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I have attempted converting $r=\tan(2θ)$ to cartesian coordinates:

$$r=\frac{2\sin(θ)\cos(θ)}{\cos^2(θ)-\sin^2(θ)}$$ $$r=\frac{2r\sin(θ)r\cos(θ)}{r^2\cos^2(θ)-r^2\sin^2(θ)}$$

$r^2 = x^2 + y^2\\ x = r \cos \theta\\ y = r \sin \theta$

$$r=\frac{2xy}{x^2-y^2} $$ $$(x^2+y^2)^{1/2}=\frac{2xy}{x^2-y^2} $$ $$(x^2+y^2)= \left(\frac{2xy}{x^2-y^2}\right)^2 $$ This doesn't graph properly on Wolfram Alpha, so I must have made a mistake.

User3910
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1 Answers1

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Not an answer, but an illustration.

For $\theta$ from $-\pi/4$ to $\pi/4$, you get the blue branch. It starts on the left for negative $\theta$. Because of the $\pi/2$ periodicity of $r$, the other branches are found by rotating the first by $\pi/2$ repeatedly.

enter image description here