MethodWhat is calculated?
The bridge is two voltage dividers on the same excitation; the output is the difference of the two divider voltages. Hence equal-sign resistance changes in adjacent arms cancel while those in opposite arms add. For small changes eq. 4.1 reduces to the linearised basic equation 4.6.
Equations
U_M/U_B = R₁/(R₁+R₂) − R₄/(R₃+R₄) (Keil Gl. 4.1)
Abgleich: R₁/R₂ = R₃/R₄
R_in = (R₁+R₂)‖(R₃+R₄)
LimitsAssumptions and typical mistake
Constant-voltage excitation and an unloaded measuring diagonal (high-impedance amplifier input). Constant-current excitation or a low-impedance load require different relations.
Assigning the arms incorrectly: R₂ and R₄ are adjacent to R₁, R₃ is opposite; swapping flips the sign.
InputsWhat you enter – and where the values come from
- Resistance R₁ [Ω]
- Resistance of the first bridge arm. In strain-gauge measurements this is usually the active gauge at its actual loaded value: unloaded nominal resistance plus resistance change. Source: precision-ohmmeter measurement or the resistance-change-from-strain calculator.
- Resistance R₂ [Ω]
- Resistance of the arm forming the first voltage divider with R₁ (‘adjacent’ to R₁). In a half bridge the second gauge or compensation gauge, in a quarter bridge a fixed resistor in the instrument. Source: nominal value or measurement.
- Resistance R₃ [Ω]
- Resistance of the arm diagonally opposite R₁. Changes here act in the same direction as at R₁. Source: nominal value or measurement; in the instrument a precision resistor for quarter/half bridges.
- Resistance R₄ [Ω]
- Resistance of the fourth arm (forms the second divider with R₃, ‘adjacent’ to R₁); in a quarter bridge a fixed resistor in the instrument. Source: nominal value or measurement.
- Excitation U_B [V]
- The bridge excitation is the DC or AC voltage with which the amplifier supplies the bridge circuit. The signal is proportional to it – which is why signals are usually stated as a ratio in mV/V and the excitation is only needed for the absolute signal voltage. Source: amplifier setting, usually 2.5 V, 5 V or 10 V; the upper limit is set by gauge self-heating (see the excitation calculator).
ContextWhat this calculator is for
Checking zero errors caused by resistance tolerances, sizing balancing resistors and verifying the signal a resistance standard produces in one arm.
What comes next
- Enter all four arm resistances including lead contributions.
- Enter the excitation and read the output voltage.
- Vary one resistance to reproduce balance or a defined unbalance.
SourceTechnical basis
Keil, Dehnungsmessstreifen, 2nd ed. 2017, secs. 4.1–4.2, eqs. (4.1)–(4.6).
The source supports the equation structure and worked examples; this calculator does not replace calibration of the measuring chain.
FAQFrequently asked questions
How does this differ from the balanced-bridge calculator?
There an unknown resistance is found from balance; here the output of the deliberately unbalanced bridge is computed, as used in strain-gauge measurement.
Why is the signal given in mV/V?
Because U_M is proportional to U_B; the ratio characterises the bridge independently of the excitation.
Is the output linear in ΔR?
Only approximately; with one active arm eq. 4.7 gives an error equal in size to the strain itself.
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