A small cylinder rolling with a velocity v along a horizontal surface encounters a smooth inclined surface. The height 'h' up to which the cylinder will ascend is

Option 1)


Option 2)


Option 3)


Option 4)


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The correct option is D: $$ \frac{v^2}{2g} $$

To determine the height ( h ) that the small cylinder will ascend, we need to consider the conservation of energy. Specifically, the initial kinetic energy of the cylinder is converted into potential energy as it climbs the incline.

Initially, the total kinetic energy consists of translational and rotational components:

$$ KE_{\text{initial}} = \frac{1}{2} m v^2 + \frac{1}{2} I \omega^2 $$

For a cylinder, the moment of inertia ( I ) around its center of mass is given by:

$$ I = \frac{1}{2} m r^2 $$

Since the cylinder is rolling without slipping, the angular velocity ( \omega ) is related to the linear velocity ( v ) by:

$$ \omega = \frac{v}{r} $$

Substituting ( I ) and ( \omega ) into the expression for kinetic energy:

$$ KE_{\text{initial}} = \frac{1}{2} m v^2 + \frac{1}{2} \left( \frac{1}{2} m r^2 \right) \left( \frac{v}{r} \right)^2 $$

Simplifying this, we get:

$$ KE_{\text{initial}} = \frac{1}{2} m v^2 + \frac{1}{4} m v^2 = \frac{3}{4} m v^2 $$

When the cylinder reaches its maximum height ( h ) on the incline, all the initial kinetic energy has been converted into gravitational potential energy ( PE_{\text{final}} ):

$$ PE_{\text{final}} = mgh $$

By the conservation of energy:

$$ KE_{\text{initial}} = PE_{\text{final}} $$


$$ \frac{3}{4} m v^2 = mgh $$

Solving for ( h ):

$$ h = \frac{\frac{3}{4} m v^2}{mg} = \frac{3v^2}{4g} $$

This suggests an error in the calculations above. Let's re-evaluate by considering contributions properly. Translational kinetic energy conversion implies:

$$ \frac{1}{2} m v^2 = mgh $$


$$ h = \frac{v^2}{2g} $$

Therefore, the correct height ( h ) is given by:

$$ \frac{v^2}{2g} $$

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