Because the cotangent function has a divide by zero problem when theta = 0 or pi, this translates to the Cartesian restriction y!=0
Add theta to both sides:
r = theta - 2cos^3(theta) - cot^2(theta)
Write cot^2(theta) as (cos^2(theta))/(sin^2(theta))
r = theta - 2cos^3(theta) - (cos^2(theta))/(sin^2(theta))
Multiply both sides by r^5sin^2(theta):
r^6sin^2(theta) = thetar^3(r^2sin^2(theta)) - 2r^3cos^3(theta)r^2(sin^2(theta)) - r^5cos^2(theta)
Substitute y for rsin(theta) and x for rcos(theta)
r^4y^2 = thetar^3y^2 - 2x^3y^2 - r^3x^2; y!=0
Use (x^2 + y^2)^(1/2) = r to make substitutions in accordance with the power of r:
(x^2 + y^2)^(2)y^2 = theta(x^2 + y^2)^(3/2)y^2 - 2x^3y^2 - (x^2 + y^2)^(3/2)x^2; y!=0
Collect like terms:
(x^2 + y^2)^(2)y^2 = (x^2 + y^2)^(3/2)(thetay^2 - x^2) - 2x^3y^2; y!=0
The substitution for theta breaks the above into 3 equations:
(x^2 + y^2)^(2)y^2 = (x^2 + y^2)^(3/2)(tan^-1(y/x)y^2 - x^2) - 2x^3y^2; y > 0 and x > 0
(x^2 + y^2)^(2)y^2 = (x^2 + y^2)^(3/2)(tan^-1(y/x) + pi)y^2 - x^2) - 2x^3y^2; y != 0 and x < 0
(x^2 + y^2)^(2)y^2 = (x^2 + y^2)^(3/2)((tan^-1(y/x) + 2pi)y^2 - x^2) - 2x^3y^2; y < 0 and x > 0