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A small ball is suspended by a string fr...

A small ball is suspended by a string from the ceiling of a car. As the car accelerates at a rate ‘a’ the string makes an angle 'a' with the vertical in equilibrium. Then the tension in the string is :

A

`m sqrt(a^(2) + g^(2))`

B

`m a sqrt(a^(2) + g^(2))`

C

`m g sin theta`

D

`m g cos theta`

Text Solution

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The correct Answer is:
To find the tension in the string when the ball is in equilibrium and the string makes an angle θ with the vertical as the car accelerates, we can follow these steps: ### Step 1: Identify the Forces Acting on the Ball When the car accelerates, two forces act on the ball: 1. The gravitational force (weight) acting downward: \( F_g = mg \) 2. The pseudo force acting horizontally due to the car's acceleration: \( F_p = ma \) ### Step 2: Analyze the Forces in the Equilibrium Condition In equilibrium, the ball is not accelerating, which means the net force acting on it is zero. The tension \( T \) in the string must balance these forces. The tension can be resolved into two components: - A vertical component \( T \cos(\theta) \) that balances the weight \( mg \). - A horizontal component \( T \sin(\theta) \) that balances the pseudo force \( ma \). ### Step 3: Set Up the Equations From the vertical forces: \[ T \cos(\theta) = mg \] (1) From the horizontal forces: \[ T \sin(\theta) = ma \] (2) ### Step 4: Divide the Two Equations To eliminate \( T \), we can divide equation (2) by equation (1): \[ \frac{T \sin(\theta)}{T \cos(\theta)} = \frac{ma}{mg} \] This simplifies to: \[ \tan(\theta) = \frac{a}{g} \] ### Step 5: Solve for Tension \( T \) Now, we can express \( T \) in terms of \( mg \) and \( \theta \): From equation (1): \[ T = \frac{mg}{\cos(\theta)} \tag{3} \] ### Step 6: Substitute \( \tan(\theta) \) into the Tension Equation Using \( \tan(\theta) = \frac{a}{g} \), we can find \( \cos(\theta) \): \[ \cos(\theta) = \frac{g}{\sqrt{g^2 + a^2}} \] Substituting this back into equation (3): \[ T = \frac{mg}{\frac{g}{\sqrt{g^2 + a^2}}} = mg \cdot \frac{\sqrt{g^2 + a^2}}{g} = m\sqrt{g^2 + a^2} \] ### Final Answer Thus, the tension in the string is: \[ T = m\sqrt{g^2 + a^2} \]

To find the tension in the string when the ball is in equilibrium and the string makes an angle θ with the vertical as the car accelerates, we can follow these steps: ### Step 1: Identify the Forces Acting on the Ball When the car accelerates, two forces act on the ball: 1. The gravitational force (weight) acting downward: \( F_g = mg \) 2. The pseudo force acting horizontally due to the car's acceleration: \( F_p = ma \) ### Step 2: Analyze the Forces in the Equilibrium Condition ...
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