Superconductors — Question 10

Section 26-8 · Physics pages 4310–4311

Question 10 A spatial distribution of transition temperatures broadens a resistance transition A long wire of length L and area A has local transition temperature Tc(x) = T1 + (T2 −T1)(x/L)2, with T2 > T1. At uniform temperature T, each slice has resistivity zero below its local Tc and constant ρn above it. Slices carry the same current; ignore proximity effects. T R T1 T2 Axes and labels specify the model; the sketch is schematic. (a) Find total R(T) for T1 < T < T2 and the limiting regimes outside that interval. (b) Find the temperature where resistance equals half its fully normal value and determine when the whole wire has zero resistance.
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Question 10 - Solution A spatial distribution of transition temperatures broadens a resistance transition T R T1 T2 (a) Method and calculation T > Tc(x) ⇒x < L √ T −T1 T2 −T1 . R(T) = Rn √ T −T1 T2 −T1 , Rn = ρnL/A. (b) Interpretation and further calculation R = Rn/2 ⇒T = T1 + (T2 −T1)/4. R = 0 (T ≤T1), R = Rn (T ≥T2). The lowest local transition temperature controls the onset of a completely zero-resistance series path. Physical check A broad measured transition can reflect inhomogeneous local critical temperatures rather than a finite resistance in every superconducting region.

Question 10

A spatial distribution of transition temperatures broadens a resistance transition

A long wire of length L and area A has local transition temperature Tc(x)=T1+(T2−T1)(x/L)2T_c(x)=T_1+(T_2-T_1)(x/L)^2, with T2>T1T_2>T_1. At uniform temperature T, each slice has resistivity zero below its local Tc and constant ρn\rho_n above it. Slices carry the same current; ignore proximity effects.

Diagram shown in the original SVG worksheet.

  1. Find total R(T) for T1<T<T2T_1<T<T_2 and the limiting regimes outside that interval.

  2. Find the temperature where resistance equals half its fully normal value and determine when the whole wire has zero resistance.

Question 10 - Solution

A spatial distribution of transition temperatures broadens a resistance transition

Diagram shown in the original SVG worksheet.

(a) Method and calculation

T>Tc(x)⇒x<LT−T1T2−T1.T>T_c(x)\Rightarrow x<L\sqrt{\frac{T-T_1}{T_2-T_1}}.R(T)=RnT−T1T2−T1,Rn=ρnL/A.R(T)=R_n\sqrt{\frac{T-T_1}{T_2-T_1}},\quad R_n=\rho_nL/A.

(b) Interpretation and further calculation

R=Rn/2⇒T=T1+(T2−T1)/4.R=R_n/2\Rightarrow T=T_1+(T_2-T_1)/4.R=0(T≤T1),R=Rn(T≥T2).R=0\ (T\le T_1),\quad R=R_n\ (T\ge T_2).The lowest local transition temperature controls the onset of a completely zero-resistance series path.

Physical check

A broad measured transition can reflect inhomogeneous local critical temperatures rather than a finite resistance in every superconducting region.