# Accelerometer – Inertia Example Problem

An accelerometer is a device to measure acceleration. One of the simplest accelerometers is a small mass hanging from a thin rod or string that can pivot freely as a body accelerates. As the body containing the accelerometer accelerates one direction, the freely hanging weight will swing in the opposite direction. How far it swings is an indication of how much the body accelerates. This example problem shows how to use an accelerometer to determine the force of gravity.

Example Problem:
A rocket ship flies over the surface of a planet. There hangs a mass suspended by a wire to act as a simple accelerometer attached to the underside of the rocket. As the rocket accelerates at 10 m/s2, the accelerometer mass is deflected by an angle of 34°. What is the acceleration due to gravity (g) of this planet?

Solution: Here is an illustration of the problem. The ship is accelerating to the right at a constant acceleration of 10 m/s². The mass is pulled down by the force of gravity, but held up by the tension in the wire. As the ship accelerates, the mass wants to stay in place but the tension in the wire pulls it along with the ship.

Here are the forces acting on the mass.

First, let’s find the forces acting in the x-direction.

ΣFx = Tsinθ

The acceleration is acting in the positive x-direction, so

ΣFx = ma.

Set these two to equal each other.

Tsinθ = ma

Now for the vertical forces.

ΣFy = Tcosθ – mg

Since the mass is not accelerating in the vertical direction, the sum of the forces vertically is equal to zero.

Tcosθ – mg = 0
Tcosθ = mg

Now we have two equations and two unknowns.

Tsinθ = ma
Tcosθ = mg

Divide the two equations into each other. tanθ = a/g

Since we want to know the gravity on the planet, solve for g.

Plug in a = 10 m/s2 and θ = 34° g = 14.8 m/s2