a m p ; cos x ( ln ( cos x ) ) 2 d y + ( sin x − 3 y ( sin x ) ln ( cos x ) ) d x = 0 a m p ; cos x ( ln ( cos x ) ) 2 d y d x − 3 sin x ⋅ ln ( cos x ) y = − sin x a m p ; d y d x − 3 tan x ln ( cos x ) y = − tan x ( ln ( cos x ) ) 2 a m p ; d y d x + 3 tan x ln ( sec x ) y = − tan x ( ln ( sec x ) ) 2 a m p ; I.F. = e ∫ 3 tan x ln ( sec x ) d x = ( ln ( sec x ) ) 3 \begin{aligned}& \cos x(\ln (\cos x))^2 d y+(\sin x-3 y(\sin x) \ln (\cos x)) d x=0 \\& \cos x(\ln (\cos x))^2 \frac{d y}{d x}-3 \sin x \cdot \ln (\cos x) y=-\sin x \\& \frac{d y}{d x}-\frac{3 \tan x}{\ln (\cos x)} y=\frac{-\tan x}{(\ln (\cos x))^2} \\& \frac{d y}{d x}+\frac{3 \tan x}{\ln (\sec x)} y=\frac{-\tan x}{(\ln (\sec x))^2} \\& \text { I.F. }=e^{\int \frac{3 \tan x}{\ln (\sec x)} d x}=(\ln (\sec x))^3\end{aligned} am p ; cos x ( ln ( cos x ) ) 2 d y + ( sin x − 3 y ( sin x ) ln ( cos x )) d x = 0 am p ; cos x ( ln ( cos x ) ) 2 d x d y − 3 sin x ⋅ ln ( cos x ) y = − sin x am p ; d x d y − ln ( cos x ) 3 tan x y = ( ln ( cos x ) ) 2 − tan x am p ; d x d y + ln ( sec x ) 3 tan x y = ( ln ( sec x ) ) 2 − tan x am p ; I.F. = e ∫ l n ( s e c x ) 3 t a n x d x = ( ln ( sec x ) ) 3
a m p ; y × ( ln ( sec x ) ) 3 = − ∫ tan x ( ln ( sec x ) ) 2 ( ln ( sec x ) ) 3 d x a m p ; y × ( ln ( sec x ) ) 3 = − 1 2 ( ln ( sec x ) ) 2 + C a m p ; Given : x = π 4 , y = − 1 ln 2 a m p ; − 1 ln 2 × ( ln 2 ) 3 = − 1 2 × ( ln 2 ) 2 + C a m p ; ⇒ − 1 8 ln 2 × ( ln 2 ) 3 = − 1 2 × 1 4 ( ln 2 ) 2 + C a m p ; − 1 8 ( ln 2 ) 2 = − 1 8 ( ln 2 ) 2 + C a m p ; ⇒ C = 0 a m p ; ∴ y ( ln ( sec x ) ) 3 = − 1 2 ( ln ( sec x ) ) 2 + 0 a m p ; y = − 1 2 ln ( sec x ) a m p ; y = 1 2 ln ( cos x ) \begin{aligned}& y \times(\ln (\sec x))^3=-\int \frac{\tan x}{(\ln (\sec x))^2}(\ln (\sec x))^3 d x \\& y \times(\ln (\sec x))^3=-\frac{1}{2}(\ln (\sec x))^2+C \\& \text { Given }: x=\frac{\pi}{4}, y=-\frac{1}{\ln 2} \\& \frac{-1}{\ln 2} \times(\ln \sqrt{2})^3=-\frac{1}{2} \times(\ln \sqrt{2})^2+C \\& \Rightarrow \frac{-1}{8 \ln 2} \times(\ln 2)^3=\frac{-1}{2} \times \frac{1}{4}(\ln 2)^2+C \\& -\frac{1}{8}(\ln 2)^2=\frac{-1}{8}(\ln 2)^2+C \\& \Rightarrow C=0 \\& \therefore y(\ln (\sec x))^3=\frac{-1}{2}(\ln (\sec x))^2+0 \\& y=\frac{-1}{2 \ln (\sec x)} \\& y=\frac{1}{2 \ln (\cos x)}\end{aligned} am p ; y × ( ln ( sec x ) ) 3 = − ∫ ( ln ( sec x ) ) 2 tan x ( ln ( sec x ) ) 3 d x am p ; y × ( ln ( sec x ) ) 3 = − 2 1 ( ln ( sec x ) ) 2 + C am p ; Given : x = 4 π , y = − ln 2 1 am p ; ln 2 − 1 × ( ln 2 ) 3 = − 2 1 × ( ln 2 ) 2 + C am p ; ⇒ 8 ln 2 − 1 × ( ln 2 ) 3 = 2 − 1 × 4 1 ( ln 2 ) 2 + C am p ; − 8 1 ( ln 2 ) 2 = 8 − 1 ( ln 2 ) 2 + C am p ; ⇒ C = 0 am p ; ∴ y ( ln ( sec x ) ) 3 = 2 − 1 ( ln ( sec x ) ) 2 + 0 am p ; y = 2 ln ( sec x ) − 1 am p ; y = 2 ln ( cos x ) 1
a m p ; ∴ y ( π 6 ) = 1 2 ln ( cos π 6 ) a m p ; = 1 2 ln ( 3 2 ) a m p ; = 1 2 ( 1 2 ln 3 − ln 2 ) a m p ; = 1 ln 3 − ln 4 \begin{aligned}& \therefore y\left(\frac{\pi}{6}\right)=\frac{1}{2 \ln \left(\cos \frac{\pi}{6}\right)} \\& =\frac{1}{2 \ln \left(\frac{\sqrt{3}}{2}\right)} \\& =\frac{1}{2\left(\frac{1}{2} \ln 3-\ln 2\right)} \\& =\frac{1}{\ln 3-\ln 4}\end{aligned} am p ; ∴ y ( 6 π ) = 2 ln ( cos 6 π ) 1 am p ; = 2 ln ( 2 3 ) 1 am p ; = 2 ( 2 1 ln 3 − ln 2 ) 1 am p ; = ln 3 − ln 4 1