Write the differential equation in standard linear form
Given
sin ( 2 x 2 ) ln ( tan x 2 ) d y + ( 4 x y − 4 2 x sin ( x 2 − π 4 ) ) d x = 0. \sin(2x^2)\,\ln(\tan x^2)\,dy + \left(4xy - 4\sqrt2\,x\sin\left(x^2-\frac\pi4\right)\right)dx=0. sin ( 2 x 2 ) ln ( tan x 2 ) d y + ( 4 x y − 4 2 x sin ( x 2 − 4 π ) ) d x = 0.
Rewrite as
sin ( 2 x 2 ) ln ( tan x 2 ) d y d x + 4 x y − 4 2 x sin ( x 2 − π 4 ) = 0. \sin(2x^2)\ln(\tan x^2)\frac{dy}{dx} + 4xy - 4\sqrt2\,x\sin\left(x^2-\frac\pi4\right)=0. sin ( 2 x 2 ) ln ( tan x 2 ) d x d y + 4 x y − 4 2 x sin ( x 2 − 4 π ) = 0.
So,
sin ( 2 x 2 ) ln ( tan x 2 ) d y d x = 4 2 x sin ( x 2 − π 4 ) − 4 x y . \sin(2x^2)\ln(\tan x^2)\frac{dy}{dx}=4\sqrt2\,x\sin\left(x^2-\frac\pi4\right)-4xy. sin ( 2 x 2 ) ln ( tan x 2 ) d x d y = 4 2 x sin ( x 2 − 4 π ) − 4 x y .
Now use
sin ( 2 x 2 ) = 2 sin ( x 2 ) cos ( x 2 ) , \sin(2x^2)=2\sin(x^2)\cos(x^2), sin ( 2 x 2 ) = 2 sin ( x 2 ) cos ( x 2 ) ,
and
2 sin ( x 2 − π 4 ) = sin x 2 − cos x 2 . \sqrt2\sin\left(x^2-\frac\pi4\right)=\sin x^2-\cos x^2. 2 sin ( x 2 − 4 π ) = sin x 2 − cos x 2 .
Hence,
4 2 x sin ( x 2 − π 4 ) = 4 x ( sin x 2 − cos x 2 ) . 4\sqrt2\,x\sin\left(x^2-\frac\pi4\right)=4x(\sin x^2-\cos x^2). 4 2 x sin ( x 2 − 4 π ) = 4 x ( sin x 2 − cos x 2 ) .
Also,
sin ( 2 x 2 ) = 2 sin x 2 cos x 2 . \sin(2x^2)=2\sin x^2\cos x^2. sin ( 2 x 2 ) = 2 sin x 2 cos x 2 .
Therefore,
\frac{dy}{dx}+rac{4x}{\sin(2x^2)\ln(\tan x^2)}y
=\frac{4x(\sin x^2-\cos x^2)}{2\sin x^2\cos x^2\ln(\tan x^2)}.
That is,
d y d x + 2 x sin x 2 cos x 2 ln ( tan x 2 ) y = 2 x ( sin x 2 − cos x 2 ) sin x 2 cos x 2 ln ( tan x 2 ) . \frac{dy}{dx}+\frac{2x}{\sin x^2\cos x^2\ln(\tan x^2)}y
=\frac{2x(\sin x^2-\cos x^2)}{\sin x^2\cos x^2\ln(\tan x^2)}. d x d y + sin x 2 cos x 2 ln ( tan x 2 ) 2 x y = sin x 2 cos x 2 ln ( tan x 2 ) 2 x ( sin x 2 − cos x 2 ) .
Recognize useful derivatives
Since
tan ( x 2 ) ′ = 2 x sec 2 ( x 2 ) , \tan(x^2)'=2x\sec^2(x^2), tan ( x 2 ) ′ = 2 x sec 2 ( x 2 ) ,
we get
d d x ln ( tan x 2 ) = 1 tan x 2 ⋅ 2 x sec 2 ( x 2 ) = 2 x sin x 2 cos x 2 . \frac{d}{dx}\ln(\tan x^2)=\frac{1}{\tan x^2}\cdot 2x\sec^2(x^2)
=\frac{2x}{\sin x^2\cos x^2}. d x d ln ( tan x 2 ) = tan x 2 1 ⋅ 2 x sec 2 ( x 2 ) = sin x 2 cos x 2 2 x .
