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Static and kinetic friction example | Forces and Newton's laws of motion | Physics | Khan Academy

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    So I have got this block of wood here that has a mass of 5 kilograms
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    and it is sitting on some dirt and we are near the surface of the earth
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    and the coefficient of static friction between this type of wood and this type of dirt is 0.60
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    and the coefficient of kinetic friction between this type of wood and this type of dirt is 0.55
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    This was measured by someone else long ago
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    or you found it in some type of a book someplace
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    And let's say we push on this side of the block with a force of a 100 N
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    What is going to happen?
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    So the first thing you might realize is if there is no friction
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    if this was a completely frictionless boundary and there is
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    no air resistance, we are assuming that there is no air resistance in this example
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    That in this dimension, in the horizontal dimension
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    there would only be one force here, this 100 N force
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    It would be completely unbalanced and that would be the net force
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    and so you would have a force going in that direction of a 100 N on a mass of 5 kilograms
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    Force = Mass times acceleration
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    acceleration and force are vector quantities
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    So you would have the force divided by the mass
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    would give you 20 meters per second of acceleration in the rightward direction
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    That is if there were no friction
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    but there is friction in this situation
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    So let's think about how we'll deal with it
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    So the coefficient of friction tells us
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    So this right here is the ratio between the magnitude of the force
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    that I have called the budging force
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    The amount of force you need to apply to get this thing to budge
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    to get this thing to start moving. So we can start using the coefficient of kinetic friction
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    It's the ratio between that and the magnitude of the force of contact
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    between this block and the floor or ground here
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    And the magnitude of that force of contact is the same thing
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    as the normal force that the ground is applying on the block
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    the magnitude of the normal force the ground is applying on the block
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    Then once its moving
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    then we can say that this is going to be--this will then be equal to
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    this over here will be equal to the force of friction
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    So this is the force that really overcome friction
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    and this over here will be equal to the force of friction
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    The magnitude of the force of friction over the force of contact
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    the contact force between those two, so over the normal force
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    and it makes sense
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    that the larger the contact force
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    the more that these are being pressed together
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    the little at the atomic level, they kind of really get into each others grooves
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    the more budging force you would need
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    or the more friction force would go against your motion
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    And in either situation
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    the force of friction is going against your motion
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    So even if you push it in that way
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    sounds like force of friction is all of a sudden going to help you
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    So let's think about what the necessary force will we need
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    to overcome the force of friction right here in the static situation
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    So the force of gravity on this block
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    is going to be the gravitational field which is 9.8 m/s^2 times 5 kilograms
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    9.8 m/s times 5 kilograms gives 49 kilogram meters per second or 49 newtons down
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    This is the force, the magnitude of the force due to gravity
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    the direction is straight down towards the center of the earth
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    The normal force, and that force is there because this block is not accelerating downwards
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    So there must be some force that completely balances off the force of gravity
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    And in this example, it is the normal force
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    So it is acting 49 newtons upward
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    and so these net out. And that's why this block does not accelerate upwards or downwards
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    So what we have is the budge the
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    magnitude of the budging force, needs to be equal to, over the magnitude of the normal force
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    well this thing right over here is going to be 49 newtons
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    Is equal to 0.60
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    Or we could say that the magnitude of the budging force
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    is equal to 49 newtons times the coefficient of static fiction
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    Or that's 49 newtons times 0.60
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    And remember coefficient of friction are unitless
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    So the units here are still going to be in newtons
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    So this 49 times .6 gives us 29.4 newtons
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    This is equal to 29.4 newtons
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    So that's the force that's started to overcome static friction
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    which we are applying more than enough of
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    so with a 100 newtons, we would just start to budge it
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    and right when we are in just in that moment
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    where that thing is just starting to move
