MCQ 1011 Mark
A thermo-dynamical system is changed from state $\left(P_1, V_1\right)$ to $\left(P_2, V_2\right)$ by two different process. The quantity which will remain same will be
- A
$\Delta Q$
- B
$\Delta W$
- C
$\Delta Q+\Delta W$
- ✓
$\Delta Q-\Delta W$
AnswerCorrect option: D. $\Delta Q-\Delta W$
(d) Change in internal energy does not depend upon path so $\Delta U=\Delta Q-\Delta W$ remain constant.
View full question & answer→MCQ 1021 Mark
When an ideal gas $(\gamma=5 / 3)$ is heated under constant pressure, then what percentage of given heat energy will be utilised in doing external work
- ✓
$40 \%$
- B
$30 \%$
- C
$60 \%$
- D
$20 \%$
AnswerCorrect option: A. $40 \%$
(a)$\Delta Q=\Delta U+\Delta W \Rightarrow \frac{\Delta W}{\Delta Q}=1\frac{\Delta U}{\Delta Q}=1-\frac{n C_V d T}{n C_P d T} $
$\Rightarrow \frac{\Delta W}{\Delta Q}=1\frac{C_V}{C_P}=1-\frac{3}{5}=\frac{2}{5}=0.4$
View full question & answer→MCQ 1031 Mark
Two moles of an ideal monoatomic gas at $27^{\circ} \mathrm{C}$ occupies a volume of $v$. If the gas is expanded adiabatically to the volume $2 \mathrm{~V}$, then the work done by the gas will be $[\gamma=5 / 3, R=8.31 \mathrm{~J} / \mathrm{mol} \mathrm{K}]$
- A
$-2767.23 \mathrm{~J}$
- ✓
$2767.23 \mathrm{~J}$
- C
$2500 \mathrm{~J}$
- D
$-2500 \mathrm{~J}$
AnswerCorrect option: B. $2767.23 \mathrm{~J}$
$W =\frac{\mu R\left(T_1-T_2\right)}{(\gamma-1)}=\frac{\mu R T_1}{(\gamma-1)}\left[1-\frac{T_2}{T_1}\right] =\frac{\mu RT_1}{(\gamma-1} \left[1\left(\frac{V_1}{V_2}\right)^{\gamma-1}\right] v$
$ =\frac{2 \times 8.31 \times 300}{\left(\frac{5}{3}-1\right)}\left[1-\left(\frac{1}{2}\right)^{\frac{5}{3}-1}\right]=+2767.23 \mathrm{~J}$
View full question & answer→MCQ 1041 Mark
A thermally insulated container is divided into two parts by a screen. In one part the pressure and temperature are $P$ and $T$ for an ideal gas filled. In the second part it is vacuum. If now a small hole is created in the screen, then the temperature of the gas will
Answer(c) This is the case of free expansion of gas. In free expansion $\Delta U=0 \Rightarrow$ Temp. remains same.
View full question & answer→MCQ 1051 Mark
A thermo-dynamical system is changed from state $\left(P_1, V_1\right)$ to $\left(P_2, V_2\right)$ by two different process. The quantity which will remain same will be
- A
$\Delta Q$
- B
$\Delta W$
- C
$\Delta Q+\Delta W$
- ✓
$\Delta Q-\Delta W$
AnswerCorrect option: D. $\Delta Q-\Delta W$
(d) Change in internal energy does not depend upon path so $\Delta U=\Delta Q-\Delta W$ remain constant.
