Analyzing the Setup
We are tasked with evaluating the definite integral ∫−23f(x)dx, where the function f(x) is defined piecewise as:
f(x)={ecosxsinx2for ∣x∣≤2otherwise
At first glance, this might look like a daunting task, but let's break it down into a logical journey.
The Strategy of Splitting
The first thing to notice is the "seam" in our function. The definition changes exactly at x=2.
In the world of integration, when a function behaves differently in different regions, we must respect those boundaries. We use the additive property of definite integrals:
∫acf(x)dx=∫abf(x)dx+∫bcf(x)dx
By splitting our integral at x=2, we transform one complex problem into two distinct, manageable ones:
The Power of Symmetry
Now, look at the first integral: I1=∫−22ecosxsinxdx. Whenever you see symmetric limits like [−a,a], your internal alarm bells should ring!
This is a massive hint to check for the parity of the function. Let g(x)=ecosxsinx. To check if it is odd or even, we evaluate g(−x).
Using the fundamental trigonometric identities, we know cos(−x)=cosx and sin(−x)=−sinx. Substituting these, we get:
This confirms that g(x) is an odd function. The beauty of an odd function over a symmetric interval is that the area below the x-axis perfectly cancels the area above it.
Thus, ∫−22ecosxsinxdx=0. The entire first part of our problem vanishes, leaving us with a much simpler task.
The Geometric Conclusion
We are left with the second integral: I2=∫232dx. This is the integral of a constant, which is geometrically equivalent to finding the area of a rectangle.
The height of this rectangle is 2, and the width is the interval length, 3−2=1. Calculating the integral, we get:
Adding our two results together, 0+2=2, we arrive at our final answer.
The final result is 2. This problem is a masterclass in observation. By identifying the piecewise boundary and the symmetry of the integrand, we bypassed complex integration techniques entirely.