Copyright © 2006 jsd

1  Simple Accelerometer

It is possible to make an accelerometer in about 20 minutes, using a lead weight, two rubber bands, a dowel rod, and some baling wire. Coat hanger wire will do, if you don’t have a supply of baling wire on hand.

Figure 1: Simple Home-Made Accelerometer

The dowel rod is 24 inches long and 0.5 inches in diameter.

First, make a “carrier” as shown in the middle of the diagram. It is made of a single piece of baling wire. The carrier wire has a straight portion about 4 inches long in this example; adjust this to fit the length of your weight. The straight portion segues into loop at each end. Each loop slides freely on the rod. During construction, twist the loop a couple of times to provide structural strength, in accordance with time-honored baling-wire construction principles. Use the very last bit of length at each end, as it emerges from the twist, to make pegs to which the lead weight attaches.

Note the spelling: baling wire not “bailing wire”.

For the weight, I used a 3 ounce piece of lead that had fallen off somebody’s tire. I picked it up from the roadside, and straightened it using an anvil and a small hammer. I drilled small holes to receive the pegs.

In the figure, I pulled the weight off one of the pegs, so you can see the straight section of the carrier wire. Normally the weight would be flush against the straight wire.

Near each end of the stick, install a loop of baling wire, twisted tight so it doesn’t slide, to serve as a retainer for the rubber band.

Cut open each rubber band to make a single filament, rather than a loop. Attach one end to the carrier using two half hitches. Attached the other end to the retainer near the end of the stick; you can use half hitches, or just pinch it between the wire and the wood.

Using flimsier rubber bands and/or a heavier weight will maximize the sensitivity of the instrument.

The instrument measures the projection of g along its length. When horizontal, as shown in the figure, it reads zero. If you hold it with the “top” end up, it reads +1. If you hold it the other way up, it reads -1.

Select one of the loops on the carrier to use as a pointer, and mark the stick with appropriate readings. (My markings are not visible in figure 1.)

For starters, just play with the instrument. Hold it horizontal, and wiggle it back and forth along its length, to convince yourself that it really does measure acceleration. Then hold it vertically right-side-up, then turn it upside-down. Dandle it up and down.

You can also attach a string and swing the instrument around and around to create a centrifugal field. Observe the angle of the string, and the corresponding accelerometer reading: a 45 degree angle should correspond to 1.41 Gees, and a 60 degree angle should correspond to 2 Gees. Here we are treating the centrifugal field on the same basis as the gravitational field, as we should. Both show up as an acceleration, in accordance with Einstein’s equivalence principle.

To use the instrument to measure the weightlessness of free fall, hold it high with one hand, drop it, and catch it with the other hand. Catch it so that you clutch the weight and the stick together, so as to preserve the free-fall reading, which you can then examine at leisure.

Another design for a home-made accelerometer can be found in reference 1. For more about the gravitational field and how we perceive it, see reference 2 and reference 3.

2  Absolute Acceleration

Galileo’s principle of relativity tells us that there is no such thing as absolute velocity. Velocity is always relative. It is relative to some chosen reference frame.

The same is not true of acceleration. There definitely is a notion of absolute acceleration. Acceleration is defined relative to a local freely-falling reference frame. (The choice of frame does not matter, so long as it is freely falling.)

Ordinary standard accelerometers measure absolute acceleration. This means that they register +1g when at rest, upright, in the lab frame. They definitely do not measure acceleration relative to the lab frame. Relative to any freely falling reference frame, the lab is being accelerated skywards at a rate of +1g, as discussed in reference 3.

Accelerometers are sometimes installed in aircraft, especially aerobatic aircraft. In straight-and-level upright flight, the accelerometer reads +1g, as shown in figure 2.

Do not be fooled by the fact that the needle is horizontal. It is pointing to +1, not 0.

Figure 2: Standard Aircraft Accelerometer: Upright

Acceleration is a vector. The instrument measures one component of this vector, namely the component in the direction indicated by the red arrow shown in the figure.

We can obtain another data point by flying inverted. In straight-and-level inverted flight, the accelerometer reads −1g. This is shown in figure 3.

Figure 3: Standard Aircraft Accelerometer: Inverted

Remember that the pilot should be upside down when viewing figure 3. You can leave the picture “as is” on your screen and do a handstand.

As another way of obtaining the same result, you can interpret figure 3 as showing the instrument at rest, upside-down on a shelf in the laboratory, with fields, trees, mountains, etc. in the background. In this case you can look at it without being inverted yourself. The meter reads −1g.

3  References

Joachim Köppen, “The Flimsy AcceleroMeter” http://astro.u-strasbg.fr/~koppen/weightless/fam/index.html

John Denker, “The Definition of Weight” www.av8n.com/physics/weight.htm

John Denker “Can You Feel Gravity?” www.av8n.com/physics/gravity-perception.htm

Copyright © 2006 jsd