Ideal Gas Equation and Vander Waal equation
Kinetic Theory of Gases

138974 As ideal monatomic gas of $\mathbf{1 . 5}$ moles is heated at a constant pressure $2 \mathrm{~atm}$ so that its temperature from $30^{\circ} \mathrm{C}$ to $130^{\circ} \mathrm{C}$. Work done by the gas is-
(Universal gas constant $=8.3 \mathrm{~J} \mathrm{~mol}^{-1} \mathrm{~K}^{-1}$ )

1 $2500 \mathrm{~J}$
2 $1450 \mathrm{~J}$
3 $1245 \mathrm{~J}$
4 $555 \mathrm{~J}$
Kinetic Theory of Gases

138975 At $30{ }^{\circ} \mathrm{C}$ volume of $\mathrm{V}$ is occupied by 2 moles of an ideal monatomic gas. If the gas expands adiabatically to the volume. $4 \mathrm{~V}$. Then the final temperature of gas approximately is
$(\sqrt[3]{2}=1.26)$

1 $150 \mathrm{~K}$
2 $100 \mathrm{~K}$
3 $120 \mathrm{~K}$
4 $140 \mathrm{~K}$
Kinetic Theory of Gases

138976 A sample of an ideal gas is taken through the cyclic process $\mathrm{ABCA}$ as shown in figure. It absorbs, $40 \mathrm{~J}$ of heat during the part $\mathrm{AB}$, no heat during $B C$ and rejects $60 \mathrm{~J}$ of heat during CA. A work of $50 \mathrm{~J}$ is done on the gas during the part BC. The internal energy of the gas at $A$ is $1560 \mathrm{~J}$. The work done by the gas during the part $C A$ is:

1 $20 \mathrm{~J}$
2 $30 \mathrm{~J}$
3 $-30 \mathrm{~J}$
4 $-60 \mathrm{~J}$
Kinetic Theory of Gases

138977 A thermally insulated vessel contains an ideal gas of molecular mass $M$ and ratio of specific heats 1.4. Vessel is moving with speed $v$ and is suddenly brought to rest. Assuming no heat is lost to the surrounding and vessel temperature of the gas increases by:
$\text { ( } \mathrm{R}=\text { universal gas constant) }$

1 $\frac{M v^{2}}{7 \mathrm{R}}$
2 $\frac{M v^{2}}{5 \mathrm{R}}$
3 $2 \frac{\mathrm{Mv}^{2}}{7 \mathrm{R}}$
4 $7 \frac{\mathrm{Mv}^{2}}{5 \mathrm{R}}$
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
Kinetic Theory of Gases

138974 As ideal monatomic gas of $\mathbf{1 . 5}$ moles is heated at a constant pressure $2 \mathrm{~atm}$ so that its temperature from $30^{\circ} \mathrm{C}$ to $130^{\circ} \mathrm{C}$. Work done by the gas is-
(Universal gas constant $=8.3 \mathrm{~J} \mathrm{~mol}^{-1} \mathrm{~K}^{-1}$ )

1 $2500 \mathrm{~J}$
2 $1450 \mathrm{~J}$
3 $1245 \mathrm{~J}$
4 $555 \mathrm{~J}$
Kinetic Theory of Gases

138975 At $30{ }^{\circ} \mathrm{C}$ volume of $\mathrm{V}$ is occupied by 2 moles of an ideal monatomic gas. If the gas expands adiabatically to the volume. $4 \mathrm{~V}$. Then the final temperature of gas approximately is
$(\sqrt[3]{2}=1.26)$

1 $150 \mathrm{~K}$
2 $100 \mathrm{~K}$
3 $120 \mathrm{~K}$
4 $140 \mathrm{~K}$
Kinetic Theory of Gases

138976 A sample of an ideal gas is taken through the cyclic process $\mathrm{ABCA}$ as shown in figure. It absorbs, $40 \mathrm{~J}$ of heat during the part $\mathrm{AB}$, no heat during $B C$ and rejects $60 \mathrm{~J}$ of heat during CA. A work of $50 \mathrm{~J}$ is done on the gas during the part BC. The internal energy of the gas at $A$ is $1560 \mathrm{~J}$. The work done by the gas during the part $C A$ is:

1 $20 \mathrm{~J}$
2 $30 \mathrm{~J}$
3 $-30 \mathrm{~J}$
4 $-60 \mathrm{~J}$
Kinetic Theory of Gases

138977 A thermally insulated vessel contains an ideal gas of molecular mass $M$ and ratio of specific heats 1.4. Vessel is moving with speed $v$ and is suddenly brought to rest. Assuming no heat is lost to the surrounding and vessel temperature of the gas increases by:
$\text { ( } \mathrm{R}=\text { universal gas constant) }$

1 $\frac{M v^{2}}{7 \mathrm{R}}$
2 $\frac{M v^{2}}{5 \mathrm{R}}$
3 $2 \frac{\mathrm{Mv}^{2}}{7 \mathrm{R}}$
4 $7 \frac{\mathrm{Mv}^{2}}{5 \mathrm{R}}$
Kinetic Theory of Gases

