Animated Solution for Mathematics - Differential Equations: If ydxdy=x[x2y2+ϕ′(x2y2)ϕ(x2y2)],x>0,ϕ>0, and y(1)=−1, then ϕ(4y2) is equal to :
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Visualized Solution
Identify the Homogeneous Form
Given equation: ydxdy=x[x2y2+ϕ′(x2y2)ϕ(x2y2)]
Observe that the equation is a function of xy, indicating it is a Homogeneous Differential Equation.
Define the Substitution y=tx
Let y=tx
Differentiating both sides with respect to x using the product rule:
dxdy=t+xdxdt
Substitute into the Original Equation
Substitute y=tx and dxdy=t+xdxdt into the equation:
tx(t+xdxdt)=x[t2+ϕ′(t2)ϕ(t2)]
Simplify the Equation
Cancel x from both sides (since x>0):
t(t+xdxdt)=t2+ϕ′(t2)ϕ(t2)
Expand the left side:
t2+xtdxdt=t2+ϕ′(t2)ϕ(t2)
Separate the Variables
Subtract t2 from both sides:
xtdxdt=ϕ′(t2)ϕ(t2)
Rearrange to separate t and x:
ϕ(t2)tϕ′(t2)dt=xdx
Integrate Both Sides
Integrate both sides: ∫ϕ(t2)tϕ′(t2)dt=∫xdx
For the left side, use substitution u=ϕ(t2)⇒du=ϕ′(t2)⋅2tdt
So, tϕ′(t2)dt=21du
Solve the Integrals
Substituting back: 21∫udu=∫xdx
Integrating gives: 21lnϕ(t2)=lnx+lnc
Using log properties: lnϕ(t2)=ln(cx)
Find the General Solution
Remove the logarithms: ϕ(t2)=cx
Square both sides: ϕ(t2)=c2x2
Let k=c2, so: ϕ(t2)=kx2
Substituting back t=xy:
ϕ(x2y2)=kx2
Apply the Initial Condition
Given y(1)=−1, which means at x=1,y=−1
Calculate t2: t2=(xy)2=(1−1)2=1
Substitute into ϕ(t2)=kx2:
ϕ(1)=k(1)2⇒k=ϕ(1)
Final Evaluation
The general solution becomes ϕ(x2y2)=ϕ(1)x2
We need to find ϕ(4y2)
Comparing the arguments, we set x2=4
Substitute x2=4 into the equation:
ϕ(4y2)=ϕ(1)⋅4=4ϕ(1)
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The Sigma Insight: Homogeneous Differential Equations
The Art of Seeing Through Complexity
Welcome, fellow traveler on the JEE Advanced journey. Today, we are going to dismantle a problem that, at first glance, looks like a nightmare of notation. You see the symbols ϕ and ϕ′, and your instinct might be to panic.
But I want you to take a deep breath. In mathematics, especially in differential equations, complexity is often just a mask. Our job is to peel back that mask and reveal the elegant, simple structure underneath.
Phase 1
The Homogeneous Insight
Let us look at the given equation:
ydxdy=x[x2y2+ϕ′(x2y2)ϕ(x2y2)]
Do you see it? The term x2y2 appears repeatedly. This is not a coincidence; it is a signal.
In the world of differential equations, when you see the ratio of variables appearing consistently, you are almost certainly dealing with a Homogeneous Differential Equation. This is your first victory. By recognizing this, you have already decided on your strategy: we are going to transform it into a language we understand.
Phase 2
The Substitution Dance
To simplify this, we introduce the classic substitution: y=tx. This is the key that unlocks the door.
But remember, we cannot just change y and leave dxdy alone. We must respect the rules of calculus. Differentiating y=tx with respect to x using the product rule gives us:
dxdy=t+xdxdt
Now, let us substitute these into our original equation. The left side becomes tx(t+xdxdt), and the right side becomes x[t2+ϕ′(t2)ϕ(t2)].
Since the problem guarantees x>0, we can divide by x without fear. Expanding the left side, we get:
t2+xtdxdt=t2+ϕ′(t2)ϕ(t2)
Look at that! The t2 terms on both sides vanish like magic. We are left with xtdxdt=ϕ′(t2)ϕ(t2). This is the moment where the problem shifts from 'terrifying' to 'solvable'.
Phase 3
The Integration Symphony
Now, we separate the variables. We want all the t terms on one side and all the x terms on the other. Rearranging, we get:
ϕ(t2)tϕ′(t2)dt=xdx
This is where many students stumble, but you won't. Look at the left side; we have ϕ(t2) in the denominator and ϕ′(t2) in the numerator. This is a classic setup for u-substitution.
Let u=ϕ(t2). Then, by the chain rule, du=ϕ′(t2)⋅2t⋅dt. This means tϕ′(t2)dt=21du.
Substituting this back, the integral becomes:
21∫udu=∫xdx
Integrating both sides gives us 21lnϕ(t2)=lnx+lnc. Using the properties of logarithms, we can simplify this to lnϕ(t2)=ln(cx).
Removing the logarithms, we arrive at ϕ(t2)=cx, or simply ϕ(t2)=kx2, where k=c2.
Phase 4
The Final Reveal
We are almost there. We have the general solution ϕ(x2y2)=kx2. Now, we apply the initial condition y(1)=−1.
At x=1, y=−1, so t2=(1−1)2=1. Plugging these into our equation, we get ϕ(1)=k(1)2, which means k=ϕ(1).
Our specific solution is ϕ(x2y2)=ϕ(1)x2. The question asks for ϕ(4y2). By comparing the arguments, we see that x2 must be 4.
Substituting x2=4 into our equation, we get ϕ(4y2)=ϕ(1)⋅4.
And there it is: 4ϕ(1). You didn't just solve a problem; you navigated a complex landscape of calculus, substitution, and logic. Remember this feeling—the feeling of turning chaos into order. That is the true essence of mathematics.