Thursday, August 9, 2007

Irodov Problem 1.72

The force diagram of the problem is shown beside. We assume that that the masses are and, the tensions in the two strings are and and their accelerations are and respectively. This is indicated in the figure.

Now let us consider the relavent forces acting on each of the two masses first.

Forces acting on mass : For this problem we need to only consider forces acting on the body1 along a direction parallel to the inclined plane . There are two forces along this direction - i) the component of force of gravity and ii) the tension in the string , as shown in the figure. The mass accelerates up the inclined plane at a rate . Thus the equation of motion for body 1 can be written as,

Forces acting on mass : There are two forces acting on this mass, i) the tension in the second string and the force of gravity as shown in the figure. Since we have assumed that body 1 is moving up the plane, the reasonable thing is to assume that body 2 moves down. Suppose that it moves down with an acceleration of . Its dynamics are given as,

Forces on the Moving Pulley holding : There are three forces acting on the pulley, i) the tensions acting to pull the pulley down from each part of the thread that holds and ii) the tension in the thread holding mass . The mass of he pulley is 0 and it will accelerate at a rate downwards. Thus, we can write the dynamics of the pulley as,

How are and related ?: There is one more piece needed to solve the problem, the fact that the accelerations of the two bodies are related to each other. The basic principle that we use in figuring this relationship out is that the length of the thread is conserved. Please refer to the figure beside to understand the explanation. Suppose that the mass moves a length x along the inclined plane upwards. The moving pulley thus will descend a distance x. The length of the thread section AB now decreases by x. Thus, as seen in the figure A' B = AB-x. Since the length of the thread (AB + CD) has to be conserved, the length of the thread section CD must thus increases by x, C'D' = CD + x. In other words, will descend a distance x relative to the moving pulley. Since the pulley itself has descended x, the total distance that descends is x + x = 2x. To summarize, if moves a distance x units moves a distance 2x units. Thus, we have,

Now we are in a position to solve the problem. We can use (3) and (4) in (1) to get,

1 comment:

Unknown said...

this is the most perfect book ever seen