x2 + y2 + 2gx + c = 0 ----------(1)
Differentiating w.r.t. x, we get:
2x + 2y(dy/dx) + 2g = 0
==> 2g = -( 2x + 2y(dy/dx) )
Substituting this value in eq(1), we get:
x2 + y2 - x[ 2x + 2y(dy/dx) ] + c = 0 ----------(2)
x2 + y2 - 2x2 - 2xy(dy/dx) + c = 0
Replacing dy/dx by -dx/dy -->
x2 + y2 - 2x2 + 2xy(dx/dy) + c = 0
y2 - x2 + 2xy(dx/dy) + c = 0
y2dy- x2dy+ 2xydx + cdy = 0
2xydx + ( y2- x2 + c )dy = 0 ----------(3)
Eq(3) is of type 3 equation:
Thus,
Here M = 2xy and N = y2- x2 + c
dN/dx = -2x
dM/dy = 2x
(Nx - My ) / M = (-2x - 2x) / 2xy
= -4x / 2xy
= -2 / y
I.F. = e∫-2/y dy = e-2logy = elog y^(-2) = y-2 = 1/y2
Multiplying I.F. with eq(3)
(1/y2) [2xydx + ( y2- x2 + c )dy = 0 ]
2x/y dx + (1 - (x/y)2 +cy-2) dy = 0 ---------(4)
This is now an exact first order differential equation, so the solution of this equation is
∫y constant Mdx + ∫(terms not containing x) = c
In eq(4), M = 2x/y
∫2x/y dx + ∫(1+cy) dy = c
x2/y + y -c/y = c
x2 + y2 - c = cy
x2 + y2 -cy - c = 0
The general equation of circle is x2 + y2 +2gx - 2fy + c = 0
Thus, x2 + y2 - (-2f)y - c = 0
x2 + y2 + 2fy - c = 0
This is the required orthognal trajectory of the eq(1).