Ohm's Law — Question 4

Section 26-4 · Physics pages 4218–4219

Question 4 Self-heating can curve a characteristic of an otherwise ohmic material A specimen obeys V = R(T)I at any fixed temperature, with R(T) = R0[1 + α(T −T0)]. During slow measurements, the supplied thermal law is T −T0 = ΘIV , where α, Θ > 0. R(T) + − I heat Schematic; labels, not drawing lengths, specify the data. (a) Derive the steady V-I relation and its admissible current domain. (b) Find the leading small-current nonlinear term and explain why this does not disprove fixed-temperature Ohm behavior.
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Question 4 - Solution Self-heating can curve a characteristic of an otherwise ohmic material R(T) + − I heat (a) Method and calculation V = R0I[1 + αΘIV ] ⇒V (1 −αΘR0I2) = R0I. V = R0I 1 −αΘR0I2 , |I| < (αΘR0)−1/2. (b) Interpretation and further calculation V = R0I + αΘR2 0I3 + O(I5). V I T fixed = R(T) = constant. The slow sweep changes temperature as well as current. Physical check The excluded pole marks failure of a finite steady solution within this linear thermal model, not a prediction of infinite physical voltage.

Question 4

Self-heating can curve a characteristic of an otherwise ohmic material

A specimen obeys V=R(T)IV=R(T)I at any fixed temperature, with R(T)=R0[1+α(T−T0)]R(T)=R_0[1+\alpha(T-T_0)]. During slow measurements, the supplied thermal law is T−T0=ΘIVT-T_0=\Theta IV, where α,Θ>0\alpha,\Theta>0.

Diagram shown in the original SVG worksheet.

  1. Derive the steady V-I relation and its admissible current domain.

  2. Find the leading small-current nonlinear term and explain why this does not disprove fixed-temperature Ohm behavior.

Question 4 - Solution

Self-heating can curve a characteristic of an otherwise ohmic material

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V=R0I[1+αΘIV]⇒V(1−αΘR0I2)=R0I.V=R_0I[1+\alpha\Theta IV]\Rightarrow V(1-\alpha\Theta R_0I^2)=R_0I.V=R0I1−αΘR0I2,|I|<(αΘR0)−1/2.V=\frac{R_0I}{1-\alpha\Theta R_0I^2},\quad |I|<(\alpha\Theta R_0)^{-1/2}.

(b) Interpretation and further calculation

V=R0I+αΘR02I3+O(I5).V=R_0I+\alpha\Theta R_0^2I^3+O(I^5).VI|Tfixed=R(T)=constant.\left.\frac VI\right|_{T\ \mathrm{fixed}}=R(T)=\text{constant}.The slow sweep changes temperature as well as current.

Physical check

The excluded pole marks failure of a finite steady solution within this linear thermal model, not a prediction of infinite physical voltage.