Conservation of Energy falling rod

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SUMMARY

The discussion focuses on determining the angle Theta at which the bottom end A of a uniform ladder, modeled as a slender rod with a mass of 14 kg and a length of 3 m, begins to lift off the ground when released from a vertical position. The conservation of energy principle is applied, utilizing equations for potential and kinetic energy, specifically T_1 + V_1 = T_2 + V_2. The moment of inertia for the rod is calculated as I = 1/3mL^2. Participants emphasize the need to analyze forces at point A and identify components of acceleration at angle Theta for a complete solution.

PREREQUISITES
  • Understanding of conservation of energy principles in physics
  • Familiarity with rotational dynamics and moment of inertia calculations
  • Knowledge of angular velocity and its relation to linear acceleration
  • Basic grasp of forces acting on rigid bodies in motion
NEXT STEPS
  • Study the derivation of the moment of inertia for different shapes, focusing on slender rods
  • Learn about the dynamics of rigid body motion and the role of forces in lifting scenarios
  • Explore the relationship between angular velocity and linear acceleration in falling objects
  • Investigate the conditions for static and dynamic equilibrium in mechanical systems
USEFUL FOR

This discussion is beneficial for physics students, educators, and anyone interested in understanding the mechanics of rigid body motion and energy conservation principles in practical scenarios.

dmoney123
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Homework Statement



A uniform ladder having mass 14kg and length 3m is released from rest when it is in the vertical position. If it is allowed to fall freely, determine the angle Theta at which the bottom end A starts to lift off the ground. For calculation assume the ladder is a slender rod and neglect friction at A.

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Homework Equations



T_1+V_1=T_2+V_2[/B]

The Attempt at a Solution



T_1=0

V_1=mgh
=mgL/2

T_2=1/2I(omega)^2
where I for end of rod = 1/3mL^2

so 1/2(1/3mL^2)(omega)^2

V_2=mgh
=mgL/2cos(Theta)

Solve T_1+V_1=T_2+V_2

g(1-cos(Theta))=(omega)^2

I think we now need solve for the forces at point A, but I don't know how...

I also don't really understand at what point A would "lift"

Any help is appreciated!

Thanks[/B]
 
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dmoney123 said:
g(1-cos(Theta))=(omega)^2
That's dimensionally wrong. You have an acceleration on the left and 1/time2 on the right.
dmoney123 said:
I think we now need solve for the forces at point A
Yes. What are the forces acting on the rod? What components of acceleration can you identify at angle theta?
 

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