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A block of weight 100N is lying on a rou...

A block of weight `100N` is lying on a rough horizontal surface.If coefficient of friction `1/sqrt3`.The least possible force that can move the block is

A

`100/sqrt3N`

B

`100sqrt3 N`

C

`50sqrt3 N`

D

`50N`

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The correct Answer is:
To solve the problem of finding the least possible force that can move a block of weight 100 N on a rough horizontal surface with a coefficient of friction of \( \frac{1}{\sqrt{3}} \), we can follow these steps: ### Step-by-Step Solution: 1. **Identify the Given Values:** - Weight of the block, \( W = 100 \, \text{N} \) - Coefficient of friction, \( \mu = \frac{1}{\sqrt{3}} \) 2. **Understand the Forces Acting on the Block:** - The weight of the block acts downwards. - The normal force \( N \) acts upwards. - A horizontal force \( F \) is applied at an angle \( \theta \) to reduce the frictional force. 3. **Resolve the Applied Force \( F \):** - The horizontal component of the force is \( F \cos \theta \). - The vertical component of the force is \( F \sin \theta \). 4. **Calculate the Normal Force:** - The normal force \( N \) can be expressed as: \[ N = W - F \sin \theta = 100 - F \sin \theta \] 5. **Determine the Frictional Force:** - The frictional force \( f \) is given by: \[ f = \mu N = \mu (100 - F \sin \theta) \] - Substituting \( \mu \): \[ f = \frac{1}{\sqrt{3}} (100 - F \sin \theta) \] 6. **Set Up the Equation for Motion:** - For the block to just start moving, the applied force's horizontal component must equal the frictional force: \[ F \cos \theta = \frac{1}{\sqrt{3}} (100 - F \sin \theta) \] 7. **Rearranging the Equation:** - Rearranging gives: \[ F \cos \theta + \frac{1}{\sqrt{3}} F \sin \theta = \frac{100}{\sqrt{3}} \] - Factoring out \( F \): \[ F \left( \cos \theta + \frac{1}{\sqrt{3}} \sin \theta \right) = \frac{100}{\sqrt{3}} \] 8. **Maximize the Denominator:** - To minimize \( F \), we need to maximize \( \cos \theta + \frac{1}{\sqrt{3}} \sin \theta \). - The maximum value of \( \cos \theta + \mu \sin \theta \) can be found using the formula: \[ \sqrt{1 + \mu^2} \] - Substituting \( \mu = \frac{1}{\sqrt{3}} \): \[ \sqrt{1 + \left(\frac{1}{\sqrt{3}}\right)^2} = \sqrt{1 + \frac{1}{3}} = \sqrt{\frac{4}{3}} = \frac{2}{\sqrt{3}} \] 9. **Calculate the Least Possible Force \( F \):** - Substitute back into the equation for \( F \): \[ F = \frac{100/\sqrt{3}}{\frac{2}{\sqrt{3}}} = \frac{100}{2} = 50 \, \text{N} \] ### Final Answer: The least possible force that can move the block is \( F = 50 \, \text{N} \).

To solve the problem of finding the least possible force that can move a block of weight 100 N on a rough horizontal surface with a coefficient of friction of \( \frac{1}{\sqrt{3}} \), we can follow these steps: ### Step-by-Step Solution: 1. **Identify the Given Values:** - Weight of the block, \( W = 100 \, \text{N} \) - Coefficient of friction, \( \mu = \frac{1}{\sqrt{3}} \) ...
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