In a strain-gauge–based strain measuring device, what is the practical output quantity of the measurement chain?

Introduction / Context:
Electrical resistance strain gauges convert mechanical strain into a change in electrical resistance. In practical instruments, this resistance change is most often measured via a Wheatstone bridge, producing a voltage output proportional to strain. Understanding both the transducer variable and the instrumented output clarifies how sensors interface with data-acquisition systems.

Given Data / Assumptions:

• The strain gauge element itself changes resistance ΔR/R ≈ kε, where ε is strain and k is gauge factor.
• Instrumentation frequently uses a bridge excited by a stable voltage, yielding a small differential voltage proportional to ΔR.
• Some simple setups may read resistance directly with ohmmeters for static tests.

Concept / Approach:
The primary transducer output is a resistance change. However, the practical system output (what the user reads) is typically a voltage after the bridge and amplifier. Thus, depending on the readout configuration, one may report either resistance (raw sensor) or voltage (conditioned signal).

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