Power in Electric Circuits — Question 8

Section 26-6 · Physics pages 4266–4267

Question 8 An adiabatic fuse model converts a current pulse into a melting criterion A short wire has mass m, specific heat c, melting temperature Tm, initial temperature T0 < Tm, and latent heat of fusion Lf. Its resistance R is treated constant; heat loss is neglected. t I Axes and labels specify the model; the sketch is schematic. (a) Find the time to melt completely under constant current I. (b) For I(t) = Ipe−t/τ, find the minimum peak current that supplies enough energy over all time.
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Question 8 - Solution An adiabatic fuse model converts a current pulse into a melting criterion t I (a) Method and calculation Wm = mc(Tm −T0) + mLf. I2Rtm = Wm ⇒tm = m[c(Tm −T0) + Lf] I2R . (b) Interpretation and further calculation W∞= R ∫∞ 0 I2 pe−2t/τdt = RI2 pτ/2. Ip ≥ √ 2Wm/(Rτ). Equality approaches complete melting only as time tends to infinity. Physical check The threshold is an ideal energy criterion; real resistance and heat losses vary during heating.

Question 8

An adiabatic fuse model converts a current pulse into a melting criterion

A short wire has mass m, specific heat c, melting temperature TmT_m, initial temperature T0<TmT_0<T_m, and latent heat of fusion LfL_f. Its resistance R is treated constant; heat loss is neglected.

Diagram shown in the original SVG worksheet.

  1. Find the time to melt completely under constant current I.

  2. For I(t)=Ipe−t/τI(t)=I_pe^{-t/\tau}, find the minimum peak current that supplies enough energy over all time.

Question 8 - Solution

An adiabatic fuse model converts a current pulse into a melting criterion

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Wm=mc(Tm−T0)+mLf.W_m=mc(T_m-T_0)+mL_f.I2Rtm=Wm⇒tm=m[c(Tm−T0)+Lf]I2R.I^2Rt_m=W_m\Rightarrow t_m=\frac{m[c(T_m-T_0)+L_f]}{I^2R}.

(b) Interpretation and further calculation

W∞=R∫0∞Ip2e−2t/τdt=RIp2τ/2.W_\infty=R\int_0^\infty I_p^2e^{-2t/\tau}dt=RI_p^2\tau/2.Ip≥2Wm/(Rτ).I_p\ge\sqrt{2W_m/(R\tau)}.Equality approaches complete melting only as time tends to infinity.

Physical check

The threshold is an ideal energy criterion; real resistance and heat losses vary during heating.