Or, changing the origin to the vertex of the figure

x2 ⁄ a2 − 2x ⁄ a + y2 ⁄ b2 = 0,

giving

(x − a)2 ⁄ a2 + y2 ⁄ b2 = 1.

Then, transferring to polar coordinates, where r · cos θ = x, r · sin θ = y, we have

(r · cos2 θ) ⁄ a2 − (2 cos θ) ⁄ a + (r · sin θ) ⁄ b2 = 0,

{564}

which is equivalent to

r = 2 a b2 cos θ ⁄ (b2 cos2 θ + a2 sin2 θ),

or, eliminating the sine-function,