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A block of mass 15 kg is placed on a lon...

A block of mass 15 kg is placed on a long trolley . The coefficient of friction between the block and the trolley is `0.18`. The trolley accelerates from rest with `0.5ms^(-2)` for 20s and then moves with uniform velocity. Discuss the motion of the block as viewed by (a) a stationary observer on the ground (b) as observer moving with the trolley.

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To solve the problem, we will analyze the motion of the block on the trolley from two perspectives: (a) a stationary observer on the ground and (b) an observer moving with the trolley. ### Step 1: Analyze the motion of the trolley The trolley accelerates from rest with an acceleration of \(0.5 \, \text{m/s}^2\) for \(20 \, \text{s}\). - **Final velocity of the trolley (v)** can be calculated using the formula: \[ v = u + at \] where \(u = 0\) (initial velocity), \(a = 0.5 \, \text{m/s}^2\), and \(t = 20 \, \text{s}\). \[ v = 0 + (0.5 \times 20) = 10 \, \text{m/s} \] ### Step 2: Calculate the distance traveled by the trolley during acceleration The distance \(s\) traveled by the trolley during the acceleration can be calculated using the formula: \[ s = ut + \frac{1}{2}at^2 \] Substituting the values: \[ s = 0 \times 20 + \frac{1}{2} \times 0.5 \times (20)^2 = \frac{1}{2} \times 0.5 \times 400 = 50 \, \text{m} \] ### Step 3: Analyze the forces acting on the block The block experiences a frictional force due to its contact with the trolley. The maximum static frictional force \(f_s\) can be calculated as: \[ f_s = \mu_s \cdot m \cdot g \] where: - \(\mu_s = 0.18\) (coefficient of friction), - \(m = 15 \, \text{kg}\) (mass of the block), - \(g = 10 \, \text{m/s}^2\) (acceleration due to gravity). Calculating \(f_s\): \[ f_s = 0.18 \cdot 15 \cdot 10 = 27 \, \text{N} \] ### Step 4: Determine if the block will slide The force required to accelerate the block along with the trolley can be calculated as: \[ F = m \cdot a = 15 \cdot 0.5 = 7.5 \, \text{N} \] Since the maximum static frictional force \(f_s = 27 \, \text{N}\) is greater than the force required to accelerate the block \(F = 7.5 \, \text{N}\), the block will not slide off the trolley during the acceleration phase. ### Step 5: Motion of the block as viewed by a stationary observer on the ground - **During acceleration (first 20 seconds)**: The block will accelerate along with the trolley at \(0.5 \, \text{m/s}^2\) and will cover a distance of \(50 \, \text{m}\). - **After 20 seconds**: The trolley moves with a constant velocity of \(10 \, \text{m/s}\). The block will also move with this constant velocity since it does not slide. ### Step 6: Motion of the block as viewed by an observer moving with the trolley - **During acceleration**: The observer on the trolley will see the block at rest relative to them since both the block and the trolley are accelerating together. - **After 20 seconds**: The observer will still see the block at rest since both are moving at the same constant velocity. ### Summary of Motion - **Stationary observer**: The block accelerates for 20 seconds and then moves with a uniform velocity. - **Observer on the trolley**: The block remains at rest relative to the trolley throughout the motion.

To solve the problem, we will analyze the motion of the block on the trolley from two perspectives: (a) a stationary observer on the ground and (b) an observer moving with the trolley. ### Step 1: Analyze the motion of the trolley The trolley accelerates from rest with an acceleration of \(0.5 \, \text{m/s}^2\) for \(20 \, \text{s}\). - **Final velocity of the trolley (v)** can be calculated using the formula: \[ v = u + at ...
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