d y d x + y ( 4 x sin ( 2 x 2 ) ln ( tan x 2 ) ) = 4 2 x sin ( x 2 − π 4 ) sin ( 2 x 2 ) ln ( tan x 2 ) {{dy} \over {dx}} + y\left( {{{4x} \over {\sin (2{x^2})\ln (\tan {x^2})}}} \right) = {{4\sqrt 2 x\sin \left( {{x^2} - {\pi \over 4}} \right)} \over {\sin (2{x^2})\ln (\tan {x^2})}} d x d y + y ( s i n ( 2 x 2 ) l n ( t a n x 2 ) 4 x ) = s i n ( 2 x 2 ) l n ( t a n x 2 ) 4 2 x s i n ( x 2 − 4 π )
I . F = e ∫ 4 x sin ( 2 x 2 ) ln ( tan x 2 ) d x I.F = {e^{\int {{{4x} \over {\sin (2{x^2})\ln (\tan {x^2})}}dx} }} I . F = e ∫ s i n ( 2 x 2 ) l n ( t a n x 2 ) 4 x d x
= e ln ∣ ln ( tan x 2 ) = ln ( tan x 2 ) = {e^{\ln |\ln (\tan {x^2})}} = \ln (\tan {x^2}) = e l n ∣ l n ( t a n x 2 ) = ln ( tan x 2 )
∴ \therefore ∴ ∫ d ( y . ln ( tan x 2 ) ) = ∫ 4 2 x sin ( x 2 − π 4 ) sin ( 2 x 2 ) d x \int {d(y.\ln (\tan {x^2})) = \int {{{4\sqrt 2 x\sin \left( {{x^2} - {\pi \over 4}} \right)} \over {\sin (2{x^2})}}dx} } ∫ d ( y . ln ( tan x 2 )) = ∫ s i n ( 2 x 2 ) 4 2 x s i n ( x 2 − 4 π ) d x
⇒ y ln ( tan x 2 ) = ln ∣ sec x 2 + tan x 2 c o s e c x 2 − cot x 2 ∣ + C \Rightarrow y\ln (\tan {x^2}) = \ln \left| {{{\sec {x^2} + \tan {x^2}} \over {{\mathop{\rm cosec}\nolimits} \,{x^2} - \cot {x^2}}}} \right| + C ⇒ y ln ( tan x 2 ) = ln cosec x 2 − c o t x 2 s e c x 2 + t a n x 2 + C
ln ( 1 3 ) = ln ( 3 3 2 − 3 ) + C \ln \left( {{1 \over {\sqrt 3 }}} \right) = \ln \left( {{{{3 \over {\sqrt 3 }}} \over {2 - \sqrt 3 }}} \right) + C ln ( 3 1 ) = ln ( 2 − 3 3 3 ) + C
e = ln ( 1 3 ) − ln ( 3 2 − 3 ) e = \ln \left( {{1 \over {\sqrt 3 }}} \right) - \ln \left( {{{\sqrt 3 } \over {2 - \sqrt 3 }}} \right) e = ln ( 3 1 ) − ln ( 2 − 3 3 )
For y ( π 3 ) y\left( {\sqrt {{\pi \over 3}} } \right) y ( 3 π )
y ln ( 3 ) = ln ∣ 2 + 3 2 3 + 1 3 ∣ + ln ( 1 3 ) − ln ( 3 2 3 ) y\ln \left( {\sqrt 3 } \right) = \ln \left| {{{2 + \sqrt 3 } \over {{2 \over {\sqrt 3 }} + {1 \over {\sqrt 3 }}}}} \right| + \ln \left( {{1 \over {\sqrt 3 }}} \right) - \ln \left( {{{\sqrt 3 } \over {2\sqrt 3 }}} \right) y ln ( 3 ) = ln 3 2 + 3 1 2 + 3 + ln ( 3 1 ) − ln ( 2 3 3 )
= ln ( 2 + 3 ) + ln ( 1 3 ) + ln ( 1 3 ) − ln ( 3 2 − 3 ) = \ln \left( {2 + \sqrt 3 } \right) + \ln \left( {{1 \over {\sqrt 3 }}} \right) + \ln \left( {{1 \over {\sqrt 3 }}} \right) - \ln \left( {{{\sqrt 3 } \over {2 - \sqrt 3 }}} \right) = ln ( 2 + 3 ) + ln ( 3 1 ) + ln ( 3 1 ) − ln ( 2 − 3 3 )
⇒ y ln 3 = ln ( 1 3 ) \Rightarrow y\ln \sqrt 3 = \ln \left( {{1 \over {\sqrt 3 }}} \right) ⇒ y ln 3 = ln ( 3 1 )
⇒ y 2 ln 3 = − 1 2 ln 3 \Rightarrow {y \over 2}\ln 3 = - {1 \over 2}\ln 3 ⇒ 2 y ln 3 = − 2 1 ln 3
⇒ y = 1 \Rightarrow y = 1 ⇒ y = 1
∴ \therefore ∴ ∣ y ( π 3 ) ∣ = 1 \left| {y\left( {\sqrt {{\pi \over 3}} } \right)} \right| = 1 y ( 3 π ) = 1 .