View full question & answer→MCQ 1061 Mark
When an ideal gas $(\gamma=5 / 3)$ is heated under constant pressure, then what percentage of given heat energy will be utilised in doing external work
- ✓
$40 \%$
- B
$30 \%$
- C
$60 \%$
- D
$20 \%$
AnswerCorrect option: A. $40 \%$
(a)$\Delta Q=\Delta U+\Delta W \Rightarrow \frac{\Delta W}{\Delta Q}=1\frac{\Delta U}{\Delta Q}=1-\frac{n C_V d T}{n C_P d T} $
$\Rightarrow \frac{\Delta W}{\Delta Q}=1\frac{C_V}{C_P}=1-\frac{3}{5}=\frac{2}{5}=0.4$
View full question & answer→MCQ 1071 Mark
Two moles of an ideal monoatomic gas at $27^{\circ} \mathrm{C}$ occupies a volume of $v$. If the gas is expanded adiabatically to the volume $2 \mathrm{~V}$, then the work done by the gas will be $[\gamma=5 / 3, R=8.31 \mathrm{~J} / \mathrm{mol} \mathrm{K}]$
- A
$-2767.23 \mathrm{~J}$
- ✓
$2767.23 \mathrm{~J}$
- C
$2500 \mathrm{~J}$
- D
$-2500 \mathrm{~J}$
AnswerCorrect option: B. $2767.23 \mathrm{~J}$
(b)$\begin{aligned}W & =\frac{\mu R\left(T_1-T_2\right)}{(\gamma-1)}=\frac{\mu R T_1}{(\gamma-1)}\left[1-\frac{T_2}{T_1}\right] \\&=\frac{\muRT_1{(\gamma-1\left[1\left(\frac{V_1}{V_2}\right)^{\gamma-1}\right] \\& =\frac{2 \times 8.31 \times 300{\left(\frac{5{3}-1\right)}\left[1-\left(\frac{1}{2}\right)^{\frac{5}{3}-1}\right]=+2767.23 \mathrm{~J}\end{aligned}$
View full question & answer→MCQ 1081 Mark
A thermally insulated container is divided into two parts by a screen. In one part the pressure and temperature are $P$ and $T$ for an ideal gas filled. In the second part it is vacuum. If now a small hole is created in the screen, then the temperature of the gas will
Answer(c) This is the case of free expansion of gas. In free expansion $\Delta U=0 \Rightarrow$ Temp. remains same.
View full question & answer→MCQ 1091 Mark
A thermo-dynamical system is changed from state $\left(P_1, V_1\right)$ to $\left(P_2, V_2\right)$ by two different process. The quantity which will remain same will be
- A
$\Delta Q$
- B
$\Delta W$
- C
$\Delta Q+\Delta W$
- ✓
$\Delta Q-\Delta W$
AnswerCorrect option: D. $\Delta Q-\Delta W$
(d) Change in internal energy does not depend upon path so $\Delta U=\Delta Q-\Delta W$ remain constant.
View full question & answer→MCQ 1101 Mark
When an ideal gas $(\gamma=5 / 3)$ is heated under constant pressure, then what percentage of given heat energy will be utilised in doing external work
- ✓
$40 \%$
- B
$30 \%$
- C
$60 \%$
- D
$20 \%$
AnswerCorrect option: A. $40 \%$
(a)$\Delta Q=\Delta U+\Delta W \Rightarrow \frac{\Delta W}{\Delta Q}=1\frac{\Delta U}{\Delta Q}=1-\frac{n C_V d T}{n C_P d T} $
$\Rightarrow \frac{\Delta W}{\Delta Q}=1\frac{C_V}{C_P}=1-\frac{3}{5}=\frac{2}{5}=0.4$
View full question & answer→MCQ 1111 Mark
Two moles of an ideal monoatomic gas at $27^{\circ} \mathrm{C}$ occupies a volume of $v$. If the gas is expanded adiabatically to the volume $2 \mathrm{~V}$, then the work done by the gas will be $[\gamma=5 / 3, R=8.31 \mathrm{~J} / \mathrm{mol} \mathrm{K}]$
- A
$-2767.23 \mathrm{~J}$
- ✓
$2767.23 \mathrm{~J}$
- C
$2500 \mathrm{~J}$
- D
$-2500 \mathrm{~J}$
AnswerCorrect option: B. $2767.23 \mathrm{~J}$
$W =\frac{\mu R\left(T_1-T_2\right)}{(\gamma-1)}=\frac{\mu R T_1}{(\gamma-1)}\left[1-\frac{T_2}{T_1}\right] =\frac{\mu RT_1}{(\gamma-1} \left[1\left(\frac{V_1}{V_2}\right)^{\gamma-1}\right] v$
