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Yes. An accelerometer can measure small acceleration signals when its selected measurement range includes the expected peaks and its resolution and noise are good enough to distinguish the signal. It also responds to gravity: a stationary sensor measures the portion of gravity acting along each axis, which is why accelerometers can measure tilt.

What “low-g” means for an accelerometer

Low-g describes the acceleration range you need to measure, not a separate sensing principle. The right device is one whose configured full-scale range covers the signal without sacrificing the sensitivity required for the measurement.

For example, the NXP MMA6361L offers selectable ±1.5 g and ±6 g ranges, while the Analog Devices ADXL203 offers ±1.7 g, ±5 g and ±18 g ranges. Vernier’s LGA-BTA covers −5 g to +5 g. These examples show why “low-g accelerometer” alone is not a sufficient specification: the useful range depends on the expected acceleration and the device’s noise and resolution. NXP MMA6361L datasheet; Analog Devices ADXL203 datasheet; Vernier LGA-BTA specifications

Why a stationary accelerometer reads gravity

Inside a MEMS accelerometer, a suspended proof mass shifts in response to acceleration. Electronics convert that shift into a voltage or digital reading. Gravity is an input to the sensor, not something it automatically removes: a stationary sensor reports gravity’s projection along its sensing axes. Rotate the sensor and those projections change, providing the basis for tilt measurement.

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The Analog Devices ADXL203 is specified for both dynamic acceleration, including vibration, and static acceleration, including gravity. Its product information says that with narrow bandwidths below 60 Hz, its typical noise floor permits signals below 1 mg to be resolved. The ADXL330 also measures static gravity for tilt sensing, as well as motion, shock and vibration; its minimum full-scale range is ±3 g. ADXL203 datasheet; ADXL330 datasheet

An accelerometer does not inherently distinguish tilt from other acceleration. If the sensor is moving, its reading combines gravity with that motion. Tilt derived from gravity is most useful when dynamic movement is limited or when filtering and other processing can separate the effects.

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Range, resolution and noise are different

Full-scale range is the interval over which the sensor can report acceleration accurately. Resolution describes the smallest change represented by its output, while noise determines how much random variation obscures small changes. A wide range helps accommodate larger peaks, but often provides fewer output counts per unit of acceleration. A narrower range can make small changes easier to discern, provided the signal never exceeds that range.

Bosch Sensortec’s BMA422, for example, has programmable ±2 g, ±4 g, ±8 g and ±16 g ranges. It specifies 12-bit resolution, 0.98 mg resolution in its ±2 g range, and typical noise density of 140 µg/√Hz. These figures describe different properties: the selected range, the output granularity and the noise level. Bosch Sensortec BMA422 product page

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What happens when acceleration exceeds the selected range?

The output saturates at the measurement limit, so it no longer accurately represents the acceleration beyond that point. Saturation is not, by itself, proof that the sensor has been damaged. Survival depends on separate absolute-maximum and shock specifications; check those ratings for the specific device and application. Analog Devices explains the distinction in its measurement-range versus absolute-maximum guidance.

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How to choose a sensor for tilt or low vibration

Start with the largest acceleration the device will experience, including movement, mounting effects and brief peaks. Select the smallest full-scale range that safely contains those peaks, then check whether noise and resolution allow the signal of interest to be measured. A narrow range is not useful if ordinary movement clips the output.

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  • For tilt: pay close attention to zero-g offset and its drift, noise and temperature stability. These can affect the inferred angle; a high shock range alone does not make a sensor suitable.
  • For vibration: check bandwidth and noise density against the frequency and amplitude of the vibration you need to capture.
  • For either use: verify full-scale range, resolution, temperature range, cross-axis sensitivity, number of axes, interface, supply voltage, power, package, calibration and shock or over-range limits.

Vernier’s LGA-BTA is an educational sensor with a −5 g to +5 g range, ±0.5 m/s² accuracy, 0–100 Hz frequency response and 0.037 m/s² typical resolution. Vernier also describes it as suitable for sensing gravity and use as an inclinometer, with angle measurements to the nearest degree. Those are the manufacturer’s published specifications; whether they suit a particular experiment depends on its required range, accuracy and bandwidth. Vernier LGA-BTA product page

For an embedded design, the Bosch BMA422 is one digital MEMS example, while the ADXL203 is an example with selectable ranges and a published low-noise capability at narrow bandwidth. Compare the specifications for the actual operating conditions rather than choosing by the “low-g” label alone.

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