Atwood machine

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.<ref>Template:Cite book Chapter 6, example 6-13</ref>

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 <math>m_1</math> and upward for <math>m_2</math>. Weight of <math>m_1</math> and <math>m_2</math> is simply <math>W_1 = m_1 g</math> and <math>W_2 = m_2 g</math> respectively.

Forces affecting m₁: <math display="block"> m_1 g - T = m_1 a</math> Forces affecting m₂: <math display="block"> T - m_2 g = m_2 a</math> and adding the two previous equations yields <math display="block"> m_1 g - m_2 g = m_1 a + m_2 a,</math> and the concluding formula for acceleration <math display="block">a = g \frac{m_1 - m_2}{m_1 + m_2}</math>

The Atwood machine is sometimes used to illustrate the Lagrangian method of deriving equations of motion.<ref>Template:Cite book Section 1-6, example 2</ref>

See also

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Notes

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External links

• A treatise on the rectilinear motion and rotation of bodies; with a description of original experiments relative to the subject by George Atwood, 1764. Drawings appear on page 450.
• Professor Greenslade's account on the Atwood Machine
• Atwood's Machine by Enrique Zeleny, The Wolfram Demonstrations Project