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Ch 08: Dynamics II: Motion in a Plane
Chapter 8, Problem 8

The weight of passengers on a roller coaster increases by 50% as the car goes through a dip with a 30 m radius of curvature. What is the car's speed at the bottom of the dip?

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Identify the forces acting on the passengers at the bottom of the dip. The forces include the gravitational force (mg) and the normal force (N) from the seat, which together provide the centripetal force required for circular motion.
Set up the equation based on the fact that the apparent weight of the passengers increases by 50%. This means the normal force at the bottom of the dip is 1.5 times the gravitational force, i.e., N = 1.5mg.
Express the net force acting on the passengers as the difference between the normal force and gravitational force, which equals the centripetal force needed for circular motion. Thus, N - mg = ma_c, where a_c is the centripetal acceleration.
Substitute the expression for the normal force and rearrange the equation to find the centripetal acceleration, a_c = 0.5g.
Use the formula for centripetal acceleration, a_c = v^2 / r, where v is the speed of the car and r is the radius of curvature (30 m), to solve for v. Substitute a_c = 0.5g and r = 30 m into the equation and solve for v.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Centripetal Force

Centripetal force is the net force required to keep an object moving in a circular path, directed towards the center of the circle. In the context of a roller coaster, this force is crucial when the car goes through dips and turns, as it ensures that the passengers remain in their seats and the car follows the curved track.
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Intro to Centripetal Forces

Weight and Normal Force

Weight is the force exerted by gravity on an object, calculated as the product of mass and gravitational acceleration. At the bottom of a dip, the normal force, which acts perpendicular to the surface, increases due to the centripetal acceleration required to keep the car moving in a circular path, resulting in an apparent increase in weight for the passengers.
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The Normal Force

Kinematics and Circular Motion

Kinematics involves the study of motion without considering the forces that cause it. In circular motion, the speed of an object at the bottom of a dip can be determined using the radius of curvature and the forces acting on it, including gravitational force and the required centripetal force, which together dictate the car's speed at that point.
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Related Practice
Textbook Question
The 10 mg bead in FIGURE  CP8.69 is free to slide on a frictionless wire loop. The loop rotates about a vertical axis with angular velocity ω. If ω is less than some critical value ω꜀, the bead sits at the bottom of the spinning loop. When ω > ω꜀, the bead moves out to some angle θ. a. What is ω꜀ in rpm for the loop shown in the figure?

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Textbook Question
A 30 g ball rolls around a 40-cm-diameter L-shaped track, shown in FIGURE P8.53, at 60 rpm. What is the magnitude of the net force that the track exerts on the ball? Rolling friction can be neglected. Hint: The track exerts more than one force on the ball.

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Textbook Question
A car drives over the top of a hill that has a radius of 50 m. What maximum speed can the car have at the top without flying off the road?
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Textbook Question
The normal force equals the magnitude of the gravitational force as a roller-coaster car crosses the top of a 40-m-diameter loop-the-loop. What is the car's speed at the top?
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Textbook Question
A 500 g ball moves in a vertical circle on a 102-cm-long string. If the speed at the top is 4.0 m/s, then the speed at the bottom will be 7.5 m/s. (You'll learn how to show this in Chapter 10.) (a) What is the gravitational force acting on the ball?
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Textbook Question
A 500 g ball moves in a vertical circle on a 102-cm-long string. If the speed at the top is 4.0 m/s, then the speed at the bottom will be 7.5 m/s. (You'll learn how to show this in Chapter 10.) (b) What is the tension in the string when the ball is at the top?
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