Animated Solution for Mathematics - Definite Integration: Find the area of the region bounded by the x-axis and the curves defined by y=tanx,−3π≤x≤3π;y=cotx,6π≤x≤23π.
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Visualized Solution
Visualizing the Curves and Domains
Given curves: y=tanx and y=cotx
Domains: −3π≤x≤3π and 6π≤x≤23π
We focus on the overlapping region where both curves are defined and positive.
Finding the Point of Intersection
To find the intersection, set tanx=cotx
tanx=tanx1⟹tan2x=1
In the interval [6π,3π], tanx=1⟹x=4π
Intersection point: (4π,1)
Identifying the Bounded Region
Left boundary: x=6π (lower limit of cotx domain)
Right boundary: x=3π (upper limit of tanx domain)
The region is bounded below by the x-axis (y=0)
The upper boundary changes at the intersection point x=4π
Setting up the Definite Integrals
Total Area A=I1+I2
First part: I1=∫π/6π/4tanxdx
Second part: I2=∫π/4π/3cotxdx
Evaluating the First Integral I1
I1=∫π/6π/4tanxdx=[ln∣secx∣]π/6π/4
I1=ln(sec4π)−ln(sec6π)
I1=ln2−ln(32)
Evaluating the Second Integral I2
I2=∫π/4π/3cotxdx=[ln∣sinx∣]π/4π/3
I2=ln(sin3π)−ln(sin4π)
I2=ln(23)−ln(21)
Combining the Logarithmic Terms
Total Area A=I1+I2
A=(ln2−ln32)+(ln23−ln21)
Use properties of logarithms: lna−lnb+lnc−lnd=ln(b⋅da⋅c)
Final Area Calculation
A=ln(32⋅212⋅23)=ln(2/36/2)
A=ln(23)=ln(1.5)
Final Answer:ln(1.5)≈0.405 sq. units
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The Sigma Insight: Area Bounded by Curves
Solution Diagram
Analyzing the Setup
Welcome, fellow traveler on the road to JEE excellence. Today, we aren't just solving a calculus problem; we are choreographing a dance between two of the most fundamental functions in trigonometry: the tangent and the cotangent.
Imagine standing on the Cartesian plane, looking at the region trapped between these two curves and the x-axis. It looks simple, but as with all things in JEE Advanced, the beauty lies in the precision of our steps.
The Intersection of Paths
First, we must orient ourselves. We are given y=tanx and y=cotx. Our goal is to find the area bounded by these curves and the x-axis.
Before we dive into integration, we need to know where these two paths cross. We set them equal: tanx=cotx. Since cotx=tanx1, this becomes tan2x=1.
In our interval of interest, this leads us to the elegant intersection point x=4π. At this point, both functions meet at the height of y=1. This point is the pivot of our entire calculation.
Defining the Boundaries
Now, look at the geometry. The region starts at x=6π and ends at x=3π. But notice the 'ceiling' of our region.
From 6π to 4π, the curve y=tanx is the one defining the upper boundary. However, as we cross the threshold of 4π, the curve y=tanx begins to climb steeply, and it is now the curve y=cotx that defines the upper boundary until we reach x=3π.
This is the 'trap'—if you try to integrate just one function, you will miss the physical reality of the shape. We must split our integral into two parts:
I1=∫π/6π/4tanxdxandI2=∫π/4π/3cotxdx
The Calculus of Elegance
I know that seeing integrals can be daunting, but let's take a breath and look at the tools in our kit. We know that ∫tanxdx=ln∣secx∣ and ∫cotxdx=ln∣sinx∣.
We are almost there. The total area A is the sum of these two values. When we add them together, we get a string of logarithms.
Using the property lna+lnb−lnc−lnd=ln(c⋅da⋅b), we can collapse this entire expression into a single, beautiful term:
A=ln(32⋅212⋅23)
After simplifying the fractions inside the logarithm, we find that the expression reduces to ln(1.5). Calculating this gives us approximately 0.405.
Take a moment to appreciate what you have done. You didn't just crunch numbers; you analyzed the behavior of functions, identified a geometric transition, and used the power of logarithmic properties to simplify a complex physical area into a single, clean value. This is the essence of physics and mathematics—finding order in the complexity.