$ =\frac{2 \times 8.31 \times 300}{\left(\frac{5}{3}-1\right)}\left[1-\left(\frac{1}{2}\right)^{\frac{5}{3}-1}\right]=+2767.23 \mathrm{~J}$
View full question & answer→MCQ 1121 Mark
If $C_V=4.96 \mathrm{cal} /$ mole $K$, then increase in internal energy when temperature of $2$ moles of this gas is increased from $340 K$ to $342 K$
- A
$27.80 \mathrm{cal}$
- ✓
$19.84 \mathrm{cal}$
- C
$13.90 \mathrm{cal}$
- D
$9.92 \mathrm{cal}$
AnswerCorrect option: B. $19.84 \mathrm{cal}$
$\Delta U=\mu C_V \Delta T$
$=2 \times 4.96 \times(342-340)$
$=19.84 \mathrm{cal}$
View full question & answer→MCQ 1131 Mark
If $C_V=4.96 \mathrm{cal} /$ mole $K$, then increase in internal energy when temperature of $2$ moles of this gas is increased from $340 K$ to $342 K$
- A
$27.80 \mathrm{cal}$
- ✓
$19.84 \mathrm{cal}$
- C
$13.90 \mathrm{cal}$
- D
$9.92 \mathrm{cal}$
AnswerCorrect option: B. $19.84 \mathrm{cal}$
$\Delta U=\mu C_V \Delta T$
$=2 \times 4.96 \times(342-340)$
$=19.84 \mathrm{cal}$
View full question & answer→MCQ 1141 Mark
If $C_V=4.96 \mathrm{cal} /$ mole $K$, then increase in internal energy when temperature of $2$ moles of this gas is increased from $340 K$ to $342 K$
- A
$27.80 \mathrm{cal}$
- ✓
$19.84 \mathrm{cal}$
- C
$13.90 \mathrm{cal}$
- D
$9.92 \mathrm{cal}$
AnswerCorrect option: B. $19.84 \mathrm{cal}$
$\Delta U=\mu C_V \Delta T$
$=2 \times 4.96 \times(342-340)$
$=19.84 \mathrm{cal}$
View full question & answer→MCQ 1151 Mark
If $\Delta Q$ and $\Delta W$ represent the heat supplied to the system and the work done on the system respectively, then the first law of thermodynamics can be written as where $\Delta U$ is the internal energy
- A
$\Delta Q=\Delta U+\Delta W$
- ✓
$\Delta Q=\Delta U-\Delta W$
- C
$\Delta Q=\Delta W-\Delta U$
- D
$\Delta Q=-\Delta W-\Delta U$
AnswerCorrect option: B. $\Delta Q=\Delta U-\Delta W$
From FLOT $\Delta Q=\Delta U+\Delta W$
$\because$ Heat supplied to the system so $\Delta Q \rightarrow$ Positive and work is done on the system so $\Delta W \rightarrow$ Negative.
Hence $+\Delta Q=\Delta U-\Delta W$
View full question & answer→MCQ 1161 Mark
If $\Delta Q$ and $\Delta W$ represent the heat supplied to the system and the work done on the system respectively, then the first law of thermodynamics can be written as where $\Delta U$ is the internal energy
- A
$\Delta Q=\Delta U+\Delta W$
- ✓
$\Delta Q=\Delta U-\Delta W$
- C
$\Delta Q=\Delta W-\Delta U$
- D
$\Delta Q=-\Delta W-\Delta U$
AnswerCorrect option: B. $\Delta Q=\Delta U-\Delta W$
From FLOT $\Delta Q=\Delta U+\Delta W$
$\because$ Heat supplied to the system so $\Delta Q \rightarrow$ Positive and work is done on the system so $\Delta W \rightarrow$ Negative.
Hence $+\Delta Q=\Delta U-\Delta W$
View full question & answer→MCQ 1171 Mark
If $\Delta Q$ and $\Delta W$ represent the heat supplied to the system and the work done on the system respectively, then the first law of thermodynamics can be written as where $\Delta U$ is the internal energy
- A
$\Delta Q=\Delta U+\Delta W$
- ✓
$\Delta Q=\Delta U-\Delta W$
- C
$\Delta Q=\Delta W-\Delta U$
- D
$\Delta Q=-\Delta W-\Delta U$
AnswerCorrect option: B. $\Delta Q=\Delta U-\Delta W$
From FLOT $\Delta Q=\Delta U+\Delta W$
$\because$ Heat supplied to the system so $\Delta Q \rightarrow$ Positive and work is done on the system so $\Delta W \rightarrow$ Negative.
