Analyzing the Setup
Welcome, future engineer. Today, we are not just solving a differential equation; we are embarking on a journey to uncover a hidden geometric truth.
When you first look at the equation
it might feel intimidating. It is a non-linear, first-order differential equation where the variables x and y are inextricably tangled inside a trigonometric function.
But here is the secret of the JEE Advanced: complexity is often just a mask for a deeper, simpler structure waiting to be revealed.
The Art of the Substitution
Imagine you are standing in front of a locked door. You have the key, but you don't know it yet. The key here is the argument of the sine function: 10x+6y.
Notice how it is a linear combination? This is a classic signature in differential equations. Whenever you see dxdy=f(ax+by+c), your intuition should immediately scream: 'Substitution!'
We define a new variable, v=10x+6y. By doing this, we are essentially changing our perspective. We are no longer looking at the curve in terms of x and y alone, but in terms of a new, unified variable v.
To make this transition complete, we must also transform our derivative. Differentiating v with respect to x, we get:
Rearranging this gives us the bridge we need:
The Transformation
Now, watch the magic happen. We substitute our new expressions back into the original equation. The equation dxdy=sin(10x+6y) transforms into:
With a little algebraic housekeeping—multiplying by 6 and adding 10 to both sides—we arrive at:
Look at that! We have successfully separated the variables. We have moved from a chaotic, tangled mess to the elegant, separable form:
The right side is trivial, but the left side? That is where the real test of your mathematical endurance lies.
The Calculus Battle
To solve ∫10+6sinvdv, we reach for the Weierstrass substitution, the 'surgical tool' of integration. We set t=tan(2v).
This substitution is powerful because it converts trigonometric functions into rational algebraic functions. Using the identity sinv=1+t22t and dv=1+t22dt, the integral becomes:
When you simplify this, the (1+t2) terms cancel out beautifully, leaving you with:
∫10t2+12t+102dt=∫5t2+6t+5dt
This is a standard integral! By completing the square in the denominator, we transform it into:
This is the classic form ∫u2+a2du=a1tan−1(au).
The Final Polish
After integrating, we obtain:
Now, we apply the boundary condition. The curve passes through the origin (0,0), which means when x=0, y=0, and consequently v=0 and t=0. Substituting these values, we find:
Finally, we substitute C back and use the inverse trigonometric identity tan−1A−tan−1B=tan−1(1+ABA−B) to combine the terms. After some careful algebraic manipulation to isolate t, and then substituting t=tan(210x+6y) back to find y, we arrive at our destination:
y=31[tan−1(4−3tan4x5tan4x)−5x]
This result is more than just a string of symbols. It is the path of a particle, the shape of a curve, and the proof of your persistence. You started with a daunting differential equation and, through the power of substitution and calculus, you tamed it.