2.2.1 Thermal Expansion of Solids, Liquids and Gases
When the temperature of a material is increased while the external pressure is kept constant, its particles gain kinetic energy, move more vigorously and tend to occupy a larger volume. This phenomenon is called thermal expansion. The amount of expansion depends on the state of matter and on the intrinsic properties of the material.
1. Qualitative Description (Constant‑Pressure)
All three states – solids, liquids and gases – expand when heated at constant pressure.
Why the magnitude differs: the average distance between particles increases most where the particles are already far apart (gases), less where they are close together (liquids), and least where they are fixed in a lattice (solids).
Solids – Linear Expansion
Particles vibrate about fixed lattice points. Heating increases the average separation slightly, so the dimensions of the solid increase.
Change in length:
\[
\Delta L = \alpha L_{0}\,\Delta T
\]
\(\Delta L\) – change in length
\(\alpha\) – coefficient of linear expansion (≈ 10⁻⁶ – 10⁻⁵ K⁻¹ for metals)
\(L_{0}\) – original length
\(\Delta T\) – temperature change (°C or K)
For an isotropic solid the volume‑expansion coefficient \(\beta\) is roughly three times the linear coefficient: \(\beta \approx 3\alpha\).
Liquids – Volume Expansion
Particles are free to slide past one another; the intermolecular forces are weaker than in solids. Heating increases the average intermolecular distance, giving a noticeable rise in volume.
Change in volume:
\[
\Delta V = \beta V_{0}\,\Delta T
\]
Gas particles are far apart and experience negligible attractive forces. Heating raises their average speed, so they strike the container walls more forcefully, expanding the gas.
For an ideal gas at constant pressure:
\[
\frac{V}{T}= \text{constant}\qquad\text{or}\qquad\frac{\Delta V}{V_{0}}=\frac{\Delta T}{T_{0}}
\]
Thus the coefficient of volume expansion for an ideal gas is
\[
\beta = \frac{1}{T}
\]
where \(T\) is the absolute temperature (K).
Expansion joints in bridges and railway tracks – metal expands in summer; joints allow movement and prevent buckling.
Concrete sidewalks and pavement – laid with regular joints; without them the concrete would crack as it expands.
Bimetallic strips in thermostats – two metals with different \(\alpha\) values bend when heated, operating a switch.
Glass laboratory containers – borosilicate or lead‑glass has a low \(\beta\) to resist cracking on heating.
Thermometers – mercury or coloured alcohol expands uniformly with temperature, giving a reliable scale.
Engine pistons and cylinder heads – designed with clearance gaps so the hot gases can expand without seizing the moving parts.
Metallic pipelines – fitted with expansion loops or flexible couplings to accommodate temperature‑induced length changes.
Railway tracks – continuous welded rail includes expansion gaps or is laid at a temperature that minimises stress throughout the year.
4. Experimental Demonstration (Practical Box)
Practical: Observing Linear Expansion of a Metal Rod
Set up a metal rod (≈ 1 m) fixed at one end on a stable bench.
Attach a small mirror to the free end and aim a laser beam at the mirror so that the reflected spot falls on a distant screen (≈ 2 m away).
Measure the initial spot position \(x_{0}\) at room temperature \(T_{0}\).
Heat the rod uniformly (e.g., by immersing it in a water bath at a known higher temperature \(T\)).
Record the new spot position \(x\). The lateral shift \(\Delta x\) is related to the change in length \(\Delta L\) by \(\Delta L = \frac{\Delta x}{2}\tan\theta\) where \(\theta\) is the angle of incidence (≈ 45° for a simple set‑up).
Calculate \(\alpha\) from \(\alpha = \frac{\Delta L}{L_{0}\Delta T}\) and compare with the literature value.
Key points for the exam: constant pressure (ambient air), measurement of \(\Delta L\), use of \(\Delta T\), and identification of sources of error (non‑uniform heating, parallax).
5. Summary
All matter expands when heated at constant pressure.
Solids: small, linear expansion; \(\Delta L = αL_{0}\Delta T\).
Liquids: moderate, volume expansion; \(\Delta V = βV_{0}\Delta T\).
Gases: large, volume expansion; obey Charles’s Law \(\displaystyle\frac{V}{T}= \text{constant}\) and \(\beta = 1/T\).
The order of magnitude (gases > liquids > solids) follows directly from how far apart the particles are in each state.
Coefficients \(α\) and \(β\) are material‑specific; engineers must provide space (expansion joints, clearances, flexible components) to accommodate the change and avoid stress or failure.
Suggested diagrams (to be drawn by the learner):
(i) Linear expansion of a metal rod – original length \(L_{0}\) and expanded length \(L\).
(ii) Volume expansion of a liquid in a bulb – initial volume \(V_{0}\) and expanded volume \(V\).
(iii) Piston moving outward as a gas expands when heated – showing constant external pressure.
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