Calculating the Capacitance — Question 4

Section 25-2 · Physics pages 4038–4039

Question 4 A floating metal slab removes voltage drop from part of a plate gap A neutral conducting slab of thickness t is placed between parallel plates of area A and separation d, with 0<t<d. It touches neither plate. The remaining vacuum gaps have widths g1 and g2. Neglect fringing. A B d t Ideal plate cross-section; fringing is neglected unless stated. (a) Find the gap fields and capacitance. (b) Determine whether moving the slab sideways along the gap normal changes C, provided it remains fully overlapping and out of contact.
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Question 4 - Solution A floating metal slab removes voltage drop from part of a plate gap A B d t (a) Method and calculation g1 + g2 = d −t, Emetal = 0, E1 = E2 = Q/(ϵ0A). V = E1g1 + E2g2 = Q(d −t) ϵ0A , C = ϵ0A d −t. (b) Interpretation and further calculation g1 →g1 + δ, g2 →g2 −δ ⇒∆(g1 + g2) = 0. C′ = C, C Cempty = d d −t > 1. Physical check Neutrality forces equal induced charge magnitudes on the slab faces; its position does not change the total vacuum thickness.

Question 4

A floating metal slab removes voltage drop from part of a plate gap

A neutral conducting slab of thickness t is placed between parallel plates of area A and separation d, with 0<t<d. It touches neither plate. The remaining vacuum gaps have widths g1 and g2. Neglect fringing.

Diagram shown in the original SVG worksheet.

  1. Find the gap fields and capacitance.

  2. Determine whether moving the slab sideways along the gap normal changes C, provided it remains fully overlapping and out of contact.

Question 4 - Solution

A floating metal slab removes voltage drop from part of a plate gap

Diagram shown in the original SVG worksheet.

(a) Method and calculation

g1+g2=d−t,Emetal=0,E1=E2=Q/(ϵ0A).g_1+g_2=d-t,\quad E_{\mathrm{metal}}=0,\quad E_1=E_2=Q/(\epsilon_0A).V=E1g1+E2g2=Q(d−t)ϵ0A,C=ϵ0Ad−t.V=E_1g_1+E_2g_2=\frac{Q(d-t)}{\epsilon_0A},\quad C=\frac{\epsilon_0A}{d-t}.

(b) Interpretation and further calculation

g1→g1+δ,g2→g2−δ⇒Δ(g1+g2)=0.g_1\to g_1+\delta,\quad g_2\to g_2-\delta\Rightarrow\Delta(g_1+g_2)=0.C′=C,CCempty=dd−t>1.C\prime=C,\quad\frac{C}{C_{\mathrm{empty}}}=\frac d{d-t}>1.

Physical check

Neutrality forces equal induced charge magnitudes on the slab faces; its position does not change the total vacuum thickness.