Analyzing the Hidden Symmetry
Welcome, future engineers! Today, we are going to peel back the layers of a differential equation that, at first glance, might seem like a standard, tedious problem.
Look at the equation:
In the world of JEE Advanced, the most powerful tool you possess is not just your ability to calculate, but your ability to observe. The left-hand side, xdxdy+y, is the ghost of the product rule.
Recall that dxd(uv)=udxdv+vdxdu. If we set u=x and v=y, then:
By recognizing this, we have instantly bypassed the need for an integrating factor. It is a moment of pure mathematical elegance.
The Integration Journey
Now that we have simplified our equation to dxd(xy)=xlogex, our path forward is clear: we must integrate both sides with respect to x. This gives us:
Now, we face the integral of xlogex. We turn to the trusty ILATE rule. Logarithmic functions take precedence over algebraic ones, so we set u=logex and dv=xdx.
Applying the integration by parts formula, ∫udv=uv−∫vdu, we get:
xy=(logex)(2x2)−∫(2x2)(x1)dx
Notice how the x terms cancel out inside the integral. We are left with ∫2xdx, which integrates to 4x2. Thus, our general solution emerges:
The Detective Work
We have the general family of curves, but we need the specific one that satisfies our initial condition: 2y(2)=loge4−1. This is where we play detective.
By substituting x=2 into our general solution, we get:
Simplifying this, we have 2y(2)=2loge2−1+C. Since loge4=2loge2, our condition becomes:
The terms cancel out perfectly, leaving us with C=0. We are left with our particular solution:
The Final Victory
We are at the finish line. We need to find y(e). We simply substitute x=e into our particular solution:
Since logee=1, this simplifies to:
Dividing both sides by e, we arrive at our final answer:
You have successfully navigated the differential equation, applied the product rule, mastered integration by parts, and solved for the constant. Keep practicing, keep observing, and keep falling in love with the process!