Superconductors — Question 5

Section 26-8 · Physics pages 4300–4301

Question 5 The magnetic field made by a wire can impose its own critical-current limit For a long round wire of radius a, use the supplied surface-field relation Bs = µ0I/(2πa). In a simplified type-I model, superconductivity requires Bs < Bc(T), where Bc(T) = Bc0[1 −(T/Tc)2]. No applied field is present. a Bs Schematic; labels, not drawing lengths, specify the data. (a) Find the critical-current boundary as a function of temperature. (b) If radius doubles at fixed temperature, compare the boundary current and its area-averaged density.
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Question 5 - Solution The magnetic field made by a wire can impose its own critical-current limit a Bs (a) Method and calculation µ0Ic/(2πa) = Bc(T). Ic(T) = 2πaBc0 µ0 [1 −(T/Tc)2]. (b) Interpretation and further calculation Ic(2a)/Ic(a) = 2, Jc = Ic/(πa2) = 2Bc/(µ0a). Jc(2a)/Jc(a) = 1/2. Physical check The self-field constraint scales with radius, not area; real critical-current behavior can involve additional mechanisms.

Question 5

The magnetic field made by a wire can impose its own critical-current limit

For a long round wire of radius a, use the supplied surface-field relation Bs=μ0I/(2πa)B_s=\mu_0I/(2\pi a). In a simplified type-I model, superconductivity requires Bs<Bc(T)B_s<B_c(T), where Bc(T)=Bc0[1−(T/Tc)2]B_c(T)=B_{c0}[1-(T/T_c)^2]. No applied field is present.

Diagram shown in the original SVG worksheet.

  1. Find the critical-current boundary as a function of temperature.

  2. If radius doubles at fixed temperature, compare the boundary current and its area-averaged density.

Question 5 - Solution

The magnetic field made by a wire can impose its own critical-current limit

Diagram shown in the original SVG worksheet.

(a) Method and calculation

μ0Ic/(2πa)=Bc(T).\mu_0I_c/(2\pi a)=B_c(T).Ic(T)=2πaBc0μ0[1−(T/Tc)2].I_c(T)=\frac{2\pi aB_{c0}}{\mu_0}[1-(T/T_c)^2].

(b) Interpretation and further calculation

Ic(2a)/Ic(a)=2,J¯c=Ic/(πa2)=2Bc/(μ0a).I_c(2a)/I_c(a)=2,\quad\overline J_c=I_c/(\pi a^2)=2B_c/(\mu_0a).J¯c(2a)/J¯c(a)=1/2.\overline J_c(2a)/\overline J_c(a)=1/2.

Physical check

The self-field constraint scales with radius, not area; real critical-current behavior can involve additional mechanisms.