The Importance of Understanding Different Formulas in Uniform Circular Motion

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The discussion centers on the confusion surrounding the application of the formula T = 2πr/v in solving for the period of a conical pendulum. While the formula is valid, the solution is expressed in terms of the angle β and the length L, making it more practical for measurement. The key point is that the velocity v depends on the angle β, which complicates direct comparisons between the two formulas. By substituting expressions for v and R that relate to β, the equivalence of the two methods for calculating the period can be demonstrated. Understanding these relationships is crucial for correctly applying the formulas in uniform circular motion scenarios.
paprika213
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https://i.imgur.com/4nynNBg.png

I cannot understand for the life of me why this problem doesn't just use T = 2πr/v to solve for the period to get T = 2π(Lsinβ)/v. Instead, it rearranges the formula for a(rad) = (4π^2R)/T^2 to solve for T, and arrives at a totally different answer, T = 2π√(Lcosβ/g).

So why doesn't the formula T = 2πr/v apply in this case?
 
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paprika213 said:
https://i.imgur.com/4nynNBg.png

I cannot understand for the life of me why this problem doesn't just use T = 2πr/v to solve for the period to get T = 2π(Lsinβ)/v. Instead, it rearranges the formula for a(rad) = (4π^2R)/T^2 to solve for T, and arrives at a totally different answer, T = 2π√(Lcosβ/g).

So why doesn't the formula T = 2πr/v apply in this case?
The formula applies but the solution is cast in terms of angle ##\beta## instead of the speed. That's because you need to measure both ##R## and ##v## to find the period. It is more practical to find the period by measuring angle ##\beta## and the unchanging length ##L##..
 
kuruman said:
The formula applies but the solution is cast in terms of angle ##\beta## instead of the speed. That's because you need to measure both ##R## and ##v## to find the period. It is more practical to find the period by measuring angle ##\beta## and the unchanging length ##L##..
Thank you, but it still doesn't seem like T = 2π(Lsinβ)/v and T = 2π√(Lcosβ/g) would equate. It seems like they would give different values for the period
 
paprika213 said:
Thank you, but it still doesn't seem like T = 2π(Lsinβ)/v and T = 2π√(Lcosβ/g) would equate. It seems like they would give different values for the period
How do you know? What is ##v## in your estimation? Note that it depends on ##\beta##. For example, if ##\beta=0## then ##v=0## because the conical pendulum will be hanging vertically. Can you relate ##v## to ##\beta##? Replacing ##v## and ##R## with expressions that depend on ##\beta## in ##T=\frac{2\pi R}{v}## should convince you that the two ways of writing the period are equivalent.
 
paprika213 said:
https://i.imgur.com/4nynNBg.png

I cannot understand for the life of me why this problem doesn't just use T = 2πr/v to solve for the period to get T = 2π(Lsinβ)/v. Instead, it rearranges the formula for a(rad) = (4π^2R)/T^2 to solve for T, and arrives at a totally different answer, T = 2π√(Lcosβ/g).

So why doesn't the formula T = 2πr/v apply in this case?
Hello @paprika213 .
:welcome:
You should use the upload button to upload any image you refer to on this forum.
Uniform Circ Mo 4nynNBg.png
 

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The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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