Let sin − 1 x α = cos − 1 x β = k ⇒ sin − 1 x + cos − 1 x = k ( α + β ) {{{{\sin }^{ - 1}}x} \over \alpha } = {{{{\cos }^{ - 1}}x} \over \beta } = k \Rightarrow {\sin ^{ - 1}}x + {\cos ^{ - 1}}x = k(\alpha + \beta ) α s i n − 1 x = β c o s − 1 x = k ⇒ sin − 1 x + cos − 1 x = k ( α + β ) ⇒ α + β = π 2 k \Rightarrow \alpha + \beta = {\pi \over {2k}} ⇒ α + β = 2 k π Now, 2 π α α + β = 2 π α π 2 k = 4 k α = 4 sin − 1 x {{2\pi \,\alpha } \over {\alpha + \beta }} = {{2\pi \,\alpha } \over {{\pi \over {2k}}}} = 4k\alpha = 4{\sin ^{ - 1}}x α + β 2 π α = 2 k π 2 π α = 4 k α = 4 sin − 1 x Here sin ( 2 π α α + β ) = sin ( 4 sin − 1 x ) \sin \left( {{{2\pi \,\alpha } \over {\alpha + \beta }}} \right) = \sin (4{\sin ^{ - 1}}x) sin ( α + β 2 π α ) = sin ( 4 sin − 1 x ) Let sin − 1 x = θ {\sin ^{ - 1}}x = \theta sin − 1 x = θ ∵ \because ∵ x ∈ ( 0 , 1 2 ) ⇒ θ ∈ ( 0 , π 4 ) x \in \left( {0,{1 \over {\sqrt 2 }}} \right) \Rightarrow \theta \in \left( {0,{\pi \over 4}} \right) x ∈ ( 0 , 2 1 ) ⇒ θ ∈ ( 0 , 4 π ) ⇒ x = sin θ \Rightarrow x = \sin \theta ⇒ x = sin θ ⇒ cos θ = 1 − x 2 \Rightarrow \cos \theta = \sqrt {1 - {x^2}} ⇒ cos θ = 1 − x 2 ⇒ sin 2 θ = 2 x . 1 − x 2 \Rightarrow \sin 2\theta = 2x\,.\,\sqrt {1 - {x^2}} ⇒ sin 2 θ = 2 x . 1 − x 2 ⇒ cos 2 θ = 1 − 4 x 2 ( 1 − x 2 ) = ( 2 x 2 − 1 ) 2 = 1 − 2 x 2 \Rightarrow \cos 2\theta = \sqrt {1 - 4{x^2}(1 - {x^2})} = \sqrt {{{(2{x^2} - 1)}^2}} = 1 - 2{x^2} ⇒ cos 2 θ = 1 − 4 x 2 ( 1 − x 2 ) = ( 2 x 2 − 1 ) 2 = 1 − 2 x 2 ∵ \because ∵ ( cos 2 θ > 0 a s 2 θ ∈ ( 0 , π 2 ) ) \left( {\cos 2\theta > 0\,\mathrm{as}\,2\theta \in \left( {0,{\pi \over 2}} \right)} \right) ( cos 2 θ > 0 as 2 θ ∈ ( 0 , 2 π ) ) ⇒ sin 4 θ = 2 . 2 x 1 − x 2 ( 1 − 2 x 2 ) \Rightarrow \sin 4\theta = 2\,.\,2x\sqrt {1 - {x^2}} (1 - 2{x^2}) ⇒ sin 4 θ = 2 . 2 x 1 − x 2 ( 1 − 2 x 2 ) = 4 x 1 − x 2 ( 1 − 2 x 2 ) = 4x\sqrt {1 - {x^2}} (1 - 2{x^2}) = 4 x 1 − x 2 ( 1 − 2 x 2 )