Parallel Axis Theorem | Kinetic and Potential Energy

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SUMMARY

The discussion focuses on the application of the Parallel Axis Theorem to calculate the angular speed of a rigid body formed by three identical rods arranged in an "H" shape. The body rotates about a horizontal axis along one leg of the "H" after being released from a horizontal position. The correct moment of inertia is derived using the formula I = I_com + Mh^2, leading to a total inertia of I_total = 4.5mL^2. The final angular speed is calculated to be ω = 6.11 rad/s, although the user expresses uncertainty regarding the rotational inertia calculations.

PREREQUISITES
  • Understanding of the Parallel Axis Theorem
  • Knowledge of rotational inertia and its calculation
  • Familiarity with energy conservation principles in mechanics
  • Basic proficiency in angular kinematics
NEXT STEPS
  • Study the derivation of the Parallel Axis Theorem in detail
  • Learn how to calculate the moment of inertia for composite bodies
  • Explore energy conservation in rotational motion
  • Investigate the differences between angular speed (ω) and linear speed (v)
USEFUL FOR

Students in physics, particularly those studying mechanics, as well as educators and anyone interested in understanding rotational dynamics and the application of the Parallel Axis Theorem.

Lahooty
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Homework Statement



A rigid body is made of three identical rods, each with length L = 0.525 m, fastened together in the form of a letter H, as in Figure 10-56 below. The body is free to rotate about a horizontal axis that runs along the length of one of the legs of the H. The body is allowed to fall from rest from a position in which the plane of the H is horizontal. What is the angular speed of the body when the plane of the H is vertical?

http://www.webassign.net/hrw/10-56.gif

Homework Equations





The Attempt at a Solution



I_1 = 0

I_2 = m/L∫x^2dx from 0 to L
I_2 = (1/3)*mL^2

I_3 = mL^2

I_total = (4/3)mL^2

E_Mec,Top = E_Mec, Bot

U_T + K_T = U_B + K_B

3*m*g*L + 0 = 0 + (1/2)*Iv^2

3*m*g*L = 1.5*m*L^2*v^2

2*g = L*v^2

[(2*g)/L]^.5 = v

v = 6.11 rad/s

This is wrong I'm pretty sure that I'm calculating the Rotational Inertia incorrectly. I don't know how to use the parallel axis theorem, especially not on three continuous bodies. I know that the formula is:

I = I_com+Mh^2

When I use that to calculate the Inertia, I get:

I_com = 3/2mL^2

I = 3/2mL^2 + 3mL^2
I = 4.5mL^2
 
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Lahooty said:
U_T + K_T = U_B + K_B

3*m*g*L + 0 = 0 + (1/2)*Iv^2
Why [itex]3mgL[/itex]? And on the right hand side, the usual symbol for angular speed is [itex]\omega[/itex], not [itex]v[/itex], which is usually taken to mean translational speed.
 

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