Two Experiments — Question 5

Section 30-1 · Physics pages 4760–4761

Question 5 A pickup-voltage integral reconstructs a linkage change without knowing the pulse shape A resistive pickup records signed emf E(t) = E0 sin(πt/T) for 0 < t < T. It is zero outside this interval. Let E0=.200 V, T=.0300 s and R=4.00 ohms. For this calibrated experiment, use signed flux linkage Λ = NΦ, E = −dΛ/dt and i = E/R; neglect pickup self-inductance. t E Schematic; labels, not drawing lengths, specify the data. (a) Find the total linkage change. (b) Find the signed transported charge and explain what remains unknown about the absolute linkage.
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Question 5 - Solution A pickup-voltage integral reconstructs a linkage change without knowing the pulse shape t E (a) Method and calculation ∆Λ = − ∫T 0 E0 sin(πt/T)dt = −2E0T π . ∆Λ = −.0120/π Wb . (b) Interpretation and further calculation Q = 1 R ∫T 0 E dt = .00300/π C . Λ(t) = Λ(0) − ∫t 0 E dt contains the unknown constant Λ(0). Physical check A pickup measures change in flux linkage, not an absolute static flux.

Question 5

A pickup-voltage integral reconstructs a linkage change without knowing the pulse shape

A resistive pickup records signed emf ℰ(t)=E0sin⁡(πt/T)\mathcal E(t)=E_0\sin(\pi t/T) for 0<t<T0<t<T. It is zero outside this interval. Let E0=.200 V, T=.0300 s and R=4.00 ohms. For this calibrated experiment, use signed flux linkage Λ=NΦ\Lambda=N\Phi, ℰ=−dΛ/dt\mathcal E=-d\Lambda/dt and i=ℰ/Ri=\mathcal E/R; neglect pickup self-inductance.

Diagram shown in the original SVG worksheet.

  1. Find the total linkage change.

  2. Find the signed transported charge and explain what remains unknown about the absolute linkage.

Question 5 - Solution

A pickup-voltage integral reconstructs a linkage change without knowing the pulse shape

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔΛ=−∫0TE0sin⁡(πt/T)dt=−2E0Tπ.\Delta\Lambda=-\int_0^T E_0\sin(\pi t/T)dt=-\frac{2E_0T}{\pi}.ΔΛ=−.0120/πWb.\boxed{\Delta\Lambda=-.0120/\pi\,\mathrm{Wb}}.

(b) Interpretation and further calculation

Q=1R∫0Tℰdt=.00300/πC.Q=\frac1R\int_0^T\mathcal E\,dt=\boxed{.00300/\pi\,\mathrm C}.Λ(t)=Λ(0)−∫0tℰdtcontains the unknown constant Λ(0).\Lambda(t)=\Lambda(0)-\int_0^t\mathcal E\,dt\quad\text{contains the unknown constant }\Lambda(0).

Physical check

A pickup measures change in flux linkage, not an absolute static flux.