The Art of Seeing the Hidden Structure
Welcome, fellow traveler on the road to JEE excellence. Today, we are going to dismantle a differential equation that, at first glance, looks like a tangled mess of variables.
You might look at dxdy=xy−1+x−y and feel a sense of dread. But I want you to take a deep breath. In mathematics, as in life, complexity is often just simplicity in disguise.
Our goal is to peel back the layers of this equation until the underlying structure reveals itself.
Phase 1
The Power of Grouping
When you encounter a differential equation where x and y are intertwined, your first instinct should be to look for symmetry. Look at the right-hand side: xy−1+x−y.
If we rearrange these terms, we get (xy+x)−(y+1). By grouping the terms, we can pull out a common factor of x from the first pair and a factor of 1 from the second.
This transforms our equation into:
Suddenly, the fog clears. We have a common binomial factor of (y+1). Factoring this out, we arrive at the elegant form:
This is the 'Aha!' moment. We have successfully separated the variables. We have turned a chaotic expression into a product of a function of y and a function of x.
Phase 2
The Dance of Integration
Now that we have dxdy=(y+1)(x−1), we can move all the y terms to one side and all the x terms to the other. This is the heart of the Variable Separable method:
Integrating both sides is our next logical step. We are looking for the antiderivative of y+11 with respect to y, and (x−1) with respect to x.
This yields:
Performing the integration, we get:
Phase 3
The Initial Condition and the Final Reveal
We are almost there. We have a general solution, but we need the particular solution that satisfies y(0)=0.
By substituting x=0 and y=0 into our equation, we find:
ln∣0+1∣=202−0+C⇒ln(1)=0+C⇒C=0
With C identified as zero, our equation simplifies beautifully to ln(y+1)=2x2−x. To isolate y, we exponentiate both sides:
y+1=e2x2−x⇒y(x)=e2x2−x−1
Finally, to find y(1), we simply plug in x=1:
Look at that! Through patience and systematic grouping, we have navigated from a daunting differential equation to a precise, elegant result.
The final answer is y(1)=e−1/2−1. Remember, the next time you face a problem that looks impossible, don't panic. Look for the hidden factors, trust your process, and let the math lead you home.