00:01
In this problem on the topic of equilibrium and elasticity, we are told that a uniform cube, which has a side length of 8 centimeters, is resting on a horizontal floor.
00:10
We know that the coefficient of static friction between the cube and the floor is new, and a pull that is horizontal is being applied to one of the vertical faces of the cube and is applied perpendicularly to that side.
00:24
The force is applied at 7 centimeters above the floor along a vertical midline of the cube's face.
00:31
If this force has its magnitude gradually increased, we want to know that during the increase, what values of mu will make the cube eventually begin to slide and eventually begin to tip.
00:46
So upon applying a horizontal force, the cube may tip or slide depending on the friction between the cube and the flow.
00:53
When the cube is about to move, we are still able to apply the equilibrium conditions, but we set static friction equal to its maximum value, and picture the normal force, fn, as a concentrated force upward on the bottom corner of the cube directly below point o where p is being applied, as we've shown in the diagram.
01:14
Thus, the line of action of fn passes through point o and exerts no talk about o.
01:20
Now, we can see that obviously fn, the normal force being applied, is equal to the weight of the cube, m -g, where m is the mass of the cube...