Bridged-T attenuator in level control and audio/RF chains
A bridged-T attenuator uses four resistors arranged as a T-network with a “bridge” resistor across the series arms. Properly designed, it can provide adjustable or fixed attenuation while keeping the input and output impedance nearly constant.
Compared with simple series pads, the bridged-T topology is often used in:
- Precision stepped attenuators for test equipment
- Audio line-level controls with constant load impedance
- RF level pads where impedance matching must be preserved
- Multi-stage attenuator ladders in measurement front-ends
Topology and resistor roles
A bridged-T network can be visualized as:
- Two series resistors in the main signal path (Rs1 and Rs2)
- One shunt resistor to ground at the junction of the series arms (Rsh)
- One bridge resistor connecting input and output nodes (Rb)
When the values are chosen according to the desired attenuation and system impedance Z0, the input and output both “see” approximately Z0 over the operating band.
Attenuation and impedance targets
For a symmetrical bridged-T attenuator in a system with characteristic impedance Z0 and target attenuation AdB, the key design goals are:
- Input impedance ≈ Z0
- Output impedance ≈ Z0
- Voltage attenuation = AdB at the design frequency
Let the voltage attenuation ratio be:
K = 10(AdB / 20)
The calculator uses standard bridged-T design equations to solve for the four resistor values so that both impedance and attenuation criteria are satisfied for the specified Z0 and K.
Advantages of bridged-T over simple pads
While simpler π or T pads are often sufficient, the bridged-T network offers useful benefits in some applications:
- Better constant-impedance behavior across a range of switched settings when used in stepped attenuators.
- Reduced insertion loss variation when stages are cascaded, maintaining more predictable gain structure.
- Convenient implementation of high-attenuation steps without excessively large resistor ratios.
In many audio and measurement systems, multiple bridged-T sections are combined on rotary switches to form accurate, low-distortion level controls.
Using the Bridged-T Attenuator Calculator
- Enter the system impedance: Specify Z0 according to your line or load (e.g. 50 Ω RF, 75 Ω video, 600 Ω legacy audio).
- Set the desired attenuation: Enter AdB in decibels for the attenuation you require at that stage.
- Read the resistor values: The calculator outputs values for Rs1, Rs2, Rsh and Rb for a constant-impedance bridged-T network.
- Map to real components: Choose the nearest standard resistor values and check the resulting attenuation and impedance with a simulator or measurement if high accuracy is required.
Worked example – 20 dB bridged-T in a 50 Ω system
- Z0 = 50 Ω
- AdB = 20 dB → K = 10(20/20) = 10
With these inputs, the calculator determines a set of resistor values such that:
- The input and output both measure close to 50 Ω
- The through signal is attenuated to 1/10 of its original voltage (1/100 in power)
- Power is shared among the resistors according to their position in the network
You can then round the results to preferred values (E24/E96 series), recalculate the exact attenuation, and choose resistor power ratings appropriate to the maximum signal level.
Design tips for bridged-T attenuators
- Start with realistic attenuation steps: Common step sizes are 1 dB, 2 dB, 3 dB, 6 dB, 10 dB and 20 dB. Extremely high or very small steps may require tight-tolerance parts.
- Consider total chain loss: In a multi-stage ladder, overall insertion loss adds up. Plan the gain structure so upstream and downstream stages remain in their linear region.
- Check power dissipation: For RF or line-level applications, calculate the power in each resistor at maximum level, and specify adequate wattage and thermal management.
- Layout matters at high frequency: Keep leads short, minimize stray capacitance and inductance, and respect the characteristic impedance of the PCB or coaxial environment.
With the bridged-T attenuator calculator, you can move directly from target attenuation and line impedance to practical resistor values, making it easier to construct accurate step pads, gain trims and level controls for RF, audio and test systems.