We have, z = 3 + 2 i c o s θ 1 − 3 i c o s θ , θ ∈ ( 0 , π 2 ) z = \dfrac{3 + 2icos\theta}{1 - 3icos\theta}, \theta \in \left(0, \dfrac{\pi}{2}\right) z = 1 − 3 i cos θ 3 + 2 i cos θ , θ ∈ ( 0 , 2 π )
⇒ z = 3 + 2 i c o s θ 1 − 3 i c o s θ × 1 + 3 i c o s θ 1 + 3 i c o s θ ⇒ z = \dfrac{3 + 2icos\theta}{1 - 3icos\theta} \times \dfrac{1 + 3icos\theta}{1 + 3icos\theta} ⇒ z = 1 − 3 i cos θ 3 + 2 i cos θ × 1 + 3 i cos θ 1 + 3 i cos θ
⇒ z = ( 3 + 2 i c o s θ ) ( 1 + 3 i c o s θ ) 1 + 9 cos 2 θ ⇒ z = \dfrac{\left(3 + 2icos\theta\right)\left(1 + 3icos\theta\right)}{1 + 9\cos^{2}\theta} ⇒ z = 1 + 9 cos 2 θ ( 3 + 2 i cos θ ) ( 1 + 3 i cos θ )
⇒ z = ( 3 − 6 cos 2 θ + 11 i c o s θ ) 1 + 9 cos 2 θ ⇒ z = \dfrac{\left(3 - 6\cos^{2}\theta + 11icos\theta\right)}{1 + 9\cos^{2}\theta} ⇒ z = 1 + 9 cos 2 θ ( 3 − 6 cos 2 θ + 11 i cos θ )
Now, R e ( z ) = 3 − 6 cos 2 θ 1 + 9 cos 2 θ = 0 Re \left(z\right) = \dfrac{3 - 6\cos^{2}\theta}{1 + 9\cos^{2}\theta} = 0 R e ( z ) = 1 + 9 cos 2 θ 3 − 6 cos 2 θ = 0
⇒ 3 − 6 cos 2 θ = 0 ⇒ 3 - 6\cos^{2}\theta = 0 ⇒ 3 − 6 cos 2 θ = 0
⇒ cos 2 θ = 3 6 ⇒ \cos^{2}\theta = \dfrac{3}{6} ⇒ cos 2 θ = 6 3
⇒ cos 2 θ = 1 2 ⇒ \cos^{2}\theta = \dfrac{1}{2} ⇒ cos 2 θ = 2 1
⇒ c o s θ = ± 1 2 ⇒ cos\theta = \pm \dfrac{1}{\sqrt{2}} ⇒ cos θ = ± 2 1
⇒ θ = π 4 , ∵ θ ∈ ( 0 , π 2 ) ⇒ \theta = \dfrac{\pi}{4}, ∵ \theta \in \left(0, \dfrac{\pi}{2}\right) ⇒ θ = 4 π , ∵ θ ∈ ( 0 , 2 π )
Hence, sin 2 3 θ + cos 2 θ \sin^{2}3\theta + \cos^{2}\theta sin 2 3 θ + cos 2 θ
= sin 2 ( 3 π 4 ) + cos 2 ( π 4 ) = \sin^{2}\left(\dfrac{3\pi}{4}\right) + \cos^{2}\left(\dfrac{\pi}{4}\right) = sin 2 ( 4 3 π ) + cos 2 ( 4 π )
= ( sin ( π − π 4 ) ) 2 + ( cos ( π 4 ) ) 2 = {\left(\sin \left(\pi - \dfrac{\pi}{4}\right)\right)}^{2} + {\left(\cos \left(\dfrac{\pi}{4}\right)\right)}^{2} = ( sin ( π − 4 π ) ) 2 + ( cos ( 4 π ) ) 2
= ( sin ( π 4 ) ) 2 + ( cos ( π 4 ) ) 2 = 1 = {\left(\sin \left(\dfrac{\pi}{4}\right)\right)}^{2} + {\left(\cos \left(\dfrac{\pi}{4}\right)\right)}^{2} = 1 = ( sin ( 4 π ) ) 2 + ( cos ( 4 π ) ) 2 = 1
Since, sin 2 θ + cos 2 θ = 1 \sin^{2}\theta + \cos^{2}\theta = 1 sin 2 θ + cos 2 θ = 1