Oops! It appears that you have disabled your Javascript. In order for you to see this page as it is meant to appear, we ask that you please re-enable your Javascript!

Notes for Friction chapter of class 11 physics. Dronstudy provides free comprehensive chapterwise class 11 physics notes with proper images & diagram.

Â

If we push a book on a horizontal table with a certain initial velocity, it eventually comes to rest. This shows that there is some force opposing the motion of the book on the table. This is called the â€˜** frictional force**â€™. It arises due to interaction between the molecules of the book and of the table.

Actually, whenever the surface of a body slides over the surface of another body, each body exerts a frictional force on the other which is parallel to the surface in contact. The frictional force on each body is opposite to the direction of its motion relative to the other. Thus, when a book slides along the surface of a table from left to right, the frictional force acting on the book is directed to the left while an equal frictional force acts on the table directed to the right. Frictional force may also exist between surfaces even before the relative motion starts.

**Static Friction**

Let us consider a block at rest on a horizontal table surface. The block is acted upon by two forces: its weight *mg *acting vertically downward at its centre of gravity, and the reactionary-force *N *exerted on it by the table which is directed vertically upward and passes through its centre of gravity. Since the block is in equilibrium, *N = mg*. In the Figure the lines of action of *mg* and *N *are shown slightly displaced for clarity.

When we apply a small horizontal force *F*, say towards right, the block does not move. The force *R *exerted on the block by the table surface is now so inclined (figure (a)) toward left that *R*, *mg *and *F *may form a â€˜closedâ€™ triangle (since the block is still in equilibrium). Figure (b).

The force *R* can be resolved into two components; *parallel* and *perpendicular *to the contact-surfaces. The component parallel to the contact surface is called the â€˜*force of static friction*â€™ *f** _{,} *which balances the applied force

Now, if the applied force

This

The limiting (maximum) static frictional force depends upon the nature of the surfaces in contact. It does not depend upon the size or area of the surfaces. For the given surfaces, the limiting frictional force *Â *is directly proportional to the normal reaction *N*.

*or *Â (for limiting frictional force)

where the constant of proportionality m_{s} is called the 'coefficient of static friction'. The above formula holds only when *Â *has its maximum (limiting) value. Before this stage, force of frictionÂ .

If the direction of the applied force *F *is reversed, the direction of *Â *also reverses, while the direction of *N *remains unchanged. In fact is always opposite to *F*.

**Angle of Friction**

In the case of limiting friction, the angle which the resultant *R* of the limiting frictional force *Â *and the normal reaction *N *makes with the normal reaction *N *is called the ** angle of friction**. If this angle is , then

ButÂ

Thus, the coefficient of static friction is equal to the tangent of the angle of friction.

**Kinetic Friction**

Once the motion starts, the frictional force acting between the surfaces decreases, so that a smaller force *F* is required to maintain uniform motion. The force acting between the surfaces in relative motion is called the â€˜** kinetic frictional force**â€™ Â which is less than the limiting force of static friction . We know from daily experiences that a lesser force is required to maintain the motion of a body than the force required to start the body from rest.

Thus, when the block is in uniform motion, the force of kinetic friction is

whereÂ is the coefficient of kinetic friction and its value is less than .

**Friction on an Inclined Plane
**In the figure(a), a block is placed on a rough inclined plane making an angle with the horizontal. Initially, the block is stationary. The F.B.D. of the block is shown in figure (b).The weight

Since the block is in equilibrium, the net force on the block parallel to the plane and also perpendicular to the plane is zero. That is

andÂ

On increasing the angle of inclination , the component Â increases, but simultaneously

ThenÂ

Substituting this value of

Â and

Hence, measuring the angle of inclination at which the block just starts sliding, the coefficient of static friction can be determined.

*A block of mass *M *= 10 kg is placed at rest on a horizontal surface as shown in the figure. The coefficient of friction between the block and the surface is Âµ = 0.3. It is pulled with a horizontal forceÂ *F*.
*

(ii)

*Solution*

The maximum value of friction force is

or

(i) To keep the block *stationary *the magnitude of friction force should be *f = F* **= **20 N since *F *< *f _{max}* . Therefore the force of friction is

**Note **Â that in this case friction force is unable to keep the block stationary and the block accelerators with

Also **note **that* friction force *is not always equal to ÂµN. It is the *limiting *or *maximum value *of friction. At any stage friction force may attain any value between 0 and Âµ *N*.

i.e.**Â **

*Application 2*

*For the system shown in the figure, the coefficient of static and kinetic friction between the block *m_{2} and the horizontal surface is Âµ_{s} and Âµ_{k}.

*If ***m_{2} = 10 kg, Âµ_{s}= 0.4 and Âµ_{k} = 0.35**

*Solution*

(i) The force which tries to accelerate the system is *m*_{1}*g*, while the opposing force is *f _{s}*. For

Thus,

Putting

*Application 3*

*A block is placed at rest on a horizontal surface. The coefficient of friction between the block and the surface is Âµ. It is pulled with a force *F* at an angle **q** with the horizontal as shown in the figure. Find the value of **q** at which minimum force is required to move the block. Also find the magnitude of this minimum force.*

*Solution*

The free body diagram of the block is shown in the figure. The friction force is maximum because the block is just about to move.

Applying Newtonâ€™s Second Law

Â Â Â Â Â Â (1)

Â Â Â Â (2)

orÂ Â Â Â Â

orÂ Â Â Â Â Â Â (3)

For minimum value of *F*,Â Â Â

Thus, differentiating equation (3) w.r.t. ,Â by applying chain rule, we get

=0

Since =0, therefore

or tan = Âµ = tan^{-}^{1} Âµ

**Note **that minimum force required to move the block is at the angle of friction**.
**Now from equation (3), withÂ q = tan

**ROUGH PULLEYS**

We know that when a string passes over a smooth pulley, the tension on each side of the string is same. But if the surface of the pulley is rough then the tensions on either side of the string are different. The difference in tension depends on the coefficient of friction (Âµ) and the angle () through which the string is wrapped over the pulley.

*ApplicationÂ 4*

*Show that the tension on two sides of the string wrapped over a rough pulley are related as
*

where Âµ is the coefficient of friction and

*Solution*

Consider a small element of string, which subtends an angle *d* at the centre.

For the equilibrium of the element

or Â Â Â (1)

* Â *(cos Â 1)

or Â *Â Â Â Â Â Â Â *(2)

From equations (1) and (2)

Â Â Â orÂ Â Â Â Â Â =

Integrating both sides, we get

Â Â orÂ Â Â

or *T _{2} *=

*ApplicationÂ 5*

*Find the minimum and maximum values of *M_{2} *for which the system remains in equilibrium. Take *M_{1} *= 10 kg and Âµ = 0.2.*

*Solution*

For minimum value of *M _{2
}* ()

or

=

Contact Us

good

So easy method of explanation.. and easily carried in our mind..

That's very nice

Very nice

Great explanation Awesome

Grt explanation

Very good

nice

u rock

good job