Rx = RN · R₁ / R₂
At null balance the bridge midpoints have equal potential, giving Rx = RN·R₁/R₂.
At null balance the bridge midpoints have equal potential, giving Rx = RN·R₁/R₂.
Select a target and calculate.
At null balance the bridge midpoints have equal potential, giving Rx = RN·R₁/R₂.
RN=100 Ω, R₁=150 Ω and R₂=100 Ω give Rx=150 Ω at null balance.
Ideal DC null balance; lead, contact and self-heating errors and residual bridge voltage are excluded.
This calculator determines an unknown resistance from a true Wheatstone-bridge null balance. It is useful for learning the balance condition and evaluating a laboratory setup.
At balance no current flows through the null detector because both bridge midpoints have equal potential. Rx then depends only on reference RN and ratio R₁/R₂, not on supply voltage or detector resistance.
Rx = RN · R₁ / R₂
Rx = RN · R₁ / R₂Balance condition: UAB = 0| Symbol / input | Meaning |
|---|---|
| Unknown resistance Rx | Resistance in the measurement arm after the null detector shows zero bridge current. |
| Reference resistance RN | Known, sufficiently accurate reference resistor in the opposite bridge arm. |
| Ratio resistor R₁ | Known resistor on the same potential side as Rx; its ratio to R₂ sets the measurement factor. |
| Ratio resistor R₂ | Known resistor in the second ratio arm; never enter zero. |
RN is the known reference resistor. R₁ and R₂ are the ratio arms and their labels must match the actual circuit. Use calibrated values or the bridge-wire reading at the exact null position.
Energise the bridge, adjust R₁/R₂ until diagonal current is zero, then enter RN, R₁ and R₂. Rx is valid only for that balanced setting.
RN=100 Ω, R₁=150 Ω and R₂=100 Ω give Rx=150 Ω.
Rx scales directly with RN and R₁ and inversely with R₂. Swapping the ratio arms therefore inverts the intended measurement factor.
All quantities are resistances; mixed Ω, kΩ and MΩ inputs are converted internally.
Resistance measurement labs, strain-gauge and temperature-sensor bridge balancing, and plausibility checks of classical null methods.
Only a balanced DC bridge is evaluated. An unbalanced bridge needs an output-voltage model; AC bridges require complex impedances and phase balance.
Common mistake: Do not calculate while the detector still deflects. Trace the actual circuit labels for R₁ and R₂ instead of guessing from drawing position.
Resistance measurement labs, strain-gauge and temperature-sensor bridge balancing, and plausibility checks of classical null methods.
RN is the known reference resistor. R₁ and R₂ are the ratio arms and their labels must match the actual circuit. Use calibrated values or the bridge-wire reading at the exact null position.
Only a balanced DC bridge is evaluated. An unbalanced bridge needs an output-voltage model; AC bridges require complex impedances and phase balance.