Law of Gases (Boyle's Law, Charles's Law, Gay-Lussac's Law, Avogadro's Law)
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
Kinetic Theory of Gases

138956 A $10 \mathrm{~kW}$ drilling machine is used to drill a bore in an aluminium block of mass $25 \mathrm{~kg}$. If the machine is on for 3 minutes and $50 \%$ of the heat liberated is taken up by the block, then the raise in temperature of the block is ${ }^{1} \mathbf{K}^{-1}$ ) (specific heat of aluminium is $900 \mathrm{~J} \mathrm{~kg}^{-}$

1 $20^{\circ} \mathrm{C}$
2 $40^{\circ} \mathrm{C}$
3 $85^{\circ} \mathrm{C}$
4 $150^{\circ} \mathrm{C}$
Kinetic Theory of Gases

138957 One mole of an ideal gas $(\gamma=1.4)$ is adiabatically compressed so that its temperature rises from $27^{0} \mathrm{C}$ to $35^{\circ} \mathrm{C}$. The change in the internal energy of the gas is $(R=$ $8.3 \mathrm{Jmol}^{-1} \mathrm{~K}^{-1}$ )

1 $-266 \mathrm{~J}$
2 $166 \mathrm{~J}$
3 $-268 \mathrm{~J}$
4 $168 \mathrm{~J}$
Kinetic Theory of Gases

138958 A gas under constant pressure of $4.5 \times 10^{5} \mathrm{~Pa}$ when subjected to $800 \mathrm{~kJ}$ of heat, changes the volume from $0.5 \mathrm{~m}^{3}$ to $2.0 \mathrm{~m}^{3}$. The change in internal energy of the gas is

1 $6.75 \times 10^{5} \mathrm{~J}$
2 $5.25 \times 10^{5} \mathrm{~J}$
3 $3.25 \times 10^{5} \mathrm{~J}$
4 $1.25 \times 10^{5} \mathrm{~J}$
Kinetic Theory of Gases

138959 A monatomic gas $\left(\gamma=\frac{5}{3}\right)$ at a pressure of $4 \mathrm{~atm}$ is compressed adiabatically so that its temperature rises from $27^{\circ} \mathrm{C}$ to $327^{\circ} \mathrm{C}$. The pressure of the gas in its final state is-

1 $2^{\frac{5}{3}} \mathrm{~atm}$
2 $2^{\frac{10}{3}} \mathrm{~atm}$
3 $2^{\frac{5}{3}} \mathrm{~atm}$
4 $2^{\frac{9}{2}} \mathrm{~atm}$
Kinetic Theory of Gases

138956 A $10 \mathrm{~kW}$ drilling machine is used to drill a bore in an aluminium block of mass $25 \mathrm{~kg}$. If the machine is on for 3 minutes and $50 \%$ of the heat liberated is taken up by the block, then the raise in temperature of the block is ${ }^{1} \mathbf{K}^{-1}$ ) (specific heat of aluminium is $900 \mathrm{~J} \mathrm{~kg}^{-}$

1 $20^{\circ} \mathrm{C}$
2 $40^{\circ} \mathrm{C}$
3 $85^{\circ} \mathrm{C}$
4 $150^{\circ} \mathrm{C}$
Kinetic Theory of Gases

138957 One mole of an ideal gas $(\gamma=1.4)$ is adiabatically compressed so that its temperature rises from $27^{0} \mathrm{C}$ to $35^{\circ} \mathrm{C}$. The change in the internal energy of the gas is $(R=$ $8.3 \mathrm{Jmol}^{-1} \mathrm{~K}^{-1}$ )

1 $-266 \mathrm{~J}$
2 $166 \mathrm{~J}$
3 $-268 \mathrm{~J}$
4 $168 \mathrm{~J}$
Kinetic Theory of Gases

138958 A gas under constant pressure of $4.5 \times 10^{5} \mathrm{~Pa}$ when subjected to $800 \mathrm{~kJ}$ of heat, changes the volume from $0.5 \mathrm{~m}^{3}$ to $2.0 \mathrm{~m}^{3}$. The change in internal energy of the gas is

1 $6.75 \times 10^{5} \mathrm{~J}$
2 $5.25 \times 10^{5} \mathrm{~J}$
3 $3.25 \times 10^{5} \mathrm{~J}$
4 $1.25 \times 10^{5} \mathrm{~J}$
Kinetic Theory of Gases

138959 A monatomic gas $\left(\gamma=\frac{5}{3}\right)$ at a pressure of $4 \mathrm{~atm}$ is compressed adiabatically so that its temperature rises from $27^{\circ} \mathrm{C}$ to $327^{\circ} \mathrm{C}$. The pressure of the gas in its final state is-

1 $2^{\frac{5}{3}} \mathrm{~atm}$
2 $2^{\frac{10}{3}} \mathrm{~atm}$
3 $2^{\frac{5}{3}} \mathrm{~atm}$
4 $2^{\frac{9}{2}} \mathrm{~atm}$
Kinetic Theory of Gases

