Speed of ball on pendulum with Mechanical Energy

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Homework Help Overview

The discussion revolves around the mechanics of a pendulum, specifically analyzing the energy transformations as it swings from an initial height to a final position. The participants explore the relationship between gravitational potential energy and kinetic energy in the context of a pendulum released from an angle.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants analyze energy conservation principles, questioning how to accurately determine the height difference in the context of the pendulum's motion. There is discussion about whether to use the full length of the pendulum or a component based on the angle of release.

Discussion Status

Several participants have provided insights into the energy conservation approach, with some clarifying the importance of height in determining gravitational potential energy. There is ongoing exploration of the trigonometric relationships involved and how they affect the calculations. The discussion is active, with participants questioning and refining their understanding of the problem.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the use of certain variables or require specific forms of the answer. The angle of release is specified in the problem statement, influencing the calculations discussed.

VaitVhat52
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Homework Statement
A pendulum consists of a small object of mass m fastened to the end of an inextensible cord of length L. Initially, the pendulum is drawn aside through an angle of 60° with the vertical and held by a horizontal string as shown in the diagram (Attached). This string is burned so that the pendulum is released to swing to and fro.
Relevant Equations
Gravitational Potential Energy = mgh
Kinetic Energy = 1/2mv^2
Screenshot 2023-12-10 162321.png


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Started by analyzing the change in energy from the initial position to the final position which gives us mgh=1/2mv^2
Since we are trying to find speed, we rearrange the equation to solve for v, which gives us √2gL.

My question is, do we need to take a component of L for √2gL because it is at an angle or is it just L since that is the height at the final position?
 
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VaitVhat52 said:
Homework Statement: A pendulum consists of a small object of mass m fastened to the end of an inextensible cord of length L. Initially, the pendulum is drawn aside through an angle of 60° with the vertical and held by a horizontal string as shown in the diagram (Attached). This string is burned so that the pendulum is released to swing to and fro.
Relevant Equations: Gravitational Potential Energy = mgh
Kinetic Energy = 1/2mv^2

View attachment 337046

View attachment 337051

Started by analyzing the change in energy from the initial position to the final position which gives us mgh=1/2mv^2
Since we are trying to find speed, we rearrange the equation to solve for v, which gives us √2gL.

My question is, do we need to take a component of L for √2gL because it is at an angle or is it just L since that is the height at the final position?
Gravitational PE depends on the height difference. Does the object start at height ##l## above the lowest point?
 
A foolproof statement of energy conservation is in terms of changes in kinetic and potential energy, $$\Delta K+\Delta U=0.$$ Here ##\Delta K = (\frac{1}{2}mv^2-0)## and ##\Delta U= mg(\text{(Final height)-(Initial height)}.## You can now answer you own question, although I see that @PeroK has already done so.
 
PeroK said:
Gravitational PE depends on the height difference. Does the object start at height ##l## above the lowest point?
No, it starts at the as high as the vertical component of L.
Would that then make it √2g(L-LCosθ) or am I missing something?
 
VaitVhat52 said:
No, it starts at the as high as the vertical component of L.
Would that then make it √2g(L-LCosθ) or am I missing something?
You're still missing something. Check your trigonometry. Which I see you've just done! Well spotted.
 
PS that expression ##L(1 - \cos \theta)## comes up in a lot of problems. It's worth making a mental note of that.
 
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One last thing:
Since it asks for the answer in terms of ##g## and ##L##, are we allowed to have ##Cosθ## as part of the answer?
 
VaitVhat52 said:
One last thing:
Since it asks for the answer in terms of ##g## and ##L##, are we allowed to have ##Cosθ## as part of the answer?
Isn't the value of θ given in the diagram?
 
kuruman said:
Isn't the value of θ given in the diagram?
Ah that's correct.
So the final answer would be ##\sqrt{2gL(1-\frac{1}{2})}##
 
  • #10
VaitVhat52 said:
Ah that's correct.
So the final answer would be ##\sqrt{2gL(1-\frac{1}{2})}##
which simplifies to…?
 

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