Animated Solution for Mathematics - Differential Equations: Let αx=exp(xβyγ) be the solution of the differential equation 2x2ydy−(1−xy2)dx=0,x>0,y(2)=loge2. Then α+β−γ equals :
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Visualized Solution
2x2ydxdy−(1−xy2)=0
Given Equation: 2x2ydy−(1−xy2)dx=0
Rearranging to find dxdy:
2x2ydy=(1−xy2)dx
dxdy=2x2y1−xy2
2x2ydxdy+xy2=1
Rearranging the terms:
2x2ydxdy+xy2=1
Divide by x2 to isolate the derivative part:
2ydxdy+x1y2=x21
y2=t
Let y2=t
Differentiating with respect to x:
dxd(y2)=dxdt
2ydxdy=dxdt
dxdt+P(x)t=Q(x)
Substitute t and dxdt into the equation:
dxdt+x1t=x21
This is a linear differential equation of the form dxdt+P(x)t=Q(x)
Where P(x)=x1 and Q(x)=x21
I.F.=e∫P(x)dx
Integrating Factor I.F.=e∫P(x)dx
I.F.=e∫x1dx
I.F.=elnx=x
t⋅(I.F.)=∫Q(x)⋅(I.F.)dx+C
Solution: t⋅(I.F.)=∫Q(x)⋅(I.F.)dx+C
t⋅x=∫x21⋅xdx+C
t⋅x=∫x1dx+C
t⋅x=lnx+C
Substitute t=y2: y2x=lnx+C
y(2)=ln2
Given: y(2)=ln2
Substitute x=2,y=ln2 into y2x=lnx+C:
(ln2)2⋅2=ln2+C
2ln2=ln2+C
C=ln2
2x=exp(x1y2)
Substitute C=ln2 back:
y2x=lnx+ln2
y2x=ln(2x)
Taking exponential on both sides:
exy2=2x
Rearranging to match αx=exp(xβyγ):
2x=exp(x1y2)
α+β−γ=1
Comparing 2x=exp(x1y2) with αx=exp(xβyγ):
α=2,β=1,γ=2
Calculate α+β−γ:
=2+1−2
=1
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The Sigma Insight: Linear Differential Equations
Solution Diagram
Analyzing the Setup
Imagine you are standing on the edge of a mathematical cliff, staring at the differential equation 2x2ydxdy−(1−xy2)=0. At first glance, it looks intimidating, perhaps even impossible.
But in the world of JEE Advanced, every equation is a puzzle waiting for the right key. Our journey begins by rearranging the terms. We move the dx component to the right, and after a bit of algebraic maneuvering, we find ourselves with:
dxdy=2x2y1−xy2
The Hidden Structure
Now, look closer. The equation is not linear in y, but it has a hidden symmetry. If we cross-multiply and bring the y terms to one side, we get 2x2ydxdy+xy2=1.
To isolate the derivative part, we divide the entire equation by x2. This gives us:
2ydxdy+x1y2=x21
Notice the structure here? It is starting to look familiar. We have a y2 term and a 2ydxdy term.
This is the 'Aha!' moment. We can make this linear using a clever substitution. Let t=y2. Differentiating with respect to x, we get:
dxdt=2ydxdy
This is perfect because 2ydxdy is exactly the first term in our rearranged equation.
The Linear Path
With our substitution t=y2 and dxdt=2ydxdy, the equation transforms into:
dxdt+x1t=x21
This is a standard linear differential equation of the form dxdt+P(x)t=Q(x), where P(x)=x1 and Q(x)=x21.
To solve this, we need the Integrating Factor (I.F.). The formula is:
I.F.=e∫P(x)dx=e∫x1dx=elnx=x
The integrating factor is simply x. Now, the general solution is t⋅(I.F.)=∫Q(x)⋅(I.F.)dx+C.
Substituting our values, we get t⋅x=∫x21⋅xdx+C, which simplifies to:
t⋅x=∫x1dx+C
Integrating x1 gives us lnx, so t⋅x=lnx+C. Replacing t with y2, we get our general solution:
y2x=lnx+C
The Final Reveal
We are given the initial condition y(2)=ln2. Substituting x=2 and y=ln2 into our general solution, we get:
(ln2)2⋅2=ln2+C
This simplifies to 2ln2=ln2+C. Thus, C=ln2.
Substituting C back, we get y2x=lnx+ln2=ln(2x). Taking the exponential on both sides, we get:
exy2=2x
Rearranging this to match the form αx=exp(xβyγ), we get 2x=exp(x1y2). Comparing this with the target expression, we find α=2, β=1, and γ=2.
The question asks for α+β−γ, which is 2+1−2=1. And there it is—the elegance of the final cancellation. You have successfully navigated the complexity and arrived at the answer 1.