Circuit Response
every model has an edge, and the figure carries it
Concept

Ladder network — where it appears

A chain of alternating series and shunt elements, each section loading the one before it. Filters, attenuators and matching networks are ladder networks, and their response is the product of the sections' chain matrices taken in order.

Named by 2 essays across 2 fields — each of them below, with the objects they name alongside it.

The best reference is the middle of the chain below 2.37 kHz and ground above it — the node the capacitors return to. computed by solving, not by drawing. The condition number of the nodal matrix of an 8-section RC ladder — 1 kΩ in series, 10 nF and 1 MΩ to ground at each node — solved at s = jω with each of its 10 nodes in turn called zero, against frequency. Drawn: ground, the input, the middle node and the far end; the others lie between. At direct current n4 is best, near the middle as the earlier resistor chain found; from 2.37 kHz ground is — well below a single section's 15.9 kHz corner, where each capacitor's admittance is already 0.15 of a series resistor's conductance, and all 8 together about 1.2 of one.

The reference a sweep should keep

At direct current the best node to call zero in a resistor chain is its middle. Put a capacitor to ground at each node and solve at s = jω, and the best reference moves: the middle of an eight-section RC ladder below 2.37 kHz, ground above it, where every capacitor returns. So a solver that chooses its reference once for a whole sweep is choosing wrongly somewhere, as the earlier essay suspected — but the two wrong choices are not alike. Kept for the whole sweep, ground is never worse than 1.27 times the best condition number, a tenth of a digit. The middle node, best at direct current and kept, is 143 times worse at a megahertz, 2.2 digits. A fifth-order LC filter says the same: ground within 2.18 times throughout.

networks · Nodal analysis Over ±25% of the centre, three elements deliver 97.3% at worst; Bode and Fano allow 99.8%. computed by solving, not by drawing. The fraction of the available power a source of 2 times its resistance in inductive reactance delivers to a resistive load through the best matching network of 0, 1, 2 and 3 reactive elements for a band of ±25 per cent about the centre, each network the one whose worst transfer in the band is largest; the vertical lines mark the band. The worst in-band transfer is 54.2%, 82.8%, 89.5%, 97.3%; the Bode–Fano limit for any lossless network, reached only with infinitely many elements, is 99.81%.

What each element buys against the limit

A source whose resistance sits behind twice as much inductive reactance can deliver, over ±25 per cent of its centre frequency, 54.2 per cent of its available power to the best plain resistor and at worst 82.8 per cent through the best single capacitor. That single-element answer is exactly the fixed load for an uncertain reactance: the capacitor makes the reactance swing ±1 across the band and the load is √2 times the source. Two elements lift the worst case to 89.5, three to 97.3, and a fourth, in a chain of single elements, to 97.4. Bode and Fano bound every lossless network at 99.81 per cent over that band — a limit three elements come within a tenth of a decibel of and no finite network reaches.

power · Power transfer

Named alongside it

The objects these essays reach for when they reach for this one.

BandwidthBode–Fano limitCondition numberFrequency responseImpedance matchingMaximum power transferMinimaxModified nodal analysisNumerical errorReactanceReference node

All concepts