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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 can apply Newton's second law, which states that the sum of forces acting on an object equals its mass times acceleration. In this case, we can account for the forces acting on A:
Putting it all together, the equation becomes: [ 3mg \sin(\alpha) - F = 3ma ]
Step 2
Answer
Using the equation derived in part (a), we can substitute for ( F ) using the friction equation:
[ F = \frac{1}{6}R = \frac{1}{6}(3mg \cos(\alpha)) ] Substituting back, we have: [ 3mg \sin(\alpha) - \frac{1}{6}(3mg \cos(\alpha)) = 3ma ]
First, we need to find ( \sin(\alpha) ) and ( \cos(\alpha) ) from ( tan(\alpha) = \frac{3}{4} ), so: [ \sin(\alpha) = \frac{3}{5}, \quad \cos(\alpha) = \frac{4}{5} ]
Now, substituting values: [ 3mg \left( \frac{3}{5} \right) - \frac{1}{6}(3mg \cdot \frac{4}{5}) = 3ma ] [ 3mg \left( \frac{3}{5} \right) - \frac{2mg}{5} = 3ma ] [ 3mg \left( \frac{3}{5} - \frac{2}{15} \right) = 3ma ]
This reduces to: [ 3mg \left( \frac{9}{15} - \frac{2}{15} \right) = 3ma ] [ 3mg \cdot \frac{7}{15} = 3ma ] Now dividing by 3m gives: [ g \cdot \frac{7}{15} = a ] Thus: [ a = \frac{7g}{15} \cdot \frac{1}{10} = \frac{1}{10}g ]
Step 3
Answer
The velocity-time graph for the motion of B can be sketched as follows:
The final graph would resemble a straight line with a positive slope from (0,0) to the point where the graph approaches a constant velocity as B nears the pulley.
Step 4
Answer
In part (b), we derived that the acceleration of stone A was ( \frac{1}{10}g ) assuming the system would accelerate uniformly after A was released. However, the moment A is released, there is a small delay until both stones start moving, leading to an initial acceleration that may be slightly less than the calculated value due to inertia. Consequently, the value of ( a ) would need to be recalibrated to account for this initial condition, which implies that the assumed constant acceleration may not hold true for the initial moments of motion.
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