Thus the equation becomes
d y d x + ( ln ( tan x 2 ) ) ′ ln ( tan x 2 ) y = ( ln ( tan x 2 ) ) ′ ln ( tan x 2 ) ( sin x 2 − cos x 2 ) . \frac{dy}{dx}+\frac{\big(\ln(\tan x^2)\big)'}{\ln(\tan x^2)}y
=\frac{\big(\ln(\tan x^2)\big)'}{\ln(\tan x^2)}(\sin x^2-\cos x^2). d x d y + ln ( tan x 2 ) ( ln ( tan x 2 ) ) ′ y = ln ( tan x 2 ) ( ln ( tan x 2 ) ) ′ ( sin x 2 − cos x 2 ) .
So it is a linear equation with integrating factor
I.F. = e ∫ ( ln ( tan x 2 ) ) ′ ln ( tan x 2 ) d x = e ln ∣ ln ( tan x 2 ) ∣ = ∣ ln ( tan x 2 ) ∣ . \text{I.F.}=e^{\int \frac{(\ln(\tan x^2))'}{\ln(\tan x^2)}dx}
= e^{\ln|\ln(\tan x^2)|}
=|\ln(\tan x^2)|. I.F. = e ∫ l n ( t a n x 2 ) ( l n ( t a n x 2 ) ) ′ d x = e l n ∣ l n ( t a n x 2 ) ∣ = ∣ ln ( tan x 2 ) ∣.
On the given interval and around the points used, we may take the integrating factor as
ln ( tan x 2 ) . \ln(\tan x^2). ln ( tan x 2 ) .
Multiply throughout by the integrating factor
Then
d d x ( y ln ( tan x 2 ) ) = d d x ln ( tan x 2 ) ⋅ ( sin x 2 − cos x 2 ) . \frac{d}{dx}\left(y\ln(\tan x^2)\right)
=\frac{d}{dx}\ln(\tan x^2)\cdot (\sin x^2-\cos x^2). d x d ( y ln ( tan x 2 ) ) = d x d ln ( tan x 2 ) ⋅ ( sin x 2 − cos x 2 ) .
But notice
d d x ( sin x 2 − cos x 2 ) = 2 x ( cos x 2 + sin x 2 ) , \frac{d}{dx}(\sin x^2-\cos x^2)=2x(\cos x^2+\sin x^2), d x d ( sin x 2 − cos x 2 ) = 2 x ( cos x 2 + sin x 2 ) ,
so a better route is to check for a simpler exact derivative.
Observe from the original rearranged equation:
ln ( tan x 2 ) d y d x + d d x ln ( tan x 2 ) y = d d x ln ( tan x 2 ) ( sin x 2 − cos x 2 ) . \ln(\tan x^2)\frac{dy}{dx}+\frac{d}{dx}\ln(\tan x^2)\,y
=\frac{d}{dx}\ln(\tan x^2)\,(\sin x^2-\cos x^2). ln ( tan x 2 ) d x d y + d x d ln ( tan x 2 ) y = d x d ln ( tan x 2 ) ( sin x 2 − cos x 2 ) .
Hence
d d x ( y ln ( tan x 2 ) ) = d d x ln ( tan x 2 ) ( sin x 2 − cos x 2 ) . \frac{d}{dx}\left(y\ln(\tan x^2)\right)
=\frac{d}{dx}\ln(\tan x^2)\,(\sin x^2-\cos x^2). d x d ( y ln ( tan x 2 ) ) = d x d ln ( tan x 2 ) ( sin x 2 − cos x 2 ) .
