The Hidden Symmetry of Differentials
Welcome, fellow traveler of the mathematical landscape. Today, we are going to unravel a differential equation that, at first glance, might seem like a tangled mess of variables.
But beneath the surface lies a beautiful, elegant structure waiting to be revealed. Let us embark on this journey together.
Phase 1
The Pattern Recognition
We start with the equation: ydx+y2dy=xdy. Our goal is to find y(−3) given that y(1)=1 and y>0.
When you see an equation like this, do not rush to integrate. Instead, pause and observe. We have ydx and xdy terms, which is a classic signature of the quotient rule in reverse.
Recall that the derivative of a quotient yx is given by:
To make this pattern appear, we first rearrange our equation: ydx−xdy+y2dy=0.
Now, the path becomes clear. If we divide the entire equation by y2, we get:
This simplifies beautifully to:
Phase 2
The Calculus Magic
Now, look at that first term. It is exactly the differential of yx. Our equation has collapsed into:
This is the moment of triumph! We have reduced a complex-looking equation into a simple sum of differentials.
Integrating both sides is now trivial:
This gives us the general solution:
Phase 3
Locking Down the Curve
We have a family of curves, but we need the specific one that passes through (1,1).
Substituting x=1 and y=1 into our equation, we get 11+1=C, which means C=2.
Our specific curve is defined by the equation:
This is the mathematical DNA of our path.
Phase 4
The Final Destination
Our mission is to find y when x=−3. Substituting x=−3 into our curve equation, we get:
To solve for y, we multiply by y to clear the fraction:
Factoring this quadratic, we find (y−3)(y+1)=0. This gives us two potential roots: y=3 and y=−1.
But remember our constraint: y>0. Therefore, we must reject y=−1.
The only valid solution is y=3.