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,