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Question 2
A small stone A of mass 3m is attached to one end of a string. A small stone B of mass m is attached to the other end of the string. Initially A is held at rest on a... show full transcript
Step 1
Answer
To find the equation of motion for stone A, we apply Newton's second law. The forces acting on A are the gravitational force component down the slope and the frictional force opposing the motion.
The equation can be expressed as:
where:
Step 2
Answer
To demonstrate that the acceleration of A is ( \frac{1}{10}g ), we resolve the forces perpendicular to and parallel to the plane.
Resolve the weight of A:
Calculate the normal force and frictional force:
Substitute into the equation of motion:
[3mg \cdot \frac{3}{5} - \frac{2mg}{5} - T = 3ma]
Considering only the system's motion, we equate: (T = 2mg \quad \text{(based on system equilibrium)})
Therefore: [\frac{7mg}{5} = 3ma + 2mg] Which leads us to: [a = \frac{1}{10}g]
Step 3
Answer
The velocity-time graph for B will reflect uniform acceleration starting from rest.
Since A starts moving down the slope, B will also begin to move upwards due to the tension in the string, gaining speed steadily.
The graph will be linear: at time (t=0), the velocity will be zero; as time progresses until B reaches the pulley, the velocity will increase uniformly until it reaches its maximum just before hitting the pulley, where it has constant acceleration until terminal speed.
The slope of the graph represents the acceleration of B, which is constant until the pulley is reached. Thus the graph will start at the origin and show a straight line with a positive slope that levels off just before point P.
Step 4
Answer
If the string is not light, the tension would vary depending on the mass of B in motion and the acceleration predicted. This means that our calculations assume a tension that would not account for the weight of B. If B has significant mass, the equation of motion derived would need revision, factoring the increased tension impacting the acceleration values for A.
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