2 Super Hard Rotational Motion Problems

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SUMMARY

This discussion focuses on solving two complex problems related to rotational motion and centripetal acceleration. The first problem involves a car navigating a banked curve with a radius of 100m, a banking angle of 10 degrees, and a coefficient of static friction of 0.10, requiring the calculation of speed ranges to avoid slipping. The second problem addresses an amusement park ride where a rotating cylinder with a radius of 3.00m and an angular speed of 5.00 rad/s necessitates determining the minimum coefficient of friction to prevent riders from slipping against the wall. Both problems emphasize the application of fundamental physics formulas such as F=ma and the relationship between friction, normal force, and centripetal acceleration.

PREREQUISITES
  • Understanding of rotational motion principles
  • Knowledge of centripetal acceleration and its formulas
  • Familiarity with static friction and its calculations
  • Ability to apply Newton's second law (F=ma)
NEXT STEPS
  • Explore the derivation of the centripetal acceleration formula
  • Study the effects of banking angles on vehicle dynamics
  • Learn about the role of friction in circular motion scenarios
  • Investigate real-world applications of rotational motion in amusement park rides
USEFUL FOR

Physics students, mechanical engineers, and anyone interested in the practical applications of rotational motion and centripetal acceleration in real-world scenarios.

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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!$!$!)(
 
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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!
 

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