Accelerometers
Root Hertz                                                                                                                                                      Selection Table for Analog Devices accelerometers

Acceleration is unlikely to be constant over an extended period, thus it forms either a short-lived fast varying signal or an alternating signal. Therefore one of the most important characteristics of an accelerometer is its frequency performance.

Basic Concepts

Acceleration = d2x/dt2 = dv/dt;
where velocity, v=dx/dt.
x is the linear displacement in metres and v is the linear velocity in metres per second.

In addition one can measure angular acceleration defined by
Ang_Accn = dw/dt where w (omega) is the angular velocity in rad/s.

For each of the axes in three dimensions, this corresponds to the three linear and three angular accelerations, for a total of six acceleration components. Typically angular acceleration is measured using linear accelerometers at know positions relative to the rotational axis of interest.

In general, accelerometers sense acceleration by using a proof mass or seismic mass, and by measuring the displacement of this mass.

mass-spring-damper
                text




An important parameter for accelerometers is the noise power. This is actually its power density spectrum - a measure of how the noise power contributed by individual frequency components is distributed over the frequency spectrum. It should be measured in watts/Hz; however the accepted practice is to use amplitude-squared as the unit of power. For electrical signals this gives units of volts-squared/Hz, or more commonly expressed as volts/root-Hertz.



If you have any questions or want further information,

please contact Professor R.B.Yates at R.Yates@mems.org.uk

©2002 R.B.Yates All rights reserved.