Analyzing the Setup
Imagine you are standing on a coordinate plane. You see a fixed circle, anchored at (0,1) with a radius of 1.
Now, imagine a second, smaller circle that is constantly moving, but it has a strict rule: it must always touch the x-axis and it must always kiss the fixed circle from the outside. This is the geometric dance we are analyzing today.
Defining the Locus
Let the center of our moving circle be (α,β). Because it touches the x-axis and stays above it, its radius r must be exactly β.
Now, consider the fixed circle with center C1=(0,1) and radius r1=1. When two circles touch externally, the distance d between their centers is the sum of their radii: d=r1+r2.
Here, r2=β, so d=1+β. Using the distance formula, we write:
Squaring both sides, we get α2+(β−1)2=(1+β)2. Expanding this, we find:
The β2 and the 1 cancel out beautifully, leaving us with α2=4β. Replacing (α,β) with (x,y), we find our locus L is the parabola x2=4y.
Calculating the Area
Now that we have our parabola y=4x2, we need to find the area bounded by this curve and the line y=4.
First, find the intersection points: 4x2=4, which gives x2=16, so x=±4. The region is symmetric about the y-axis.
We can calculate the area in the first quadrant and double it. The area A is given by:
Integrating term by term, we get:
Plugging in the limits, we have:
2[16−1264]=2[16−316]=2[332]=364
The final area is 364 square units. It is a beautiful result, isn't it? The complexity of the moving circle simplifies into the elegant geometry of a parabola.