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How is heat transferred and how do ideal gases behave?

Internal energy and temperature, specific heat capacity and specific latent heat, the ideal gas laws and equation of state, and the kinetic theory of gases.

A focused answer to the Edexcel 9PH0 thermal physics content, covering internal energy and temperature, specific heat capacity and latent heat, the ideal gas laws and equation of state, and the kinetic theory of gases.

Generated by Claude Opus 4.812 min answer

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What this dot point is asking

Edexcel wants you to relate internal energy to temperature, use specific heat capacity and specific latent heat, apply the ideal gas laws and the equation of state pV=nRTpV = nRT, and explain gas behaviour using the kinetic theory.

The answer

Internal energy and temperature

Raising the temperature increases the average kinetic energy of the particles. Converting between Celsius and kelvin uses T(K)=θ(deg C)+273T(\text{K}) = \theta(\text{deg C}) + 273. During a change of state the temperature (and so average kinetic energy) stays constant while the potential energy of the particles changes.

Specific heat capacity and latent heat

Specific heat capacity is the energy to raise 11 kg by 11 K. Latent heat is the energy to change the state of 11 kg with no temperature change; this energy goes into separating the particles (breaking bonds) rather than speeding them up, which is why a heating curve has flat sections at the melting and boiling points.

The ideal gas laws

Temperatures in these laws must be in kelvin. An ideal gas is one that obeys pV=nRTpV = nRT exactly; real gases approach this at low pressure and high temperature.

Kinetic theory

The kinetic theory models a gas as many tiny particles in random motion, colliding elastically with the walls and each other. Deriving the pressure from the rate of change of molecular momentum at the walls gives:

This shows directly that absolute temperature is proportional to the mean kinetic energy of the molecules, the microscopic meaning of temperature. The assumptions (point particles, no intermolecular forces except in collisions, elastic collisions, random motion) define the ideal gas.

Examples in context

Water's high specific heat capacity makes it an excellent coolant and moderates coastal climates. Latent heat of vaporisation explains why sweating cools the body and why steam burns are worse than boiling-water burns. The gas laws govern engines, weather balloons, and the pressure changes in scuba diving. Kinetic theory underpins the design of pressure vessels and explains why gases exert more pressure when heated, the principle behind the internal combustion engine.

Try this

Q1. State what absolute temperature measures at the molecular level. [1 mark]

  • Cue. The average random kinetic energy per particle.

Q2. Find the energy to heat 2.02.0 kg of water by 3030 K. Take c=4200c = 4200 J per kg per K. [2 marks]

  • Cue. Q=mcΔθ=2.0×4200×30=2.5×105Q = mc\Delta\theta = 2.0 \times 4200 \times 30 = 2.5 \times 10^{5} J.

Q3. A gas at 1.0×1051.0 \times 10^{5} Pa and 2.0×1032.0 \times 10^{-3} cubic metres is compressed at constant temperature to 0.50×1030.50 \times 10^{-3} cubic metres. Find the new pressure. [2 marks]

  • Cue. Boyle's law: p2=p1V1V2=1.0×105×2.0×1030.50×103=4.0×105p_2 = \frac{p_1 V_1}{V_2} = \frac{1.0 \times 10^{5} \times 2.0 \times 10^{-3}}{0.50 \times 10^{-3}} = 4.0 \times 10^{5} Pa.

Exam-style practice questions

Practice questions written in the style of Pearson Edexcel exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

Edexcel 20184 marksCalculate the energy needed to raise the temperature of 0.500.50 kg of water from 2020 degrees C to 100100 degrees C, then boil 0.100.10 kg of it. Specific heat capacity of water =4200= 4200 J per kg per K; specific latent heat of vaporisation =2.3×106= 2.3 \times 10^{6} J per kg.
Show worked answer →

Heating: Q1=mcΔθ=0.50×4200×(10020)=0.50×4200×80=1.68×105Q_1 = mc\Delta\theta = 0.50 \times 4200 \times (100 - 20) = 0.50 \times 4200 \times 80 = 1.68 \times 10^{5} J.

Boiling 0.100.10 kg: Q2=mL=0.10×2.3×106=2.3×105Q_2 = mL = 0.10 \times 2.3 \times 10^{6} = 2.3 \times 10^{5} J.

Total: Q=1.68×105+2.3×105=4.0×105Q = 1.68 \times 10^{5} + 2.3 \times 10^{5} = 4.0 \times 10^{5} J.

Markers reward Q=mcΔθQ = mc\Delta\theta for the heating, Q=mLQ = mL for the boiling, and the total about 4.0×1054.0 \times 10^{5} J.

Edexcel 20215 marksA fixed mass of ideal gas has volume 2.0×1032.0 \times 10^{-3} cubic metres at a pressure of 1.0×1051.0 \times 10^{5} Pa and temperature 300300 K. Determine the number of moles, then find the new pressure if the gas is heated to 450450 K at constant volume. Take R=8.31R = 8.31 J per mol per K.
Show worked answer →

Number of moles from pV=nRTpV = nRT: n=pVRT=1.0×105×2.0×1038.31×300=2002493=0.080n = \frac{pV}{RT} = \frac{1.0 \times 10^{5} \times 2.0 \times 10^{-3}}{8.31 \times 300} = \frac{200}{2493} = 0.080 mol.

Constant volume: p1T1=p2T2\frac{p_1}{T_1} = \frac{p_2}{T_2}, so p2=p1×T2T1=1.0×105×450300=1.5×105p_2 = p_1 \times \frac{T_2}{T_1} = 1.0 \times 10^{5} \times \frac{450}{300} = 1.5 \times 10^{5} Pa.

Markers reward n=pVRT=0.080n = \frac{pV}{RT} = 0.080 mol, the pressure law at constant volume, and the value 1.5×1051.5 \times 10^{5} Pa.

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