Mixing of Non-reacting gases and Mean Free Path
Kinetic Theory of Gases

139374 The number of air molecules per $\mathrm{cm}^{3}$ increased from $3 \times 10^{19}$ to $12 \times 10^{19}$. The ratio of collision frequency of air molecules before and after the increase in number respectively is

1 1.25
2 0.25
3 0.75
4 0.50
Kinetic Theory of Gases

139375 Two gases having equal temperature $T$, equal pressure $P$ and equal volume $V$ are mixed together, If temperature of the mixture is $T$ and volume is $V$, then its pressure will be

1 $\mathrm{P}$
2 $\mathrm{P} / 2$
3 $2 \mathrm{P}$
4 $4 \mathrm{P}$
Kinetic Theory of Gases

139376 If the absolute temperature of a closed volume of gas is doubled, the mean free path of the molecules will be

1 halved
2 doubled
3 unchanged
4 decreased by a factor $\sqrt{2}$
Kinetic Theory of Gases

139378 The mean free path $\lambda$ for a gas, with molecular diameter $d$ and number density $n$ can be expressed as

1 $\frac{1}{\sqrt{2} \mathrm{n} \pi \mathrm{d}^{2}}$
2 $\frac{1}{\sqrt{2} \mathrm{n}^{2} \pi \mathrm{d}^{2}}-$
3 $\frac{1}{\sqrt{2} \mathrm{n}^{2} \pi \mathrm{d}^{2}}$
4 $\frac{1}{\sqrt{2} \mathrm{n} \pi \mathrm{d}}$
Kinetic Theory of Gases

139379 When two prefect gas at absolute temperatures $T_{1}$ and $T_{2}$ are mixed, there is no loss of energy. If the masses of the molecules are $\mathrm{m}_{1}$ and $\mathrm{m}_{2}$ and the number of molecules of each gas are $n_{1}$ and $n_{2}$ respectively, then find the temperature of the mixture:

1 $\mathrm{T}_{1}+\mathrm{T}_{2}$
2 $\frac{T_{1}+T_{2}}{2}$
3 $\frac{\mathrm{n}_{1} \mathrm{~T}_{1}+\mathrm{n}_{2} \mathrm{~T}_{2}}{\mathrm{n}_{1}+\mathrm{n}_{2}}$
4 $\frac{\mathrm{n}_{1} \mathrm{~T}_{1}-\mathrm{n}_{2} \mathrm{~T}_{2}}{\mathrm{n}_{1}+\mathrm{n}_{2}}$
Kinetic Theory of Gases

139374 The number of air molecules per $\mathrm{cm}^{3}$ increased from $3 \times 10^{19}$ to $12 \times 10^{19}$. The ratio of collision frequency of air molecules before and after the increase in number respectively is

1 1.25
2 0.25
3 0.75
4 0.50
Kinetic Theory of Gases

139375 Two gases having equal temperature $T$, equal pressure $P$ and equal volume $V$ are mixed together, If temperature of the mixture is $T$ and volume is $V$, then its pressure will be

1 $\mathrm{P}$
2 $\mathrm{P} / 2$
3 $2 \mathrm{P}$
4 $4 \mathrm{P}$
Kinetic Theory of Gases

139376 If the absolute temperature of a closed volume of gas is doubled, the mean free path of the molecules will be

1 halved
2 doubled
3 unchanged
4 decreased by a factor $\sqrt{2}$
Kinetic Theory of Gases

139378 The mean free path $\lambda$ for a gas, with molecular diameter $d$ and number density $n$ can be expressed as

1 $\frac{1}{\sqrt{2} \mathrm{n} \pi \mathrm{d}^{2}}$
2 $\frac{1}{\sqrt{2} \mathrm{n}^{2} \pi \mathrm{d}^{2}}-$
3 $\frac{1}{\sqrt{2} \mathrm{n}^{2} \pi \mathrm{d}^{2}}$
4 $\frac{1}{\sqrt{2} \mathrm{n} \pi \mathrm{d}}$
Kinetic Theory of Gases

