00:01
So we can be looking at problem 41 of chapter i of the physics fifth.
00:04
The question simply asks us, knowing the designed traffic speed for a banked circular highway is radius and how fast traffic i'm moving along on a stormy day.
00:18
What is the minimum coefficient of friction between the tires and road that will allow the cars to negotiate the term without sliding? and for part b, with this value of the coefficient of friction, what is the greatest speed of which the curve can be negotiated without sliding? so first things first is to work at a theta and we know this from our definition but previously, which is the inverse tan of v squared over gr.
00:40
And our v in this case is 95 kilometers per hour which is 26 .3 meters per second and our r is 210 meters.
00:49
So our theta is therefore 18 .7 degrees, the inverse town of 26 .3 squared over 9 .81 times 210.
00:59
So this is the triangle we get.
01:05
We have some acceleration going inwards, which is a prime, and it's split up into a perpendicular, which is the acceleration perpendicular of the road, and a parallel, which is the acceleration parallel to the road.
01:19
We also have our friction force going up the slope and our normal force going perpendicularly upwards...