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A 500-g collar can slide without friction along the semicircular rod BCD. The spring is of constant 320 N/m and its undeformed length is 200 mm. Knowing that the collar is released from rest at B, determine (a) the speed of the collar as it passes through C, (b) the force exerted by the rod on the collar at C.

Short Answer

Expert verified
(a) The speed of the collar at C is approximately 1.98 m/s. (b) The force exerted by the rod on the collar at C is 9.81 N.

Step by step solution

01

Determine the change in spring length

The collar moves from point B to point C along the semicircular path. At point B, the spring is undeformed, and as the collar reaches point C, the spring extends. First, find the distance BC, which is the radius of the semicircle, equivalent to 200 mm or 0.2 m. At point C, the spring is stretched from 0.2 m to the semicircle's chord BC, which also equals 0.2 m.
02

Calculate the change in potential energy of the spring

The potential energy stored in the spring at point C can be calculated using the formula for spring potential energy: \[ PE_{spring} = \frac{1}{2} k x^2 \] where \(k = 320\ N/m\) is the spring constant and \(x\) is the deformation of the spring from its natural length. Since the collar moves to C, the deformation \(x = 0.2\ m - 0.2\ m = 0\ m\), resulting in no change in spring energy: \[ \Delta PE_{spring} = 0 \]
03

Determine the gravitational potential energy change

The collar moves vertically downward by the height of the semicircle (radius = 0.2 m), altering its gravitational potential energy. The change in gravitational potential energy is calculated as: \[ \Delta PE_{gravity} = mgh \] where \(m = 0.5\ kg\), \(g = 9.81\ m/s^2\), and \(h = 0.2\ m\). Therefore, \[ \Delta PE_{gravity} = 0.5 \times 9.81 \times 0.2 = 0.981\ J \]
04

Apply the conservation of energy

The initial energy (at rest) is all potential energy, and the final energy is kinetic when reaching C. Using energy conservation principles: \[ \Delta KE = \Delta PE_{total} = \Delta PE_{spring} + \Delta PE_{gravity} \] Since \( \Delta PE_{spring} = 0 \) and \( \Delta PE_{gravity} = 0.981\ J\), \[ \Delta KE = 0.981\ J \] The kinetic energy is given by \( \frac{1}{2}mv^2 \) so: \[ \frac{1}{2} \times 0.5 \times v^2 = 0.981 \] Solving for \(v\): \[ v^2 = \frac{2 \times 0.981}{0.5} = 3.924 \] \[ v = \sqrt{3.924} \approx 1.98\ m/s \]
05

Calculate the force exerted by the rod on the collar at C

At point C, the force exerted by the rod will be the normal force, which balances the centripetal force needed to maintain motion along the semicircular path. The centripetal force is given by: \[ F_c = \frac{mv^2}{r} \] Substituting \( m = 0.5\ kg, v = 1.98\ m/s, r = 0.2\ m\): \[ F_c = \frac{0.5 \times (1.98)^2}{0.2} \approx 9.81\ N \] Since there's no vertical force component (as vertical forces cancel out due to equilibrium), the normal force \(F_n = F_c = 9.81\ N\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Energy Conservation
Energy conservation is a key principle in mechanics, especially when analyzing the motion and forces acting on objects. It states that energy cannot be created or destroyed, only transformed from one form to another. When the collar slides along the semicircular rod, energy conservation helps us understand how potential energy is converted into kinetic energy.

At the beginning, the collar is at rest at point B, possessing potential energy due to its height. As it moves towards point C, this potential energy reduces as gravitational energy is transformed into kinetic energy.

This transformation is captured in the energy conservation equation:
  • Initial Energy = Total Potential Energy (at B)
  • Final Energy = Kinetic Energy (at C)
Because the spring’s deformation energy remains zero between B and C, only gravitational potential energy changes to kinetic energy. This insight ensures energy conservation's role in explaining and calculating the collar's motion and velocity.
Potential Energy
Potential energy is the stored energy of an object due to its position or state. In the context of this problem, there are two types of potential energy to consider: gravitational potential energy and spring potential energy.

  • Gravitational Potential Energy: This energy changes as the collar slides downwards along the semicircle. The height decreases by the semicircle's radius, leading to a reduction in gravitational potential energy.
  • Spring Potential Energy: At point B, the spring is not deformed, so its potential energy is initially zero. As the collar moves to C, and since there is no deformation (the spring remains at its original length), spring potential energy doesn't change.
Understanding how these energies change is crucial to solve for speed and forces acting on the collar as it moves along its path.
Kinetic Energy
Kinetic energy is the energy of motion. For the collar, as it moves from point B to C, the potential energy lost is converted into kinetic energy. This energy allows us to determine how fast the collar moves at point C.

The formula for kinetic energy is \[ KE = \frac{1}{2}mv^2 \] where:
  • \(m\) = mass of the object
  • \(v\) = velocity of the object
With energy conservation, once the potential energy value is known, this value equals the kinetic energy at C, allowing calculation of the collar's speed using the above formula. Hence, when solving for \(v\), we found it to be approximately 1.98 m/s. This demonstrates how potential energy converts into kinetic energy along the collar's journey.
Centripetal Force
Centripetal force is essential for understanding how objects move along curved paths. It is the force that keeps an object moving in a circular trajectory. For the collar at point C, the centripetal force is provided by the interaction with the rod, ensuring it continues along its semicircular path.

The centripetal force is calculated with the formula: \[ F_c = \frac{mv^2}{r} \] where:
  • \(m\) = mass of the collar
  • \(v\) = velocity at point C
  • \(r\) = radius of the path
Using this formula, we compute the required centripetal force, which is approximately 9.81 N. This force, balancing any vertical forces, is perceived as the normal force exerted by the rod on the collar. Understanding centripetal force is crucial for predicting the motion and stability of objects on curved paths.

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