139379 When two prefect gas at absolute temperatures $T_{1}$ and $T_{2}$ are mixed, there is no loss of energy. If the masses of the molecules are $\mathrm{m}_{1}$ and $\mathrm{m}_{2}$ and the number of molecules of each gas are $n_{1}$ and $n_{2}$ respectively, then find the temperature of the mixture:

1 $\mathrm{T}_{1}+\mathrm{T}_{2}$
2 $\frac{T_{1}+T_{2}}{2}$
3 $\frac{\mathrm{n}_{1} \mathrm{~T}_{1}+\mathrm{n}_{2} \mathrm{~T}_{2}}{\mathrm{n}_{1}+\mathrm{n}_{2}}$
4 $\frac{\mathrm{n}_{1} \mathrm{~T}_{1}-\mathrm{n}_{2} \mathrm{~T}_{2}}{\mathrm{n}_{1}+\mathrm{n}_{2}}$
Kinetic Theory of Gases

139374 The number of air molecules per $\mathrm{cm}^{3}$ increased from $3 \times 10^{19}$ to $12 \times 10^{19}$. The ratio of collision frequency of air molecules before and after the increase in number respectively is

1 1.25
2 0.25
3 0.75
4 0.50
Kinetic Theory of Gases

139375 Two gases having equal temperature $T$, equal pressure $P$ and equal volume $V$ are mixed together, If temperature of the mixture is $T$ and volume is $V$, then its pressure will be

1 $\mathrm{P}$
2 $\mathrm{P} / 2$
3 $2 \mathrm{P}$
4 $4 \mathrm{P}$
Kinetic Theory of Gases

139376 If the absolute temperature of a closed volume of gas is doubled, the mean free path of the molecules will be

1 halved
2 doubled
3 unchanged
4 decreased by a factor $\sqrt{2}$
Kinetic Theory of Gases

139378 The mean free path $\lambda$ for a gas, with molecular diameter $d$ and number density $n$ can be expressed as

1 $\frac{1}{\sqrt{2} \mathrm{n} \pi \mathrm{d}^{2}}$
2 $\frac{1}{\sqrt{2} \mathrm{n}^{2} \pi \mathrm{d}^{2}}-$
3 $\frac{1}{\sqrt{2} \mathrm{n}^{2} \pi \mathrm{d}^{2}}$
4 $\frac{1}{\sqrt{2} \mathrm{n} \pi \mathrm{d}}$
Kinetic Theory of Gases

139379 When two prefect gas at absolute temperatures $T_{1}$ and $T_{2}$ are mixed, there is no loss of energy. If the masses of the molecules are $\mathrm{m}_{1}$ and $\mathrm{m}_{2}$ and the number of molecules of each gas are $n_{1}$ and $n_{2}$ respectively, then find the temperature of the mixture:

1 $\mathrm{T}_{1}+\mathrm{T}_{2}$
2 $\frac{T_{1}+T_{2}}{2}$
3 $\frac{\mathrm{n}_{1} \mathrm{~T}_{1}+\mathrm{n}_{2} \mathrm{~T}_{2}}{\mathrm{n}_{1}+\mathrm{n}_{2}}$
4 $\frac{\mathrm{n}_{1} \mathrm{~T}_{1}-\mathrm{n}_{2} \mathrm{~T}_{2}}{\mathrm{n}_{1}+\mathrm{n}_{2}}$
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
Kinetic Theory of Gases

139374 The number of air molecules per $\mathrm{cm}^{3}$ increased from $3 \times 10^{19}$ to $12 \times 10^{19}$. The ratio of collision frequency of air molecules before and after the increase in number respectively is

1 1.25
2 0.25
3 0.75
4 0.50
Kinetic Theory of Gases

139375 Two gases having equal temperature $T$, equal pressure $P$ and equal volume $V$ are mixed together, If temperature of the mixture is $T$ and volume is $V$, then its pressure will be

1 $\mathrm{P}$
2 $\mathrm{P} / 2$
3 $2 \mathrm{P}$
4 $4 \mathrm{P}$
Kinetic Theory of Gases