Now simplify the right-hand side:
d d x ln ( tan x 2 ) = 2 x sin x 2 cos x 2 , \frac{d}{dx}\ln(\tan x^2)=\frac{2x}{\sin x^2\cos x^2}, d x d ln ( tan x 2 ) = sin x 2 cos x 2 2 x ,
so
d d x ln ( tan x 2 ) ( sin x 2 − cos x 2 ) = 2 x ( sin x 2 − cos x 2 ) sin x 2 cos x 2 . \frac{d}{dx}\ln(\tan x^2)(\sin x^2-\cos x^2)
=\frac{2x(\sin x^2-\cos x^2)}{\sin x^2\cos x^2}. d x d ln ( tan x 2 ) ( sin x 2 − cos x 2 ) = sin x 2 cos x 2 2 x ( sin x 2 − cos x 2 ) .
But
sin x 2 − cos x 2 sin x 2 cos x 2 = 1 cos x 2 − 1 sin x 2 = sec x 2 − csc x 2 . \frac{\sin x^2-\cos x^2}{\sin x^2\cos x^2}
=\frac{1}{\cos x^2}-\frac{1}{\sin x^2}
=\sec x^2-\csc x^2. sin x 2 cos x 2 sin x 2 − cos x 2 = cos x 2 1 − sin x 2 1 = sec x 2 − csc x 2 .
This suggests direct integration is cumbersome. Instead, try the substitution
z = y − ( sin x 2 + cos x 2 ) . z=y-(\sin x^2+\cos x^2). z = y − ( sin x 2 + cos x 2 ) .
Then
z ′ = y ′ − 2 x sin x 2 + 2 x cos x 2 = y ′ + 2 x ( cos x 2 − sin x 2 ) . z'=y'-2x\sin x^2+2x\cos x^2 = y'+2x(\cos x^2-\sin x^2). z ′ = y ′ − 2 x sin x 2 + 2 x cos x 2 = y ′ + 2 x ( cos x 2 − sin x 2 ) .
From the differential equation in linear form,
y ′ + 2 x sin x 2 cos x 2 ln ( tan x 2 ) y = 2 x ( sin x 2 − cos x 2 ) sin x 2 cos x 2 ln ( tan x 2 ) . y'+\frac{2x}{\sin x^2\cos x^2\ln(\tan x^2)}y
=\frac{2x(\sin x^2-\cos x^2)}{\sin x^2\cos x^2\ln(\tan x^2)}. y ′ + sin x 2 cos x 2 ln ( tan x 2 ) 2 x y = sin x 2 cos x 2 ln ( tan x 2 ) 2 x ( sin x 2 − cos x 2 ) .
Now note that
sin x 2 cos x 2 ( sec x 2 − csc x 2 ) = sin x 2 − cos x 2 . \sin x^2\cos x^2(\sec x^2-\csc x^2)=\sin x^2-\cos x^2. sin x 2 cos x 2 ( sec x 2 − csc x 2 ) = sin x 2 − cos x 2 .
So the RHS is exactly
( ln ( tan x 2 ) ) ′ ln ( tan x 2 ) ( sin x 2 − cos x 2 ) . \frac{(\ln(\tan x^2))'}{\ln(\tan x^2)}(\sin x^2-\cos x^2). ln ( tan x 2 ) ( ln ( tan x 2 ) ) ′ ( sin x 2 − cos x 2 ) .
A natural trial solution is
y = sin x 2 − cos x 2 . y=\sin x^2-\cos x^2. y = sin x 2 − cos x 2 .
Check it:
y ′ = 2 x cos x 2 + 2 x sin x 2 = 2 x ( sin x 2 + cos x 2 ) . y'=2x\cos x^2+2x\sin x^2=2x(\sin x^2+\cos x^2). y ′ = 2 x cos x 2 + 2 x sin x 2 = 2 x ( sin x 2 + cos x 2 ) .
Then
y ′ + 2 x sin x 2 cos x 2 ln ( tan x 2 ) y = 2 x ( sin x 2 + cos x 2 ) + 2 x ( sin x 2 − cos x 2 ) sin x 2 cos x 2 ln ( tan x 2 ) , y'+\frac{2x}{\sin x^2\cos x^2\ln(\tan x^2)}y
=2x(\sin x^2+\cos x^2)+\frac{2x(\sin x^2-\cos x^2)}{\sin x^2\cos x^2\ln(\tan x^2)}, y ′ + sin x 2 cos x 2 ln ( tan x 2 ) 2 x y = 2 x ( sin x 2 + cos x 2 ) + sin x 2 cos x 2 ln ( tan x 2 ) 2 x ( sin x 2 − cos x 2 ) ,
which does not match. So instead solve systematically.
