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A block of mass 1kg hangs without vibrat...

A block of mass `1kg` hangs without vibrations at the end of a spring with a force constant `1 N//m` attached to the ceilling of an elevator. The elevator is rising with an upward acceleration of `g//4`. The acceleration of the elevator suddenly ceases. What is the amplitude of the resulting oscillations?

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To solve the problem step by step, we need to analyze the forces acting on the block when the elevator is accelerating and when it suddenly stops. ### Step 1: Understanding the Forces Acting on the Block When the elevator is rising with an upward acceleration of \( \frac{g}{4} \), the effective force acting on the block due to gravity is modified by the pseudo force due to the elevator's acceleration. The effective gravitational force \( F_g \) acting on the block while the elevator is accelerating is given by: \[ F_g = mg + ma \] where: - \( m = 1 \, \text{kg} \) (mass of the block) - \( g = 10 \, \text{m/s}^2 \) (acceleration due to gravity) - \( a = \frac{g}{4} = \frac{10}{4} = 2.5 \, \text{m/s}^2 \) (upward acceleration of the elevator) Substituting the values: \[ F_g = 1 \times 10 + 1 \times 2.5 = 10 + 2.5 = 12.5 \, \text{N} \] ### Step 2: Finding the Spring Force at Equilibrium At equilibrium, the spring force \( F_s \) is equal to the effective gravitational force: \[ F_s = kx \] where: - \( k = 1 \, \text{N/m} \) (spring constant) - \( x \) is the extension of the spring from its natural length. Setting the forces equal gives: \[ kx = 12.5 \] Substituting \( k \): \[ 1 \cdot x = 12.5 \implies x = 12.5 \, \text{m} \] ### Step 3: Analyzing the Situation When the Elevator Stops When the elevator suddenly ceases to accelerate, the only force acting on the block is the gravitational force. The spring will now exert a force equal to the weight of the block: \[ F_s = mg = 1 \times 10 = 10 \, \text{N} \] ### Step 4: Finding the Amplitude of Oscillation The difference in forces when the elevator stops creates a net force that will cause the block to oscillate. The maximum extension (amplitude \( A \)) of the spring will be when the spring force equals the new effective gravitational force: \[ F_s = kA \] The net force when the elevator stops is: \[ F_{\text{net}} = F_g - F_s = 12.5 - 10 = 2.5 \, \text{N} \] Setting this equal to the spring force at maximum extension: \[ kA = 2.5 \implies 1 \cdot A = 2.5 \implies A = 2.5 \, \text{m} \] ### Final Answer The amplitude of the resulting oscillations is: \[ \boxed{2.5 \, \text{m}} \]

To solve the problem step by step, we need to analyze the forces acting on the block when the elevator is accelerating and when it suddenly stops. ### Step 1: Understanding the Forces Acting on the Block When the elevator is rising with an upward acceleration of \( \frac{g}{4} \), the effective force acting on the block due to gravity is modified by the pseudo force due to the elevator's acceleration. The effective gravitational force \( F_g \) acting on the block while the elevator is accelerating is given by: \[ F_g = mg + ma ...
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