Atwood machine

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File:Atwoods machine.png
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 m1Script error: No such module "Check for unknown parameters". and m2Script error: No such module "Check for unknown parameters"., connected by an inextensible massless string over an ideal massless pulley.[1]

Both masses experience uniform acceleration. When m1 = m2Script error: No such module "Check for unknown parameters"., the machine is in neutral equilibrium regardless of the position of the weights.

Equation for constant acceleration

File:Atwood.svg
The free body diagrams of the two hanging masses of the Atwood machine. Our sign convention, depicted by the acceleration vectors is that m1Script error: No such module "Check for unknown parameters". accelerates downward and that m2Script error: No such module "Check for unknown parameters". accelerates upward, as would be the case if m1 > m2Script error: No such module "Check for unknown parameters".

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 (W1Script error: No such module "Check for unknown parameters". and W2Script error: No such module "Check for unknown parameters".). To find an acceleration, consider the forces affecting each individual mass. Using Newton's second law (with a sign convention of m1>m2) 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. Script error: No such module "citation/CS1". Chapter 6, example 6-13
  2. Script error: No such module "citation/CS1". Section 1-6, example 2

External links

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