Animated Solution for Mathematics - Differential Equations: Let the solution curve y=f(x) of the differential equation dxdy+x2−1xy=1−x2x4+2x,x∈(−1,1) pass through the origin. Then ∫−2323f(x)dx is equal to
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Visualized Solution
Identifying the Differential Equation
The given equation is a First-Order Linear Differential Equation.
Standard form: dxdy+P(x)y=Q(x)
Here, P(x)=x2−1x and Q(x)=1−x2x4+2x
Domain constraint: x∈(−1,1), which implies x2<1.
Calculating the Integrating Factor
Integrating Factor (I.F.) =e∫P(x)dx
Substitute P(x): I.F.=e∫x2−1xdx
Multiply and divide by 2 to use ∫f(x)f′(x)dx=ln∣f(x)∣
∫x2−1xdx=21ln∣x2−1∣
Simplifying the I.F. for the Domain
We have I.F.=e21ln∣x2−1∣
Given x∈(−1,1)⟹x2<1, so ∣x2−1∣=1−x2.
I.F.=eln(1−x2)21
I.F.=1−x2
General Solution of the DE
General Solution: y⋅(I.F.)=∫Q(x)⋅(I.F.)dx+C
Substitute I.F. and Q(x):
y1−x2=∫(1−x2x4+2x)⋅1−x2dx
Notice how the 1−x2 terms cancel out perfectly!
y1−x2=∫(x4+2x)dx
Evaluating the Integral on the RHS
Integrating the RHS:
∫x4dx=5x5
∫2xdx=x2
So, y1−x2=5x5+x2+C
Applying the Initial Condition (0,0)
The problem states the curve passes through the origin (0,0).
Substitute x=0,y=0 into our equation:
0⋅1−0=505+02+C
0=0+0+C⟹C=0
Expressing the Function f(x)
Substitute C=0 back into the equation.
y1−x2=5x5+x2
Isolate y to get f(x):
f(x)=51−x2x5+1−x2x2
We need to evaluate: I=∫−2323f(x)dx
Using Odd and Even Function Properties
Property: ∫−aag(x)dx=0 if g(x) is odd.
Property: ∫−aag(x)dx=2∫0ag(x)dx if g(x) is even.
First term g1(x)=51−x2x5 is odd (since (−x)5=−x5).
Second term g2(x)=1−x2x2 is even (since (−x)2=x2).
Simplifying the Integral
The integral of the odd part vanishes: ∫−232351−x2x5dx=0
The integral of the even part doubles:
I=2∫0231−x2x2dx
We have significantly simplified the problem!
Trigonometric Substitution
To solve I=2∫0231−x2x2dx, use substitution.
Let x=sinθ⟹dx=cosθdθ
Change limits:
Lower limit: x=0⟹sinθ=0⟹θ=0
Upper limit: x=23⟹sinθ=23⟹θ=3π
Integrating the sin2θ Term
Substitute into the integral:
I=2∫03π1−sin2θsin2θcosθdθ
Since 1−sin2θ=cosθ, the cosθ terms cancel out.
I=2∫03πsin2θdθ
Use the half-angle identity: sin2θ=21−cos2θ
Final Evaluation
I=∫03π(1−cos2θ)dθ
Integrate term by term: I=[θ−2sin2θ]03π
Substitute upper limit: (3π−2sin(32π))
Substitute lower limit: (0−0)
Since sin(32π)=23, we get:
I=3π−43
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The Sigma Insight: Linear Differential Equations
Solution Diagram
The Detective's Guide to Differential Equations
Welcome, future engineer. Today, we are not just solving a problem; we are embarking on a mathematical investigation. When you look at a differential equation like
dxdy+x2−1xy=1−x2x4+2x
it is easy to feel overwhelmed. It looks messy, doesn't it? But remember, in the world of JEE Advanced, complexity is often a mask for elegance. Let us peel back that mask together.
Phase 1
The Anatomy of the Equation
First, we identify our target. This is a classic First-Order Linear Differential Equation. It follows the standard form
dxdy+P(x)y=Q(x)
By simply comparing terms, we identify our P(x)=x2−1x and our Q(x)=1−x2x4+2x.
But wait! Look at the domain constraint: x∈(−1,1). This is your first clue. In JEE, constraints are never accidental.
They are the guardrails that keep you from driving off a cliff. Because x2<1, we know that x2−1 is negative. Keep this in your back pocket; it will save us in the next step.
Phase 2
The Integrating Factor (The Magic Step)
To solve this, we need the Integrating Factor (I.F.), defined as e∫P(x)dx. Substituting our P(x), we get
e∫x2−1xdx
If we multiply and divide by 2, we get 21∫x2−12xdx. This is a standard logarithmic integral: 21ln∣x2−1∣.
Now, here is where the domain constraint comes into play. We have ln∣x2−1∣. Since x2<1, x2−1 is negative.
To remove the absolute value, we must write it as 1−x2. Thus, our I.F. becomes eln(1−x2)1/2, which simplifies beautifully to 1−x2. See how the complexity just melted away?
Phase 3
The Collapse
The general solution is y⋅(I.F.)=∫Q(x)⋅(I.F.)dx+C. When we multiply our Q(x) by our I.F., something miraculous happens.
The 1−x2 in the denominator of Q(x) and the 1−x2 from our I.F. cancel out perfectly! We are left with the integral of a simple polynomial:
∫(x4+2x)dx
This is the moment where you should smile. The hard part is over.
Integrating this gives us
y1−x2=5x5+x2+C
Since the curve passes through the origin (0,0), we find that C=0. Our function is simply
f(x)=51−x2x5+1−x2x2
Phase 4
The Symmetry Shortcut
We need to evaluate
∫−2323f(x)dx
Whenever you see symmetric limits like [−a,a], stop and check for odd and even functions. The first term, 51−x2x5, is an odd function because replacing x with −x negates the entire term.
The integral of an odd function over symmetric limits is zero. Poof! It vanishes. We are left with
2∫0231−x2x2dx
This is much cleaner.
Phase 5
The Final Push
To solve this, we use the substitution x=sinθ. Then dx=cosθdθ. When x=0, θ=0. When x=23, θ=3π.
The integral becomes
2∫03πcosθsin2θ⋅cosθdθ=2∫03πsin2θdθ
Using the identity sin2θ=21−cos2θ, we get
∫03π(1−cos2θ)dθ
Evaluating this, we get
[θ−2sin2θ]03π=3π−2sin(32π)=3π−43
And there you have it. A complex differential equation, tamed by domain constraints, symmetry, and trigonometric substitution. You have the tools; now go forth and conquer.