Let
tan − 1 x = θ \tan^{- 1}x = \theta tan − 1 x = θ ⇒ x = t a n θ ⇒ s i n θ = x 1 + x 2 ⇒ x = tan\theta ⇒ sin\theta = \dfrac{x}{\sqrt{1 + {x}^{2}}} ⇒ x = t an θ ⇒ s in θ = 1 + x 2 x
So, y = ( x 1 + x 2 + 1 1 + x 2 ) 2 − 1 y = {\left(\dfrac{x}{\sqrt{1 + {x}^{2}}} + \dfrac{1}{\sqrt{1 + {x}^{2}}}\right)}^{2} - 1 y = ( 1 + x 2 x + 1 + x 2 1 ) 2 − 1
⇒ y = ( x + 1 ) 2 1 + x 2 − 1 ⇒ y = \dfrac{{\left(x + 1\right)}^{2}}{1 + {x}^{2}} - 1 ⇒ y = 1 + x 2 ( x + 1 ) 2 − 1
⇒ y = 2 x 1 + x 2 = f ( x ) ⇒ y = \dfrac{2x}{1 + {x}^{2}} = f\left(x\right) ⇒ y = 1 + x 2 2 x = f ( x )
Now, d y d x = 1 2 1 1 − f 2 × f ′ ( x ) \dfrac{dy}{dx} = \dfrac{1}{2}\dfrac{1}{\sqrt{1 - {f}^{2}}} \times {f}^{'}\left(x\right) d x d y = 2 1 1 − f 2 1 × f ′ ( x )
= 1 2 1 1 − 4 x 2 ( 1 + x 2 ) 2 f ( x ) = \dfrac{1}{2}\dfrac{1}{\sqrt{1 - \dfrac{4{x}^{2}}{{\left(1 + {x}^{2}\right)}^{2}}}}f\left(x\right) = 2 1 1 − ( 1 + x 2 ) 2 4 x 2 1 f ( x )
= ( 1 + x 2 ) 2 ( x 2 − 1 ) f ′ ( x ) = \dfrac{\left(1 + {x}^{2}\right)}{2\left({x}^{2} - 1\right)}{f}^{'}\left(x\right) = 2 ( x 2 − 1 ) ( 1 + x 2 ) f ′ ( x )
= 1 + x 2 2 ( x 2 − 1 ) × 2 1 + x 2 − 2 x 2 ( 1 + x 2 ) 2 = \dfrac{1 + {x}^{2}}{2\left({x}^{2} - 1\right)} \times 2\dfrac{1 + {x}^{2} - 2{x}^{2}}{{\left(1 + {x}^{2}\right)}^{2}} = 2 ( x 2 − 1 ) 1 + x 2 × 2 ( 1 + x 2 ) 2 1 + x 2 − 2 x 2
⇒ d y d x = 1 − x 2 ( x 2 − 1 ) ( 1 + x 2 ) ⇒ \dfrac{dy}{dx} = \dfrac{1 - {x}^{2}}{\left({x}^{2} - 1\right)\left(1 + {x}^{2}\right)} ⇒ d x d y = ( x 2 − 1 ) ( 1 + x 2 ) 1 − x 2
⇒ d y = 1 − x 2 ( x 2 − 1 ) ( 1 + x 2 ) d x ⇒ dy = \dfrac{1 - {x}^{2}}{\left({x}^{2} - 1\right)\left(1 + {x}^{2}\right)}dx ⇒ d y = ( x 2 − 1 ) ( 1 + x 2 ) 1 − x 2 d x
Integrating both sides with respect to x x x
∫ d y = ∫ 1 − x 2 ( x 2 − 1 ) ( 1 + x 2 ) d x ∫ dy = ∫ \dfrac{1 - {x}^{2}}{\left({x}^{2} - 1\right)\left(1 + {x}^{2}\right)}dx ∫ d y = ∫ ( x 2 − 1 ) ( 1 + x 2 ) 1 − x 2 d x
⇒ y = − tan − 1 x + c ⇒ y = - \tan^{- 1}x + c ⇒ y = − tan − 1 x + c
Given, y ( 3 ) = π 6 ⇒ π 6 = − π 3 + c ⇒ c = π 2 y\left(\sqrt{3}\right) = \dfrac{\pi}{6} ⇒ \dfrac{\pi}{6} = - \dfrac{\pi}{3} + c ⇒ c = \dfrac{\pi}{2} y ( 3 ) = 6 π ⇒ 6 π = − 3 π + c ⇒ c = 2 π
y = − tan − 1 x + π 2 = cot − 1 x y = - \tan^{- 1}x + \dfrac{\pi}{2} = \cot^{- 1}x y = − tan − 1 x + 2 π = cot − 1 x
Now, y ( − 3 ) = cot − 1 x ( − 3 ) = 5 π 6 y\left(- \sqrt{3}\right) = \cot^{- 1}x\left(- \sqrt{3}\right) = \dfrac{5\pi}{6} y ( − 3 ) = cot − 1 x ( − 3 ) = 6 5 π