138956 A $10 \mathrm{~kW}$ drilling machine is used to drill a bore in an aluminium block of mass $25 \mathrm{~kg}$. If the machine is on for 3 minutes and $50 \%$ of the heat liberated is taken up by the block, then the raise in temperature of the block is ${ }^{1} \mathbf{K}^{-1}$ ) (specific heat of aluminium is $900 \mathrm{~J} \mathrm{~kg}^{-}$

1 $20^{\circ} \mathrm{C}$
2 $40^{\circ} \mathrm{C}$
3 $85^{\circ} \mathrm{C}$
4 $150^{\circ} \mathrm{C}$
Kinetic Theory of Gases

138957 One mole of an ideal gas $(\gamma=1.4)$ is adiabatically compressed so that its temperature rises from $27^{0} \mathrm{C}$ to $35^{\circ} \mathrm{C}$. The change in the internal energy of the gas is $(R=$ $8.3 \mathrm{Jmol}^{-1} \mathrm{~K}^{-1}$ )

1 $-266 \mathrm{~J}$
2 $166 \mathrm{~J}$
3 $-268 \mathrm{~J}$
4 $168 \mathrm{~J}$
Kinetic Theory of Gases

138958 A gas under constant pressure of $4.5 \times 10^{5} \mathrm{~Pa}$ when subjected to $800 \mathrm{~kJ}$ of heat, changes the volume from $0.5 \mathrm{~m}^{3}$ to $2.0 \mathrm{~m}^{3}$. The change in internal energy of the gas is

1 $6.75 \times 10^{5} \mathrm{~J}$
2 $5.25 \times 10^{5} \mathrm{~J}$
3 $3.25 \times 10^{5} \mathrm{~J}$
4 $1.25 \times 10^{5} \mathrm{~J}$
Kinetic Theory of Gases

138959 A monatomic gas $\left(\gamma=\frac{5}{3}\right)$ at a pressure of $4 \mathrm{~atm}$ is compressed adiabatically so that its temperature rises from $27^{\circ} \mathrm{C}$ to $327^{\circ} \mathrm{C}$. The pressure of the gas in its final state is-

1 $2^{\frac{5}{3}} \mathrm{~atm}$
2 $2^{\frac{10}{3}} \mathrm{~atm}$
3 $2^{\frac{5}{3}} \mathrm{~atm}$
4 $2^{\frac{9}{2}} \mathrm{~atm}$
Kinetic Theory of Gases

138956 A $10 \mathrm{~kW}$ drilling machine is used to drill a bore in an aluminium block of mass $25 \mathrm{~kg}$. If the machine is on for 3 minutes and $50 \%$ of the heat liberated is taken up by the block, then the raise in temperature of the block is ${ }^{1} \mathbf{K}^{-1}$ ) (specific heat of aluminium is $900 \mathrm{~J} \mathrm{~kg}^{-}$

1 $20^{\circ} \mathrm{C}$
2 $40^{\circ} \mathrm{C}$
3 $85^{\circ} \mathrm{C}$
4 $150^{\circ} \mathrm{C}$
Kinetic Theory of Gases

138957 One mole of an ideal gas $(\gamma=1.4)$ is adiabatically compressed so that its temperature rises from $27^{0} \mathrm{C}$ to $35^{\circ} \mathrm{C}$. The change in the internal energy of the gas is $(R=$ $8.3 \mathrm{Jmol}^{-1} \mathrm{~K}^{-1}$ )

1 $-266 \mathrm{~J}$
2 $166 \mathrm{~J}$
3 $-268 \mathrm{~J}$
4 $168 \mathrm{~J}$
Kinetic Theory of Gases

138958 A gas under constant pressure of $4.5 \times 10^{5} \mathrm{~Pa}$ when subjected to $800 \mathrm{~kJ}$ of heat, changes the volume from $0.5 \mathrm{~m}^{3}$ to $2.0 \mathrm{~m}^{3}$. The change in internal energy of the gas is

1 $6.75 \times 10^{5} \mathrm{~J}$
2 $5.25 \times 10^{5} \mathrm{~J}$
3 $3.25 \times 10^{5} \mathrm{~J}$
4 $1.25 \times 10^{5} \mathrm{~J}$
Kinetic Theory of Gases

138959 A monatomic gas $\left(\gamma=\frac{5}{3}\right)$ at a pressure of $4 \mathrm{~atm}$ is compressed adiabatically so that its temperature rises from $27^{\circ} \mathrm{C}$ to $327^{\circ} \mathrm{C}$. The pressure of the gas in its final state is-

1 $2^{\frac{5}{3}} \mathrm{~atm}$
2 $2^{\frac{10}{3}} \mathrm{~atm}$
3 $2^{\frac{5}{3}} \mathrm{~atm}$
4 $2^{\frac{9}{2}} \mathrm{~atm}$