f ( cos 4 θ ) = 2 2 − sec 2 θ f(\cos 4\theta)=\dfrac{2}{2-\sec^{2}\theta} f ( cos 4 θ ) = 2 − sec 2 θ 2
θ ∈ ( 0 , π 4 ) ∪ ( π 4 , π 2 ) \theta\in\left(0,\dfrac{\pi}{4}\right)\cup\left(\dfrac{\pi}{4},\dfrac{\pi}{2}\right) θ ∈ ( 0 , 4 π ) ∪ ( 4 π , 2 π )
f : ( − 1 , 1 ) → R f:(-1,1)\to\mathbb{R} f : ( − 1 , 1 ) → R
To find: f ( 1 3 ) \text{To find: } f\left(\dfrac{1}{3}\right) To find: f ( 3 1 )
( 1 ) 1 − 3 2 ( 2 ) 1 + 3 2 (1)\ 1-\sqrt{\dfrac{3}{2}} \qquad (2)\ 1+\sqrt{\dfrac{3}{2}} ( 1 ) 1 − 2 3 ( 2 ) 1 + 2 3
( 3 ) 1 − 2 3 ( 4 ) 1 + 2 3 (3)\ 1-\sqrt{\dfrac{2}{3}} \qquad (4)\ 1+\sqrt{\dfrac{2}{3}} ( 3 ) 1 − 3 2 ( 4 ) 1 + 3 2
Plan: simplify RHS using cos 2 θ \text{Plan: simplify RHS using } \cos 2\theta Plan: simplify RHS using cos 2 θ
then put cos 4 θ = 1 3 ⇒ cos 2 θ = ? \text{then put } \cos 4\theta=\dfrac{1}{3} \Rightarrow \cos 2\theta = ? then put cos 4 θ = 3 1 ⇒ cos 2 θ = ?
cos 2 θ = 2 cos 2 θ − 1 ⇒ cos 2 θ = 1 + cos 2 θ 2 \cos 2\theta=2\cos^{2}\theta-1 \Rightarrow \cos^{2}\theta=\dfrac{1+\cos 2\theta}{2} cos 2 θ = 2 cos 2 θ − 1 ⇒ cos 2 θ = 2 1 + cos 2 θ
sec 2 θ = 1 cos 2 θ = 2 1 + cos 2 θ \sec^{2}\theta=\dfrac{1}{\cos^{2}\theta}=\dfrac{2}{1+\cos 2\theta} sec 2 θ = cos 2 θ 1 = 1 + cos 2 θ 2
2 2 − sec 2 θ = 2 ( 1 + cos 2 θ ) 2 ( 1 + cos 2 θ ) − 2 \dfrac{2}{2-\sec^{2}\theta}=\dfrac{2(1+\cos 2\theta)}{2(1+\cos 2\theta)-2} 2 − sec 2 θ 2 = 2 ( 1 + cos 2 θ ) − 2 2 ( 1 + cos 2 θ )
= 1 + cos 2 θ cos 2 θ = 1 + sec 2 θ =\dfrac{1+\cos 2\theta}{\cos 2\theta}=1+\sec 2\theta = cos 2 θ 1 + cos 2 θ = 1 + sec 2 θ
f ( cos 4 θ ) = 1 + sec 2 θ f(\cos 4\theta)=1+\sec 2\theta f ( cos 4 θ ) = 1 + sec 2 θ
cos 4 θ = 2 cos 2 2 θ − 1 \cos 4\theta=2\cos^{2}2\theta-1 cos 4 θ = 2 cos 2 2 θ − 1
2 cos 2 2 θ − 1 = 1 3 ⇒ cos 2 2 θ = 2 3 2\cos^{2}2\theta-1=\dfrac{1}{3} \Rightarrow \cos^{2}2\theta=\dfrac{2}{3} 2 cos 2 2 θ − 1 = 3 1 ⇒ cos 2 2 θ = 3 2
cos 2 θ = ± 2 3 , sec 2 θ = ± 3 2 \cos 2\theta=\pm\sqrt{\dfrac{2}{3}},\qquad \sec 2\theta=\pm\sqrt{\dfrac{3}{2}} cos 2 θ = ± 3 2 , sec 2 θ = ± 2 3
θ ∈ ( 0 , π 4 ) : 2 θ ∈ ( 0 , π 2 ) ⇒ cos 2 θ > 0 \theta\in\left(0,\dfrac{\pi}{4}\right):\ 2\theta\in\left(0,\dfrac{\pi}{2}\right)\Rightarrow \cos 2\theta>0 θ ∈ ( 0 , 4 π ) : 2 θ ∈ ( 0 , 2 π ) ⇒ cos 2 θ > 0
f ( 1 3 ) = 1 + 3 2 f\left(\dfrac{1}{3}\right)=1+\sqrt{\dfrac{3}{2}} f ( 3 1 ) = 1 + 2 3
θ ∈ ( π 4 , π 2 ) : 2 θ ∈ ( π 2 , π ) ⇒ cos 2 θ < 0 \theta\in\left(\dfrac{\pi}{4},\dfrac{\pi}{2}\right):\ 2\theta\in\left(\dfrac{\pi}{2},\pi\right)\Rightarrow \cos 2\theta<0 θ ∈ ( 4 π , 2 π ) : 2 θ ∈ ( 2 π , π ) ⇒ cos 2 θ < 0
f ( 1 3 ) = 1 − 3 2 f\left(\dfrac{1}{3}\right)=1-\sqrt{\dfrac{3}{2}} f ( 3 1 ) = 1 − 2 3
Both attained: 1 + 3 2 and 1 − 3 2 \text{Both attained: } 1+\sqrt{\dfrac{3}{2}} \ \text{ and } \ 1-\sqrt{\dfrac{3}{2}} Both attained: 1 + 2 3 and 1 − 2 3
f ( 1 3 ) = 1 ± 3 2 ⇒ ( 1 ) and ( 2 ) \boxed{f\left(\dfrac{1}{3}\right)=1\pm\sqrt{\dfrac{3}{2}}}\quad\Rightarrow\ (1)\ \text{and}\ (2) f ( 3 1 ) = 1 ± 2 3 ⇒ ( 1 ) and ( 2 )