Hence $+\Delta Q=\Delta U-\Delta W$
View full question & answer→MCQ 1181 Mark
Unit mass of a liquid with volume $V_1$ is completely changed into a gas of volume $V_2$ at a constant external pressure $P$ and temperature $T$. If the latent heat of evaporation for the given mass is $L$, then the increase in the internal energy of the system is
AnswerCorrect option: C. $L-P\left(V_2-V_1\right)$
$\Delta Q=\Delta V+P \Delta V $
$\Rightarrow m L=\Delta U+P(V-V)$
$\Rightarrow \Delta U=L-P(V-V) \quad(\because m=1)$
View full question & answer→MCQ 1191 Mark
Unit mass of a liquid with volume $V_1$ is completely changed into a gas of volume $V_2$ at a constant external pressure $P$ and temperature $T$. If the latent heat of evaporation for the given mass is $L$, then the increase in the internal energy of the system is
AnswerCorrect option: C. $L-P\left(V_2-V_1\right)$
$\Delta Q=\Delta V+P \Delta V $
$\Rightarrow m L=\Delta U+P(V-V)$
$\Rightarrow \Delta U=L-P(V-V) \quad(\because m=1)$
View full question & answer→MCQ 1201 Mark
Unit mass of a liquid with volume $V_1$ is completely changed into a gas of volume $V_2$ at a constant external pressure $P$ and temperature $T$. If the latent heat of evaporation for the given mass is $L$, then the increase in the internal energy of the system is
AnswerCorrect option: C. $L-P\left(V_2-V_1\right)$
$\Delta Q=\Delta V+P \Delta V $
$\Rightarrow m L=\Delta U+P(V-V)$
$\Rightarrow \Delta U=L-P(V-V) \quad(\because m=1)$
View full question & answer→MCQ 1211 Mark
A thermodynamic process in which temperature $T$ of the system remains constant though other variable $P$ and $V$ may change, is called
AnswerIn isothermal process, temperature remains constant.
View full question & answer→MCQ 1221 Mark
A thermodynamic process in which temperature $T$ of the system remains constant though other variable $P$ and $V$ may change, is called
AnswerIn isothermal process, temperature remains constant.
View full question & answer→MCQ 1231 Mark
A thermodynamic process in which temperature $T$ of the system remains constant though other variable $P$ and $V$ may change, is called
AnswerIn isothermal process, temperature remains constant.
View full question & answer→MCQ 1241 Mark
One mole of an ideal monoatomic gas is heated at a constant pressure of one atmosphere from $0^{\circ} \mathrm{C}$ to $100^{\circ} \mathrm{C}$. Then the change in the internal energy is
AnswerCorrect option: C. $12.48 \times 10^2$ joules
Change in internal energy is always equal to the heat supplied at constant volume.
i.e. $\Delta U=(\Delta Q)_V=\mu C_V\Delta T$.
Form onoatomicgas $(C_V=\frac{3}{2R})$
$\Rightarrow \Delta U =\mu\left(\frac{3}{2} R\right) \Delta T$
$=1 \times\frac{3}{2}\times8.31\times(100-0)$
$ =12.48 \times 10^2 J$
View full question & answer→MCQ 1251 Mark
One mole of an ideal monoatomic gas is heated at a constant pressure of one atmosphere from $0^{\circ} \mathrm{C}$ to $100^{\circ} \mathrm{C}$. Then the change in the internal energy is
AnswerCorrect option: C. $12.48 \times 10^2$ joules
Change in internal energy is always equal to the heat supplied at constant volume.
i.e. $\Delta U=(\Delta Q)_V=\mu C_V\Delta T$.
