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Zobel network and L-pad calculator

Two small networks almost every passive crossover needs: the Zobel network flattens a driver's impedance rise, the L-pad lowers the level of a tweeter that is too loud – without the amplifier seeing a different load.

Zobel network

Ω
mH
PartPositionValue
R1in series (R + C), across the driver5.6 Ω
C1in series (R + C), across the driver12 µF

Formulas

R = Re
C = Le / Re²
Simulate in Crover with real measurements

Opens a new project with exactly this circuit. Works as a guest without an account; then load your drivers' FRD/ZMA.

L-pad

dB
Ω
PartPositionValue
R1in series (R1)2.4 Ω
R2across the driver (R2)20 Ω

50 % of the power for this driver turns into heat in the resistors – choose R1's power rating accordingly.

Formulas

k = 10^(dB / 20)
R1 = Z · (k − 1) / k   (in series)
R2 = Z / (k − 1)   (across the driver)
Simulate in Crover with real measurements

Opens a new project with exactly this circuit. Works as a guest without an account; then load your drivers' FRD/ZMA.

Zobel network

Above resonance the voice coil acts like a resistance Re with an inductance Le in series – the impedance rises with frequency. An R-C branch with R = Re and C = Le/Re² across the driver turns this into a constant resistance Re on paper (Zobel's constant-resistance network). A crossover calculated for Re then works as it should.

Re and Le are in the datasheet – but Le is often given at 1 kHz only. Estimated from an impedance measurement (ZMA), the value fits the crossover region better; Crover's Zobel tool in the editor does that for you.

L-pad

An L-pad is one resistor in series and one across the driver. Sized right, the amplifier still sees the impedance Z while the driver gets less voltage. The formula assumes a constant impedance – on a real tweeter with a resonance peak, the shunt resistor also changes the Q of the high-pass.