Static and kinetic friction example | Forces and Newton's laws of motion | Physics | Khan Academy
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0:01 - 0:05So I have got this block of wood here that has a mass of 5 kilograms
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0:05 - 0:09and it is sitting on some dirt and we are near the surface of the earth
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0:09 - 0:17and the coefficient of static friction between this type of wood and this type of dirt is 0.60
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0:17 - 0:23and the coefficient of kinetic friction between this type of wood and this type of dirt is 0.55
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0:23 - 0:26This was measured by someone else long ago
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0:26 - 0:28or you found it in some type of a book someplace
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0:28 - 0:32And let's say we push on this side of the block with a force of a 100 N
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0:32 - 0:34What is going to happen?
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0:34 - 0:37So the first thing you might realize is if there is no friction
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0:37 - 0:39if this was a completely frictionless boundary and there is
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0:39 - 0:43no air resistance, we are assuming that there is no air resistance in this example
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0:43 - 0:45That in this dimension, in the horizontal dimension
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0:45 - 0:48there would only be one force here, this 100 N force
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0:48 - 0:52It would be completely unbalanced and that would be the net force
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0:52 - 0:56and so you would have a force going in that direction of a 100 N on a mass of 5 kilograms
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0:56 - 1:00Force = Mass times acceleration
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1:00 - 1:02acceleration and force are vector quantities
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1:02 - 1:04So you would have the force divided by the mass
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1:04 - 1:09would give you 20 meters per second of acceleration in the rightward direction
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1:09 - 1:11That is if there were no friction
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1:11 - 1:13but there is friction in this situation
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1:13 - 1:15So let's think about how we'll deal with it
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1:15 - 1:18So the coefficient of friction tells us
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1:18 - 1:23So this right here is the ratio between the magnitude of the force
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1:23 - 1:24that I have called the budging force
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1:24 - 1:29The amount of force you need to apply to get this thing to budge
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1:29 - 1:33to get this thing to start moving. So we can start using the coefficient of kinetic friction
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1:33 - 1:38It's the ratio between that and the magnitude of the force of contact
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1:38 - 1:41between this block and the floor or ground here
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1:41 - 1:44And the magnitude of that force of contact is the same thing
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1:44 - 1:48as the normal force that the ground is applying on the block
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1:48 - 1:53the magnitude of the normal force the ground is applying on the block
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1:53 - 1:54Then once its moving
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1:54 - 1:59then we can say that this is going to be--this will then be equal to
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1:59 - 2:02this over here will be equal to the force of friction
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2:02 - 2:05So this is the force that really overcome friction
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2:05 - 2:08and this over here will be equal to the force of friction
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2:08 - 2:13The magnitude of the force of friction over the force of contact
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2:13 - 2:17the contact force between those two, so over the normal force
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2:17 - 2:18and it makes sense
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2:18 - 2:21that the larger the contact force
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2:21 - 2:23the more that these are being pressed together
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2:23 - 2:26the little at the atomic level, they kind of really get into each others grooves
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2:26 - 2:28the more budging force you would need
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2:28 - 2:32or the more friction force would go against your motion
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2:32 - 2:34And in either situation
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2:34 - 2:36the force of friction is going against your motion
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2:36 - 2:37So even if you push it in that way
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2:37 - 2:40sounds like force of friction is all of a sudden going to help you
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2:40 - 2:44So let's think about what the necessary force will we need
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2:44 - 2:48to overcome the force of friction right here in the static situation
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2:48 - 2:52So the force of gravity on this block
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2:52 - 2:58is going to be the gravitational field which is 9.8 m/s^2 times 5 kilograms
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2:58 - 3:069.8 m/s times 5 kilograms gives 49 kilogram meters per second or 49 newtons down
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3:06 - 3:08This is the force, the magnitude of the force due to gravity
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3:08 - 3:12the direction is straight down towards the center of the earth
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3:12 - 3:17The normal force, and that force is there because this block is not accelerating downwards
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3:17 - 3:21So there must be some force that completely balances off the force of gravity
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3:21 - 3:26And in this example, it is the normal force
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3:26 - 3:30So it is acting 49 newtons upward
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3:30 - 3:35and so these net out. And that's why this block does not accelerate upwards or downwards
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3:35 - 3:37So what we have is the budge the
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3:37 - 3:41magnitude of the budging force, needs to be equal to, over the magnitude of the normal force
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3:41 - 3:44well this thing right over here is going to be 49 newtons
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3:44 - 3:47Is equal to 0.60
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3:47 - 3:52Or we could say that the magnitude of the budging force
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3:52 - 3:57is equal to 49 newtons times the coefficient of static fiction
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3:57 - 4:07Or that's 49 newtons times 0.60
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4:07 - 4:10And remember coefficient of friction are unitless
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4:10 - 4:13So the units here are still going to be in newtons
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4:13 - 4:23So this 49 times .6 gives us 29.4 newtons
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4:23 - 4:31This is equal to 29.4 newtons
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4:31 - 4:35So that's the force that's started to overcome static friction
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4:35 - 4:37which we are applying more than enough of
