Adjacent corners of a square loop: the short edge plus the long detour
Four equal capacitors in a ring, with P and Q on neighbouring corners. One route is the single edge between them; the other is the rest of the loop in series. They run in parallel.
Four capacitors, each \(1\,\mu\text{F}\), are connected in a square as shown. Find the equivalent capacitance between P and Q.
- Each capacitor1 μF
- Count4 (square ring)
- CornersP · Q · M · N
- TerminalsP–Q (adjacent)
The equivalent capacitance \(C_{PQ}\) across the two adjacent corners P and Q.
A ring gives two parallel routes between any two terminals. From P to Q:
Short route — the single capacitor on the bottom edge, \(1\,\mu\text{F}\).
Long route — the other three capacitors (left, top, right) in series: \(P\!-\!N\!-\!M\!-\!Q\). Three \(1\,\mu\text{F}\) in series give \(\tfrac{1}{3}\,\mu\text{F}\).
Same endpoints, so the two routes add in parallel.
- Long route (series of three). $$\frac{1}{C_{long}}=\frac{1}{1}+\frac{1}{1}+\frac{1}{1}=3 \;\Rightarrow\; C_{long}=\frac{1}{3}\,\mu\text{F}$$
- Add the short route (parallel). $$C_{PQ}=1+\frac{1}{3}=\frac{4}{3}\,\mu\text{F}$$
Equal-C square, adjacent corners → \(C+\tfrac{C}{3}=\tfrac{4C}{3}\). With \(C=1\): straight to \(\tfrac{4}{3}\). (Diagonal corners would instead give \(C\) — worth keeping both in your pocket.)
Sanity: the answer must beat the single direct edge (1 μF) but only slightly, since the detour adds just \(\tfrac13\). That rules out the inflated 4 and the too-small 1/4, 3/4.
Direct edge 1 μF in parallel with the three-in-series detour \(\tfrac13\) μF:
$$C_{PQ}=1+\frac{1}{3}=\frac{4}{3}\,\mu\text{F}$$