Analyzing the Setup
Imagine you are standing before a complex, winding path—a differential equation that seems to twist and turn in ways that defy simple integration. Today, we are looking at the equation 2x2dy=(2xy+y2)dx.
Our first step is to act like detectives. We rearrange the equation to isolate the derivative:
Now, look closely at the structure. The numerator has terms 2xy and y2, both of which have a degree of 2. The denominator, 2x2, also has a degree of 2.
This is not a coincidence; it is the hallmark of a homogeneous differential equation. This symmetry is our golden ticket.
The Transformation
Changing Our Perspective
When we encounter a homogeneous equation, we don't fight it head-on. Instead, we change our perspective. We use the substitution y=vx, where v is a function of x.
To make this work, we must also transform our derivative. Using the product rule on y=vx, we get:
Now, we substitute these into our original equation:
v+xdxdv=2x22x(vx)+(vx)2
Simplifying the right side, we get:
Notice how the x2 terms cancel out beautifully? We are left with:
This further simplifies to:
Subtracting v from both sides gives us the elegant result:
The Calculus of Separation
We have arrived at the heart of the problem. The equation is now in variable separable form:
We integrate both sides:
The integral of v−2 is −v−1, so the left side becomes −v2. The right side is simply ln∣x∣+C. Substituting back v=xy, we get:
This is our general solution, the map of all possible curves that satisfy the differential equation.
The Final Reveal
We know the curve passes through (1,2), so we plug in x=1 and y=2 to find C:
−22(1)=ln∣1∣+C⇒−1=0+C⇒C=−1
Our particular solution is:
Finally, to find f(21), we set x=21:
This simplifies to:
Multiplying by −1, we get:
Taking the reciprocal, we find our final answer: