(x2+y2)(cos2θsin2α+sin2θ)=(xtanα−ysinθ)2(x2+y2)(cos2θsin2α+sin2θ)=x2tan2α+y2sin2θ−2xytanαsinθ(cos2θsin2α+sin2θ−tan2α)x2+(cos2θsin2α+sin2θ−sin2θ)y2+2xytanαsinθ=0(cos2θsin2α+sin2θ−tan2α)x2+(cos2θsin2α)y2+2xytanαsinθ=0tanϕ=∣∣ ∣∣2√h2−aba+b∣∣ ∣∣tanϕ=2√4tan2αsin2θ−(cos2θsin2α+sin2θ−tan2α)(cos2θsin2α)(cos2θsin2α+sin2θ−tan2α)+(cos2θsin2α)
Taking the Numerator of R.H.S of (i)
=2√tan2αsin2θ−(cos2θsin2α+sin2θ−tan2α)cos2θsin2α∵cos2θsin2α=cos2θcos2αtan2α
Rearranging and factorising we get
=2tanα√(sin2θ+cos2θsin2α)(1−cos2θcos2α)=2tanα√(sin2θ+cos2θsin2α)(sin2θ+cos2θ−cos2θcos2α){∵1=sin2θ+cos2θ}=2tanα√(sin2θ+cos2θsin2α){sin2θ+cos2θ(1−cos2α)}=2tanα√(sin2θ+cos2θsin2α)(sin2θ+cos2θsin2α)=2tanα(sin2θ+cos2θsin2α)
Taking the Denomirator of (i) we get
=2cos2θsin2α+sin2θ−tan2α=1cos2α(2cos2θsin2αcos2α+sin2θcos2α−sin2α)=1cos2α(2cos2θsin2αcos2α+sin2θcos2α−(sin2θ+cos2θ)sin2α)=1cos2α(sin2θ(cos2α−sin2α)+cos2θsin2α(2cos2α−1))=cos2α−sin2αcos2α(sin2θ+cos2θsin2α)=(1−tan2α)(sin2θ+cos2θsin2α)
Now using (i)
tanϕ=NumeratorDenomirator⇒tanϕ=2tanα(sin2θ+cos2θsin2α)(1−tan2α)(sin2θ+cos2θsin2α)⇒tanϕ=2tanα(1−tan2α)⇒tanϕ=tan2α⇒ϕ=2α
Hence proved.