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Physics · Ch 2 — Electrostatic Potential and Capacitance

Capacitors in Series

2.15.1

Capacitors in Series

In a series combination, capacitors C1,C2,C3,…C_1, C_2, C_3, \ldots are connected end to end in a single chain, with only the two OUTER ends of the chain connected to the source of potential difference VV.

Same charge on every capacitor. Consider, for simplicity, two capacitors C1C_1 and C2C_2 in series. The inner plate connecting them (the right plate of C1C_1 joined to the left plate of C2C_2) is electrically isolated from the rest of the circuit -- charge cannot flow onto or off this isolated inner conductor from anywhere else, so it must carry exactly zero NET charge; but if the outer plate of C1C_1 carries charge +Q+Q, it must induce an equal −Q-Q on the near face of that isolated inner conductor, which in turn forces an equal and opposite +Q+Q to appear on its far face (facing C2C_2), and so on down the chain. The upshot is that every capacitor in a series chain carries exactly the same charge magnitude QQ -- the same charge that flows from the battery's terminals into the two outermost plates.

Voltages add. The total potential difference supplied by the source is shared, unequally in general, across the individual capacitors:

V=V1+V2+V3+⋯=QC1+QC2+QC3+⋯V = V_1 + V_2 + V_3 + \cdots = \frac{Q}{C_1} + \frac{Q}{C_2} + \frac{Q}{C_3} + \cdots

using Vi=Q/CiV_i = Q/C_i for each capacitor, since QQ is common to all of them. Defining the equivalent capacitance CsC_s by V=Q/CsV = Q/C_s, and dividing the equation above through by QQ,

1Cs=1C1+1C2+1C3+⋯\frac{1}{C_s} = \frac{1}{C_1} + \frac{1}{C_2} + \frac{1}{C_3} + \cdots …