Form onoatomicgas $(C_V=\frac{3}{2R})$
$\Rightarrow \Delta U =\mu\left(\frac{3}{2} R\right) \Delta T$
$=1 \times\frac{3}{2}\times8.31\times(100-0)$
$ =12.48 \times 10^2 J$
View full question & answer→MCQ 1261 Mark
One mole of an ideal monoatomic gas is heated at a constant pressure of one atmosphere from $0^{\circ} \mathrm{C}$ to $100^{\circ} \mathrm{C}$. Then the change in the internal energy is
AnswerCorrect option: C. $12.48 \times 10^2$ joules
Change in internal energy is always equal to the heat supplied at constant volume.
i.e. $\Delta U=(\Delta Q)_V=\mu C_V\Delta T$.
Form onoatomicgas $(C_V=\frac{3}{2R})$
$\Rightarrow \Delta U =\mu\left(\frac{3}{2} R\right) \Delta T$
$=1 \times\frac{3}{2}\times8.31\times(100-0)$
$ =12.48 \times 10^2 J$
View full question & answer→MCQ 1271 Mark
A container that suits the occurrence of an isothermal process should be made of
AnswerAn isothermal process takes place at constant temperature, must be carried out in a vessel with conducting wall so that heat generated should go out at once.
View full question & answer→MCQ 1281 Mark
A container that suits the occurrence of an isothermal process should be made of
AnswerAn isothermal process takes place at constant temperature, must be carried out in a vessel with conducting wall so that heat generated should go out at once.
View full question & answer→MCQ 1291 Mark
A container that suits the occurrence of an isothermal process should be made of
AnswerAn isothermal process takes place at constant temperature, must be carried out in a vessel with conducting wall so that heat generated should go out at once.
View full question & answer→MCQ 1301 Mark
A carnot engine has the same efficiency between $800 K$ to $500 K$ and $x K$ to $600 K$. The value of $x$ is
- A
$1000 \mathrm{~K}$
- ✓
$960 K$
- C
$846 K$
- D
$754 K$
AnswerCorrect option: B. $960 K$
In first case, $\left(\eta_1\right)=1-\frac{500}{800}=\frac{3}{8}$ and
in second case, $\left(\eta_2\right)=1-\frac{600}{x}$
Since $\eta_1=\eta_2$,
therefore $\frac{3}{8}=1-\frac{600}{x}$
$\text { or } \frac{600}{x}=1-\frac{3}{8}=\frac{5}{8} \text { or }x=\frac{600 \times 8}{5}=960 \mathrm{~K}$
View full question & answer→MCQ 1311 Mark
A carnot engine has the same efficiency between $800 K$ to $500 K$ and $x K$ to $600 K$. The value of $x$ is
- A
$1000 \mathrm{~K}$
- ✓
$960 K$
- C
$846 K$
- D
$754 K$
AnswerCorrect option: B. $960 K$
In first case, $\left(\eta_1\right)=1-\frac{500}{800}=\frac{3}{8}$ and
in second case, $\left(\eta_2\right)=1-\frac{600}{x}$
Since $\eta_1=\eta_2$,
therefore $\frac{3}{8}=1-\frac{600}{x}$
$\text { or } \frac{600}{x}=1-\frac{3}{8}=\frac{5}{8} \text { or }x=\frac{600 \times 8}{5}=960 \mathrm{~K}$
View full question & answer→MCQ 1321 Mark
A carnot engine has the same efficiency between $800 K$ to $500 K$ and $x K$ to $600 K$. The value of $x$ is
- A
$1000 \mathrm{~K}$
- ✓
$960 K$
- C
$846 K$
- D
$754 K$
AnswerCorrect option: B. $960 K$
In first case, $\left(\eta_1\right)=1-\frac{500}{800}=\frac{3}{8}$ and
in second case, $\left(\eta_2\right)=1-\frac{600}{x}$
Since $\eta_1=\eta_2$, therefore $\frac{3}{8}=1-\frac{600}{x}$
$\text { or } \frac{600}{x}=1-\frac{3}{8}=\frac{5}{8}$
$\text { or }x=\frac{600 \times 8}{5}=960 \mathrm{~K}$
View full question & answer→MCQ 1331 Mark
A gas is suddenly compressed to one fourth of its original volume. What will be its final pressure, if its initial pressure is $P$
