Power in Electric Circuits — Question 7

Section 26-6 · Physics pages 4264–4265

Question 7 A heater with a positive temperature coefficient responds differently to fixed current and voltage A heater has R = R0(1 + α∆T) and loses heat at rate H∆T, with H and alpha positive. Treat its temperature as uniform. R0(1 + α∆T) + − I H∆T Schematic; labels, not drawing lengths, specify the data. (a) At fixed current I, find steady temperature rise and its stability condition. (b) At fixed voltage V, find the positive steady temperature rise and compare thermal feedback signs.
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Question 7 - Solution A heater with a positive temperature coefficient responds differently to fixed current and voltage R0(1 + α∆T) + − I H∆T (a) Method and calculation I2R0(1 + α∆T) = H∆T ⇒∆T = I2R0 H −αI2R0 . H > αI2R0 for a positive stable equilibrium. (b) Interpretation and further calculation V 2 R0(1 + α∆T) = H∆T. ∆T = √ 1 + 4αV 2/(HR0) −1 2α . Current drive increases heating with temperature; voltage drive decreases it, giving negative feedback. Physical check Stability follows the slope of heating minus cooling; the fixed-current denominator must remain positive.

Question 7

A heater with a positive temperature coefficient responds differently to fixed current and voltage

A heater has R=R0(1+αΔT)R=R_0(1+\alpha\Delta T) and loses heat at rate HΔTH\Delta T, with H and alpha positive. Treat its temperature as uniform.

Diagram shown in the original SVG worksheet.

  1. At fixed current I, find steady temperature rise and its stability condition.

  2. At fixed voltage V, find the positive steady temperature rise and compare thermal feedback signs.

Question 7 - Solution

A heater with a positive temperature coefficient responds differently to fixed current and voltage

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I2R0(1+αΔT)=HΔT⇒ΔT=I2R0H−αI2R0.I^2R_0(1+\alpha\Delta T)=H\Delta T\Rightarrow\Delta T=\frac{I^2R_0}{H-\alpha I^2R_0}.H>αI2R0for a positive stable equilibrium.H>\alpha I^2R_0\quad\text{for a positive stable equilibrium}.

(b) Interpretation and further calculation

V2R0(1+αΔT)=HΔT.\frac{V^2}{R_0(1+\alpha\Delta T)}=H\Delta T.ΔT=1+4αV2/(HR0)−12α.\Delta T=\frac{\sqrt{1+4\alpha V^2/(HR_0)}-1}{2\alpha}.Current drive increases heating with temperature; voltage drive decreases it, giving negative feedback.

Physical check

Stability follows the slope of heating minus cooling; the fixed-current denominator must remain positive.