Your cousin Throckmorton skateboards from rest down a curved ramp in the form of a quarter circle of radius R = 2.50m

Your cousin Throckmorton skateboards from rest down a curved ramp in the form of a quarter circle of radius R = 2.50m. Assume that the wheels of the skateboard roll without slipping and that the friction in the wheel bearings is negligible. If we treat Throcky and his skateboard as a particle of mass m = 27.0kg, he undergoes (nonuniform) circular motion as he rides down the ramp.
a) When Throcky has descended half the distance to the bottom, so that the surface of the ramp is at 45° to the horizontal, what is his instantaneous speed?
b) What is the magnitude of the normal force acting on Throcky at that moment?

The Correct Answer and Explanation is :

Let’s analyze Throckmorton’s motion down the quarter-circle ramp to determine his instantaneous speed and the magnitude of the normal force acting on him when the ramp is at a 45° angle to the horizontal.

Part (a): Instantaneous Speed at 45°

At the top of the ramp, Throcky has only gravitational potential energy, which converts into kinetic energy as he descends. At the 45° point, half of the ramp’s height has been descended, so the change in height (Δh) is:

Δh = R – R * cos(45°) = R * (1 – cos(45°))

The potential energy lost equals the kinetic energy gained:

m * g * Δh = 0.5 * m * v²

Simplifying and solving for v:

v = √(2 * g * Δh)

Substituting Δh:

v = √(2 * g * R * (1 – cos(45°)))

Given R = 2.50 m and g ≈ 9.81 m/s²:

v ≈ √(2 * 9.81 * 2.50 * (1 – cos(45°)))

v ≈ 5.00 m/s

Part (b): Magnitude of the Normal Force at 45°

At the 45° point, the forces acting on Throcky are:

  • Gravitational force (mg) acting vertically downward.
  • Normal force (N) exerted by the ramp, acting perpendicular to the surface.
  • Centripetal force required for circular motion, which is provided by the radial component of the normal force.

The centripetal force (Fc) is given by:

Fc = m * v² / R

At 45°, the radial component of the normal force (N_radial) must provide this centripetal force:

N_radial = N * cos(45°)

Equating N_radial to Fc:

N * cos(45°) = m * v² / R

Solving for N:

N = (m * v²) / (R * cos(45°))

Substituting known values:

N = (27.0 kg * (5.00 m/s)²) / (2.50 m * cos(45°))

N ≈ 27.0 kg * 25.0 m²/s² / (2.50 m * 0.707)

N ≈ 27.0 kg * 25.0 m/s² / 1.768

N ≈ 381.5 N

Therefore, the magnitude of the normal force acting on Throcky at the 45° point is approximately 381.5 N.

This analysis assumes that Throcky’s motion is purely due to gravity, with no frictional losses, and that the ramp’s curvature provides the necessary centripetal force for circular motion.

For a visual explanation of how to gain speed on ramps, you might find the following video helpful:

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