Gravitational potential energy

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SUMMARY

The discussion focuses on calculating the gravitational potential energy of a teeter toy, consisting of a massless central stick of length L and two massless sticks of length l, each with a mass m at the end. The expression derived for gravitational potential energy as a function of the tilt angle θ is U(θ) = mg(L - Lcos(θ)). This equation indicates that at θ = 0, the potential energy is zero, and at θ = 90°, it reaches mgL. The importance of considering the center of mass for the two masses in the system is emphasized for accurate calculations.

PREREQUISITES
  • Understanding of gravitational potential energy (U = mgh)
  • Knowledge of trigonometric functions and their applications in physics
  • Familiarity with the concept of center of mass in a two-mass system
  • Basic principles of rotational dynamics and angular displacement
NEXT STEPS
  • Study the concept of center of mass in multi-body systems
  • Learn about the derivation of gravitational potential energy in different configurations
  • Explore the application of trigonometric identities in physics problems
  • Investigate the effects of angular displacement on potential energy in various mechanical systems
USEFUL FOR

Students studying physics, particularly those focusing on mechanics, educators teaching gravitational concepts, and anyone interested in understanding the dynamics of systems involving multiple masses and their potential energy calculations.

Lis
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Homework Statement


A teeter toy is composed of a massless central stick of length L and two massless sticks of length l attached at angles α, each with a mass m at the end (see the figure). We imagine tilting the toy by an angle θ from the upright position.

a) Find an expression for the gravitational potential energy of the whole object, as a function of θ.

Homework Equations



U=mgh

The Attempt at a Solution



U(θ) = mg(L-Lcos(θ))
 
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Lis said:
U(θ) = mg(L-Lcos(θ))
Can you provide your reasoning how you got this equation? A drawing would be helpful.
 
Skjermbilde 2016-10-19 kl. 12.27.59.png
 
Thanks for the drawing.
Lis said:
U(θ) = mg(L-Lcos(θ))
Is this correct? Let's see. It says that when θ = 0 (top figure), the potential energy is zero. That's defines your choice of reference. Your expression also says that when θ = 90o, the potential energy is mgL. Does that look right? What exactly finds itself at distance L above your reference when the toy is tipped 90o? To see how to treat the problem sensibly, consider that gravity is an external force acting on a system of two masses. Therefore we can view gravity as acting on the ____ of the two masses. (Fill in the blank.)
 
I don't think i understand you quite. Do you mean " Therefore we can view gravity as acting on the length of the two masses"?
 
You have a system of two equal masses. If you were to treat this system as if its entire mass of 2m were concentrated at one point, where would that point be?
 
on the top off L?
 
Potential energy, $$U_{total}= m_{total} \cdot g\cdot h_{center~of~mass}$$
Or you can calculate the height for the two masses separately, then calculate their respective potential energy and add them.
 

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