Right triangle, describe dx as dθ

quantum13
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1. Homework Statement
This is part of a find the electric field problem. I've narrowed down the part I find confusing.

Consider a right triangle, with legs of length x and R. Angle θ is opposite x. Leg x is a segment of a ray starting where lines x and R intersect. There is a differential length dx along line x (it is at a vertex of the right triangle). Find dx in terms of R and θ.


2. Homework Equations
standard trig functions, pythagorean theorem?


3. The Attempt at a Solution
The answer according to the solutions manual is dx = (R/cos^2 θ) dθ. Obviously, I cannot understand at all where that came from.

I did get R tan ( θ + dθ) = x + dx but that isn't very helpful either
 
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Since x = R tan(θ), then dx/dθ = R sec2θ.

So what does this give for dx?
 
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man, this makes me feel dumb

thanks for pointing out that dx = (1 / cos2θ) dθ. i would have never guessed that trick by myself

but where does the R come into that equation?
 
Just a careless typo. I fixed it with an edit. dx/dθ = R sec2θ
 
this stupid part is i didnt realize it was a typo either.. but thank you for this trick. i never thought like that before
 
Prove $$\int\limits_0^{\sqrt2/4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx = \frac{\pi^2}{8}.$$ Let $$I = \int\limits_0^{\sqrt 2 / 4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx. \tag{1}$$ The representation integral of ##\arcsin## is $$\arcsin u = \int\limits_{0}^{1} \frac{\mathrm dt}{\sqrt{1-t^2}}, \qquad 0 \leqslant u \leqslant 1.$$ Plugging identity above into ##(1)## with ##u...
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