- A
Lesss than $P$
- ✓
More than $P$
- C
$P$
- D
AnswerCorrect option: B. More than $P$
$P V^\gamma=\text { constant } $
$\Rightarrow \frac{P_2}{P_1}=\left(\frac{V_1}{V_2}\right)^\gamma=\left(\frac{V_1}{V_1 / 4}\right)^\gamma=4^\gamma $
$\Rightarrow P_2=4^\gamma P$
As $\gamma$ is always greater than one so $4^\gamma>4 \Rightarrow P_2>4 P$
View full question & answer→MCQ 1341 Mark
A gas is suddenly compressed to one fourth of its original volume. What will be its final pressure, if its initial pressure is $P$
- A
Lesss than $P$
- ✓
More than $P$
- C
$P$
- D
AnswerCorrect option: B. More than $P$
$P V^\gamma=\text { constant } $
$\Rightarrow \frac{P_2}{P_1}=\left(\frac{V_1}{V_2}\right)^\gamma=\left(\frac{V_1}{V_1 / 4}\right)^\gamma=4^\gamma $
$\Rightarrow P_2=4^\gamma P$
As $\gamma$ is always greater than one so $4^\gamma>4 \Rightarrow P_2>4 P$
View full question & answer→MCQ 1351 Mark
A gas is suddenly compressed to one fourth of its original volume. What will be its final pressure, if its initial pressure is $P$
- A
Lesss than $P$
- ✓
More than $P$
- C
$P$
- D
AnswerCorrect option: B. More than $P$
$P V^\gamma=\text { constant }$
$ \Rightarrow \frac{P_2}{P_1}=\left(\frac{V_1}{V_2}\right)^\gamma=\left(\frac{V_1}{V_1 / 4}\right)^\gamma=4^\gamma $
$\Rightarrow P_2=4^\gamma P$
As $\gamma$ is always greater than one so $4^\gamma>4 \Rightarrow P_2 > 4 P$
View full question & answer→MCQ 1361 Mark
If $300 \mathrm{ml}$ of a gas at $27^{\circ} \mathrm{C}$ is cooled to $7^{\circ} \mathrm{C}$ at constant pressure, then its final volume will be
- A
$540 \mathrm{ml}$
- B
$350 \mathrm{ml}$
- ✓
$280 \mathrm{ml}$
- D
$135 \mathrm{ml}$
AnswerCorrect option: C. $280 \mathrm{ml}$
$V \propto T$ at constant pressure
$\Rightarrow \frac{V_1}{V_2}=\frac{T_1}{T_2}$
$\Rightarrow V_2=\frac{V_1 T_2}{T_1}$
$=\frac{300 \times 280}{300}$
$=280 \mathrm{ml} \text {. }$
View full question & answer→MCQ 1371 Mark
If $300 \mathrm{ml}$ of a gas at $27^{\circ} \mathrm{C}$ is cooled to $7^{\circ} \mathrm{C}$ at constant pressure, then its final volume will be
- A
$540 \mathrm{ml}$
- B
$350 \mathrm{ml}$
- ✓
$280 \mathrm{ml}$
- D
$135 \mathrm{ml}$
AnswerCorrect option: C. $280 \mathrm{ml}$
$V \propto T$ at constant pressure $\Rightarrow \frac{V_1}{V_2}=\frac{T_1}{T_2}$
$\Rightarrow V_2=\frac{V_1 T_2}{T_1}$
$=\frac{300 \times 280}{300}$
$=280 \mathrm{ml} \text {. }$
View full question & answer→MCQ 1381 Mark
If $300 \mathrm{ml}$ of a gas at $27^{\circ} \mathrm{C}$ is cooled to $7^{\circ} \mathrm{C}$ at constant pressure, then its final volume will be
- A
$540 \mathrm{ml}$
- B
$350 \mathrm{ml}$
- ✓
$280 \mathrm{ml}$
- D
$135 \mathrm{ml}$
AnswerCorrect option: C. $280 \mathrm{ml}$
$V \propto T$ at constant pressure
$\Rightarrow \frac{V_1}{V_2}=\frac{T_1}{T_2}$
$\Rightarrow V_2=\frac{V_1 T_2}{T_1}$
$=\frac{300 \times 280}{300}$
$=280 \mathrm{ml} \text {. }$
View full question & answer→MCQ 1391 Mark
The latent heat of vaporisation of water is $2240 \mathrm{~J} / \mathrm{gm}$. If the work done in the process of expansion of $1 \mathrm{~g}$ is $168 \mathrm{~J}$, then increase in internal energy is
- A
$2408 \mathrm{~J}$
- B
$2240 \mathrm{~J}$
- ✓
$2072 \mathrm{~J}$
- D
$1904 \mathrm{~J}$
AnswerCorrect option: C. $2072 \mathrm{~J}$
$\Delta Q=\Delta U+\Delta W$
$ \Rightarrow \Delta U=\Delta Q-\Delta W$
$=2240-168$
$=2072\mathrm{~J}$.