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    the net force--
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    so we have a 100 newtons going in that direction
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    and the force of static friction is going to go in this direction--
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    maybe I could draw it down here to show it's coming from right over here
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    The force of static friction is going to be 29.4 newtons that way
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    and so right when I am just starting to budge this
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    just when that little movement--
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    because once I do that, then all of a sudden it's moving
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    and then kinetic friction starts to matter, but just for that moment
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    just for that moment I'll have a net force of 100 - 29.4
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    to the right, so I have a net force of 70.6 N
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    for just a moment while I budge it
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    So just exactly while I'm budging it
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    While we're overcoming the static friction, we have a 70.6 N net force in the right direction
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    And so just for that moment, you divide it by 5 kg mass
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    So just for that moment, it will be accelerating at 14.12 m/s^2
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    So you'll have an acceleration of 14.1 m/s^2 to the right
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    but that will just be for that absolute moment, because once I budge it
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    all of a sudden the block will start to be moving
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    And once it's moving, the coefficient of kinetic friction starts to matter
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    We've got the things out of their little grooves
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    and so they're kind of gliding past each other on the top, although there still is resistant
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    So once we budge it, we'll have that acceleration for just a moment
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    Now all of a sudden, the coefficient of kinetic friction comes to play
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    And the force of friction, assuming we're moving
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    the magnitude of the force of friction will always go against our movement
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    is going to be--remember, our normal force is 49 N
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    So we can multiply both sides of this times 49
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    We get 49 N times 0.55 which is equal to 26.95 N
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    This is the force of friction; this is the magnitude
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    and it's going to go against our motions
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    So as soon as we start to move in that direction, the force of friction
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    is going to be going in that direction
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    So once we start moving, assuming that I'm continuing to apply this 100 newtons of force
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    what is the net force? So I have 100 N going that way
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    and I have 26.95 going that way
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    Remember, with vectors, I don't have to draw them here
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    I can draw all of their tails start at the center of mass of the
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    object. I can draw them whatever, but remember this is acting on the object
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    If we want to be precise, we can show it on the center of mass because
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    we can view all of these atoms as one collective object
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    But anyway, what is the net force now?
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    We have 100 N to the right; we have 26.95 to the left
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    100 minus 26.95
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    100 N that I'm applying to the right
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    - 26.95 N which is the force of friction to the left always acting against us
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    means that there's a net force to the right of 73.05
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    So once we're moving, we have a net force to the right of 73.05 N
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    This is the net force and it's acting to the right
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    Right after we budge it, how quickly will this accelerate?
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    Well, 73.05 divided by the mass, divided by 5 kg, gives us 14.61
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    So the acceleration once we're moving is going to be 14.61 m/s squared
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    to the right
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    So I really want to make sure you understand what's happening here
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    We always have enough force to start budging it
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    but right when we budged it
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    we overcome the static friction for just a moment
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    our acceleration was slower
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    because we're overcoming that static friction
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    but once we budged it and once it's moving
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    and assuming that we're continuing to apply a constant force over here
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    then all of a sudden, the force of friction since
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    we're kind of bump it along the top now and not stuck in their grooves
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    we're now using the coefficient of kinetic friction
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    And so once it's moving, the net force becomes greater in the rightward direction because
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    you can kind of view that force of friction will become less once it starts moving
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    And so now the force of friction went down a little bit to 26.95 N
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    And so now we're accelerating to right at a slightly faster rate 14.61 m/s^2
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    So right when you budge it, it accelerates at 14.1 m/s^2
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    but just for a moment, almost unnoticeable moment once it starts moving
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    Then you're going to be going to the right with this constant acceleration
Title:
Static and kinetic friction example | Forces and Newton's laws of motion | Physics | Khan Academy
Description:

Thinking about the coefficients of static and kinetic friction. Created by Sal Khan.

Watch the next lesson: https://www.khanacademy.org/science/physics/forces-newtons-laws/tension-tutorial/v/the-force-of-tension?utm_source=YT&utm_medium=Desc&utm_campaign=physics

Missed the previous lesson? https://www.khanacademy.org/science/physics/forces-newtons-laws/inclined-planes-friction/v/intuition-on-static-and-kinetic-friction-comparisons?utm_source=YT&utm_medium=Desc&utm_campaign=physics

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Video Language:
English
Team:
Khan Academy
Duration:
09:50

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