2 Super Hard Rotational Motion Problems

AI Thread Summary
The discussion focuses on two challenging problems related to rotational motion and centripetal acceleration. The first problem involves calculating the range of speeds for a car on a banked curve, considering the radius, banking angle, and coefficient of static friction. The second problem examines the minimum coefficient of friction required for riders to remain against the wall of a rotating amusement park ride after the floor drops away. Participants emphasize the importance of applying fundamental physics formulas, such as F=ma and the relationship between friction and normal force. The overall sentiment reflects frustration with the complexity of these concepts while highlighting the necessity of mastering them.
ScoutFCM
Messages
17
Reaction score
0
1.) A car rounds a banked curve where the radius of curvature for the road is R, the banking angle is 0(theta), and the coefficient of static friction is [mu]. (a) Determine the range of speeds the car can have without slipping up or down the road. (b) What is the range of speeds possible if R = 100m, 0(theta)=10, and [mu]=0.10 (slippery conditions)?

2.) In a popular amusement park ride, a rotating cylinder of radium 3.00m is set in rotation at an angular speed of 5.00rad/s. The floor then drops away, leaving the riders suspended against the wall in a vertical position. What minimum coefficient of friction between a rdier's clothing and the wall is needed to keep the rider from slipping? (hint: recall that the magnitude of the max force of static friction is equal to [mu]n, where n is the normal force - in this case, the force causing the centripetal acceleration.

DAMN YOU ROTATIONAL MOTION AND CENTRIPETAL ACCELERATION. I HATE YOU!$!$!)(
 
Physics news on Phys.org
Well, take a crack at them and show your work. Demonstrate that you know something about Fnet = ma, centripetal acceleration, and friction.

Start, as always, by identifying all the forces acting on the objects in question. (Car in 1; rider in 2) Have fun!
 
Don't look all that "super-hard" to me- just apply the formulas that you already know:

1. F= ma and, for a friction coefficient of μ, F= mμ. Since the road is banked at angle θ, there is a force down the slope of mg cos(&theta). In order not to slip downward, You must have
ma> mg cos(&theta)- m&mu; and in order not to slip upward, you must have ma< mg cos(&theta)+ m&mu; You also should know the formula for the acceleration of a car going around a circle at constant speed. Put that in for a and solve for v.

2. Friction force is &mu; time "normal force". In this case the normal force is ma where a is the "acceleration" due to the rotation around a circle at constant speed (you'll need that formula again).
The friction force, &mu;(ma) must be at least the force of gravity, mg. Solve &mu;ma= mg for &mu;

DAMN YOU ROTATIONAL MOTION AND CENTRIPETAL ACCELERATION. I HATE YOU!$!$!)(

Yeah, It's just awful when people expect you to actually learn how to apply formulas!
 
Thread 'Collision of a bullet on a rod-string system: query'
In this question, I have a question. I am NOT trying to solve it, but it is just a conceptual question. Consider the point on the rod, which connects the string and the rod. My question: just before and after the collision, is ANGULAR momentum CONSERVED about this point? Lets call the point which connects the string and rod as P. Why am I asking this? : it is clear from the scenario that the point of concern, which connects the string and the rod, moves in a circular path due to the string...
Back
Top