Topic 7 of 9
Capacitor combinations
Capacitor combinations follow charge and voltage constraints. Identify which plates share a node and whether charge can enter an intermediate node before choosing a rule.
For a capacitor with equal and opposite plate charges, C = Q/V, where Q is the magnitude on one plate and V is the p.d. magnitude. The net charge of the two-plate device can be zero while it stores energy. Capacitance has unit farad: 1 F = 1 C/V, with 1 µF = 10-6 F and 1 µC = 10-6 C. The capacitance explanation develops these quantities.
Parallel: the same p.d. across both capacitors
Both capacitors have 12 V across A/C. The equivalent is 9 microfarad; the source supplies 108 microcoulomb to the positive-plate side.
Series: the isolated middle conductor has zero net charge
All four plate-charge magnitudes are 24 microcoulomb. B has zero net charge under the stated initial conditions; zero net charge does not imply zero potential.
A third capacitor joins A to C
Reduce the 3/6 microfarad series branch first, then add the parallel 4 microfarad branch. Source charge is 72 microcoulomb.
Parallel: the same p.d.
Capacitors in parallel share both endpoints and therefore V. The total charge supplied to the positive plates is the sum:
Cparallel = C1 + C2 + …
For 3.0 µF and 6.0 µF in parallel across 12 V, Cequivalent = 9.0 µF. The plate-charge magnitudes are 36 and 72 µC, giving total supplied charge 108 µC. Do not double this by adding both positive and negative plate-charge magnitudes.
Series: the middle-node charge constraint
Start with uncharged capacitors and keep their intermediate node isolated from any other conducting connection. No net charge can enter that node, so its two connected plates acquire equal and opposite charges. The series capacitors therefore have equal plate-charge magnitudes Q, while their voltages add:
1/Cseries = 1/C1 + 1/C2 + …
For 3.0 µF on A/B and 6.0 µF on B/C across 12 V:
Q = (2.0 µF)(12 V) = 24 µC
VAB = 24/3.0 = 8.0 V
VBC = 24/6.0 = 4.0 V
With C at 0 V and A at 12 V, B is at 4 V. Its connected plates carry -24 and +24 µC, so B has zero net charge, not zero potential. The smaller capacitance has the greater p.d. under this equal-charge condition.
Initially charged capacitors can leave a nonzero net charge on an isolated middle node. Then conserve that given node charge rather than assuming equal magnitudes automatically. The combination rules above use the stated initial and connection conditions.
A mixed arrangement and an energy check
Add a 4.0 µF capacitor directly across A/C, in parallel with the 2.0 µF series equivalent. The complete capacitance is 6.0 µF. At 12 V the added branch has 48 µC, while the series branch still has 24 µC, giving total supplied charge 72 µC.
For an ideal capacitor, stored energy is U = ½CV2. Add each component's energy using its own voltage:
| Arrangement | Component energies / µJ | Total / µJ |
|---|---|---|
| 3 and 6 µF parallel | 216 + 432 | 648 |
| 3 and 6 µF series | 96 + 48 | 144 |
| Series pair plus 4 µF branch | 96 + 48 + 288 | 432 |
Each total also equals ½CequivalentVsupply2. These are final stored energies, not automatically all the energy supplied during charging. An ideal capacitor has no steady conduction through its dielectric; the charging process determines the transient currents and other energy transfers.