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We can accelerate rolling by applying force through its center of mass. As discussed earlier, friction in such case acts in the backward direction to counteract sliding in the forward direction. However, it is difficult to visualize a mechanical force that can be applied through center of mass of a rolling body. Incidentally, gravity provides a ready made arrangement in which force acts through center of mass.

A ball rolling along an incline is one such example, in which external force is gravity. Its component along the plane “mgsinθ” acts through COM of the rolling body.

Accelerated rolling motion and friction

Force of gravity acts through center of mass.

The friction, in this case, acts in the backward direction as shown in the figure above.

Another way to accelerate rolling is to impart a force such that its line of action does not pass through center of mass. In this case, force constitutes a torque that imparts angular acceleration in addition to translational acceleration.

Such is the case with all transporting vehicles having wheels. The internal drive rotates the shaft, which in turn tends to rotate the wheel. We can visualize the situation better for the case of bicycle. When a bicycle is peddled, torque is imparted to the wheel. The chain – socket arrangement rotates the wheel. As discussed earlier, the friction, in this case, is in the direction of the acceleration of COM.

Accelerated rolling motion and friction

Torques causes acceleration in forward direction.
Torques causes acceleration in backward direction.

What if we apply the brake? The sole purpose of applying the brake is to apply a torque in the opposite direction to the direction of rotation. The brake pad jams on the rim. The tangential friction force constitutes the torque opposing the rotation. There is a corresponding linear deceleration of the wheel. A linear deceleration is equivalent to an acceleration in the backward direction. The friction between the wheel and surface, therefore, also acts backward along the backward direction of acceleration (i.e. deceleration) as shown in the right figure above.

Problem : A spool is pulled by a force, “F”, in vertical direction with the help of a rope wrapped on it as shown. If the spool does not loose contact with the surface, then what is the direction of friction.

Spool and rope system

A force is applied on the spool in the vertical direction.

Solution : The tension in the rope is equal to the force applied. This force does not pass through center of mass. The torque due to the force causes angular acceleration of the spool. Since there is no motion in the vertical direction (in the direction of force), there is no vertical linear acceleration involved.

Spool and rope system

A force is applied on the spool in the vertical direction.

We must note here that the arrangement has created a special situation. In the normal case of a force not passing through center of mass has dual effects of rotation and translation. However, the mechanical arrangement here ensures that there is no vertical motion (weight of the spool does not allow vertical motion for the given situation).

Now, the torque is anticlockwise. As such, the spool tends to slide towards right. In response, static friction acts towards left as shown in the figure above. Though, it is not required in the question to ascertain the translational motion, but we should be aware that friction towards left will cause a translational acceleration in its direction.

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Summary

1: The friction between surface and rolling body is self adjusting static friction for accelerated rolling.

2: The friction between surface and rolling body is less than that in the case of sliding.

3: Friction facilitates simultaneous occurrence of two types of acceleration as a response to external stimuli (force or torque or both).

4: Direction of friction :

(i) If the force passes through center of mass, then there is sliding tendency in the forward direction of applied force. In turn, friction acts in backward direction of the external force.

(ii) If the force does not pass through center of mass, then it constitutes torque. There is sliding tendency due to torque in the backward direction of applied force. The net result is that there is either no net friction (in special circumstance) or there is friction in the forward direction.

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Source:  OpenStax, Physics for k-12. OpenStax CNX. Sep 07, 2009 Download for free at http://cnx.org/content/col10322/1.175
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