Math Problem Statement

A uniform rod of mass 4.2 kg is 8 m long. The rod is pivoted about a horizontal, frictionless pin at the end of a thin extension (of negligible mass) a distance 8 m from the center of mass of the rod. The rod is released from rest at an initial angle of 58 with respect to the horizontal, as shown.

What is the angular speed of the rod at the instant the rod is in a horizontal position? The acceleration due to gravity is 9.8 m/s? and the moment of inertia of the rod about its center of mass is Icm= 1/12 ml^2 Answer in units of rad/s. Answer in units of rad/s.

Solution

To find the angular speed of the rod when it reaches a horizontal position, we can use the principles of conservation of energy and rotational dynamics.

Given Data

  • Mass of the rod, m=4.2m = 4.2 kg
  • Length of the rod, l=8l = 8 m
  • Initial angle, θ0=58\theta_0 = 58^\circ
  • Gravitational acceleration, g=9.8g = 9.8 m/s²

Moment of Inertia

The moment of inertia of the rod about its center of mass is given by: Icm=112ml2I_{\text{cm}} = \frac{1}{12} m l^2 Substituting the values: Icm=112×4.2kg×(8m)2=112×4.2×64=22.4kgm2I_{\text{cm}} = \frac{1}{12} \times 4.2 \, \text{kg} \times (8 \, \text{m})^2 = \frac{1}{12} \times 4.2 \times 64 = 22.4 \, \text{kg} \cdot \text{m}^2

Parallel Axis Theorem

Since the pivot is not at the center of mass but at a distance d=8md = 8 \, \text{m} from the center of mass, we apply the parallel axis theorem: I=Icm+md2I = I_{\text{cm}} + m d^2 Where d=8md = 8 \, \text{m}: I=22.4+4.2×(82)=22.4+4.2×64=22.4+268.8=291.2kgm2I = 22.4 + 4.2 \times (8^2) = 22.4 + 4.2 \times 64 = 22.4 + 268.8 = 291.2 \, \text{kg} \cdot \text{m}^2

Potential Energy Change

When the rod is at the initial angle, it has potential energy given by: PE=mghPE = mgh Where hh is the height of the center of mass relative to the horizontal position. The center of mass is at l2=4m\frac{l}{2} = 4 \, \text{m} from the pivot. At an angle 5858^\circ: h=4sin(58)h = 4 \sin(58^\circ) Calculating hh: h=4sin(58)4×0.52992.1196mh = 4 \sin(58^\circ) \approx 4 \times 0.5299 \approx 2.1196 \, \text{m} Thus, PE=4.2×9.8×2.11964.2×20.887.696JPE = 4.2 \times 9.8 \times 2.1196 \approx 4.2 \times 20.8 \approx 87.696 \, \text{J}

Kinetic Energy in Horizontal Position

When the rod is horizontal, all the potential energy converts to rotational kinetic energy: KE=12Iω2KE = \frac{1}{2} I \omega^2 Setting PE=KEPE = KE: 87.696=12×291.2×ω287.696 = \frac{1}{2} \times 291.2 \times \omega^2 Solving for ω\omega: 87.696=145.6ω287.696 = 145.6 \omega^2 ω2=87.696145.60.6014\omega^2 = \frac{87.696}{145.6} \approx 0.6014 ω0.60140.775rad/s\omega \approx \sqrt{0.6014} \approx 0.775 \, \text{rad/s}

Conclusion

The angular speed of the rod when it is in a horizontal position is approximately 0.775 rad/s.

If you have any questions or need further details, feel free to ask! Here are some related questions you might consider:

  1. How would the result change if the mass of the rod was different?
  2. What would happen if the rod were not uniform?
  3. How does the angle of release affect the final angular speed?
  4. What is the effect of friction at the pivot point on the result?
  5. How would you calculate the linear speed of the end of the rod in the horizontal position?

Tip: When analyzing problems involving rotation and energy, always consider the conservation laws, as they simplify the calculations significantly.

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Math Problem Analysis

Mathematical Concepts

Physics
Rotational Dynamics
Conservation of Energy

Formulas

Icm = (1/12) * m * l^2
PE = mgh
KE = (1/2) * I * ω^2

Theorems

Parallel Axis Theorem

Suitable Grade Level

Grades 11-12