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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 derive the equation of motion for A, we start by considering the forces acting on it. The forces include the gravitational force, the tension in the string, and friction. The equation can be presented as:
Where:
Step 2
Answer
For the motion of A along the plane, we resolve the forces:
Where (R) can be found using the relationship (R = 3mg \cos(\alpha)). Thus substituting this into our previous equation:
Using (\tan(\alpha) = \frac{3}{4}), we can derive (\sin(\alpha)) and (\cos(\alpha)):
From here, solving for (a) will yield:
Step 3
Answer
The motion of B can be illustrated in a velocity-time graph beginning from rest. The graph will show a linear increase in the velocity of B as A moves down the plane, up until it reaches a maximum velocity just before reaching the pulley. First, label the time on the x-axis and the velocity on the y-axis. As A starts moving, B starts accelerating:
Step 4
Answer
If the string is not light, there would be additional tension due to the weight of the string itself, influencing the net forces acting on both A and B. This means we cannot simply treat tensions with the assumption that they are constant throughout the string. Thus, we would have different tensions in both segments of the string, impacting the derived acceleration value in part (b) since additional tension from the non-negligible weight of the string needs to be factored into the equations of motion.
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