^Oblique pull

^Oblique pull

Suppose a block of mass ‘m’ placed on a rough horizontal plane is pulled by a constant force F acting at an angle θ to horizontal,

let Fsinθ < mg, then,  N = mg – Fsinθ

Force needed to start the block moving is,

Fcosθ = fL

Using law of friction the limiting friction is,

fL = μS N

Combining above equations, we get,

Using tanα = μS, we get,

At θ = α, the force required to pull becomes minimum & given by

 

 

^f versus F graph

^f versus F graph

For the static body the f versus F graph will be a straight line passing through origin making an angle 450 with the F axis. It will be a horizontal line when the body starts moving, because kinetic friction is constant.

 

 

 

^Motion of a body on a fixed rough horizontal surface 

^Motion of a body on a fixed rough horizontal surface 

Suppose a block of mass ‘m’ placed on a rough horizontal plane is pulled by a horizontal force F.

Following are the various possibilities:

  1. If F = 0, then the frictional force acting on the block will be zero & the block will remain stationary.
  2. If F < fL, then the frictional force acting on the block will be equal to F & the block again will remain stationary.
  3. If F = fL, then the frictional force acting on the block will be equal to fL & the block will be at the verge of motion i.e. about to move.
  4. If F > fL, then the frictional force acting on the block will be equal to fK & the block will move with acceleration   a= f- fk /m   in the direction of force applied F.

 

^Oblique pulling is easier than pushing

^Oblique pulling is easier than pushing

Let 1 oblique pushing & 2 oblique pulling

⇒ Force required for oblique pushing is greater than that for oblique pulling. i.e. oblique pulling is easier than oblique pushing. Check yourself that there is no difference between pushing & pulling if the force applied is horizontal.

 

^Angle of friction

^Angle of friction

The angle between the normal reaction & the resultant of normal reaction & limiting friction on a horizontal rough surface is called angle of friction (α).

On an inclined plane angle of friction is also called angle of repose (β).

α = β = tan– 1static)

 

^Condition to start relative motion

^Condition to start relative motion

Suppose a body A at rest over another body B. Let the limiting friction acing between them is fLAB. If a net force F acts on A which tends to start motion of A relative to B then the condition to start motion of A relative to B is F > fLAB. If F > fLAB then A will remain at rest relative to B. However if

F > fLAB then  A accelerates relative to B & a kinetic friction between A & B acts.

^Static friction, fk

^Static friction, fk

The frictional force acting between two surfaces at rest with respect to each other is called static friction. Static friction is a self adjusting force. It adjusts itself from zero to a maximum value called limiting friction.

fs = 0 to μs N (called fL)

^Coefficient of friction 

^Coefficient of friction 

  1. Coefficient of friction is abbreviated by the symbol μ.
  2. It is a unit less dimensionless constant.
  3. Its value decides the extent of roughness or smoothness of two contact surfaces.
  4. Its value is low for smooth, wet & moving surfaces, and high for rough, dry & static surfaces.
  5. Generally μ < 1 but can be > 1 also. Coefficients of static (μs) & kinetic friction (μk) are experimentally obtained and depend entirely on the two interacting surfaces.
  6. It is independent of normal reaction & frictional force.

 

^Kinetic friction, fk

^Kinetic friction, fk

Frictional force acting between two surfaces moving with respect to each other is called kinetic friction. Kinetic friction is independent of amount of velocity. Its amount is given by fk = mk N.

Here μk is called coefficient of friction.

^Friction, f

^Friction, f

A tangential contact force opposing relative motion between two surfaces is called friction.

It is two types static & kinetic.

 

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