# Atwood machine

The **Atwood machine** (or **Atwood's machine**) was invented in 1784 by the English mathematician George Atwood as a laboratory experiment to verify the mechanical laws of motion with constant acceleration. Atwood's machine is a common classroom demonstration used to illustrate principles of classical mechanics.

The ideal Atwood Machine consists of two objects of mass *m*_{1} and *m*_{2}, connected by an inextensible massless string over an ideal massless pulley.^{[1]}

When m_{1} = m_{2}, the machine is in neutral equilibrium regardless of the position of the weights.

When m_{1} ≠ m_{2} both masses experience uniform acceleration.

## Contents

## Equation for constant acceleration[edit]

We are able to derive an equation for the acceleration by using force analysis. If we consider a massless, inextensible string and an ideal massless pulley, the only forces we have to consider are: tension force (*T*), and the weight of the two masses (*W _{1}* and

*W*). To find an acceleration we need to consider the forces affecting each individual mass. Using Newton's second law (with a sign convention of ) we can derive a system of equations for the acceleration (

_{2}*a*).

As a sign convention, we assume that *a* is positive when downward for and upward for . Weight of and is simply and respectively.

Forces affecting m_{1}:

Forces affecting m_{2}:

and adding the two previous equations we obtain

,

and our concluding formula for acceleration

Conversely, the acceleration due to gravity, *g*, can be found by timing the movement of the weights, and calculating a value for the uniform acceleration *a*: .

The Atwood machine is sometimes used to illustrate the Lagrangian method of deriving equations of motion.^{[2]}

## Equation for tension[edit]

It can be useful to know an equation for the tension in the string. To evaluate tension, substitute the equation for acceleration in either of the 2 force equations.

For example, substituting into , results in

## Equations for a pulley with inertia and friction[edit]

For very small mass differences between *m*_{1} and *m*_{2}, the rotational inertia *I* of the pulley of radius r cannot be neglected. The angular acceleration of the pulley is given by the no-slip condition:

where is the angular acceleration. The net torque is then:

Combining with Newton's second law for the hanging masses, and solving for *T _{1}*,

*T*, and

_{2}*a*, we get:

Acceleration:

Tension in string segment nearest *m _{1}*:

Tension in string segment nearest *m _{2}*:

Should bearing friction be negligible (but not the inertia of the pulley and not the traction of the string on the pulley rim), these equations simplify as the following results:

Acceleration:

Tension in string segment nearest *m _{1}*:

Tension in string segment nearest *m _{2}*:

### Practical implementations[edit]

Atwood's original illustrations show the main pulley's axle resting on the rims of another four wheels, to minimize friction forces from the bearings. Many historical implementations of the machine follow this design.

An elevator with a counterbalance approximates an ideal Atwood machine and thereby relieves the driving motor from the load of holding the elevator cab — it has to overcome only weight difference and inertia of the two masses. The same principle is used for funicular railways with two connected railway cars on inclined tracks, and for the elevators on the Eiffel Tower which counterbalance each other. Ski lifts are another example, where the gondolas move on a closed (continuous) pulley system up and down the mountain. The ski lift is similar to the counter-weighted elevator, but with a constraining force provided by the cable in the vertical dimension thereby achieving work in both the horizontal and vertical dimensions. Boat lifts ^{[3]} are another type of counter-weighted elevator system approximating an Atwood machine.

## See also[edit]

Wikimedia Commons has media related to .Atwood's machine |

## Notes[edit]

**^**Tipler, Paul A. (1991).*Physics For Scientists and Engineers*(3rd, extended ed.). New York: Worth Publishers. p. 160. ISBN 0-87901-432-6. Chapter 6, example 6-13**^**Goldstein, Herbert (1980).*Classical Mechanics*(2nd ed.). New Delhi: Addison-Wesley/Narosa Indian Student Edition. pp. 26–27. ISBN 81-85015-53-8. Section 1-6, example 2**^**See Wikipedia article: https://en.wikipedia.org/wiki/Boat_lift