Normal Force at Highest Point of a Rotating Ferris Wheel

In summary, a person with a weight of 670 N sitting on a bench attached to a Ferris wheel with radius 5.0 m and a rotation period of 8.0 s will experience an apparent weight of 460 N at the highest point of their motion. This is determined by calculating the normal force using the equation \vec F_N = mg - \frac {4 \pi^2 mr} {T^2} and the mass of the person is found to be 68.367 kg.
  • #1
logan3
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2

Homework Statement


A Ferris wheel has radius 5.0 m and makes one revolution every 8.0 s with uniform rotation. A person who normally weighs 670 N is sitting on one of the benches attached at the rim of the wheel. What is the apparent weight (the normal force exerted on her by the bench) of the person as she passes through the highest point of her motion?

[itex]r = 5.0m[/itex]
[itex]T = 8.0s[/itex]
[itex]\vec F_W = 670N[/itex]
[itex]g = 9.8 m/s^2[/itex]

Homework Equations


Circular motion has centripetal force and acceleration pointing perpendicular and inwards of the path. Thus,
[itex]\sum \vec F = \vec F_c = \vec F_W - \vec F_N \Rightarrow \vec F_N = \vec F_W - \vec F_c = mg - \frac {mv^2} {r}[/itex].

Since [itex]v = \frac {2 \pi r} {T}[/itex], then [itex]\vec F_N = mg - \frac {m(\frac {2 \pi r} {T})^2} {r} = mg - \frac {4 \pi^2 mr} {T^2}[/itex].

The mass of the person is: [itex]\vec F_W = mg \Rightarrow m = \frac {F_W} {g}[/itex].

The Attempt at a Solution


[itex]m = \frac {670N} {9.8 m/s^2} = 68.367 kg[/itex]
[itex]\vec F_N = 670N - \frac {4 \pi^2 (68.367 kg)(5.0m)} {(8.0)^2} = 670N - 210.86N = 459.14N \sim 460N[/itex]
 
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  • #2
Looks good to me.
 
  • #3
Thank-you : )
 

Related to Normal Force at Highest Point of a Rotating Ferris Wheel

1. What is the normal force at the highest point of a rotating Ferris wheel?

The normal force at the highest point of a rotating Ferris wheel is equal to the weight of the rider and the centripetal force acting on them. The normal force acts in the opposite direction of the weight to keep the rider in circular motion.

2. How does the normal force change at different points on a rotating Ferris wheel?

The normal force varies depending on the position of the rider on the Ferris wheel. At the bottom of the wheel, the normal force is at its maximum as it must counteract the full weight of the rider. As the rider moves up the wheel, the normal force decreases until it reaches zero at the highest point, and then increases again as the rider moves down the wheel.

3. Why does the normal force decrease at the highest point of a rotating Ferris wheel?

The normal force decreases at the highest point because the centripetal force acting on the rider decreases as they move farther away from the center of the wheel. This results in a decrease in the overall force that must be countered by the normal force.

4. How does the normal force affect the motion of a rider on a rotating Ferris wheel?

The normal force is crucial to keeping a rider in circular motion on a rotating Ferris wheel. Without the normal force, the rider would continue in a straight line, causing them to fly off the wheel. The normal force also helps to maintain the rider's speed and direction of motion.

5. Can the normal force at the highest point of a rotating Ferris wheel ever be zero?

Yes, the normal force at the highest point of a rotating Ferris wheel can be zero if the centripetal force acting on the rider is equal to their weight. This can occur if the wheel is moving at a constant speed, and the rider is at a specific distance from the center of the wheel.

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