00:01
So a quick reminder about how static friction works.
00:04
If you push on an object on a surface with static friction, you can push harder and harder and harder and harder, and the object may not move.
00:16
The reason being static friction acts kind of like a glue in between the surface of the floor, for example.
00:25
And in this case, we'll think of a box.
00:27
So you can continue to push and push and push until you break the glue.
00:34
And so the way we talk about the force of static friction, little f sub s, it is less than or equal to the coefficient mu sub s times the normal force, which is pushing the two surfaces together.
00:51
So remember when you glue objects together, you have to get the bonding to work by pushing the surfaces together.
00:59
And that is called the normal force.
01:03
Now the critical condition beyond which the box will become unglued, we'll call that critical condition.
01:12
It doesn't mean anybody's getting in bad shape.
01:15
It just means that the static friction has reached its maximum value.
01:22
That is equal to mu -s, times the normal force.
01:27
So as an example of this, we're going to figure out the force needed to get a 34 -kilogram crate to move on a surface with a given static friction coefficient.
01:40
And as usual, what we want to think through with forces is newton's second law.
01:50
So i usually like to draw a force diagram, a free -body diagram, when i'm doing these kind of things.
01:57
But right at the critical point, what we know is we have the critical condition.
02:04
And we also have the sum of the forces in the x direction just barely equal to zero.
02:11
And of course, the sum of the y forces is also equal to zero being on a surface.
02:19
Looking at a free body diagram, we of course have the weight downwards.
02:25
M .g is 34 kilograms times 9 .8 meters per second squared.
02:35
Newton's, that n is for newton's.
02:44
So that's about 33.
02:47
Newton's.
02:48
I'll go ahead and calculate that.
02:50
The force downwards has both an x and a y component, being at 21 degrees.
03:03
The static friction is opposite along the surface, and there is the normal force.
03:12
I'll call it f sub -n, just so we don't get it mixed up with newton's.
03:25
That's always a little awkward to have more than one meaning for a symbol.
03:30
So let's divide our motion up into two different directions...