How can the forces on a pendulum be calculated when encountering a peg?

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SUMMARY

The discussion focuses on calculating the forces acting on a pendulum when it encounters a peg during its swing. The pendulum, defined by mass m and length L, is initially pulled back at an angle θ and released. The key equations derived involve the conservation of energy and projectile motion principles, leading to the conclusion that the relationship between cosθ, r, and α can be expressed as cosθ = r/L cosα - √3/2(1 - r/L). The solution emphasizes the importance of analyzing the pendulum's motion at the point of slack string and the transition to projectile motion.

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  • Understanding of pendulum dynamics and forces
  • Familiarity with conservation of energy principles
  • Knowledge of projectile motion equations
  • Basic trigonometry, specifically cosine functions
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  • Learn about projectile motion and its equations of motion
  • Explore the dynamics of pendulum motion and tension forces
  • Investigate the effects of angular displacement on pendulum behavior
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Homework Statement


a pendulum of mass m and length L is pulled back an angle θ and released. After the pendulum swings through its lowest point, it encounters a peg α degrees out and r meters from the top of the string. The mass swings up about the peg until the string becomes slack with the mass falling inward and hitting the peg. show that cosθ=r/Lcosα-√3/2(1-r/L)
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The Attempt at a Solution



I tried to find the forces on the pendulum at the initial and final position
Lcosθ-mg=0
Lsinθ=ma
rcosθ-mg=0
rsinθ=ma
but it doesn't seem to work at all. what I get is that r=L which is impossible.
 
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use conservation of energy, forces arent going to help you much here
 
You need to set up equations for each of the following:
1. The projectile motion problem that starts when the string is no longer taught.
2. The position (angle) at which the ball enters projectile motion (when the gravitational force inward surpasses the necessary centripetal force).
3. The ball's velocity (using conservation of energy) when it enters projectile motion.

Then you will need to combine all of those so that the angle you found in (2) cancels out, the time component you introduced in (1) also cancels out, and the velocity you solved for in (3) should cancel out. Once you solve this for cos(θ) you should get the answer written.
 

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