S+λP=0 forms a coaxial system, the radical axis being P=0 for all values of λ. Let g,f,c be the circle orthogonal to S+λP=0. Applying the condition of orthogonality, we get
2a(1+λ)g+2b(1−λ)f=0+c
or 2(ag−bf)λ+2(ag+bf)−c=0
Above relation holds for all values of λ and hence
2(ag−bf)=0,2(ag+bf)−c=0
∴g=c/4a,f=c/4b.
x2+y2+(c/2a)x+(c/2b)y+c=0.