UPSC Combined Geo-Scientist, Mains · 2022 · Mains Paper II
Q1(c). Temperature coefficient of conductivity: metal and semiconductor
Question
A temperature variation study of conductivity can distinguish between a metallic conductor and a semiconductor — Explain.
Answer in brief
Metal: σ falls slowly as T rises (more lattice scattering); intrinsic semiconductor: σ rises exponentially (more carriers across the gap); the sign of dσ/dT is the test.
Key points
- Metal: partly filled (overlapping) bands; carrier number n is large (10²⁸–10²⁹ m⁻³) and independent of T.
- Rising T ⇒ stronger lattice vibrations (phonons) ⇒ more electron scattering ⇒ mobility μ falls ⇒ σ falls; Cu, 300 → 310 K: σ drops by about 4%.
- Semiconductor: filled valence band, empty conduction band, small band gap Eg; carriers are made thermally, n ∝ exp(−Eg/2kBT), and this rise outweighs the small fall in μ.
- Si, 300 → 310 K: σ310/σ300 = 2.01, the conductivity doubles.
- Metals show a positive temperature coefficient of resistance, semiconductors a negative one (thermistors); ln σ against 1/T has slope −Eg/2kB, which gives Eg.
The full model answer
As written for the answer booklet: the diagram carries the working, the lines stay short. Read here only; it is not offered as a download.

Coversband theorysemiconductormetallic conductorband gaptemperature coefficient of resistanceelectrical conductivity
All parts of Question 1
- 1(a) Postulates of kinetic theory and the two that fail5 marks
- 1(b) Boyle temperature of oxygen as a van der Waals gas5 marks
- 1(c) Temperature coefficient of conductivity: metal and semiconductor5 marks
- 1(d) Why KCl diffracts like a simple cubic lattice5 marks
- 1(e) Reversal of HCl + NH₃ ⇌ NH₄Cl with temperature5 marks
- 1(f) ΔG for compressing a real gas, from fugacities5 marks
- 1(g) Half-life of a second-order reaction5 marks
- 1(h) Brownian movement and Tyndall effect: why only colloids5 marks
- 1(i) Nernst equation for the redox electrode Pt | Cr⁶⁺, Cr³⁺5 marks
- 1(j) Same electrode positive or negative5 marks
- 1(k) Energy uncertainty of an excited state5 marks
- 1(l) Eigenvalues of a Hermitian operator are real5 marks
- 1(m) Rotational constants of ¹⁴N¹⁶O and ¹⁵N¹⁶O5 marks
- 1(n) Photon–molecule interaction in rotating HCl5 marks
- 1(o) Why radiative transitions are drawn vertical5 marks
- 1(p) Energy of one einstein at 600 nm and 300 nm5 marks