Physics Dynamics: Atwood Machine Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund 2012-2014 Department.

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Physics Dynamics: Atwood Machine Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund Department of Curriculum and Pedagogy FACULTY OF EDUCATION a place of mind

The Atwood Machine

The Atwood Machine is a pulley system consisting of two weights connected by string. We will assume no friction and that both the string and pulley are massless. If the masses of the two weights are different, the weights will accelerate uniformly by a. Our axis is defined such that positive a indicates that m 1 accelerates downwards, while m 2 accelerates upwards.

The Atwood Machine I Let W 1 be the weight of m 1, and W 2 be the weight of m 2. Let the tension of the string be T. Assume that m 1 > m 2. Which of the following is the correct free body diagram (force diagram) of m 1 ?

Answer: A Justification: There are only two forces acting on m 1, the force of tension due to the string pulling it up and the force of its own weight pulling it down. C and D are incorrect because g itself is not a force. B and E are incorrect because W 2 is not a force acting directly on m 1. Any force due to weight must point in the direction of g, which is downwards. Solution

The Atwood Machine II According to Newton’s second law, which of the following expressions is true?

Answer: B Justification: From the force diagram and taking downwards as positive acceleration for a, Therefore, by Newton’s second law, Solution (Add forces in the same direction as a, subtract forces in the opposite direction of a )

The Atwood Machine III Which of the following is the correct expression obtained by applying Newton’s second law for m 2 ? Press for hint

Answer: A Justification: This question is solved in the same way we as the previous question, for m 1. It is a good idea to start by drawing the free body diagram for m 2. Notice that the magnitude of T is the same for both m 1 and m 2. However, in the case of m 2, it is acting in the same direction as the acceleration rather than opposing it. Solution (Add forces in the same direction as a, subtract forces in the opposite direction of a )

The Atwood Machine IV What is the acceleration of the two weights?

Answer: E Justification: We have already found two expressions for the acceleration, although they contain the unknown quantity T. Since T is equal along all points on the string, it is the same in both equations. Adding the two equations will eliminate T : Solution

The Atwood Machine V Now that we have found an equation for the acceleration, we can analyze some how the Atwood Machine behaves. Under what conditions will a be negative?

Answer: E Justification: Recall that positive a implies that m 1 accelerates downwards, while m 2 accelerates upwards. If a is negative, this means that m 2 will accelerates downwards. Solution We know intuitively that m 2 will accelerate downwards if m 2 > m 1. This is also reflected in the formula we derived. since

The Atwood Machine VI How should the masses of the weights be chosen such that the neither weight accelerates?

Answer: C Justification: If neither weight accelerates, then a = 0. This occurs when m 1 = m 2. No matter where the two weights are positioned, the weights will not move. Solution since

The Atwood Machine VII Suppose that m 1 >> m 2 (one of the weights is much heavier than the other). How can the acceleration be approximated in this case?

Answer: D Justification: If m 1 >> m 2, then we can make the following approximations: Solution Compared to m 1, we can approximate that m 2 = 0. We can treat m 1 as if it were in freefall.

The Atwood Machine VIII Depending on the values chosen for the mass for m 1 and m 2, we can achieve a variety of values for a. What are all the possible values of a that can be obtained by varying the masses?

Answer: D Justification: The largest possible value for a is obtained when m 2 = 0. The smallest value of a is obtained when m 1 = 0. Solution No matter how large we choose m 1, the weights cannot accelerate upwards or downwards faster than g. What would happen if this were not true?

The Atwood Machine IX What is the tension on the string? Press for hint

Answer: B Justification: We can substitute the solution for a into either one of the force equations: For example, using the top equation gives: Solution

Answer: B Justification: Many answers can be ruled out by doing a few quick calculations. Answer A is incorrect because it does not have units of force. Answer C and D are incorrect because it is possible to obtain negative values for tension. Suppose we let m 1 = 0. We should expect our formula to return T = 0, since m 2 is in freefall. This is not true for answer E. Solution Continued

The Atwood Machine X Suppose m 1 is fixed, although we are free to choose any value for m 2. How should m 2 be chosen (in terms of m 1 ) such that T = m 1 g ?

Answer: C Justification: If the tension of the string is equal to the weight of m 1, then m 1 is not accelerating. Recall that there is no acceleration when m 1 = m 2. From the formula: Solution

The Atwood Machine XI What is the force on the pulley required to hold it up along the ceiling? (Recall that we are assuming a massless pulley and string)

Answer: C Justification: The pulley must be held up by twice the tension on the string. Solution Notice that in the formula above, F = 0 if either m 1 or m 2 is zero. Since the masses will be in freefall, no force is required to hold the massless pulley up. Also notice that F pulley = m 1 g + m 2 g, the sum of the weight of the two masses, only when the weights are not accelerating ( m 1 = m 2 ).