The 125-lb boy in the figure coasts (without pedaling) his bike off the top of a hill at a speed of 10 ft/s. When he reaches the bottom of the hill, having ρ = 50 ft, what will the normal force on the wheels of the bike be?

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Chapter1: Units, Trigonometry. And Vectors
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The 125-lb boy in the figure coasts (without pedaling) his bike off the top of a hill at a speed of 10 ft/s. When he reaches the bottom of the hill, having ρ = 50 ft, what will the normal force on the wheels of the bike be?
The image shows a cyclist traveling along a wavy path. The cyclist starts at point A, located at the top of an initial hill, with a velocity \( v_A = 10 \, \text{ft/s} \). The height of the hill at point A is 30 feet.

As the cyclist moves down from point A and along the undulating path, they reach the bottom at point B. The path has a curvature with a radius \( \rho = 50 \, \text{ft} \) as the cyclist descends towards point B. The path surface is smooth, influencing the cyclist's motion.

The diagram illustrates key physics concepts related to motion, such as initial velocity, gravitational potential energy at the hilltop, and kinetic energy as the cyclist descends the slope. The transition from potential to kinetic energy is a practical example of energy conservation in physics.

This setup can be used to study the dynamics of motion on curved paths and the influence of gravitational forces on moving objects.
Transcribed Image Text:The image shows a cyclist traveling along a wavy path. The cyclist starts at point A, located at the top of an initial hill, with a velocity \( v_A = 10 \, \text{ft/s} \). The height of the hill at point A is 30 feet. As the cyclist moves down from point A and along the undulating path, they reach the bottom at point B. The path has a curvature with a radius \( \rho = 50 \, \text{ft} \) as the cyclist descends towards point B. The path surface is smooth, influencing the cyclist's motion. The diagram illustrates key physics concepts related to motion, such as initial velocity, gravitational potential energy at the hilltop, and kinetic energy as the cyclist descends the slope. The transition from potential to kinetic energy is a practical example of energy conservation in physics. This setup can be used to study the dynamics of motion on curved paths and the influence of gravitational forces on moving objects.
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