View full question & answer→MCQ 1401 Mark
The latent heat of vaporisation of water is $2240 \mathrm{~J} / \mathrm{gm}$. If the work done in the process of expansion of $1 \mathrm{~g}$ is $168 \mathrm{~J}$, then increase in internal energy is
- A
$2408 \mathrm{~J}$
- B
$2240 \mathrm{~J}$
- ✓
$2072 \mathrm{~J}$
- D
$1904 \mathrm{~J}$
AnswerCorrect option: C. $2072 \mathrm{~J}$
$\Delta Q=\Delta U+\Delta W$
$ \Rightarrow \Delta U=\Delta Q-\Delta W$
$=2240-168$
$=2072\mathrm{~J}$.
View full question & answer→MCQ 1411 Mark
The latent heat of vaporisation of water is $2240 \mathrm{~J} / \mathrm{gm}$. If the work done in the process of expansion of $1 \mathrm{~g}$ is $168 \mathrm{~J}$, then increase in internal energy is
- A
$2408 \mathrm{~J}$
- B
$2240 \mathrm{~J}$
- ✓
$2072 \mathrm{~J}$
- D
$1904 \mathrm{~J}$
AnswerCorrect option: C. $2072 \mathrm{~J}$
$\Delta Q=\Delta U+\Delta W $
$\Rightarrow \Delta U=\Delta Q-\Delta W$
$=2240-168$
$=2072\mathrm{~J}$.
View full question & answer→MCQ 1421 Mark
A measure of the degree of disorder of a system is known as
View full question & answer→MCQ 1431 Mark
A measure of the degree of disorder of a system is known as
View full question & answer→MCQ 1441 Mark
A measure of the degree of disorder of a system is known as
View full question & answer→MCQ 1451 Mark
The process in which no heat enters or leaves the system is termed as
AnswerIn adiabatic process, no transfer of heat takes place between system and surrounding.
View full question & answer→MCQ 1461 Mark
The process in which no heat enters or leaves the system is termed as
AnswerIn adiabatic process, no transfer of heat takes place between system and surrounding.
View full question & answer→MCQ 1471 Mark
The process in which no heat enters or leaves the system is termed as
AnswerIn adiabatic process, no transfer of heat takes place between system and surrounding.
View full question & answer→MCQ 1481 Mark
During an adiabatic expansion of $2$ moles of a gas, the change in internal energy was found $-50.$ The work done during the process is
AnswerCorrect option: D. $50$ J
For adiabatic forces $\Delta W=-\Delta U \quad(\because \Delta Q=0)$
$\Rightarrow \Delta W=-(-50)=+50 \mathrm{~J}$
View full question & answer→MCQ 1491 Mark
During an adiabatic expansion of $2$ moles of a gas, the change in internal energy was found $-50.$ The work done during the process is
AnswerCorrect option: D. $50$ J
For adiabatic forces $\Delta W=-\Delta U \quad(\because \Delta Q=0)$
$\Rightarrow \Delta W=-(-50)=+50 \mathrm{~J}$
View full question & answer→MCQ 1501 Mark
During an adiabatic expansion of $2$ moles of a gas, the change in internal energy was found $-50.$ The work done during the process is
AnswerCorrect option: D. $50$ J
For adiabatic forces $\Delta W=-\Delta U \quad(\because \Delta Q=0)$
$\Rightarrow \Delta W=-(-50)=+50 \mathrm{~J}$
View full question & answer→