Charge Is Conserved — Question 3

Section 21-5 · Physics pages 3456–3457

Question 3 A time-dependent charge influx can reverse accumulation during one pulse A region begins with Q(0) = 0. From 0 to τ, its inward conventional charge rate is I0 sin(πt/τ) and its outward rate is I0/2, where I0 = 2.00 nC/s and τ = 3.00 s. These rates are defined as charge per time and need not be constant. t rate Axes and labels specify the model; the sketch is schematic. (a) Integrate the net rate to obtain Q(t) and the final charge Q(τ). (b) Find the times of the minimum and maximum charge during the pulse, and verify their classification from the signs of the accumulation rate.
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Question 3 - Solution A time-dependent charge influx can reverse accumulation during one pulse t rate (a) Method and calculation dQ dt = I0[sin(πt/τ) −1/2]. Q(t) = I0 [τ π(1 −cos(πt/τ)) −t 2 ] . Q(τ) = I0τ(2/π −1/2) ≈.819719 nC. (b) Interpretation and further calculation sin(πt/τ) = 1/2 ⇒tmin = τ/6 = .500 s, tmax = 5τ/6 = 2.50 s. Qmin = I0τ[(1 − √ 3/2)/π −1/12], Qmax = I0τ[(1 + √ 3/2)/π −5/12]. The rate is negative, then positive, then negative on the three successive intervals. These extrema are also the global minimum and maximum over the pulse. Physical check Net positive charge at the end does not imply positive accumulation at every earlier instant.

Question 3

A time-dependent charge influx can reverse accumulation during one pulse

A region begins with Q(0)=0Q(0)=0. From 00 to τ\tau, its inward conventional charge rate is I0sin⁡(πt/τ)I_0\sin(\pi t/\tau) and its outward rate is I0/2I_0/2, where I0=2.00I_0=2.00 nC/s and τ=3.00\tau=3.00 s. These rates are defined as charge per time and need not be constant.

Diagram shown in the original SVG worksheet.

  1. Integrate the net rate to obtain Q(t)Q(t) and the final charge Q(τ)Q(\tau).

  2. Find the times of the minimum and maximum charge during the pulse, and verify their classification from the signs of the accumulation rate.

Question 3 - Solution

A time-dependent charge influx can reverse accumulation during one pulse

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dQdt=I0[sin⁡(πt/τ)−1/2].\frac{dQ}{dt}=I_0[\sin(\pi t/\tau)-1/2].Q(t)=I0[τπ(1−cos(πt/τ))−t2].Q(t)=I_0\left[\frac\tau\pi(1-\cos(\pi t/\tau))-\frac t2\right].Q(τ)=I0τ(2/π−1/2)≈.819719nC.Q(\tau)=I_0\tau(2/\pi-1/2)\approx.819719\,\mathrm{nC}.

(b) Interpretation and further calculation

sin⁡(πt/τ)=1/2⇒tmin=τ/6=.500s,tmax=5τ/6=2.50s.\sin(\pi t/\tau)=1/2\Rightarrow t_{\min}=\tau/6=.500\,\mathrm s,\quad t_{\max}=5\tau/6=2.50\,\mathrm s.Qmin=I0τ[(1−3/2)/π−1/12],Qmax=I0τ[(1+3/2)/π−5/12].Q_{\min}=I_0\tau[(1-\sqrt3/2)/\pi-1/12],\quad Q_{\max}=I_0\tau[(1+\sqrt3/2)/\pi-5/12].The rate is negative, then positive, then negative on the three successive intervals. These extrema are also the global minimum and maximum over the pulse.

Physical check

Net positive charge at the end does not imply positive accumulation at every earlier instant.