The Electrical Properties of Solids — Question 7

Section 41-1 · Physics pages 6804–6805

Question 7 Local Joule heating can be obtained without a lumped resistor model A homogeneous solid has conductivity σ = 4.00 × 104 S/m in a uniform field E = 30.0 V/m. Its active volume is Vs = 2.00 × 10−8 m3. I L A Schematic; labels, not drawing lengths, specify the data. (a) Derive the heating power per volume and calculate total power. (b) If conductivity doubles, compare power at fixed E and at fixed current density J.
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Question 7 - Solution Local Joule heating can be obtained without a lumped resistor model I L A (a) Method and calculation pv = J · E = σE2 = 3.60 × 107 W/m3 . P = pvVs = .720 W . (b) Interpretation and further calculation E fixed : pv ∝σ ⇒pv′ = 2pv . J fixed : pv = J2/σ ⇒pv′ = pv/2 . Physical check The same material change produces opposite power trends depending on the electrical constraint. Field and current density cannot both remain fixed when conductivity changes.

Question 7

Local Joule heating can be obtained without a lumped resistor model

A homogeneous solid has conductivity σ=4.00×104S/m\sigma=4.00\times10^4\,\mathrm{S/m} in a uniform field E=30.0V/mE=30.0\,\mathrm{V/m}. Its active volume is Vs=2.00×10−8m3V_s=2.00\times10^{-8}\,\mathrm{m^3}.

Diagram shown in the original SVG worksheet.

  1. Derive the heating power per volume and calculate total power.

  2. If conductivity doubles, compare power at fixed E and at fixed current density J.

Question 7 - Solution

Local Joule heating can be obtained without a lumped resistor model

Diagram shown in the original SVG worksheet.

(a) Method and calculation

pv=𝑱⋅𝑬=σE2=3.60×107W/m3.p_v=\boldsymbol J\cdot\boldsymbol E=\sigma E^2=\boxed{3.60\times10^7\,\mathrm{W/m^3}}.P=pvVs=.720W.\boxed{P=p_vV_s=.720\,\mathrm W}.

(b) Interpretation and further calculation

E fixed:pv∝σ⇒pv′=2pv.E\text{ fixed}:\quad p_v\propto\sigma\Rightarrow\boxed{p_v\prime=2p_v}.J fixed:pv=J2/σ⇒pv′=pv/2.J\text{ fixed}:\quad p_v=J^2/\sigma\Rightarrow\boxed{p_v\prime=p_v/2}.

Physical check

The same material change produces opposite power trends depending on the electrical constraint. Field and current density cannot both remain fixed when conductivity changes.