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IB Physics SL B 3 Gas Laws Questions

Practise IB Physics SL B.3 by modelling pressure, volume, amount and absolute temperature with ideal-gas equations and molecular explanations.

Syllabus
First assessment 2025
Course
Physics SL
Level
SL

Exam points

  • Apply P=F/A to find pressure or normal force on doors, cylinder walls and stoppers.
  • Convert gas mass to moles or atoms with molar mass and N=nN_A, including isotope data.
  • Use pV/T=constant to compare gas states and interpret pressure–volume or temperature graphs.
  • Apply PV=nRT or PV=NkBT to calculate gas states, amount or particle number from data.
  • Explain pressure through molecular collisions and momentum transfer at walls; use P=⅓ρv².
  • Calculate monatomic-gas internal energy with U=3/2NkBT=3/2nRT and link it to total kinetic energy.
  • Judge ideal-gas validity from pressure, temperature and density at low pressure, high temperature or small volumes.

Question 1

[Maximum number: 9]

A solid cylinder of height h and density ρ\rho rests on a flat surface.

Figure for Question 1 — IB Physics SL

Question (a)

(a)

Show that the pressure pCp_{\mathrm{C}} exerted by the cylinder on the surface is given by pC=ρghp_{\mathrm{C}}=\rho g h.

[ 2 ]

Question (b)

(b)

A tube of constant circular cross-section, sealed at one end, contains an ideal gas trapped by a cylinder of mercury of length 0.035 m . The whole arrangement is in the Earth's atmosphere. The density of mercury is 1.36×104 kg m−31.36 \times 10^{4} \mathrm{~kg} \mathrm{~m}^{-3}.

Figure for Question (b) — IB Physics SL

When the mercury is above the gas column the length of the gas column is 0.190 m .

[ 7 ]

Question (i)

(i)

Show that (po+pm)×0.190=nRTA\left(p_{\mathrm{o}}+p_{\mathrm{m}}\right) \times 0.190=\frac{n R T}{A} where
po=p_{\mathrm{o}}= atmospheric pressure
pm=p_{\mathrm{m}}= pressure due to the mercury column
T= temperature of the trapped gas
n= number of moles of the trapped gas
A= cross-sectional area of the tube.

[ 2 ]

Question (ii)

(ii)

The tube is slowly rotated until the gas column is above the mercury.

Figure for Question (ii) — IB Physics SL

The length of the gas column is now 0.208 m . The temperature of the trapped gas does not change during the process.

Determine the atmospheric pressure. Give a suitable unit for your answer.

[ 4 ]

Question (iii)

(iii)

Outline why the gas particles in the tube hit the mercury surface less often after the tube has been rotated.

[ 1 ]

Question 2

[Maximum number: 6]

This question is in two parts. Part 1 is about ideal gases and specific heat capacity. Part 2 is about simple harmonic motion and waves.
Part 1 Ideal gases and specific heat capacity

Question (a)

(a)

State two assumptions of the kinetic model of an ideal gas.

[ 2 ]

Question (b)

(b)

Argon behaves as an ideal gas for a large range of temperatures and pressures. One mole of argon is confined in a cylinder by a freely moving piston.

[ 1 ]

Question (i)

(i)

Define what is meant by the term one mole of argon.

[ 1 ]

Question (c)

(c)

At the temperature of 350 K , the piston in (b) is now freed and the argon expands until its temperature reaches 300 K .
Explain, in terms of the molecular model of an ideal gas, why the temperature of argon decreases on expansion.

[ 3 ]

Question 3

[Maximum number: 6]

The equipment shown in the diagram was used by a student to investigate the variation with volume, of the pressure p of air, at constant temperature. The air was trapped in a tube of constant cross-sectional area above a column of oil.

Figure for Question 3 — IB Physics SL

The pump forces oil to move up the tube decreasing the volume of the trapped air.

Question (a)

(a)

Outline how the results of this experiment are consistent with the ideal gas law at constant temperature.

