Solving the Geneva Wheel Problem Homework

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SUMMARY

The Geneva Wheel Problem was successfully solved using trigonometric relationships and calculus, specifically the quotient rule and chain rule for derivatives. The key equation derived was ωφ = ωθ (√2 cosθ - 1)/(3 - 2√2 cosθ), which expresses the angular velocity of φ in terms of θ. The solution involved recognizing the relationships between the sine and cosine functions and applying the Pythagorean theorem to derive necessary values. The discussion highlights the complexity of the problem and the potential for simpler methods.

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  • Understanding of trigonometric functions (sine, cosine, tangent)
  • Familiarity with calculus concepts (derivatives, chain rule, quotient rule)
  • Knowledge of angular motion analysis
  • Ability to apply the Pythagorean theorem in problem-solving
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Homework Statement


I'll attach the screenshot, it has everything.

Homework Equations


This is in the section of absolute motion analysis.

The Attempt at a Solution


I actually was able to solve the problem correctly, but it was annoyingly complicated and I'm curious as to whether there's a better way.

So, first off, I wanted to find a way to write \varphi in terms of \theta.

So, recognize that tan\varphi = Dsin\varphi/Dcos\varphi

The D*sin\varphi is always going to be equal to 100sinθ.

For cos\varphi it was a bit more tricky, but it's easy to recognize the relationship because the distance stays constant.

100√2 - 100cos(θ) = D*cos\varphi

So now we have:

tan\varphi = 100sinθ/(100√2 - 100cosθ)

And now I take the derivative. This is a quotient rule, and the derivative is going to be with respect to time, so through the chain rule we will have our angular velocities pulled out. Note that this derivative has been simplified from the raw form just a little.

sec2\varphi*ωphi = ωθ (√2*cosθ - 1)/(√2 - cosθ)2

So now the next conundrum is how to get rid of the damn sec2\varphi

Well, we recongnize that sec = Hypotenuse / Adjacent side,

And we've solved for the adjacent side already, it is equal to the cos\varphi equation, which is:

100√2 - 100cosθ

But what is the hypotenuse? Well, by the pythagorean theorem:

H2 = (100sinθ)2 + (100√2 - 100cosθ)2

So, now we have our values, and since it is sec2\varphi, we will use:

H2 / B2

Which gives (after some more excessive simplifying):

ωphi(3 - 2√2 cosθ)/(√2 - cosθ)2 = ωθ (√2*cosθ - 1)/(√2 - cosθ)2

Now notice the denominators are the same, they cancel out. Then just divide to solve for the angular velocity with respect to \varphi

You GET:

ωphi = ωθ (√2 cosθ - 1)/(3 - 2√2 cosθ)

And that IS the correct answer, it's just that it took a really long time and a ton of failed attempts before I finally solved it. I'm just wondering if there's a better way! Thanks!
 

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Your approach looks about as straight-forward as I could make it. I don't quite get your answer, but I've probably tripped on the trig and have't gone back to check.

You know your answer is correct, so well done! :smile:
 

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