Animated Solution for Mathematics - Differential Equations: Let y=y(x) be the solution of the differential equation dxdy=sinx(secx−sinxtanx)(tanx)+y,x∈(0,2π) satisfying the condition y(4π)=2. Then, y(3π) is
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Visualized Solution
The Given Equation
Given differential equation: dxdy=sinx(secx−sinxtanx)tanx+y
Domain: x∈(0,2π)
Initial condition: y(4π)=2
Simplifying the Denominator
Let's focus on the denominator: D=sinx(secx−sinxtanx)
We need to convert everything to sine and cosine.
Substitute secx=cosx1 and tanx=cosxsinx
Substituting Sine and Cosine
D=sinx(cosx1−cosxsin2x)
D=sinx(cosx1−sin2x)
Applying Trigonometric Identity
Using the fundamental identity: 1−sin2x=cos2x
D=sinx(cosxcos2x)
D=sinxcosx
Rearranging to Standard Form
The equation becomes: dxdy=sinxcosxtanx+y
Split the fraction: dxdy=sinxcosxtanx+sinxcosxy
Simplifying the Terms
First term: sinxcosxtanx=cosxsinxcosxsinx=cos2x1=sec2x
Second term: sinxcosxy=2sinxcosx2y=2ycsc2x
dxdy=sec2x+2ycsc2x
Standard Linear Differential Equation
Rearrange to standard LDE form: dxdy−(2csc2x)y=sec2x
Substitute these values: 2⋅cot(4π)=ln∣tan(4π)∣+C
Finding the Constant C
We know cot(4π)=1 and tan(4π)=1
2(1)=ln(1)+C
Since ln(1)=0, we get C=2
Particular solution: ycotx=ln∣tanx∣+2
Explicit form: y(x)=tanx(ln∣tanx∣+2)
Final Substitution for y(3π)
We need to find the value of y at x=3π
Substitute x=3π into the explicit form:
y(3π)=tan(3π)(ln∣tan(3π)∣+2)
Final Calculation
We know tan(3π)=3
y(3π)=3(ln3+2)
Rearranging to match options: y(3π)=3(2+ln3)
This matches option A.
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The Sigma Insight: Linear Differential Equations
The Art of Simplifying the Chaos
Welcome, fellow traveler on the JEE journey. Today, we are going to dismantle a problem that, at first glance, looks like a nightmare of trigonometric functions.
You see an expression like
dxdy=sinx(secx−sinxtanx)tanx+y
and your instinct might be to panic. But let me tell you a secret: in the world of JEE Advanced, complexity is often just a mask for elegance. Our job is to peel back that mask.
Phase 1
The Trigonometric Cleanup
Look at that denominator: D=sinx(secx−sinxtanx). It is a mess of secants and tangents.
Whenever you face such a situation, do not try to force a complex identity. Instead, go back to the roots. Convert everything to sinx and cosx.
By substituting secx=cosx1 and tanx=cosxsinx, the denominator becomes:
D=sinx(cosx1−cosxsin2x)
Suddenly, the fog clears. We have a common denominator of cosx, leading us to:
D=sinx(cosx1−sin2x)
And what is 1−sin2x? It is the fundamental identity cos2x. The expression simplifies to:
D=sinx(cosxcos2x)=sinxcosx
Just like that, the chaos has vanished, replaced by a clean, manageable product.
Phase 2
The Linear Differential Equation
Now that we have our simplified denominator, our equation looks like this:
dxdy=sinxcosxtanx+y
To see the structure, we split the fraction:
dxdy=sinxcosxtanx+sinxcosxy
Let's tackle the first term:
sinxcosxtanx=sinxcosxsinx/cosx=cos2x1=sec2x
For the second term, we have sinxcosxy. Multiplying the numerator and denominator by 2, we get:
2sinxcosx2y=2ycsc2x
Our equation is now dxdy=sec2x+2ycsc2x. Rearranging this into the standard form:
dxdy−(2csc2x)y=sec2x
We have successfully identified a Linear Differential Equation where P(x)=−2csc2x and Q(x)=sec2x.
Phase 3
The Integrating Factor
This is where the magic happens. To solve an LDE, we need the Integrating Factor (IF), defined as:
IF=e∫P(x)dx
Substituting our P(x), we get IF=e∫−2csc2xdx. Using the standard integral ∫cscθdθ=ln∣tan2θ∣, we find that:
∫−2csc2xdx=−2(21ln∣tanx∣)=−ln∣tanx∣
Thus, our IF is:
IF=e−ln∣tanx∣=eln∣cotx∣=cotx
The integrating factor is simply cotx. How elegant is that?
Phase 4
The Final Stretch
With the IF in hand, the general solution is y⋅(IF)=∫Q(x)⋅(IF)dx+C. Substituting our values, we get:
ycotx=∫sec2xcotxdx+C
The integrand sec2xcotx simplifies to:
cos2x1⋅sinxcosx=sinxcosx1=2csc2x
The integral of 2csc2x is ln∣tanx∣. So, ycotx=ln∣tanx∣+C.
Using the initial condition y(4π)=2, we find:
2cot(4π)=ln(tan4π)+C
Since cot(4π)=1 and ln(1)=0, we get C=2. Our particular solution is:
ycotx=ln∣tanx∣+2⟹y=tanx(ln∣tanx∣+2)
Finally, evaluating at x=3π, we get:
y(3π)=tan(3π)(ln(tan3π)+2)=3(ln3+2)
This matches our target perfectly. You see? With patience and systematic steps, even the most daunting problems yield to the beauty of mathematics.