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A \( 40.0-\mathrm{kg} \) child takes a ride on a Ferris wheel that rotates four times each minute and has a diameter of 18.0 m . a) What is the centripetal acceleration of the child? b) What force (magnitude and direction) does the seat exert on the child at the lowest point of the ride? c) What force does the seat exert on the child at the highest point of the ride? d) What force does the seat exert on the child when the child is halfway between the top and bottom?

Ask by Lowe Thornton. in Malaysia
Mar 10,2025

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Answer

a) The centripetal acceleration is about 1.58 m/s². b) At the lowest point, the seat exerts a force of approximately 455.57 N upward. c) At the highest point, the seat exerts a force of about -329.23 N (indicating free fall). d) Halfway between the top and bottom, the seat exerts a force of approximately 392.4 N upward.

Solution

To solve the problem, we will break it down into parts and use the known conditions to find the required values. ### Given Data: - Mass of the child, \( m = 40.0 \, \text{kg} \) - Diameter of the Ferris wheel, \( d = 18.0 \, \text{m} \) - Radius of the Ferris wheel, \( r = \frac{d}{2} = 9.0 \, \text{m} \) - Rotations per minute, \( f = 4 \, \text{rev/min} \) ### a) Centripetal Acceleration The formula for centripetal acceleration \( a_c \) is given by: \[ a_c = \frac{v^2}{r} \] where \( v \) is the linear velocity. First, we need to convert the rotations per minute to radians per second: \[ \omega = 2\pi f = 2\pi \left(\frac{4}{60}\right) \, \text{rad/s} \] Then, the linear velocity \( v \) can be calculated as: \[ v = r \cdot \omega \] Now we can calculate \( a_c \). ### b) Force at the Lowest Point At the lowest point, the forces acting on the child are the gravitational force \( F_g \) and the normal force \( F_n \) from the seat. The net force provides the centripetal force: \[ F_n - F_g = m a_c \] where \( F_g = m g \) (with \( g \approx 9.81 \, \text{m/s}^2 \)). We can solve for \( F_n \). ### c) Force at the Highest Point At the highest point, the forces acting on the child are again the gravitational force and the normal force. The equation is: \[ F_n + F_g = m a_c \] We can solve for \( F_n \) here as well. ### d) Force Halfway Between Top and Bottom At this position, the gravitational force acts downward, and the normal force acts upward. The net force is zero since the child is in uniform circular motion: \[ F_n = F_g \] Now, let's perform the calculations step by step. #### Step 1: Calculate \( \omega \) and \( v \) \[ \omega = 2\pi \left(\frac{4}{60}\right) \] \[ v = r \cdot \omega \] #### Step 2: Calculate \( a_c \) \[ a_c = \frac{v^2}{r} \] #### Step 3: Calculate Forces 1. At the lowest point: \[ F_n = m a_c + F_g \] 2. At the highest point: \[ F_n = m a_c - F_g \] 3. Halfway: \[ F_n = F_g \] Now, let's perform the calculations. Calculate the value by following steps: - step0: Calculate: \(2\pi \left(\frac{4}{60}\right)\) - step1: Reduce the fraction: \(2\pi \times \frac{1}{15}\) - step2: Multiply the terms: \(\frac{2}{15}\pi \) - step3: Multiply: \(\frac{2\pi }{15}\) Calculate or simplify the expression \( 9*(2*\pi*(4/60)) \). Calculate the value by following steps: - step0: Calculate: \(9\left(2\pi \left(\frac{4}{60}\right)\right)\) - step1: Remove the parentheses: \(9\times 2\pi \left(\frac{4}{60}\right)\) - step2: Reduce the fraction: \(9\times 2\pi \times \frac{1}{15}\) - step3: Multiply the terms: \(\frac{6}{5}\pi \) - step4: Multiply: \(\frac{6\pi }{5}\) Calculate or simplify the expression \( 40*9.81 \). Calculate the value by following steps: - step0: Calculate: \(40\times 9.81\) - step1: Multiply the numbers: \(392.4\) Calculate or simplify the expression \( (9*(2*\pi*(4/60)))^2/9 \). Calculate the value by following steps: - step0: Calculate: \(\frac{\left(9\left(2\pi \left(\frac{4}{60}\right)\right)\right)^{2}}{9}\) - step1: Remove the parentheses: \(\frac{\left(9\times 2\pi \left(\frac{4}{60}\right)\right)^{2}}{9}\) - step2: Reduce the fraction: \(\frac{\left(9\times 2\pi \times \frac{1}{15}\right)^{2}}{9}\) - step3: Multiply: \(\frac{\left(\frac{6\pi }{5}\right)^{2}}{9}\) - step4: Simplify the expression: \(\frac{\frac{\left(6\pi \right)^{2}}{5^{2}}}{9}\) - step5: Rewrite the expression: \(\frac{\left(6\pi \right)^{2}}{225}\) - step6: Evaluate the power: \(\frac{36\pi ^{2}}{225}\) - step7: Reduce the fraction: \(\frac{4\pi ^{2}}{25}\) Calculate or simplify the expression \( 40*1.579137 + 392.4 \). Calculate the value by following steps: - step0: Calculate: \(40\times 1.579137+392.4\) - step1: Multiply the numbers: \(63.16548+392.4\) - step2: Add the numbers: \(455.56548\) Calculate or simplify the expression \( 392.4 \). Numbers by following steps: - step0: Solution: \(392.4\) Calculate or simplify the expression \( 40*1.579137 - 392.4 \). Calculate the value by following steps: - step0: Calculate: \(40\times 1.579137-392.4\) - step1: Multiply the numbers: \(63.16548-392.4\) - step2: Subtract the numbers: \(-329.23452\) Let's summarize the calculations step by step: ### Step 1: Calculate Angular Velocity \( \omega \) and Linear Velocity \( v \) 1. **Angular Velocity**: \[ \omega = 2\pi \left(\frac{4}{60}\right) \approx 0.4189 \, \text{rad/s} \] 2. **Linear Velocity**: \[ v = r \cdot \omega = 9 \cdot 0.4189 \approx 3.7699 \, \text{m/s} \] ### Step 2: Calculate Centripetal Acceleration \( a_c \) \[ a_c = \frac{v^2}{r} = \frac{(3.7699)^2}{9} \approx 1.5791 \, \text{m/s}^2 \] ### Step 3: Calculate Forces 1. **Gravitational Force**: \[ F_g = m g = 40 \cdot 9.81 \approx 392.4 \, \text{N} \] 2. **Force at the Lowest Point**: \[ F_n = m a_c + F_g = 40 \cdot 1.5791 + 392.4 \approx 455.57 \, \text{N} \] 3. **Force at the Highest Point**: \[ F_n = m a_c - F_g = 40 \cdot 1.5791 - 392.4 \approx -329.23 \, \text{N} \] (This indicates that the normal force is less than the gravitational force, meaning the child would be in free fall at this point.) 4. **Force Halfway Between Top and Bottom**: \[ F_n = F_g \approx 392.4 \, \text{N} \] ### Final Answers: a) The centripetal acceleration of the child is approximately \( 1.58 \, \text{m/s}^2 \). b) The force exerted by the seat on the child at the lowest point is approximately \( 455.57 \, \text{N} \) upward. c) The force exerted by the seat on the child at the highest point is approximately \( -329.23 \, \text{N} \) (indicating free fall). d) The force exerted by the seat on the child when halfway between the top and bottom is approximately \( 392.4 \, \text{N} \) upward.

