The Electrical Properties of Solids — Question 8

Section 41-1 · Physics pages 6806–6807

Question 8 A temperature sweep separates activation from a geometrical resistance change An insulating specimen has ρ(T) = ρaeEa/(kBT), with constant prefactor and negligible thermal expansion. Measured resistances satisfy R(300 K)/R(400 K) = 10. Use kB = 8.617 × 10−5 eV/K. 1/T ln R Schematic; labels, not drawing lengths, specify the data. (a) Infer the activation energy. (b) Find the ratio R(400 K)/R(600 K).
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Question 8 - Solution A temperature sweep separates activation from a geometrical resistance change 1/T ln R (a) Method and calculation ln(R300/R400) = Ea kB (1/300 −1/400). Ea = 1200kB ln 10 = .2381 eV . (b) Interpretation and further calculation 1/400 −1/600 = 1/1200. R400/R600 = eEa/(1200kB) = 10 . Physical check The equal ratios follow equal differences in inverse temperature, not equal temperature increments. This activation model does not describe an ordinary metal over the same interval.

Question 8

A temperature sweep separates activation from a geometrical resistance change

An insulating specimen has ρ(T)=ρaeEa/(kBT)\rho(T)=\rho_a e^{E_a/(k_BT)}, with constant prefactor and negligible thermal expansion. Measured resistances satisfy R(300K)/R(400K)=10R(300\,\mathrm K)/R(400\,\mathrm K)=10. Use kB=8.617×10−5eV/Kk_B=8.617\times10^{-5}\,\mathrm{eV/K}.

Diagram shown in the original SVG worksheet.

  1. Infer the activation energy.

  2. Find the ratio R(400K)/R(600K)R(400\,\mathrm K)/R(600\,\mathrm K).

Question 8 - Solution

A temperature sweep separates activation from a geometrical resistance change

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ln⁡(R300/R400)=EakB(1/300−1/400).\ln(R_{300}/R_{400})=\frac{E_a}{k_B}(1/300-1/400).Ea=1200kBln⁡10=.2381eV.\boxed{E_a=1200k_B\ln10=.2381\,\mathrm{eV}}.

(b) Interpretation and further calculation

1/400−1/600=1/1200.1/400-1/600=1/1200.R400/R600=eEa/(1200kB)=10.\boxed{R_{400}/R_{600}=e^{E_a/(1200k_B)}=10}.

Physical check

The equal ratios follow equal differences in inverse temperature, not equal temperature increments. This activation model does not describe an ordinary metal over the same interval.