The friction force comes from where?

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Homework Help Overview

The discussion revolves around the concept of friction, particularly its direction and relationship to motion. Participants explore the interpretation of the statement "friction always opposes the motion" through various examples, including a heavy box and a mass on a rotating disc. The inquiry focuses on the quantitative meaning of motion and how friction behaves in different scenarios.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants discuss the microscopic nature of friction and its dependence on relative motion. Questions arise regarding the direction of friction in relation to displacement vectors, particularly in cases of static and kinetic friction. The original poster seeks clarification on how to interpret friction in scenarios with no motion versus those with relative motion.

Discussion Status

The discussion is active, with various perspectives being shared. Some participants provide insights into the types of friction and their characteristics, while others question the assumptions about friction's direction in different contexts. There is an ongoing exploration of how to analyze the movement of a mass on a rotating disc when angular velocity exceeds a certain threshold.

Contextual Notes

Participants note the complexity of friction's behavior in different scenarios, including static versus kinetic friction and the effects of angular velocity on a mass on a rotating disc. The discussion acknowledges the need for further clarification on these concepts without reaching a definitive conclusion.

mrsobhan
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Homework Statement


We always encounter this expression: "Friction always opposes the motion". But what does it mean exactly? For example when we push a heavy box and it does not move we consider the friction opposite to the applied force. The second case when the box moves. In this case if we show the displacement by vector X the friction will be a vector opposite to X. Now consider a mass on an rotating horizontal disc. In this case we consider the friction equal to mrw^2 which w is the angular velocity and we consider the friction towards the center of rotation. How can we interpret the expression "friction is opposite to the motion". In the first case we don't have any motion at all. At the third case the displacement vector is different to the friction.
What is the quantitative meaning of "motion"? Can we consider it the displacement vector?
Can you explain this?

Homework Equations


The Attempt at a Solution

 
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I don't quite see it the way you do. The microscopic picture of friction involves the formation of temporary bonds b/w atoms of surfaces in contact. You see such a large surface in contact but actually due to the irregularities the actual area of contact is a small fraction of it. High pressure at these points leads to these bonds, something known as cold welding. Due to these electrostatic interactions RELATIVE motion is opposed, in whatever direction force acts on the object.
And friction is a real force.
 
aim1732 said:
I don't quite see it the way you do. The microscopic picture of friction involves the formation of temporary bonds b/w atoms of surfaces in contact. You see such a large surface in contact but actually due to the irregularities the actual area of contact is a small fraction of it. High pressure at these points leads to these bonds, something known as cold welding. Due to these electrostatic interactions RELATIVE motion is opposed, in whatever direction force acts on the object.
And friction is a real force.

ok i accept. But you did not answer the question. What is the direction of the friction with respect to the motion. Suppose that the motion is shown with a vector. For example vector X for displacement. Can you show the direction of the friction force?
 
No I can't.
Friction's direction w.r.t actual motion is not always the same. It only opposes relative motion. For example, a block on an accelerating body experiences friction in direction of its actual displacement but a little thought shows that had friction not been there it would have gone backwards - relative motion b/w the body and block.
Similarly in your example of rotating frames, if you observe w.r.t the rotating frame there is a centrifugal force away from center so friction is radial. In this case too dispalcement vector and friction have no relation.
 
To add on, there are actually three key types of friction between surfaces: static friction, kinetic friction, and rolling friction. The classic cases of friction involve the first two types of friction.

Kinetic friction is the force that opposes the relative motion between two surfaces that are in contact and moving relative to each other. Static friction is the force that opposes the relative tendency motion between two surfaces that are in contact but not moving relative to each other.

Static friction adopts a range of values from zero to a maximum value denoted the "limiting friction". It is dependent on the force that is attempting to cause the surfaces to move relative to each other (but no motion occurs yet). Kinetic friction, on the other hand, has an approximately constant value given the two surfaces. The value of the kinetic friction is usually a little less than the limiting friction.
 
Fightfish said:
To add on, there are actually three key types of friction between surfaces: static friction, kinetic friction, and rolling friction. The classic cases of friction involve the first two types of friction.

Kinetic friction is the force that opposes the relative motion between two surfaces that are in contact and moving relative to each other. Static friction is the force that opposes the relative tendency motion between two surfaces that are in contact but not moving relative to each other.

Static friction adopts a range of values from zero to a maximum value denoted the "limiting friction". It is dependent on the force that is attempting to cause the surfaces to move relative to each other (but no motion occurs yet). Kinetic friction, on the other hand, has an approximately constant value given the two surfaces. The value of the kinetic friction is usually a little less than the limiting friction.

Thanks. We reached the good point now.
Consider a rotating disc with a mass on it without motion with respect to the disc. As you mentioned above this a case of static friction with the limitation equals to μN. Now the angular velocity of the disc (W) begins to increase. The maximum angular velocity which the mass can stay without any motion with respect to the disc is when mrW^2 = μN. After this velocity the mass will move relative to the disc. Suppose we increase the velocity of the disc a bit more than this threshold velocity. Is it possible to analysis the movement of the mass, for example determine the path it moves.
 
i believe with the law of inertia of Newton, there will be a centrifugal force exists, hence the mass will try to move away from the centre of rotation, with the increase in the angular velocity of the disc, such force will increase as well.

hence, the motion of the mass will be more likely to be same as the motion of escaping velocity, see the links
http://en.wikipedia.org/wiki/Escape_velocity

of course if the gain in centrifugal force < limiting friction, the mass will only circulate in the disc

however, this is just my thinking, need someone to clarify it
 

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