# [Maxwell Bridge Calculator](https://blog.hirnschall.net/tools/maxwell-bridge/)

author: [Sebastian Hirnschall](https://blog.hirnschall.net/about/)

meta description: Calculate unknown inductance and series resistance from a balanced Maxwell-Wien bridge. Enter R2, R3, R4, C4 at null; L_x, R_x, and Q are computed.

meta title: Maxwell Bridge Calculator — Inductance and Series Resistance

date published: 11.05.2026 (DD.MM.YYYY format)
date last modified: 11.05.2026 (DD.MM.YYYY format)

---

Calculator
----------

Enter the four bridge components at balance. The unknown inductance \( L\_x \) and its series resistance \( R\_x \) are calculated from the balance conditions. Providing the test frequency also yields the quality factor \( Q \).

* R2 (ratio arm):
* Ω
  kΩ
  MΩ

* R3 (ratio arm):
* Ω
  kΩ
  MΩ

* R4 (standard arm, variable):
* Ω
  kΩ
  MΩ

* C4 (standard arm, parallel with R4):
* µF
  nF
  pF

---

* Test frequency (f) — optional:
* Hz
  kHz

Enter all four bridge components to calculate.

Calculate



Maxwell Bridge — Explanation
----------------------------

The Maxwell bridge (more precisely the Maxwell-Wien bridge) is an AC bridge circuit used to measure the inductance and series resistance of an unknown inductor. It places the unknown inductor \( L\_x \) with its winding resistance \( R\_x \) in one arm, balances it against a known capacitor in an adjacent arm, and reads off \( L\_x \) and \( R\_x \) directly from the values of the calibrated components at null.

The bridge has four arms. The unknown arm contains \( L\_x \) in series with \( R\_x \). The opposite arm (the standard arm) contains a known resistor \( R\_4 \) in parallel with a known capacitor \( C\_4 \). The two remaining arms are plain resistors \( R\_2 \) and \( R\_3 \). An AC source drives one diagonal and a null detector (galvanometer or oscilloscope) monitors the other.

Balance Conditions
------------------

At balance, no current flows through the detector. Setting the complex impedance products of opposite arm pairs equal and separating real and imaginary parts gives two independent equations:
\[
L\_x = R\_2 \cdot R\_3 \cdot C\_4
\]
\[
R\_x = \frac{R\_2 \cdot R\_3}{R\_4}
\]
These two conditions are independent of frequency, which is one of the key practical advantages of the Maxwell bridge: the source frequency does not need to be known precisely. The ratio arms \( R\_2 \) and \( R\_3 \) always appear as a product, so only their product \( R\_2 R\_3 \) matters — in practice one is often kept fixed while the other is adjusted in decade steps to set the range.

The quality factor of the measured inductor at the test frequency \( f \) is:
\[
Q = \frac{\omega L\_x}{R\_x} = \omega C\_4 R\_4
\]
where \( \omega = 2\pi f \). \( Q \) can be read directly from the standard arm components once the bridge is balanced.

Valid Q Range
-------------

The Maxwell bridge works well for medium-Q inductors, typically in the range \( 1 \leq Q \leq 10 \). Outside this range, balance becomes difficult to achieve because the real and imaginary balance conditions become nearly dependent, making the null hard to locate. For high-Q inductors (\( Q > 10 \)) the Hay bridge is the better choice: it uses a capacitor in series rather than parallel with \( R\_4 \), which suits high-Q measurements naturally. The calculator outputs a warning when the computed Q falls outside the useful range.

Purpose of the Calculator
-------------------------

In a physical measurement, the bridge is brought to null by adjusting the variable components (typically \( R\_4 \) for the resistive balance and \( R\_3 \) or \( C\_4 \) for the reactive balance). Once the detector reads zero, the component values at that point are entered here to recover \( L\_x \) and \( R\_x \). No frequency measurement is needed for \( L\_x \) and \( R\_x \); frequency is only required if Q is also wanted.

The formulas can also be rearranged for component selection when designing a bridge for a target inductance range. Fixing \( C\_4 \) and choosing \( R\_2 R\_3 = L\_x / C\_4 \) sets the inductance scale, and choosing \( R\_4 = R\_2 R\_3 / R\_x \) sets the resistance scale.

Related Tools
-------------

* [Schering Bridge Calculator](https://blog.hirnschall.net/tools/schering-bridge/) — the capacitive equivalent: measures unknown capacitance and dissipation factor.
* [Wheatstone Bridge Calculator](https://blog.hirnschall.net/tools/wheatstone-bridge/) — DC bridge for measuring unknown resistance.
* [Inductor Impedance Calculator](https://blog.hirnschall.net/tools/inductor-impedance/) — compute \( X\_L \) and \( |Z| \) from the measured \( L\_x \) and \( R\_x \).
* [Inductor Energy Calculator](https://blog.hirnschall.net/tools/inductor-stored-energy/) — compute the energy stored in the measured inductor at a given current.

More calculators: [blog.hirnschall.net/tools/](https://blog.hirnschall.net/tools/).