Kinetic Theory of an Ideal Gas
PHXI13:KINETIC THEORY

360217 Pressure of ideal gas at constant volume is proportional to

1 total energy of the gas
2 average kinetic energy of the molecules
3 force between the molecules
4 average potential energy of the molecules
PHXI13:KINETIC THEORY

360218 In an ideal gas at temperature \(T\), the average force that a molecule applies on the walls of a closed container depends on\(T\) as \({T^q}\). A good estimate for \(q\) is:

1 \(\dfrac{1}{2}\)
2 2
3 1
4 \(\dfrac{1}{4}\)
PHXI13:KINETIC THEORY

360219 Relationship between \(P, V\) and \(E\) for a gas is ( \(E\) is the kinetic energy of the gas)

1 \(P V=\dfrac{3}{2} E\)
2 \(V=\dfrac{2}{3} E P\)
3 \(P=\dfrac{3}{2} E V\)
4 \(P V=\dfrac{2}{3} E\)
PHXI13:KINETIC THEORY

360220 In outer space there are 10 molecules per \(c{m^3}\) on the average and the temperature there is \(3 K\). The average pressure of this light gas is

1 \({10^5}N{m^{ - 2}}\)
2 \(5 \times {10^{ - 14}}N{m^{ - 2}}\)
3 \(0.4 \times {10^{ - 16}}N{m^{ - 2}}\)
4 \(4.14 \times {10^{ - 16}}N{m^{ - 2}}\)
PHXI13:KINETIC THEORY

360217 Pressure of ideal gas at constant volume is proportional to

1 total energy of the gas
2 average kinetic energy of the molecules
3 force between the molecules
4 average potential energy of the molecules
PHXI13:KINETIC THEORY

360218 In an ideal gas at temperature \(T\), the average force that a molecule applies on the walls of a closed container depends on\(T\) as \({T^q}\). A good estimate for \(q\) is:

1 \(\dfrac{1}{2}\)
2 2
3 1
4 \(\dfrac{1}{4}\)
PHXI13:KINETIC THEORY

360219 Relationship between \(P, V\) and \(E\) for a gas is ( \(E\) is the kinetic energy of the gas)

1 \(P V=\dfrac{3}{2} E\)
2 \(V=\dfrac{2}{3} E P\)
3 \(P=\dfrac{3}{2} E V\)
4 \(P V=\dfrac{2}{3} E\)
PHXI13:KINETIC THEORY

360220 In outer space there are 10 molecules per \(c{m^3}\) on the average and the temperature there is \(3 K\). The average pressure of this light gas is

1 \({10^5}N{m^{ - 2}}\)
2 \(5 \times {10^{ - 14}}N{m^{ - 2}}\)
3 \(0.4 \times {10^{ - 16}}N{m^{ - 2}}\)
4 \(4.14 \times {10^{ - 16}}N{m^{ - 2}}\)
PHXI13:KINETIC THEORY

360217 Pressure of ideal gas at constant volume is proportional to

1 total energy of the gas
2 average kinetic energy of the molecules
3 force between the molecules
4 average potential energy of the molecules
PHXI13:KINETIC THEORY

360218 In an ideal gas at temperature \(T\), the average force that a molecule applies on the walls of a closed container depends on\(T\) as \({T^q}\). A good estimate for \(q\) is:

1 \(\dfrac{1}{2}\)
2 2
3 1
4 \(\dfrac{1}{4}\)
PHXI13:KINETIC THEORY

360219 Relationship between \(P, V\) and \(E\) for a gas is ( \(E\) is the kinetic energy of the gas)

1 \(P V=\dfrac{3}{2} E\)
2 \(V=\dfrac{2}{3} E P\)
3 \(P=\dfrac{3}{2} E V\)
4 \(P V=\dfrac{2}{3} E\)
PHXI13:KINETIC THEORY

360220 In outer space there are 10 molecules per \(c{m^3}\) on the average and the temperature there is \(3 K\). The average pressure of this light gas is

1 \({10^5}N{m^{ - 2}}\)
2 \(5 \times {10^{ - 14}}N{m^{ - 2}}\)
3 \(0.4 \times {10^{ - 16}}N{m^{ - 2}}\)
4 \(4.14 \times {10^{ - 16}}N{m^{ - 2}}\)
PHXI13:KINETIC THEORY

360217 Pressure of ideal gas at constant volume is proportional to

1 total energy of the gas
2 average kinetic energy of the molecules
3 force between the molecules
4 average potential energy of the molecules
PHXI13:KINETIC THEORY

360218 In an ideal gas at temperature \(T\), the average force that a molecule applies on the walls of a closed container depends on\(T\) as \({T^q}\). A good estimate for \(q\) is:

1 \(\dfrac{1}{2}\)
2 2
3 1
4 \(\dfrac{1}{4}\)
PHXI13:KINETIC THEORY

360219 Relationship between \(P, V\) and \(E\) for a gas is ( \(E\) is the kinetic energy of the gas)

1 \(P V=\dfrac{3}{2} E\)
2 \(V=\dfrac{2}{3} E P\)
3 \(P=\dfrac{3}{2} E V\)
4 \(P V=\dfrac{2}{3} E\)
PHXI13:KINETIC THEORY

360220 In outer space there are 10 molecules per \(c{m^3}\) on the average and the temperature there is \(3 K\). The average pressure of this light gas is

1 \({10^5}N{m^{ - 2}}\)
2 \(5 \times {10^{ - 14}}N{m^{ - 2}}\)
3 \(0.4 \times {10^{ - 16}}N{m^{ - 2}}\)
4 \(4.14 \times {10^{ - 16}}N{m^{ - 2}}\)