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In deep space, three masses are held in fixed positions (by rods light compared

ID: 2021879 • Letter: I

Question

In deep space, three masses are held in fixed positions (by rods light compared to the masses) at three corners of a square of side length as shown. A fourth mass is placed at point A, and released from rest. By symmetry it accelerates straight down and reaches point B (the midpoint between the two 3.0 Times 104 kg masses). How fast is the fourth mass moving at point B? (Note: the acceleration is not constant.) If the fourth mass is 70 kg, what is the magnitude of the net force acting on it at point A?

Explanation / Answer

part a: easiest to handle this as an energy problem.

Before you begin, note that the distances are easy because A to B to either of the 3 * 109 masses is a 3-4-5-Pythagorean triangle. So initial distances from A are 5,8, and 5 m; final distances are 3, 3, and 3 m.

U = -GMm/r   [ formula for gravitational potential energy ]

So initial U = -(6.67 * 10-11)(3 * 109 kg)(70 kg)/(5 m) = -2.803 J   for each of the two masses on the side

U = -(6.67 * 10-11)(5.64 * 109 kg)(70 kg)/(8 m) = -3.2935 J for the other mass

Total initial U is -8.8995 J

Final U is calculated by repeating the above calculation with all distances changed to 3 m.

Final U is -18.126 J. The 70 kg mass has converted 9.2265 J of potential energy into kinetic energy. Solving for v using (1/2)mv2, we get v = 0.5134 m/s.

part b: force from bottom mass: GMm/r2 = (6.67 * 10-11)(5.64 * 109 kg)(70 kg)/(8 m)2 = 0.412 N

which is directed all vertically.

force from each side mass: (6.67 * 10-11)(3 * 109 kg)(70 kg)/(5 m)2 = 0.561 N but this force is not directed vertically; vertical component is F cos 36.87 = F * .8 so each side mass contributes: 0.448 N

Total force: 1.31 N, all vertical

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