Superconductors — Question 2

Section 26-8 · Physics pages 4294–4295

Question 2 A persistent-current experiment gives a very small resistance bound A closed loop is modeled by L dI/dt + RI = 0, where L=2.00 H is its inductance and R is a possible constant residual resistance. Over T = 106 s, current falls by less than one part in 105. I Closed loop; the stated lumped model specifies its electrical behavior. (a) Derive the current decay and the upper bound on R. (b) Compare with the approximation obtained from −ln(1 −δ) ≃δ, where δ = 10−5.
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Question 2 - Solution A persistent-current experiment gives a very small resistance bound I (a) Method and calculation I(t) = I0e−Rt/L, I(T)/I0 > 1 −δ. R < −L T ln(1 −δ) = 2.00001 × 10−11 Ω. (b) Interpretation and further calculation Rapprox < Lδ/T = 2.00 × 10−11 Ω. −ln(1 −δ) δ = 1 + δ/2 + O(δ2). The approximate bound differs by about 5 parts per million. Physical check Long observation time constrains small resistance even without resolving an instantaneous voltage.

Question 2

A persistent-current experiment gives a very small resistance bound

A closed loop is modeled by LdI/dt+RI=0L\,dI/dt+RI=0, where L=2.00 H is its inductance and R is a possible constant residual resistance. Over T=106T=10^6 s, current falls by less than one part in 10510^5.

Diagram shown in the original SVG worksheet.

  1. Derive the current decay and the upper bound on R.

  2. Compare with the approximation obtained from −ln⁡(1−δ)≃δ-\ln(1-\delta)\simeq\delta, where δ=10−5\delta=10^{-5}.

Question 2 - Solution

A persistent-current experiment gives a very small resistance bound

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I(t)=I0e−Rt/L,I(T)/I0>1−δ.I(t)=I_0e^{-Rt/L},\quad I(T)/I_0>1-\delta.R<−LTln⁡(1−δ)=2.00001×10−11Ω.R<-\frac LT\ln(1-\delta)=2.00001\times10^{-11}\,\Omega.

(b) Interpretation and further calculation

Rapprox<Lδ/T=2.00×10−11Ω.R_{\mathrm{approx}}<L\delta/T=2.00\times10^{-11}\,\Omega.−ln⁡(1−δ)δ=1+δ/2+O(δ2).\frac{-\ln(1-\delta)}\delta=1+\delta/2+O(\delta^2).The approximate bound differs by about 5 parts per million.

Physical check

Long observation time constrains small resistance even without resolving an instantaneous voltage.