Atwood machine

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Illustration of the Atwood machine, 1905.

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 Template:Math and Template:Math, connected by an inextensible massless string over an ideal massless pulley.[1]

Both masses experience uniform acceleration. When Template:Math, the machine is in neutral equilibrium regardless of the position of the weights.

Equation for constant acceleration

The free body diagrams of the two hanging masses of the Atwood machine. Our sign convention, depicted by the acceleration vectors is that Template:Math accelerates downward and that Template:Math accelerates upward, as would be the case if Template:Math

An equation for the acceleration can be derived by analyzing forces. Assuming a massless, inextensible string and an ideal massless pulley, the only forces to consider are: tension force (Template:Mvar), and the weight of the two masses (Template:Math and Template:Math). To find an acceleration, consider the forces affecting each individual mass. Using Newton's second law (with a sign convention of Template:Nowrap derive a system of equations for the acceleration (Template:Mvar).

As a sign convention, assume that a is positive when downward for m1 and upward for m2. Weight of m1 and m2 is simply W1=m1g and W2=m2g respectively.

Forces affecting m1: m1gT=m1a Forces affecting m2: Tm2g=m2a and adding the two previous equations yields m1gm2g=m1a+m2a, and the concluding formula for acceleration a=gm1m2m1+m2

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

See also

Notes

  1. Template:Cite book Chapter 6, example 6-13
  2. Template:Cite book Section 1-6, example 2

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