Superconductors — Question 8

Section 26-8 · Physics pages 4306–4307

Question 8 A quench can convert stored loop energy into a temperature rise A loop of inductance L initially carries I0. A quench creates resistance Rq > 0 and the supplied decay is I(t) = I0e−Rqt/L. Assume all Joule heat remains in a body of constant heat capacity C, with no energy extraction. I Rq Closed loop; the stated lumped model specifies its electrical behavior. (a) Find heat deposited up to time t and the final temperature rise. (b) Find the time when half the total heat has been deposited and the maximum initial current for an allowed rise ∆Tmax.
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Question 8 - Solution A quench can convert stored loop energy into a temperature rise I Rq (a) Method and calculation Q(t) = ∫t 0 RqI2 0e−2Rqt′/Ldt′ = 1 2LI2 0(1 −e−2Rqt/L). ∆T∞= Q(∞)/C = LI2 0/(2C). (b) Interpretation and further calculation 1 −e−2Rqt1/2/L = 1/2 ⇒t1/2 = L ln 2 2Rq . I0 ≤ √ 2C∆Tmax/L. Physical check Resistance determines how quickly heat is released; the total comes from the initial stored energy.

Question 8

A quench can convert stored loop energy into a temperature rise

A loop of inductance L initially carries I0I_0. A quench creates resistance Rq>0R_q>0 and the supplied decay is I(t)=I0e−Rqt/LI(t)=I_0e^{-R_qt/L}. Assume all Joule heat remains in a body of constant heat capacity C, with no energy extraction.

Diagram shown in the original SVG worksheet.

  1. Find heat deposited up to time t and the final temperature rise.

  2. Find the time when half the total heat has been deposited and the maximum initial current for an allowed rise ΔTmax\Delta T_{\max}.

Question 8 - Solution

A quench can convert stored loop energy into a temperature rise

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q(t)=∫0tRqI02e−2Rqt′/Ldt′=12LI02(1−e−2Rqt/L).Q(t)=\int_0^t R_qI_0^2e^{-2R_qt\prime/L}dt\prime=\tfrac12LI_0^2(1-e^{-2R_qt/L}).ΔT∞=Q(∞)/C=LI02/(2C).\Delta T_\infty=Q(\infty)/C=LI_0^2/(2C).

(b) Interpretation and further calculation

1−e−2Rqt1/2/L=1/2⇒t1/2=Lln⁡22Rq.1-e^{-2R_qt_{1/2}/L}=1/2\Rightarrow t_{1/2}=\frac{L\ln2}{2R_q}.I0≤2CΔTmax/L.I_0\le\sqrt{2C\Delta T_{\max}/L}.

Physical check

Resistance determines how quickly heat is released; the total comes from the initial stored energy.