A drum of radius R and mass M, rolls down without slipping along an inclined plane of angle \(\theta\) .The frictional force
dissipates energy as heat
decreases the rotational motion
decreases the rotational and translational motion
We have,
mg\(\times\)sinA−f=ma ________________________ (1)
in pure rolling \(\alpha\) =\(\frac{a}{r}\)
\(\alpha\) = angular acceleration
Now,τ=I\(\alpha\)
I = moment of inertia
f\(\times\)r = I\(\alpha\)
f\(\times\)r = I\(\frac{a}{r}\)
\(\therefore\) f =Iar2 ________________________________ (2)
Substituting (2)in (1)
we have mgsinA−I\(\frac{a}{r^2}\)=ma
here I of solid cylinder=\(\frac{mr^2}{2}\)
mgsinA−\(\frac{ma}{2}\)=ma
a=\(\frac{(2gsinA)}{3}\)
Now
from (2) we have
f =\(\frac{la}{r^2}\)
f =\(\frac{ma}{2}\) which should be less than or equal to μN otherwise body will slip (where u is coefficient of friction and N is normal acting on cylinder which is equal to mg cos A)
\(\frac{ma}{2}\)\(\leq\) \(\mu\)mgcosA
putting value of a
\(\frac{(m\times g \times \sin A)}{3}\) \(\leq\) \(\mu\)mgcosA
tanA \(\leq\) 3μ
Therefore, the correct option is (A): converts translational energy to rotational energy
Identify the major product C formed in the following reaction sequence:
Rotational motion can be defined as the motion of an object around a circular path, in a fixed orbit.
The wheel or rotor of a motor, which appears in rotation motion problems, is a common example of the rotational motion of a rigid body.
Other examples: