Short notes

Transducers Short Notes

Connect a PT100 RTD to a Wheatstone bridge and as temperature rises from 0°C to 100°C the resistance changes from 100 Ω to 138.5 Ω — that 38.5 Ω change is the PT100 converting a physical quantity (temperature) into an electrical signal. That conversion, in either direction, is what the word transducer means in your instrumentation exam.

EEE, EI

How it works

Active transducers generate their own EMF without an external power supply — thermocouples (Type K: Chromel-Alumel, ~41 µV/°C), piezoelectric crystals (quartz under stress), and photovoltaic cells fall here. Passive transducers need excitation: RTDs, strain gauges (GF ≈ 2 for metallic foil, 50–150 for semiconductor), LVDTs, and capacitive sensors. Dynamic characteristics matter for fast signals: rise time, time constant τ (for a first-order sensor like RTD in water, τ ≈ 5–10 s), and frequency response. Sensitivity = output change / input change, e.g., 41 µV/°C for Type K thermocouple.

Key points to remember

Key performance specs examiners test: sensitivity, resolution (smallest detectable change), accuracy, precision, hysteresis, repeatability, and linearity. A bonded metallic strain gauge at 120 Ω with gauge factor GF = 2 gives ΔR/R = GF × ε; for a strain ε = 500 µε, ΔR = 120 × 2 × 500×10⁻⁶ = 0.12 Ω. Thermocouples need cold junction compensation because the reference junction must be at a known temperature. Piezoelectric transducers cannot measure static (DC) pressures because charge leaks away — they are suitable only for dynamic measurements above a few Hz.

Exam tip

The examiner always asks you to compare active vs passive transducers with two examples each — thermocouples and piezoelectric for active, RTD and strain gauge for passive is the safest answer.

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