Use the substitution t = ln ( tan x 2 ) t=\ln(\tan x^2) t = ln ( tan x 2 )
Then
d t d x = 2 x sin x 2 cos x 2 . \frac{dt}{dx}=\frac{2x}{\sin x^2\cos x^2}. d x d t = sin x 2 cos x 2 2 x .
The differential equation becomes
d y d x + t ′ t y = t ′ t ( sin x 2 − cos x 2 ) . \frac{dy}{dx}+\frac{t'}{t}y=\frac{t'}{t}(\sin x^2-\cos x^2). d x d y + t t ′ y = t t ′ ( sin x 2 − cos x 2 ) .
Multiply by t t t :
t d y d x + t ′ y = t ′ ( sin x 2 − cos x 2 ) . t\frac{dy}{dx}+t'y=t'(\sin x^2-\cos x^2). t d x d y + t ′ y = t ′ ( sin x 2 − cos x 2 ) .
Thus
d d x ( t y ) = t ′ ( sin x 2 − cos x 2 ) . \frac{d}{dx}(ty)=t'(\sin x^2-\cos x^2). d x d ( t y ) = t ′ ( sin x 2 − cos x 2 ) .
Now let u = x 2 u=x^2 u = x 2 . Then d u = 2 x d x du=2x\,dx d u = 2 x d x , and
t = ln ( tan u ) , t ′ d x = d ( ln ( tan u ) ) . t=\ln(\tan u), \qquad t'\,dx=d(\ln(\tan u)). t = ln ( tan u ) , t ′ d x = d ( ln ( tan u )) .
So
t y = ∫ ( sin u − cos u ) d ( ln ( tan u ) ) + C . ty=\int (\sin u-\cos u)\,d(\ln(\tan u))+C. t y = ∫ ( sin u − cos u ) d ( ln ( tan u )) + C .
Use
d ( ln ( tan u ) ) = d u sin u cos u . d(\ln(\tan u))=\frac{du}{\sin u\cos u}. d ( ln ( tan u )) = sin u cos u d u .
Hence
∫ ( sin u − cos u ) d ( ln ( tan u ) ) = ∫ sin u − cos u sin u cos u d u = ∫ ( sec u − csc u ) d u . \int (\sin u-\cos u)\,d(\ln(\tan u))
=\int \frac{\sin u-\cos u}{\sin u\cos u}\,du
=\int (\sec u-\csc u)\,du. ∫ ( sin u − cos u ) d ( ln ( tan u )) = ∫ sin u cos u sin u − cos u d u = ∫ ( sec u − csc u ) d u .
Now,
∫ sec u d u = ln ∣ sec u + tan u ∣ , \int \sec u\,du=\ln|\sec u+\tan u|, ∫ sec u d u = ln ∣ sec u + tan u ∣ ,
∫ csc u d u = ln ∣ csc u − cot u ∣ . \int \csc u\,du=\ln|\csc u-\cot u|. ∫ csc u d u = ln ∣ csc u − cot u ∣.
Therefore,
∫ ( sec u − csc u ) d u = ln ∣ sec u + tan u ∣ − ln ∣ csc u − cot u ∣ + C . \int (\sec u-\csc u)du
=\ln|\sec u+\tan u| - \ln|\csc u-\cot u| + C. ∫ ( sec u − csc u ) d u = ln ∣ sec u + tan u ∣ − ln ∣ csc u − cot u ∣ + C .
Using identities,
sec u + tan u = 1 + sin u cos u , csc u − cot u = 1 − cos u sin u . \sec u+\tan u=\frac{1+\sin u}{\cos u},
\qquad
\csc u-\cot u=\frac{1-\cos u}{\sin u}. sec u + tan u = cos u 1 + sin u , csc u − cot u = sin u 1 − cos u .