[ 2 ]

Question (b)

(b)

The cross-sectional area of the tube is 1.3×10−3 m21.3 \times 10^{-3} \mathrm{~m}^{2} and the temperature of air is 300 K . Estimate the number of moles of air in the tube.

[ 2 ]

Question (c)

(c)

The equation of the line of best fit is:

p=a+bHp=a+\frac{b}{H}

The equation above may be used to predict the pressure of the air at extremely large values of 1H\frac{1}{H}. Suggest why this will be an unreliable estimate of the pressure.

[ 2 ]

Question 4

[Maximum number: 2]

A solid cylinder of height h and density ρ\rho rests on a flat surface.

Figure for Question 4 — IB Physics SL

Show that the pressure pCp_{\mathrm{C}} exerted by the cylinder on the surface is given by pC=ρghp_{\mathrm{C}}=\rho g h.

Question 5

[Maximum number: 1]

This question is in two parts. Part 1 is about ideal gases and specific heat capacity. Part 2 is about simple harmonic motion and waves.
Part 1 Ideal gases and specific heat capacity

Argon behaves as an ideal gas for a large range of temperatures and pressures. One mole of argon is confined in a cylinder by a freely moving piston.

Define what is meant by the term one mole of argon.

Question 6

[Maximum number: 2]

This question is in two parts. Part 1 is about ideal gases and specific heat capacity. Part 2 is about simple harmonic motion and waves.
Part 1 Ideal gases and specific heat capacity

State two assumptions of the kinetic model of an ideal gas.

Question 7

[Maximum number: 2]

The equipment shown in the diagram was used by a student to investigate the variation with volume, of the pressure p of air, at constant temperature. The air was trapped in a tube of constant cross-sectional area above a column of oil.

Figure for Question 7 — IB Physics SL

The pump forces oil to move up the tube decreasing the volume of the trapped air.

Outline how the results of this experiment are consistent with the ideal gas law at constant temperature.

Question 8

[Maximum number: 2]

The equipment shown in the diagram was used by a student to investigate the variation with volume, of the pressure p of air, at constant temperature. The air was trapped in a tube of constant cross-sectional area above a column of oil.

Figure for Question 8 — IB Physics SL

The pump forces oil to move up the tube decreasing the volume of the trapped air.

The cross-sectional area of the tube is 1.3×10−3 m21.3 \times 10^{-3} \mathrm{~m}^{2} and the temperature of air is 300 K . Estimate the number of moles of air in the tube.

Question 9

[Maximum number: 1]

A solid cylinder of height h and density ρ\rho rests on a flat surface.

Figure for Question 9 — IB Physics SL

A tube of constant circular cross-section, sealed at one end, contains an ideal gas trapped by a cylinder of mercury of length 0.035 m . The whole arrangement is in the Earth's atmosphere. The density of mercury is 1.36×104 kg m−31.36 \times 10^{4} \mathrm{~kg} \mathrm{~m}^{-3}.

Figure for Question 9 — IB Physics SL

When the mercury is above the gas column the length of the gas column is 0.190 m .

Outline why the gas particles in the tube hit the mercury surface less often after the tube has been rotated.

Question 10

[Maximum number: 3]

This question is in two parts. Part 1 is about ideal gases and specific heat capacity. Part 2 is about simple harmonic motion and waves.
Part 1 Ideal gases and specific heat capacity

At the temperature of 350 K , the piston in (b) is now freed and the argon expands until its temperature reaches 300 K .
Explain, in terms of the molecular model of an ideal gas, why the temperature of argon decreases on expansion.

Question 11

[Maximum number: 2]

The equipment shown in the diagram was used by a student to investigate the variation with volume, of the pressure p of air, at constant temperature. The air was trapped in a tube of constant cross-sectional area above a column of oil.

Figure for Question 11 — IB Physics SL

The pump forces oil to move up the tube decreasing the volume of the trapped air.

The equation of the line of best fit is:

p=a+bHp=a+\frac{b}{H}

The equation above may be used to predict the pressure of the air at extremely large values of 1H\frac{1}{H}. Suggest why this will be an unreliable estimate of the pressure.

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