Describe, qualitatively, the thermal expansion of solids, liquids and gases at constant pressure

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:
    \[ \Delta V = \beta V_{0}\,\Delta T \]
    • \(\Delta V\) – change in volume
    • \(\beta\) – coefficient of volume expansion (typically 10⁻⁴ – 10⁻³ K⁻¹)
    • \(V_{0}\) – original volume
    • \(\Delta T\) – temperature change

Gases – Volume Expansion (Charles’s Law)

  • 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).

2. Typical Coefficients of Expansion

Material State Coefficient of Linear Expansion \(α\) (K⁻¹) Coefficient of Volume Expansion \(β\) (K⁻¹)
Aluminium Solid 2.4 × 10⁻⁵ ≈ 7.2 × 10⁻⁵
Glass (typical) Solid 9 × 10⁻⁶ ≈ 2.7 × 10⁻⁵
Water Liquid 2.1 × 10⁻⁴ (20 °C → 30 °C)
Air (ideal gas) Gas ≈ 1/T (≈ 3.6 × 10⁻³ at 300 K)

3. Everyday Applications & Consequences (IGCSE‑relevant examples)

  • 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
  1. Set up a metal rod (≈ 1 m) fixed at one end on a stable bench.
  2. 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).
  3. Measure the initial spot position \(x_{0}\) at room temperature \(T_{0}\).
  4. Heat the rod uniformly (e.g., by immersing it in a water bath at a known higher temperature \(T\)).
  5. 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).
  6. 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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