How Is the Arctan Derived in Relativistic Coulomb Scattering?

Trickster2004
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Hi. Landau and Lifgarbages give an equation describing the angle of deflection of a charged particle of a given initial velocity and impact parameter. It's given on page 102 of their Classical Theory of Fields, available here: http://books.google.com/books?id=QI...X&oi=book_result&ct=result&resnum=5#PPA102,M1. It's in the solution to Problem 1, at the bottom of the page.

I'm just curious where the equation in Problem 1 came from, in particular where the arctan came from. It's simple to solve 39.4 for the angle letting r-->infinity, but that gives an arccos, not an arctan. L-L just state that as the answer without working through it, as if it's obvious. Does anyone see how to derive it?

Thanks!
 
on Phys.org
If you have an equation of the form [tex]\cos\theta=\frac{a}{b}[/tex], then you can think of [itex]a[/itex] being the adjacent side of a right triangle, [itex]b[/itex] being the hypotenuse and hence [itex]\sqrt{b^2-a^2}[/itex] as the opposite side [tex]\implies \tan\theta=\frac{\sqrt{b^2-a^2}}{a}[/tex]
 

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