Proper Acceleration In Accelerometer ?

AI Thread Summary
The discussion focuses on the concept of proper acceleration as measured by accelerometers, highlighting the distinction between the forces acting on the accelerometer case and the test mass. When an accelerometer is stationary on a table, it outputs 1G due to the normal force acting on the case, while the test mass experiences no deflection from gravity alone. In free fall, both the case and test mass experience the same gravitational force, resulting in a reading of 0G since there is no relative acceleration. The conversation emphasizes that accelerometers measure the specific force acting on themselves, not gravitational forces, which do not cause deflection of the test mass in free fall. The key takeaway is that the internal forces between the case and test mass determine the accelerometer's output, illustrating the complexities of measuring acceleration in different contexts.
Lync
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Hi guys,
I'm working on my project with accelerometer. I know that accelerometer measure specific force or proper acceleration in general by deflection of proof mass.
Proper acceleration is relative to free fall which could be analogy that proper acceleration is the relative acceleration between accelerometer(A) and a free fall object (B) .
+ Case 1: When accelerometer is on a table, it output 1G in Z direction.
proper acceleration Z = m[ F(external) + F(gravity A) - F (gravity B) ] = 1G
=> what is external force that make accelerometer output 1G, is it normal force from the table ?
+ Case 2: When accelerate in +X direction , the proof mass is deflected by fictitious force.
proper acceleration X = m[ F - F(gravity B) which I think is wrong.
The fictitious force make the proof mass deflect in -X direction, how could it output positive value?
Many thanks !



 
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Lync said:
what is external force that make accelerometer output 1G, is it normal force from the table ?
Right.
Lync said:
The fictitious force make the proof mass deflect in -X direction, how could it output positive value?
Same case as for the normal force. Non-gravitational forces always act on the case and not on the test mass. The device "knows" that and flips the sign internally.
 
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Can you give me some glues about non-gravitational force. Normal force and fictitious are non-gravitational force?
As I understand, since normal force is not non-gravitational force , it would not act on test mass. Gravity force is the only force that make it deflect in -Z direction in case accelerometer is on a table. That sound reasonable

mfb said:
Non-gravitational forces always act on the case and not on the test mass.
If the fictitious force is also a non-gravitational, it is not acting on test mass. How can the test mass deflect ?
 
Lync said:
If the fictitious force is also a non-gravitational, it is not acting on test mass. How can the test mass deflect ?

Start by looking at this system from the point of view of an observer who is not accelerating, just watching the accelerometer being accelerated past him. The test mass is trying to move in a straight line at a constant velocity because that's what's inertia says masses do. Meanwhile, the case of the accelerometer is accelerating because it's in the lab which is being accelerated by the 1G force in the +x direction you describe in your post #1 above. The test mass is connected by a spring to the case (because that's how accelerometers work) and as the case accelerates it pulls on the spring; the spring in turn applies a force to the test mass pulling it along with the accelerating case - if it didn't, the inside wall of the case would smash into the test mass. Thus, the test mass is being deflected from straight-line inertial motion by the only force acting on it, namely the very real force from the spring.

The fictitious force appears when we instead look at the system from the point of view of someone who is at rest relative to the accelerating accelerometer. Like the first observer, they see the test mass and the inside wall of the case threatening to smash together, with the collision prevented only by the tension of the spring. However, the test mass is not accelerating under the influence of that force, so they have to invent a fictitious force that appears to be pulling everything in the -x direction to cancel out the force from the spring.
 
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Gravity acts on both case and test mass, it does not influence the result at all. Accelerometers cannot measure gravitational forces.
What they can measure is the force from the table, pushing the accelerometer upwards. That's completely analogous to your hand pushing it sidewards. In both cases the test mass has inertia, so relative to the case (and in this frame) it feels a fictitious force against the direction of the external force.
 
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Lync said:
The fictitious force make the proof mass deflect in -X direction, how could it output positive value?
The accelerometer is measuring acceleration by real contact forces, not by fictitious forces.
 
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mfb said:
Accelerometers cannot measure gravitational forces.
What they can measure is the force from the table, pushing the accelerometer upwards.
I don't understand why accelerometer cannot measure gravitational force while it is the only force that acts on the test mass, causing it to deflect. The normal force acts on the case (housing) only.

So, the ouput acceleration is the acceleration of test mass or the case ? .

Furthermore , I found a lab instruction from UC Berkeley in which they state that :
"An accelerometer measures proper acceleration of itself, which does not necessarily correlate to coordinate
acceleration; to be precise, it measures specific force. An accelerometer can be thought of as a spring and mass
system: coordinate acceleration (meaning the device physically moves in space) results in displacement of
the mass, but because the mass is freely movable, gravity also displaces it. This means that an accelerometer
measures gravity even if the device is not moving in space."
 
Lync said:
I don't understand why accelerometer cannot measure gravitational force while it is the only force that acts on the test mass, causing it to deflect.
Will the test mass be deflected if gravitational force is the only force acting (accelerometer in free fall)?

Lync said:
The normal force acts on the case (housing) only.
Right, for the test mass to be deflected you need such froces that are not acting on everything, propotially to it's mass.
 
A.T. said:
Will the test mass be deflected if gravitational force is the only force acting (accelerometer in free fall)?

yup, it's exactly what I'm wondering.
Gravitational force act all both case and I see that it the only acted on test mass.
Why one is deflected and the other is not ?

I'm undergraduate in Electrical Engineering, I'm not very familiar with these Physics knowledge :(
 
  • #10
Lync said:
yup, it's exactly what I'm wondering.
Well, have you tried to drop the accelerometer to see what it measures in free fall?
 
  • #11
A.T. said:
Well, have you tried to drop the accelerometer to see what it measures in free fall?
yeah, I know that if we drop it in free fall, it will return 0G which means test mass is not deflected.
If we explain it as proper acceleration concept . The relative acceleration between it and frame of reference ( by assume a free fall of object with zero proper acceleration) is zero. The output value is 0 which is totally reasonable.

From my point of view , both cases (on table & free fall) are the same except there is normal force which acts on accelerometer while it is on the table and no other force in free fall. However, this normal force does not act on test mass. So why there is difference in output value ?
 
  • #12
Lync said:
yeah, I know that if we drop it in free fall, it will return 0G which means test mass is not deflected.
If we explain it as proper acceleration concept . The relative acceleration between it and frame of reference ( by assume a free fall of object with zero proper acceleration) is zero. The output value is 0 which is totally reasonable.

From my point of view , both cases (on table & free fall) are the same except there is normal force which acts on accelerometer while it is on the table and no other force in free fall. However, this normal force does not act on test mass. So why there is difference in output value ?
The normal force does not act on the test mass, correct. There is another force that does -- the force from the supports that bind the test mass to the case. That force is monitored by strain gauges.

In free fall, the supports for the test mass are under no strain. When the case is being deflected from a free fall trajectory by an applied force, the supports for the test mass are under a strain because they have to keep the test mass on the same trajectory as the case.
 
  • #13
Lync said:
However, this normal force does not act on test mass. So why there is difference in output value ?
Because there is difference in the internal force between test mass and accelerometer case. Such internal force is required when the external forces alone cannot produce the same acceleration of both parts.
 
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