Instrumentation amplifiers, Wheatstone bridge circuits, and the techniques that take a raw sensor signal and make it measurable with confidence.
A standard op-amp rejects common-mode signals imperfectly when built with discrete resistors due to resistor mismatch. The instrumentation amplifier solves this with a three-op-amp architecture where a single external resistor RG sets the gain precisely without affecting CMRR.
Gain (A_d) = 1 + (2R / R_G)
where R is an internal precision resistor (e.g., 24.7 kΩ for INA128)
CMRR (dB) = 20 · log_10(A_d / A_cm)
A good INA: CMRR > 100 dB at DC, > 80 dB at 60 Hz
Common-Mode Rejection Ratio (CMRR) quantifies how well the amplifier rejects a voltage that appears equally on both inputs (e.g., 60 Hz interference from power lines or ground loops). Higher is better. CMRR degrades at higher frequencies.
The INA amplifies only the difference between the two input terminals (V+ − V−). This is the desired sensor signal.
Any voltage present equally on both inputs (noise, ground offset). The INA suppresses this. CMRR = 20·log(A_d / A_cm).
INAs include clamping diodes and series resistors to protect against overvoltage on the input pins from sensor cable transients.
A small DC error voltage at the input. Multiplied by gain, it appears at the output. Reduced by trimming or choosing a low-offset INA.
A Wheatstone bridge converts a small resistance change (from a strain gauge, RTD, or thermistor) into a measurable voltage. A balanced bridge (all arms equal) produces zero output. A resistance change in one or more arms produces a differential output proportional to that change.
V_out = V_ex · [ R_4/(R_3+R_4) − R_2/(R_1+R_2) ]
For a quarter-bridge (one active arm, gauge factor G_f, strain ε):
ΔR/R = G_f · ε
V_out ≈ V_ex · (G_f · ε) / 4 (for small ΔR/R)
For remote installations, the resistance of lead wires adds to the gauge resistance and changes with temperature. A 3-wire connection moves one lead wire into each of two adjacent bridge arms, so their resistances cancel in the bridge output. A 4-wire Kelvin connection completely separates force-current and sense-voltage paths.
Constant-voltage excitation is simpler and most common. Self-heating error exists because power dissipated in the gauge = Vex² / (4R). Constant-current excitation eliminates self-heating variation with resistance change but requires a precision current source. The choice depends on gauge resistance, thermal conductivity of the substrate, and required accuracy.
A_d = 1 + 2R/R_G → R_G = 2R / (A_d − 1) = 2(24700) / (100 − 1) = 49400 / 99 ≈ 499 Ω
R_G ≈ 499 Ω (use standard 499 Ω 1% resistor)
V_out = V_ex · (G_f · ε) / 4 = 5.0 × (2.05 × 800×10&sup-⁶) / 4
= 5.0 × 0.001640 / 4 = 5.0 × 0.000410 = 0.00205 V
V_out ≈ 2.05 mV
CMRR = 20 · log10(200 / 0.001) = 20 · log10(200,000) = 20 × 5.301 = 106 dB
CMRR = 106 dB (excellent)