Analyzing the Setup
Imagine you are standing at the intersection of two vast mathematical landscapes: Linear Algebra and Calculus. Often, these subjects feel like separate islands, but today, we are building a bridge between them.
The problem before us is a masterclass in how different branches of mathematics speak the same language. We are given a differential equation involving the determinant of a matrix A, and our goal is to find the specific path of the function y(x).
Unmasking the Determinant
At first glance, the matrix A is defined as:
A determinant is a single scalar value that summarizes the 'volume' or 'scaling factor' of the matrix. To find it, we expand along the first row.
We take y and multiply it by the minor (−x1−0), subtract sinx times its minor (0−2), and add 1 times its minor (0−(−2)). When we simplify this, we obtain:
Suddenly, the matrix has vanished, leaving behind a beautiful, manageable expression. This is the heart of the problem: transforming a complex structure into a simple, solvable differential equation.
The Dance of the Differential Equation
Now, we substitute our determinant back into the given equation: dxdy−∣A∣=0. This yields:
Rearranging this into the standard linear form, we get:
This is a classic first-order linear differential equation where P(x)=x1 and Q(x)=2sinx+2. To solve this, we calculate the Integrating Factor (I.F.), defined as e∫P(x)dx.
Since ∫x1dx=lnx, our I.F. is simply elnx=x. This is a moment of pure elegance—the complexity of the exponential and logarithmic functions collapses into a simple variable x.
The Integration Journey
Multiplying our entire equation by x, we obtain:
Now, we integrate both sides. The right side requires us to evaluate ∫(2xsinx+2x)dx. We split this into two parts.
The integral ∫2xdx is trivial, giving us x2. The integral ∫2xsinxdx requires Integration by Parts. By setting u=x and dv=sinxdx, we find that:
Combining these, we arrive at the general solution:
The Final Reveal
We use the initial condition y(π)=π+2. Substituting x=π and y=π+2 into our equation, we find:
Since cosπ=−1 and sinπ=0, the equation simplifies to π2+2π=π2+2π+c, which forces c=0. With c gone, our specific solution is xy=x2−2xcosx+2sinx.
Finally, to find y(2π), we substitute x=2π. The term cos(2π) becomes 0, and sin(2π) becomes 1. We are left with:
Dividing by 2π, we reach our destination: