Other Single-Loop Circuits — Question 8

Section 27-4 · Physics pages 4386–4387

Question 8 Opposite temperature coefficients can stabilize a series current Two resistors obey R1(T) = R10(1 + a∆T) and R2(T) = R20(1 −b∆T), with a = .0040 K−1 and b = .0020 K−1. They share a uniform temperature and an ideal 12.0 V source. + − 12 V R1(T) R2(T) I Circuit connections and marked polarities define the model; wire lengths are schematic. (a) Choose positive R10 and R20 so the current is .100 A and its first-order temperature coefficient vanishes. (b) Within the supplied linear laws, find the exact total resistance and state the temperature range required for both individual resistances to remain positive.
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Question 8 - Solution Opposite temperature coefficients can stabilize a series current + − 12 V R1(T) R2(T) I (a) Method and calculation R10 + R20 = 12/.100 = 120 Ω, aR10 −bR20 = 0. R20 = 2R10 ⇒R10 = 40.0 Ω, R20 = 80.0 Ω. (b) Interpretation and further calculation R1 + R2 = 120 + (aR10 −bR20)∆T = 120 Ω. 1 + a∆T > 0, 1 −b∆T > 0 ⇒−250 < ∆T < 500 K. The empirical linear laws may be valid only over a much smaller interval. Physical check Cancellation is exact within the specified linear model, but is not guaranteed for real nonlinear temperature dependence.

Question 8

Opposite temperature coefficients can stabilize a series current

Two resistors obey R1(T)=R10(1+aΔT)R_1(T)=R_{10}(1+a\Delta T) and R2(T)=R20(1−bΔT)R_2(T)=R_{20}(1-b\Delta T), with a=.0040a=.0040 K−1^{-1} and b=.0020b=.0020 K−1^{-1}. They share a uniform temperature and an ideal 12.0 V source.

Diagram shown in the original SVG worksheet.

  1. Choose positive R10 and R20 so the current is .100 A and its first-order temperature coefficient vanishes.

  2. Within the supplied linear laws, find the exact total resistance and state the temperature range required for both individual resistances to remain positive.

Question 8 - Solution

Opposite temperature coefficients can stabilize a series current

Diagram shown in the original SVG worksheet.

(a) Method and calculation

R10+R20=12/.100=120Ω,aR10−bR20=0.R_{10}+R_{20}=12/.100=120\,\Omega,\quad aR_{10}-bR_{20}=0.R20=2R10⇒R10=40.0Ω,R20=80.0Ω.R_{20}=2R_{10}\Rightarrow R_{10}=40.0\,\Omega,\quad R_{20}=80.0\,\Omega.

(b) Interpretation and further calculation

R1+R2=120+(aR10−bR20)ΔT=120Ω.R_1+R_2=120+(aR_{10}-bR_{20})\Delta T=120\,\Omega.1+aΔT>0,1−bΔT>0⇒−250<ΔT<500K.1+a\Delta T>0,\ 1-b\Delta T>0\Rightarrow-250<\Delta T<500\,\mathrm K.The empirical linear laws may be valid only over a much smaller interval.

Physical check

Cancellation is exact within the specified linear model, but is not guaranteed for real nonlinear temperature dependence.