Analyzing the Setup
Imagine you are standing on a vast, empty plane. You have two fixed anchors: a large circle S1 centered at the origin (0,0) with a radius of 3, and a smaller circle S2 centered at (2,0) with a radius of 1.
Now, imagine a third, smaller circle S that is constantly moving. This circle is a traveler; it touches the inner boundary of the large circle S1 and simultaneously kisses the outer boundary of the small circle S2.
As this circle S moves, its center P(x,y) traces a path. Today, we are going to uncover the hidden geometry behind this motion.
The Geometry of Constraints
Let the center of our variable circle S be P(x,y) and its radius be r. When a circle touches another internally, the distance between their centers is the difference of their radii.
Thus, for S and S1, we have the distance PA=∣r1−r∣=3−r. Conversely, when a circle touches another externally, the distance between their centers is the sum of their radii.
For S and S2, we have PB=r2+r=1+r.
The Master Equation
Look at these two equations. We have a variable r that we don't really care about—it's just a parameter of the circle's size. To find the locus of P, we need to eliminate r.
If we add these two equations together, something magical happens:
The r terms vanish, leaving us with a beautiful, constant sum: PA+PB=4.
The Birth of the Ellipse
In the language of coordinate geometry, the locus of a point such that the sum of its distances from two fixed points (the foci) is constant is the definition of an ellipse. Our fixed points are A(0,0) and B(2,0).
The constant sum is 2a=4, which tells us that the semi-major axis a is 2. Since the foci are at (0,0) and (2,0), the center of our ellipse must be the midpoint of the segment AB, which is (1,0).
The distance between the foci is 2ae=2. With a=2, we find the eccentricity e=21.
Now, we need the minor axis b. Using the fundamental relation for an ellipse, b2=a2(1−e2), we calculate:
The Final Equation
With the center (h,k)=(1,0), a2=4, and b2=3, we can write the standard equation of our locus:
This equation represents the entire path of the center P. To verify which points lie on this path, we simply test the options provided.
Taking the point (2,±23), we substitute these coordinates into our equation:
4(2−1)2+3(±23)2=41+39/4=41+43=1
The equation holds true!
Reflection
Isn't it fascinating? What started as a complex problem of moving circles resolved into the elegant, symmetric form of an ellipse.
Whenever you face a problem involving moving objects and constraints, look for the quantities that cancel out. Often, the physics or geometry is hiding a simple, beautiful truth waiting for you to uncover it.
Keep exploring, keep questioning, and most importantly, keep enjoying the process of discovery.