139376 If the absolute temperature of a closed volume of gas is doubled, the mean free path of the molecules will be

1 halved
2 doubled
3 unchanged
4 decreased by a factor $\sqrt{2}$
Kinetic Theory of Gases

139378 The mean free path $\lambda$ for a gas, with molecular diameter $d$ and number density $n$ can be expressed as

1 $\frac{1}{\sqrt{2} \mathrm{n} \pi \mathrm{d}^{2}}$
2 $\frac{1}{\sqrt{2} \mathrm{n}^{2} \pi \mathrm{d}^{2}}-$
3 $\frac{1}{\sqrt{2} \mathrm{n}^{2} \pi \mathrm{d}^{2}}$
4 $\frac{1}{\sqrt{2} \mathrm{n} \pi \mathrm{d}}$
Kinetic Theory of Gases

139379 When two prefect gas at absolute temperatures $T_{1}$ and $T_{2}$ are mixed, there is no loss of energy. If the masses of the molecules are $\mathrm{m}_{1}$ and $\mathrm{m}_{2}$ and the number of molecules of each gas are $n_{1}$ and $n_{2}$ respectively, then find the temperature of the mixture:

1 $\mathrm{T}_{1}+\mathrm{T}_{2}$
2 $\frac{T_{1}+T_{2}}{2}$
3 $\frac{\mathrm{n}_{1} \mathrm{~T}_{1}+\mathrm{n}_{2} \mathrm{~T}_{2}}{\mathrm{n}_{1}+\mathrm{n}_{2}}$
4 $\frac{\mathrm{n}_{1} \mathrm{~T}_{1}-\mathrm{n}_{2} \mathrm{~T}_{2}}{\mathrm{n}_{1}+\mathrm{n}_{2}}$
Kinetic Theory of Gases

139374 The number of air molecules per $\mathrm{cm}^{3}$ increased from $3 \times 10^{19}$ to $12 \times 10^{19}$. The ratio of collision frequency of air molecules before and after the increase in number respectively is

1 1.25
2 0.25
3 0.75
4 0.50
Kinetic Theory of Gases

139375 Two gases having equal temperature $T$, equal pressure $P$ and equal volume $V$ are mixed together, If temperature of the mixture is $T$ and volume is $V$, then its pressure will be

1 $\mathrm{P}$
2 $\mathrm{P} / 2$
3 $2 \mathrm{P}$
4 $4 \mathrm{P}$
Kinetic Theory of Gases

139376 If the absolute temperature of a closed volume of gas is doubled, the mean free path of the molecules will be

1 halved
2 doubled
3 unchanged
4 decreased by a factor $\sqrt{2}$
Kinetic Theory of Gases

139378 The mean free path $\lambda$ for a gas, with molecular diameter $d$ and number density $n$ can be expressed as

1 $\frac{1}{\sqrt{2} \mathrm{n} \pi \mathrm{d}^{2}}$
2 $\frac{1}{\sqrt{2} \mathrm{n}^{2} \pi \mathrm{d}^{2}}-$
3 $\frac{1}{\sqrt{2} \mathrm{n}^{2} \pi \mathrm{d}^{2}}$
4 $\frac{1}{\sqrt{2} \mathrm{n} \pi \mathrm{d}}$
Kinetic Theory of Gases

139379 When two prefect gas at absolute temperatures $T_{1}$ and $T_{2}$ are mixed, there is no loss of energy. If the masses of the molecules are $\mathrm{m}_{1}$ and $\mathrm{m}_{2}$ and the number of molecules of each gas are $n_{1}$ and $n_{2}$ respectively, then find the temperature of the mixture:

1 $\mathrm{T}_{1}+\mathrm{T}_{2}$
2 $\frac{T_{1}+T_{2}}{2}$
3 $\frac{\mathrm{n}_{1} \mathrm{~T}_{1}+\mathrm{n}_{2} \mathrm{~T}_{2}}{\mathrm{n}_{1}+\mathrm{n}_{2}}$
4 $\frac{\mathrm{n}_{1} \mathrm{~T}_{1}-\mathrm{n}_{2} \mathrm{~T}_{2}}{\mathrm{n}_{1}+\mathrm{n}_{2}}$