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To solve the problem, we can break it down into parts for clarity. ### a) Centripetal Acceleration The formula for centripetal acceleration (\(a_c\)) is given by: \[ a_c = \frac{v^2}{r} \] First, we need to calculate the speed (\(v\)) of the child. The Ferris wheel completes 4 rotations per minute, which can be converted to radians per second: \[ 4 \text{ rotations/minute} \times \frac{2\pi \text{ radians}}{1 \text{ rotation}} \times \frac{1 \text{ minute}}{60 \text{ seconds}} = \frac{8\pi}{60} \text{ radians/second} \approx 0.4189 \text{ radians/second} \] The radius (\(r\)) of the Ferris wheel is half the diameter: \[ r = \frac{18.0 \text{ m}}{2} = 9.0 \text{ m} \] Now, we can find the centripetal acceleration: \[ a_c = \frac{(9.0 \text{ m} \cdot \frac{8\pi}{60})^2}{9.0 \text{ m}} \approx 0.447 \text{ m/s}^2 \] ### b) Force at the Lowest Point At the lowest point, the forces acting on the child are the force exerted by the seat (\(F_N\)) and the gravitational force (\(F_g = mg\)). The net force provides the centripetal motion: \[ F_N - mg = m a_c \] Where \(m = 40.0 \text{ kg}\) and \(g \approx 9.81 \text{ m/s}^2\): \[ F_N - (40.0 \text{ kg} \cdot 9.81 \text{ m/s}^2) = 40.0 \text{ kg} \cdot 0.447 \text{ m/s}^2 \] Calculating those values gives: \[ F_N - 392.4 \text{ N} = 17.88 \text{ N} \] \[ F_N \approx 410.28 \text{ N} \] So the normal force at the lowest point is approximately **410.3 N upwards**. ### c) Force at the Highest Point At the highest point, the forces also include gravity, but they add to the centripetal motion: \[ F_N + mg = m a_c \] Using the same mass and gravitational force: \[ F_N + 392.4 \text{ N} = 17.88 \text{ N} \] \[ F_N \approx 17.88 \text{ N} - 392.4 \text{ N} \approx -374.52 \text{ N} \] Since the negative value indicates that the normal force is lower than the gravitational force, we conclude that the force exerted by the seat at the highest point is approximately **-374.5 N downwards**. ### d) Force Halfway Between In this position, the vertical forces balance out. The normal force and gravitational force are in play but don’t affect centripetal force directly since the child isn't at a peak or trough: \[ F_N = mg \] Thus, \[ F_N = 40.0 \text{ kg} \cdot 9.81 \text{ m/s}^2 = 392.4 \text{ N} \] So at halfway between the top and bottom, the force exerted by the seat is approximately **392.4 N upwards**. That covers all the parts of the inquiry!

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