138974 As ideal monatomic gas of $\mathbf{1 . 5}$ moles is heated at a constant pressure $2 \mathrm{~atm}$ so that its temperature from $30^{\circ} \mathrm{C}$ to $130^{\circ} \mathrm{C}$. Work done by the gas is-
(Universal gas constant $=8.3 \mathrm{~J} \mathrm{~mol}^{-1} \mathrm{~K}^{-1}$ )

1 $2500 \mathrm{~J}$
2 $1450 \mathrm{~J}$
3 $1245 \mathrm{~J}$
4 $555 \mathrm{~J}$
Kinetic Theory of Gases

138975 At $30{ }^{\circ} \mathrm{C}$ volume of $\mathrm{V}$ is occupied by 2 moles of an ideal monatomic gas. If the gas expands adiabatically to the volume. $4 \mathrm{~V}$. Then the final temperature of gas approximately is
$(\sqrt[3]{2}=1.26)$

1 $150 \mathrm{~K}$
2 $100 \mathrm{~K}$
3 $120 \mathrm{~K}$
4 $140 \mathrm{~K}$
Kinetic Theory of Gases

138976 A sample of an ideal gas is taken through the cyclic process $\mathrm{ABCA}$ as shown in figure. It absorbs, $40 \mathrm{~J}$ of heat during the part $\mathrm{AB}$, no heat during $B C$ and rejects $60 \mathrm{~J}$ of heat during CA. A work of $50 \mathrm{~J}$ is done on the gas during the part BC. The internal energy of the gas at $A$ is $1560 \mathrm{~J}$. The work done by the gas during the part $C A$ is:

1 $20 \mathrm{~J}$
2 $30 \mathrm{~J}$
3 $-30 \mathrm{~J}$
4 $-60 \mathrm{~J}$
Kinetic Theory of Gases

138977 A thermally insulated vessel contains an ideal gas of molecular mass $M$ and ratio of specific heats 1.4. Vessel is moving with speed $v$ and is suddenly brought to rest. Assuming no heat is lost to the surrounding and vessel temperature of the gas increases by:
$\text { ( } \mathrm{R}=\text { universal gas constant) }$

1 $\frac{M v^{2}}{7 \mathrm{R}}$
2 $\frac{M v^{2}}{5 \mathrm{R}}$
3 $2 \frac{\mathrm{Mv}^{2}}{7 \mathrm{R}}$
4 $7 \frac{\mathrm{Mv}^{2}}{5 \mathrm{R}}$
Kinetic Theory of Gases

138974 As ideal monatomic gas of $\mathbf{1 . 5}$ moles is heated at a constant pressure $2 \mathrm{~atm}$ so that its temperature from $30^{\circ} \mathrm{C}$ to $130^{\circ} \mathrm{C}$. Work done by the gas is-
(Universal gas constant $=8.3 \mathrm{~J} \mathrm{~mol}^{-1} \mathrm{~K}^{-1}$ )

1 $2500 \mathrm{~J}$
2 $1450 \mathrm{~J}$
3 $1245 \mathrm{~J}$
4 $555 \mathrm{~J}$
Kinetic Theory of Gases

138975 At $30{ }^{\circ} \mathrm{C}$ volume of $\mathrm{V}$ is occupied by 2 moles of an ideal monatomic gas. If the gas expands adiabatically to the volume. $4 \mathrm{~V}$. Then the final temperature of gas approximately is
$(\sqrt[3]{2}=1.26)$

1 $150 \mathrm{~K}$
2 $100 \mathrm{~K}$
3 $120 \mathrm{~K}$
4 $140 \mathrm{~K}$
Kinetic Theory of Gases

138976 A sample of an ideal gas is taken through the cyclic process $\mathrm{ABCA}$ as shown in figure. It absorbs, $40 \mathrm{~J}$ of heat during the part $\mathrm{AB}$, no heat during $B C$ and rejects $60 \mathrm{~J}$ of heat during CA. A work of $50 \mathrm{~J}$ is done on the gas during the part BC. The internal energy of the gas at $A$ is $1560 \mathrm{~J}$. The work done by the gas during the part $C A$ is:

1 $20 \mathrm{~J}$
2 $30 \mathrm{~J}$
3 $-30 \mathrm{~J}$
4 $-60 \mathrm{~J}$
Kinetic Theory of Gases

138977 A thermally insulated vessel contains an ideal gas of molecular mass $M$ and ratio of specific heats 1.4. Vessel is moving with speed $v$ and is suddenly brought to rest. Assuming no heat is lost to the surrounding and vessel temperature of the gas increases by:
$\text { ( } \mathrm{R}=\text { universal gas constant) }$

1 $\frac{M v^{2}}{7 \mathrm{R}}$
2 $\frac{M v^{2}}{5 \mathrm{R}}$
3 $2 \frac{\mathrm{Mv}^{2}}{7 \mathrm{R}}$
4 $7 \frac{\mathrm{Mv}^{2}}{5 \mathrm{R}}$