Help with extracting alpha from: -alpha-asin(sin(alpha)(r/l)

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The discussion focuses on extracting the angle α from a complex equation involving the Law of Cosines and trigonometric functions. The original poster seeks guidance on solving the equation for α while treating other variables as constants. Participants clarify issues with bracket placement and discuss the implications of the term (r/l) in the equation. It is noted that extracting α directly may not be feasible without clever manipulation or numerical methods, and that arcsine may be undefined for certain values of α. The conversation emphasizes the need for careful consideration of the equation's structure and constraints.
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I am using the Law of Cosines to extract and angle I need from a shaft that is turning on an air engine by piston oscillation and I am having a brain fart on if there are any identities I am missing that can help me pull '\alpha' from the right side of my equation:

acos(((h-pl)^{2}-r^{2}-l^{2})/(-2*r*l))-\pi=-\alpha-asin(sin(\alpha)(r/l))

I would like to solve the entire equation for \alpha and the other variables can be treated like constants.

Thanks for the help or attempts in advance.
 
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well - you didn't close the brackets in the arcsine, so it's hard to tell - but asin(sin(x))=x
 
I fixed the bracket issue, I apologize about that.

I am concerned with the (r/l) term inside of the equation. I understand that asin(sin(x))=x .. but I'm certain that asin(sin(x)(r/l)) --DNE-- (r/l)x
 
Oh I think I see, it wasn't clear to me if the r/l was multiplied with the alpha or the sine-alpha, or with the arcsine.
This what you mean?

\sin^{-1}( \frac{r}{l}\sin\alpha )

... afaik you can't extract alpha from this sort of equation - you need to be cleverer in the setup or use an approximation (or use a numerical method).

Equation is of form: x+sin-1(A.sin(x))=b ... solve for x. argh. (assuming the RHS is all constants)

Note: the arcsin will be undefined for some alpha, depending on the value of rl - you want |sin(α)| < l/r (something...)

Where did you start from?
 
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I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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