Equivalent acceleration of an accelerometer

In summary, the conversation discusses the concept of forces and accelerations in inertial and non-inertial reference frames, specifically in the context of an accelerometer. The negative signs in the equations are a result of balancing the inertial force on the test mass with the restoring force of the spring. The output of the accelerometer can be either positive or negative, depending on whether it reports the calculated acceleration or the apparent acceleration in the non-inertial frame. The factor of g also depends on the calibration of the accelerometer.
  • #1
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Hi there,

I am reading this old journal and found this formulaes.

forces on the seismic mass, expressed in inertial reference coordinates, are given by Newton's law as

sum of force in x direction = m * x''
sum of force in y direction = m * y'' = Fy = mg

the equivalent acceleration of the accelerometer are
ax = -F/m = -x''
ay = -F/m = -y'' - g

i am rather concerned with the change in sign direction. i vaguely understand the concept of inertial and non inertial ref frame. but i don't know why it will cause a diff to the axial acceleration. hope to hear from someone.
 
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  • #2
I'm not sure I understand your notation (Fy is force in the y direction, and ax and ay are accelerations in the x and y directions, right? x" is also acceleration in x direction?)

In any case, however, the negative signs probably come from balancing the inertial force on the test mass, which results from the external acceleration that you're measuring, with the restoring force of the spring (assuming that's what supplies the balancing force in the accelerometer) - equal and opposite forces, you know. In other words, if the system is accelerating to the right (positive direction), the mass will swing to the left (negative direction), so it applies a force in the negative direction. If you want to think about the non-inertial frame of the accelerometer, it just means that a tiny observer in that frame would see the mass move to the left and interpret that as a force (and acceleration) to the left.

That's my guess, anyway - it's kind of hard to be sure since you haven't given much explanation.
 
  • #3
this will come to a qn which i have, i have an accelerometer, when i swing it to its positive direction, will it be a positive or a negative output?

so (to be more specific) to a right accelerating accelerometer (positive is right), what should be my output? positive or negative?

>> I'm not sure I understand your notation (Fy is force in the y direction, and ax and ay are accelerations in the x and y directions, right? x" is also acceleration in x direction?)
- Yes.

i guess we can see it when one is a in plane, when it is accelerating, we cannot anticipate/follow up, so we get push back to our seats? the seats gives the 0 opposite force, which is the spring in your explanation?

BUT, the weird thing is the sign of the g. which is -g? in the case of a resting accelerometer, in a inertial ref frame, it should be -1g. but in a non-inertial, it should be +1g? I notice this from a analog devices (crossbow) development board i have.
 
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  • #4
The output can be either - it's just a matter of convention. If the output reports the calculated acceleration on the whole system, then it will be positive (in your example). If it reports the apparent acceleration of the mass in the non-inertial internal system (which is the "raw" information it measures) and leaves you to convert that back to the system acceleration, then it would report a negative (left) acceleration.

Yes, I think you're correct about the plane example: the plane accelerates forward during take-off, but inside, in our non-inertial frame, we feel a force that accelerates us backwards into the seat. We stop when the seat cushion is compressed enough to provide an opposing force equal to the inertial force of our bodies, and if the cushion happened to calibrated to provide a nice measurement of that compression, we could determine the rate of acceleration of the plane.

As for the factor of g, that has to do with whether we're reporting the "sensed" acceleration or the "true" acceleration. This in turn depends on how the accelerometer is calibrated, i.e. under what circumstance does it read 0 vertical acceleration. It could be when it is at rest, i.e. when it senses an acceleration of -g, or it could be when it is actually falling at an acceleration of -g, so it senses no net acceleration.
 

What is equivalent acceleration of an accelerometer?

Equivalent acceleration of an accelerometer is the acceleration that produces the same output voltage as the measured acceleration by the accelerometer. It is usually expressed in units of g (gravity), where 1 g is equal to the acceleration due to gravity on Earth (9.8 m/s²).

How is equivalent acceleration calculated?

Equivalent acceleration is calculated by dividing the measured output voltage of the accelerometer by its sensitivity. The sensitivity is a constant value that is determined by the manufacturer and is expressed in units of volts per g.

Why is equivalent acceleration important?

Equivalent acceleration is important because it allows for the conversion of the output voltage of an accelerometer into a more meaningful and easily understandable unit of acceleration. This is necessary for accurately measuring and interpreting the data collected by the accelerometer.

Can equivalent acceleration be negative?

No, equivalent acceleration cannot be negative. The output voltage of an accelerometer is directly proportional to the acceleration being measured, so a negative equivalent acceleration would indicate a negative acceleration, which is not physically possible.

How does equivalent acceleration differ from actual acceleration?

Equivalent acceleration is a calculated value that represents the acceleration being measured by the accelerometer. Actual acceleration, on the other hand, is the true physical acceleration of an object. The two can differ due to factors such as noise, drift, and other errors in the measurement process.

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