Question 14 Marks
Read the passage given below and answer the following questions from $1$ to $5.$ Friction: Let us return to the example of a body of mass m at rest on a horizontal table. The force of gravity $(mg)$ is cancelled by the normal reaction force $(N)$ of the table. Now suppose a force F is applied horizontally to the body. We know from experience that a small applied force may not be enough to move the body. But if the applied force F were the only external force on the body, it must move with acceleration F/m, however small. Clearly, the body remains at rest because some other force comes into play in the horizontal direction and opposes the applied force F, resulting in zero net force on the body. This force fs parallel to the surface of the body in contact with the table is known as frictional force, or simply friction. When there is no applied force, there is no static friction. It comes into play the moment there is an applied force. As the applied force $F$ increases, fs also increases, remaining equal and opposite to the applied force $($up to a certain limit$),$ keeping the body at rest. Hence, it is called static friction. Static friction opposes impending motion. The term impending motion means motion that would take place $($but does not actually take place$)$ under the applied force, if friction were absent. It is found experimentally that the limiting value of static friction $(fs )$ max f is independent of the area of contact and varies with the normal force$(N)$ approximately as: $(\text{f}_{\text{s}})\text{max}=\mu\text{N}$ where μs is a constant of proportionality depending only on the nature of the surfaces in contact. The constant μs is called the coefficient of static friction. The law of static friction may thus be written as $(\text{f}_{\text{s}})\leq\mu\text{sN}$ Frictional force that opposes relative motion between surfaces in contact is called kinetic or sliding friction and is denoted by $fk$. Kinetic friction, like static friction, is found to be independent of the area of contact. Further, it is nearly independent of the velocity. It satisfies a law similar to that for static friction: $(\text{f}_{\text{k}})=\mu_{\text{k}}\text{N}$
- Force of static friction is directly proportional to:
- Normal reaction
- Force by gravity
- Velocity of body
- None of these
- Coefficient of kinetic friction is independent of area of contact. True or false?
- True
- False
- Give formula for law of static friction
- Explain law of static friction
- Explain kinetic friction.
Answer
Where \mu s is coefficient of static friction and N is normal reaction.
View full question & answer→- (a) Normal reaction
- (a) True
- The law of static friction can be written as
Where \mu s is coefficient of static friction and N is normal reaction.
- It is found experimentally that the limiting value of static friction $(fs)$ max $f$ is independent of the area of contact and varies with the normal force(N) approximately as: $(\text{f}_{\text{s}})\text{max}=\mu\text{N}.$ where $\mu$ s is a constant of proportionality depending only on the nature of the surfaces in contact. The constant $\mu$ s is called the coefficient of static friction. The law of static friction may thus be written as $(\text{f}_{\text{s}})\leq\mu\text{sN}$
- Frictional force that opposes relative motion between surfaces in contact is called kinetic or sliding friction and is denoted by $f_k$ and given by $(\text{f}_{\text{k}})=\mu_{\text{k}}\text{N}$