This simplifies, but we do not actually need the full closed form. We use the given points where u = π 6 u=\frac\pi6 u = 6 π and u = π 3 u=\frac\pi3 u = 3 π .
Apply the initial condition
At
x = π 6 , u = π 6 , x=\sqrt{\frac\pi6}, \quad u=\frac\pi6, x = 6 π , u = 6 π ,
we have
y = 1 , y=1, y = 1 ,
and
t = ln ( tan π 6 ) = ln ( 1 3 ) = − 1 2 ln 3. t=\ln\left(\tan\frac\pi6\right)=\ln\left(\frac1{\sqrt3}\right)=-\frac12\ln 3. t = ln ( tan 6 π ) = ln ( 3 1 ) = − 2 1 ln 3.
So
t y = − 1 2 ln 3. ty=-\frac12\ln 3. t y = − 2 1 ln 3.
Now evaluate the integral from u = π 6 u=\frac\pi6 u = 6 π to u = π 3 u=\frac\pi3 u = 3 π :
( t y ) ∣ π / 3 − ( t y ) ∣ π / 6 = ∫ π / 6 π / 3 ( sec u − csc u ) d u . (ty)\Big|_{\pi/3}-(ty)\Big|_{\pi/6}
=\int_{\pi/6}^{\pi/3}(\sec u-\csc u)du. ( t y ) π /3 − ( t y ) π /6 = ∫ π /6 π /3 ( sec u − csc u ) d u .
But note the symmetry:
sec ( π 2 − u ) = csc u , csc ( π 2 − u ) = sec u . \sec\left(\frac\pi2-u\right)=\csc u,
\qquad
\csc\left(\frac\pi2-u\right)=\sec u. sec ( 2 π − u ) = csc u , csc ( 2 π − u ) = sec u .
Since the interval [ π 6 , π 3 ] \left[\frac\pi6,\frac\pi3\right] [ 6 π , 3 π ] is symmetric about π 4 \frac\pi4 4 π , we get
∫ π / 6 π / 3 sec u d u = ∫ π / 6 π / 3 csc u d u . \int_{\pi/6}^{\pi/3}\sec u\,du = \int_{\pi/6}^{\pi/3}\csc u\,du. ∫ π /6 π /3 sec u d u = ∫ π /6 π /3 csc u d u .
Hence
∫ π / 6 π / 3 ( sec u − csc u ) d u = 0. \int_{\pi/6}^{\pi/3}(\sec u-\csc u)du=0. ∫ π /6 π /3 ( sec u − csc u ) d u = 0.
Therefore,
( t y ) ∣ π / 3 = ( t y ) ∣ π / 6 = − 1 2 ln 3. (ty)\Big|_{\pi/3}=(ty)\Big|_{\pi/6}=-\frac12\ln 3. ( t y ) π /3 = ( t y ) π /6 = − 2 1 ln 3.
At x = π 3 x=\sqrt{\frac\pi3} x = 3 π , i.e. u = π 3 u=\frac\pi3 u = 3 π ,
t = ln ( tan π 3 ) = ln ( 3 ) = 1 2 ln 3. t=\ln\left(\tan\frac\pi3\right)=\ln(\sqrt3)=\frac12\ln 3. t = ln ( tan 3 π ) = ln ( 3 ) = 2 1 ln 3.
Thus
1 2 ln 3 ⋅ y ( π 3 ) = − 1 2 ln 3. \frac12\ln 3\cdot y\left(\sqrt{\frac\pi3}\right)=-\frac12\ln 3. 2 1 ln 3 ⋅ y ( 3 π ) = − 2 1 ln 3.
So
y ( π 3 ) = − 1. y\left(\sqrt{\frac\pi3}\right)=-1. y ( 3 π ) = − 1.
Hence
∣ y ( π 3 ) ∣ = 1. \left|y\left(\sqrt{\frac\pi3}\right)\right|=1. y ( 3 π ) = 1.
Final answer
1 \boxed{1} 1