Friction Flashcards

You may prefer our related Brainscape-certified flashcards:
1
Q

Draw the graph of external Force F and friction f? Explain the various segments?

A
  1. Segment ab - Block is at rest, F is not sufficient to move block. Static friction opposes the applied F
  2. At b, Static friction reaches its max value, also called at fl
  3. Segment cd : Block is moving Kinetic friction takes over. Kinetic friction is less than Max static friction. Kinetic friction is always constant and does not vary
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

Which form of friction is higher ? What is the maximumim value of friction?

A
  1. The Maximum value of static friction is always higher than the Kinectic friction
    fs-max > fk
  2. The maximum value of friction is
    fs-max = 𝛍sN
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

What is the direction of Friction?

A

Friction is always in the **opposite direction **to the motion of a body or the relation motion between two bodies.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

What is the formula for the two frictional forces in the below system?

A

N2 = m2g

N1 = (m1+m2)g

Assuming slipping at all places
f1 = 𝛍1N1 = 𝛍1(m1+m2)g
f2 = 𝛍2N2 = 𝛍2m2g

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

What takes more effort to over to overcome friction - pushing or pulling?

A

Pushing takes more over effort to overcome friction

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

Why does pushing take more effort to overcome friction.

A

When you are pushing a block, the pushing force exerts a component of force (FSinϴ) vertically down. This adds to the down force and hence the Normal acting on the body by the surface increases by this amount.
Npush = mg + FSinϴ

Where while pulling at the same angle, the pulling force exerts a component of force (FSinϴ) vertically updward direction. This reduces downwards and hence the Normal acting on the body by the surface decreases by this amount.
Npull = mg - FSinϴ

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

What is the minimum pulling force required to be applied for a block to start slipping?

A

To start slipping, horizontal component of applied force should be equal to the max frictional force

FCosϴ = fs-max = 𝛍N
FCosϴ = 𝛍 (mg - FSinϴ)
F = 𝛍mg / (Cosϴ + 𝛍Sinϴ)

To minimise F, (Cosϴ + 𝛍Sinϴ) needs to maxmized. Which means differentiating (Cosϴ + 𝛍Sinϴ) and equating to zero. This gives us
tanϴ = 𝛍
Fmin = 𝛍mg / (√(𝛍2 + 1))

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

Define the contact force and provide its formula? What are its minimum and maximum values?

A

Contact force is the resultant of the Normal and the Friction force.
It is given by
Fc = √(N2+f2)
Fc, min = N, as f = 0
Fc, max = N √(1+𝛍2), as f = 𝛍N

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

What is the angle of repose? Derive the angle of repose.

A

Angle of repose is the minimum angle at which the body slips due to its weight.
Mathematically, block will start to slip when
mgsin𝝷 = fs, max,
mgsin𝝷 = 𝛍N, N = mgcos𝝷
mgsin𝝷 = 𝛍mgcos𝝷
tan𝝷 = 𝛍 or 𝝷 = tan-1𝛍

  1. If 𝝷 < tan-1𝛍, then no slipping
    1. If 𝝷 > tan-1𝛍, then block starts to slip
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

What is the acceleration of the block on a rough inclined plane?

A

Using NLM,
mgsin𝝷 - f = ma
mgsin𝝷 - 𝛍N= ma
mgsin𝝷 - 𝛍mgcos𝝷= ma
a= gsin𝝷 - 𝛍gcos𝝷

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

Briefly explain the movement and forces at play in a block over block system?

A
  1. Block B will never move before Block A
  2. Minimum force F required to move A = 𝛍 (m1+m2)g
  3. On further increasing force F, upto a Fmax</max> , then m2 and m1 moves together (doesn’t slip).
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

Consider a block over block system acted upon by a force F on the lower block? What is the acceleration and the maximum Force required to move both blocks without the top block slipping?

A

Since the top block isnt slipping, its acceleration is same as of the system.
Applying NLM on top block, we get
f2, max = m2a,
𝛍2m2g = m2a,
⇒ a = 𝛍2g….(i)

Applying NLM to lower block, we get
Fmax - f1 = (m1+m2)a, substituting for a from (i)
Fmax - f1 = (m1+m2)𝛍2g

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

What is the maximum hanging length of the chain after which it starts to slip?

A

Using NLM on the non-hanging portion of chain on the surface, we get
fmax = 𝛍N,
∵ N = mass of non-hanging length * g, we have
fmax = 𝛍(m/L * (L-x)) g
we also know that
fmax = m1g where m1 is the hanging mass.
Substituting we get
m1g = 𝛍(m/L * (L-x)) g
∴ x = 𝛍L / (1+𝛍)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly