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A 2kg block hangs without vibrating at t...

A `2kg` block hangs without vibrating at the bottom end of a spring with a force constant of `400 N//m`. The top end of the spring is attached to the ceiling of an elevator car. The car is rising with an upward acceleration of `5 m//s^(2)` when the acceleration suddenly ceases at time `t = 0` and the car moves upward with constant speed `(g = 10 m//s^(2)`
The amplitude of the oscillation is

A

`(a)7.5cm`

B

`(b)5 cm`

C

`(c)2.5 cm`

D

`(d)1 cm`

Text Solution

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The correct Answer is:
To solve the problem, we need to determine the amplitude of oscillation of a block attached to a spring when the elevator's upward acceleration ceases. Here’s a step-by-step solution: ### Step 1: Identify the Forces Acting on the Block When the elevator is accelerating upward, two forces act on the block: 1. The gravitational force (weight) acting downward: \( F_g = mg \) 2. The pseudo force due to the elevator's upward acceleration: \( F_p = ma \) Where: - \( m = 2 \, \text{kg} \) (mass of the block) - \( g = 10 \, \text{m/s}^2 \) (acceleration due to gravity) - \( a = 5 \, \text{m/s}^2 \) (upward acceleration of the elevator) ### Step 2: Calculate the Total Downward Force The total downward force when the elevator is accelerating is: \[ F_{\text{total}} = mg + ma = m(g + a) \] Substituting the values: \[ F_{\text{total}} = 2 \, \text{kg} \times (10 \, \text{m/s}^2 + 5 \, \text{m/s}^2) = 2 \, \text{kg} \times 15 \, \text{m/s}^2 = 30 \, \text{N} \] ### Step 3: Relate the Forces to the Spring Constant The spring force when the elevator is accelerating is equal to the total downward force: \[ F_{\text{spring}} = kx_1 \] Where: - \( k = 400 \, \text{N/m} \) (spring constant) - \( x_1 \) is the extension of the spring when the elevator is accelerating. Setting the forces equal gives: \[ kx_1 = 30 \, \text{N} \] Solving for \( x_1 \): \[ x_1 = \frac{30 \, \text{N}}{400 \, \text{N/m}} = 0.075 \, \text{m} \] ### Step 4: Analyze the Situation When the Elevator Stops Accelerating At \( t = 0 \), the elevator stops accelerating, and the only force acting on the block is its weight: \[ F_{\text{gravity}} = mg \] The spring force now balances only the weight of the block: \[ kx_2 = mg \] Where \( x_2 \) is the new extension of the spring after the acceleration stops. Substituting the values: \[ kx_2 = 2 \, \text{kg} \times 10 \, \text{m/s}^2 = 20 \, \text{N} \] Solving for \( x_2 \): \[ x_2 = \frac{20 \, \text{N}}{400 \, \text{N/m}} = 0.05 \, \text{m} \] ### Step 5: Calculate the Amplitude of Oscillation The amplitude of oscillation is the difference between the two extensions: \[ A = x_1 - x_2 \] Substituting the values: \[ A = 0.075 \, \text{m} - 0.05 \, \text{m} = 0.025 \, \text{m} \] Converting to centimeters: \[ A = 0.025 \, \text{m} = 2.5 \, \text{cm} \] ### Final Answer The amplitude of the oscillation is **2.5 cm**. ---

To solve the problem, we need to determine the amplitude of oscillation of a block attached to a spring when the elevator's upward acceleration ceases. Here’s a step-by-step solution: ### Step 1: Identify the Forces Acting on the Block When the elevator is accelerating upward, two forces act on the block: 1. The gravitational force (weight) acting downward: \( F_g = mg \) 2. The pseudo force due to the elevator's upward acceleration: \( F_p = ma \) Where: ...
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