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The maximum tension in the string of a p...

The maximum tension in the string of a pendulum is two times the minimum tension. Let `theta_(0)` is then what is angular amplitude

A

`1/2`

B

`3/4`

C

`2/3`

D

`3/5`

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The correct Answer is:
To solve the problem step by step, we can break it down as follows: ### Step 1: Understand the Problem We have a pendulum where the maximum tension in the string is twice the minimum tension. We need to find the angular amplitude \( \theta_0 \). ### Step 2: Define Tension at Maximum and Minimum Points 1. **Maximum Tension** \( T_{max} \): - At the highest point of the swing, the tension \( T_{max} \) can be expressed as: \[ T_{max} = mg + \frac{mv^2}{L} \] where \( m \) is the mass of the pendulum bob, \( g \) is the acceleration due to gravity, \( v \) is the velocity at the lowest point, and \( L \) is the length of the pendulum. 2. **Minimum Tension** \( T_{min} \): - At the lowest point of the swing, the tension \( T_{min} \) is given by: \[ T_{min} = mg \cos \theta \] where \( \theta \) is the angle at the lowest point. ### Step 3: Set Up the Equation Based on Given Information According to the problem, we know: \[ T_{max} = 2 \times T_{min} \] Substituting the expressions for \( T_{max} \) and \( T_{min} \): \[ mg + \frac{mv^2}{L} = 2(mg \cos \theta) \] ### Step 4: Simplify the Equation Rearranging the equation gives: \[ mg + \frac{mv^2}{L} = 2mg \cos \theta \] Dividing through by \( mg \) (assuming \( m \neq 0 \)): \[ 1 + \frac{v^2}{gL} = 2 \cos \theta \] ### Step 5: Express Velocity in Terms of Height Using the conservation of energy, we can express the velocity \( v \) at the lowest point in terms of the height \( h \): \[ h = L - L \cos \theta = L(1 - \cos \theta) \] The potential energy at height \( h \) converts to kinetic energy: \[ mgh = \frac{1}{2} mv^2 \implies v^2 = 2gh \] Substituting for \( h \): \[ v^2 = 2gL(1 - \cos \theta) \] ### Step 6: Substitute Back into the Tension Equation Substituting \( v^2 \) into the tension equation: \[ 1 + \frac{2gL(1 - \cos \theta)}{gL} = 2 \cos \theta \] This simplifies to: \[ 1 + 2(1 - \cos \theta) = 2 \cos \theta \] \[ 1 + 2 - 2 \cos \theta = 2 \cos \theta \] \[ 3 = 4 \cos \theta \] \[ \cos \theta = \frac{3}{4} \] ### Step 7: Find the Angular Amplitude Finally, we find the angle \( \theta \): \[ \theta = \cos^{-1}\left(\frac{3}{4}\right) \] ### Final Answer The angular amplitude \( \theta_0 \) is: \[ \theta_0 = \cos^{-1}\left(\frac{3}{4}\right) \] ---
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