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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 stone A, we begin by applying Newton's second law. The forces acting on A include:
Resolving forces along the plane gives:
Substituting for ( F ) we get:
Next, we must resolve the normal force:
Thus, the final equation of motion becomes:
Step 2
Answer
From the equation derived in part (a), first we resolve the angle α. We know that:
Using this, we can find ( \sin \alpha ) and ( \cos \alpha ):
( \sin \alpha = \frac{3}{5} ) and ( \cos \alpha = \frac{4}{5} ).
Substituting these into the equations, we find:
Now, substituting these into the equation:
This simplifies to:
For equilibrium of the entire system, tension must be equal on both ends of the pulley, and the net motion leads us to solve for acceleration:
Ultimately, solving gives:
Step 3
Answer
The velocity-time graph for stone B can be sketched based on the acceleration derived in part (b). Initially, when A is released, both stones are at rest, hence the graph starts at the origin (0,0).
As A begins to move down the plane due to gravity, B will start gaining velocity because of the inextensibility of the string. Since the acceleration was found to be ( \frac{1}{10} g ), the graph will be a straight line with a gentle positive slope, indicating uniform acceleration.
The slope of this line represents the acceleration of stone B.
The final point on the graph will represent the velocity of B just before it reaches the pulley. Assuming the distance traveled is moderate, the final velocity will be a value proportional to the acceleration multiplied by the time taken until B reaches the pulley.
Thus the sketch will show a linear increase in velocity over time.
Step 4
Answer
If stone B was not light, the analysis in part (b) would be affected. The tension would vary depending on the mass of B, altering the net forces acting on A. Since we modeled B as a particle with negligible mass, this assumption may lead to incorrect results since a heavier B would create greater tension in the string.
This would change the equations of motion for A and its acceleration would not be ( \frac{1}{10} g ), but would instead depend on the mass of B. Hence, more complex calculations would be required considering the mass of both stones equally.
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