INTRODUCTION
It has been established since long that all surfaces of the bodies are never perfectly smooth. It has been observed that whenever, even a very smooth surface is viewed under a microscope, it is found to have some roughness and irregularities, which may not be detected by an ordinary touch. It will be interesting to know that if a block of one substance is placed over the level surface of the same or different material, a certain degree of interlocking of the minutely projecting particles takesplace. This does not involve any force, so long as the block does not move or tends to move. But whenever one of the blocks moves or tends to move tangentially with respect to the surface, on which it rests, the interlocking property of the projecting particles opposes the motion. This opposing force, which acts in the opposite direction of the movement of the block, is called force of friction or simply friction. It is of the following two types:
1. Static friction.
2. Dynamic friction.
STATIC FRICTION
It is the friction experienced by a body when it is at rest. Or in other words, it is the friction when the body tends to move.
DYNAMIC FRICTION
It is the friction experienced by a body when it is in motion. It is also called kinetic friction. The dynamic friction is of the following two types :
1. Sliding friction. It is the friction, experienced by a body when it slides over another body.
2. Rolling friction. It is the friction, experienced by a body when it rolls over another body.
LIMITING FRICTION
It has been observed that when a body, lying over another body, is gently pushed, it does not move because of the frictional force, which prevents the motion. It shows that the force of the hand is being exactly balanced by the force of friction, acting in the opposite direction. If we again push the body, a little harder, it is still found to be in equilibrium. It shows that the force of friction has increased itself so as to become equal and opposite to the applied force. Thus the force of friction has a remarkable property of adjusting its magnitude, so as to become exactly equal and opposite to the applied force, which tends to produce motion. There is, however, a limit beyond which the force of friction cannot increase. If the applied force exceeds this limit, the force of friction cannot balance it and the body begins to move, in the direction of the applied force. This maximum value of frictional force, which comes into play, when a body just begins to slide over the surface of the other body, is known as limiting friction. It may be noted that when the applied force is less than the limiting friction, the body remains at rest, and the
friction is called static friction, which may have any value between zero and limiting friction.
NORMAL REACTION
It has been experienced that whenever a body, lying on a horizontal or an inclined surface, is in equilibrium, its weight acts vertically downwards through its centre of gravity. The surface, in turn,exerts an upward reaction on the body. This reaction, which is taken to act perpendicular to the plane, is called normal reaction and is, generally, denoted by R. It will be interesting to know that the term ‘normal reaction’ is very important in the field of friction, as the force of friction is directly proportional to it.
ANGLE OF FRICTION
Consider a body of weight W resting on an inclined plane as shown in Fig. 8.1. We know that the body is in equilibrium under the action of the following forces :
1. Weight (W) of the body, acting vertically downwards,
2. Friction force (F) acting upwards along the plane, and
3. Normal reaction (R) acting at right angles to the plane.
Let the angle of inclination (á) be gradually increased, till the body just starts sliding down the plane. This angle of inclined plane, at which a body just begins to slide down the plane, is called the angle of friction. This is also equal to the angle, which the normal reaction makes with the vertical.
COEFFICIENT OF FRICTION
LAWS OF FRICTION
Prof. Coulomb, after extensive experiments, gave some laws of friction, which may be grouped under the following heads :
1. Laws of static friction, and
2. Laws of kinetic or dynamic friction.
LAWS OF STATIC FRICTION
Following are the laws of static friction :
1. The force of friction always acts in a direction, opposite to that in which the body tends to move, if the force of friction would have been absent.
2. The magnitude of the force of friction is exactly equal to the force, which tends to move the body.
3. The magnitude of the limiting friction bears a constant ratio to the normal reaction between the two surfaces. Mathematically :
4. The force of friction is independent of the area of contact between the two surfaces.
5. The force of friction depends upon the roughness of the surfaces.
LAWS OF KINETIC OR DYNAMIC FRICTION
Following are the laws of kinetic or dynamic friction :
1. The force of friction always acts in a direction, opposite to that in which the body is moving.
2. The magnitude of kinetic friction bears a constant ratio to the normal reaction between the two surfaces. But this ratio is slightly less than that in case of limiting friction.
3. For moderate speeds, the force of friction remains constant. But it decreases slightly with the increase of speed
EQUILIBRIUM OF A BODY ON A ROUGH HORIZONTAL PLANE
We know that a body, lying on a rough horizontal plane will remain in equilibrium. But whenever a force is applied on it, the body will tend to move in the direction of the force. In such cases,
equilibrium of the body is studied first by resolving the forces horizontally and then vertically. Now the value of the force of friction is obtained from the relation :
