Sensors & Measurement · Study deck
Bridge Linearity and Instrumentation
Picture a strain gauge that changes slightly while its display stays at zero.
Physics Phoebe is your guide for this deck.
After studying this chapter
Learning objectives
You will be able to:
- Explain why bridge circuits cancel large sensor baselines before amplification.
- Estimate quarter-bridge output voltage from gauge factor, strain, and excitation voltage.
- Choose instrumentation-amplifier gain from the worst-case differential signal and ADC range.
- Use common-mode rejection and dummy gauges to suppress cable noise and thermal drift.
Major section
Start With the Measurement Story
An analog-to-digital converter is the circuit that turns a measured voltage into a digital number.
- This proves one measurement chain and range, not every installation; the deeper sections cover bridge balance, linearity, gain, common-mode limits, and calibration.
- A bridge circuit can reveal a tiny physical change, but only if the weak differential signal survives imbalance, noise, and loading.
- The long folded track is the active element: bonding it to the test surface makes strain lengthen or compress that path, producing a very small resistance change.
Major section
Tiny Signals on Large Baselines
The Wheatstone bridge subtracts a matched reference so that, at rest, the output is zero and only the change appears as a small differential voltage.
- Intuition: the bridge is two voltage dividers side by side.
- In a single divider with another 350 Ω resistor, the midpoint sits near 2.500 V.

Major section
Tiny Signals on Large Baselines (continued)
A simple half-bridge divider is not globally linear.
- As |DeltaR| grows relative to R + R0, the quadratic and higher-order terms stop being negligible.
- A real part makes the gain concrete.
- The AD620 instrumentation amplifier sets its gain with one external resistor: G = 1 + 49.4 kΩ / RG.
Major section
CMRR and Thermal Cancellation
The wanted signal is the difference between the two bridge midpoints.
- It amplifies the difference and rejects the common-mode part.
- A quick noise budget shows why common-mode rejection matters.
- With a plain single-ended amplifier at gain 100, the noise would try to become 10 V and would slam the output into a rail.
Deck summary
Key takeaways
An analog-to-digital converter is the circuit that turns a measured voltage into a digital number.
- The Wheatstone bridge subtracts a matched reference so that, at rest, the output is zero and only the change appears as a small differential voltage.
- A simple half-bridge divider is not globally linear.
- The wanted signal is the difference between the two bridge midpoints.
Retrieval practice
Recall check 1 of 4

Physics Phoebe says: answer from memory, then check your reasoning.
Q1Why is a Wheatstone bridge preferred over a single voltage divider for a strain gauge whose resistance changes by only about 0.1%?
Show answer
Answer: B Cancelling the baseline first lets the amplifier and ADC work on the small differential signal instead of the offset.
Retrieval practice
Recall check 2 of 4

Physics Phoebe says: answer from memory, then check your reasoning.
Q2A quarter-bridge with GF = 2.0 and Vex = 5 V is loaded to 500 microstrain. Approximately what raw bridge output (before amplification) should you expect?
Show answer
Answer: A ΔR/R = 2.0 × 0.0005 = 0.001, and Vout = 5 × 0.001 / 4 = 1.25 mV.
Retrieval practice
Recall check 3 of 4

Physics Phoebe says: answer from memory, then check your reasoning.
Q3A bridge can produce 3.75 mV at overload and feeds an ADC limited to 3.3 V. Which is the highest safe gain listed?
Show answer
Answer: B 500 × 3.75 mV = 1.875 V, below the 3.3 V ADC limit.
Retrieval practice
Recall check 4 of 4

Physics Phoebe says: answer from memory, then check your reasoning.
Q4A long cable runs from a bridge sensor to its amplifier and picks up 50 Hz mains hum on both conductors equally. Why does an instrumentation amplifier suppress this interference?
Show answer
Answer: C Interference shared by both wires is common-mode and is rejected; only the differential signal is amplified.
Print reference
Answers
Answer key.
- B · Cancelling the baseline first lets the amplifier and ADC work on the small differential signal instead of the offset.
- A · ΔR/R = 2.0 × 0.0005 = 0.001, and Vout = 5 × 0.001 / 4 = 1.25 mV.
- B · 500 × 3.75 mV = 1.875 V, below the 3.3 V ADC limit.
- C · Interference shared by both wires is common-mode and is rejected; only the differential signal is amplified.