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4:37 - 4:40so with a 100 newtons, we would just start to budge it
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4:40 - 4:42and right when we are in just in that moment
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4:42 - 4:44where that thing is just starting to move
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4:44 - 4:46the net force--
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4:46 - 4:48so we have a 100 newtons going in that direction
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4:48 - 4:51and the force of static friction is going to go in this direction--
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4:51 - 4:54maybe I could draw it down here to show it's coming from right over here
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4:54 - 4:58The force of static friction is going to be 29.4 newtons that way
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4:58 - 5:01and so right when I am just starting to budge this
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5:01 - 5:03just when that little movement--
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5:03 - 5:05because once I do that, then all of a sudden it's moving
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5:05 - 5:09and then kinetic friction starts to matter, but just for that moment
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5:10 - 5:16just for that moment I'll have a net force of 100 - 29.4
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5:16 - 5:29to the right, so I have a net force of 70.6 N
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5:29 - 5:33for just a moment while I budge it
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5:33 - 5:35So just exactly while I'm budging it
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5:35 - 5:42While we're overcoming the static friction, we have a 70.6 N net force in the right direction
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5:43 - 5:48And so just for that moment, you divide it by 5 kg mass
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5:48 - 5:52So just for that moment, it will be accelerating at 14.12 m/s^2
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5:53 - 6:00So you'll have an acceleration of 14.1 m/s^2 to the right
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6:00 - 6:04but that will just be for that absolute moment, because once I budge it
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6:04 - 6:07all of a sudden the block will start to be moving
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6:07 - 6:11And once it's moving, the coefficient of kinetic friction starts to matter
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6:11 - 6:13We've got the things out of their little grooves
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6:13 - 6:17and so they're kind of gliding past each other on the top, although there still is resistant
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6:17 - 6:21So once we budge it, we'll have that acceleration for just a moment
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6:21 - 6:24Now all of a sudden, the coefficient of kinetic friction comes to play
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6:24 - 6:27And the force of friction, assuming we're moving
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6:27 - 6:31the magnitude of the force of friction will always go against our movement
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6:32 - 6:35is going to be--remember, our normal force is 49 N
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6:36 - 6:39So we can multiply both sides of this times 49
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6:39 - 6:58We get 49 N times 0.55 which is equal to 26.95 N
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6:58 - 7:00This is the force of friction; this is the magnitude
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7:01 - 7:02and it's going to go against our motions
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7:02 - 7:06So as soon as we start to move in that direction, the force of friction
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7:06 - 7:09is going to be going in that direction
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7:10 - 7:15So once we start moving, assuming that I'm continuing to apply this 100 newtons of force
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7:15 - 7:18what is the net force? So I have 100 N going that way
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7:18 - 7:23and I have 26.95 going that way
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7:23 - 7:25Remember, with vectors, I don't have to draw them here
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7:25 - 7:29I can draw all of their tails start at the center of mass of the
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7:29 - 7:33object. I can draw them whatever, but remember this is acting on the object
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7:33 - 7:37If we want to be precise, we can show it on the center of mass because
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7:37 - 7:40we can view all of these atoms as one collective object
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7:40 - 7:42But anyway, what is the net force now?
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7:42 - 7:46We have 100 N to the right; we have 26.95 to the left
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7:47 - 7:52100 minus 26.95
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7:52 - 7:54100 N that I'm applying to the right
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7:54 - 7:59- 26.95 N which is the force of friction to the left always acting against us
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7:59 - 8:03means that there's a net force to the right of 73.05
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8:03 - 8:11So once we're moving, we have a net force to the right of 73.05 N
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8:11 - 8:18This is the net force and it's acting to the right
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8:18 - 8:23Right after we budge it, how quickly will this accelerate?
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8:23 - 8:33Well, 73.05 divided by the mass, divided by 5 kg, gives us 14.61
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8:33 - 8:40So the acceleration once we're moving is going to be 14.61 m/s squared
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8:41 - 8:44to the right
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8:44 - 8:47So I really want to make sure you understand what's happening here
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8:47 - 8:51We always have enough force to start budging it
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8:52 - 8:54but right when we budged it
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8:54 - 8:56we overcome the static friction for just a moment
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8:56 - 9:00our acceleration was slower
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9:00 - 9:02because we're overcoming that static friction
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9:02 - 9:05but once we budged it and once it's moving
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9:05 - 9:09and assuming that we're continuing to apply a constant force over here
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9:09 - 9:10then all of a sudden, the force of friction since
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9:10 - 9:14we're kind of bump it along the top now and not stuck in their grooves
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9:15 - 9:18we're now using the coefficient of kinetic friction
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9:18 - 9:23And so once it's moving, the net force becomes greater in the rightward direction because
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9:23 - 9:28you can kind of view that force of friction will become less once it starts moving
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9:28 - 9:32And so now the force of friction went down a little bit to 26.95 N
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9:32 - 9:39And so now we're accelerating to right at a slightly faster rate 14.61 m/s^2
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9:39 - 9:42So right when you budge it, it accelerates at 14.1 m/s^2
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9:42 - 9:45but just for a moment, almost unnoticeable moment once it starts moving
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9:45 - 9:49Then 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:
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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
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