.$$ Also, $${P_{{\text{ext}}}} = 0,$$ hence $$w = 0$$
From 1st law of thermodynamics, $$\Delta U = q + w$$
$$\therefore \,\,\Delta U = 0$$ ( for ideal gas )
$$\therefore \,\,\Delta T = 0$$ or $${T_2} = {T_1}$$
[ $$\because $$ Internal energy of an ideal gas is a function of temperature. ]
Applying ideal gas equation, $$PV = nRT$$
where $$n, R$$ and $$T$$ are constant. Then $${P_1}{V_1} = {P_2}{V_2}$$
58.
Bond energies of few bonds are given below :
$$Cl - Cl \Rightarrow 242.8\,kJ\,mo{l^{ - 1}},$$ $$H - Cl \Rightarrow 431.8\,kJ\,mo{l^{ - 1}},$$
$$O - H \Rightarrow 464\,kJ\,mo{l^{ - 1}},$$ $$O = O \Rightarrow 442\,kJ\,mo{l^{ - 1}}$$
Using the $$B.E.,$$ calculate $$\Delta H$$ for the following reaction, $$2C{l_2} + 2{H_2}O \to 4HCl + {O_2}$$
59.
The difference between the reaction enthalpy change $$\left( {{\Delta _r}H} \right)$$ and reaction internal energy change $$\left( {{\Delta _r}U} \right)$$ for the reaction :
$$2{C_6}{H_6}\left( l \right) + 15{O_2}\left( g \right) \to 12C{O_2}\left( g \right) + 6{H_2}O\left( l \right)$$ at $$300\,K$$ is $$\left( {R = 8.314\,J\,mo{l^{ - 1}}{K^{ - 1}}} \right)$$
A
$$0\,J\,mo{l^{ - 1}}$$
B
$$2490\,J\,mo{l^{ - 1}}$$
C
$$ - 2490\,J\,mo{l^{ - 1}}$$
D
$$ - 7482\,J\,mo{l^{ - 1}}$$
Answer :
$$ - 7482\,J\,mo{l^{ - 1}}$$
$$\eqalign{
& \Delta H = \Delta U + \Delta {n_g}RT \cr
& {\text{For the reaction}}\,\,\Delta {n_g} = 12 - 15 = - 3 \cr
& \Delta H - \Delta U = - 3 \times 8.314 \times 300 \cr
& = - 7482\,J\,mo{l^{ - 1}} \cr} $$
60.
For the reaction $$CO\left( g \right) + \frac{1}{2}{O_2}\left( g \right) \to C{O_2}\left( g \right),\Delta H,$$ and $$\Delta S$$ are $$ - 283\,kJ$$ and $$ - 87\,J{K^1},$$ respectively. It was intended to carry out this reaction at 1000, 1500, 3000 and 3500 $$K.$$ At which of these temperatures would this reaction be thermodynamically spontaneous?
A
1500 and 3500 $$K$$
B
3000 and 3500 $$K$$
C
1000, 1500 and 3000 $$K$$
D
1500, 3000 and 3500 $$K$$
Answer :
1000, 1500 and 3000 $$K$$
$$\because \,\,\Delta G = \Delta H - T \times \Delta S$$
For a spontaneous reaction, $$\Delta G$$ should be negative
$$\Delta H = - 238\,kJ,\,\Delta S = - 87\,J{K^{ - 1}}$$
Hence, reaction will be spontaneous when $$\Delta H > T \times \Delta S.$$ Therefore, at 1000, 1500 and 3000 $$K$$ the reaction would be spontaneous.