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Power Plane Cavity Resonance Calculator

Plane-pair cavity modes analytical
Cavity modes up to the chosen frequency

Two parallel planes are a cavity. When a plane's length is a whole number of half wavelengths, a standing wave builds up between its edges and the plane pair's impedance peaks. Those peaks are where power-plane noise and edge radiation concentrate — and where decoupling has the hardest job.

Reading the numbers

Every value is in the address bar as you change it, so a link reproduces the calculation exactly. Type values with SI prefixes — 100n, 2.2p, 16G — or drag the sliders; a bare number keeps the prefix already shown.

The formulas

fm,n = ( c / 2√Dk ) · √( (m/a)² + (n/b)² ) Magnetic-wall edges: the plane edges are open, so the voltage is at a maximum there.
Go deeper — assumptions, how it is checked, and sources

Assumptions. A bare rectangular cavity with open edges. Fringing at the edges lowers every mode slightly; the planes' own loss, and any capacitors or vias across them, damp the peaks and shift them. The cavity is thin compared with a wavelength, so only the in-plane modes exist.

How it is checked. An air-filled 150 mm plane has its first mode at exactly c/2a; a square plane has (1,0) and (0,1) at the same frequency and (1,1) at √2 times it; and (2,0) is exactly twice (1,0).

Source. G.-T. Lei, R. W. Techentin and B. K. Gilbert, “High-frequency characterization of power/ground-plane structures,” IEEE Trans. Microwave Theory Tech., vol. 47, no. 5, 1999.

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