Analyzing the Setup
Imagine you are standing on the coordinate plane, looking at a collection of circles. Every single one of these circles is anchored to the origin, passing through the point (0,0).
Their centers are not floating randomly; they are strictly constrained to the x-axis. As you slide the center along the x-axis, the circle breathes—expanding or shrinking to maintain its connection to the origin.
Defining the Blueprint
To describe this family, we need a mathematical blueprint. Let the center of any circle in this family be C(a,0), where a is an arbitrary constant that defines the specific circle.
Because the circle must pass through the origin (0,0), the distance from the center C(a,0) to the origin must be the radius r. Using the distance formula:
Thus, the radius is simply r=∣a∣. Now, we invoke the standard equation of a circle: (x−h)2+(y−k)2=r2.
Substituting our center (h,k)=(a,0) and radius r=a, we get the equation:
Simplifying this, we have (x−a)2+y2=a2.
The Algebraic Dance
Now, let's expand the term (x−a)2. Using the identity (A−B)2=A2−2AB+B2, we get:
Notice the beauty of the symmetry here: we have an a2 on both sides of the equation. They cancel out perfectly, leaving us with:
This is our fundamental equation, Equation 1. It elegantly captures the relationship between x, y, and the parameter a.
The Calculus of Elimination
Our goal is to find the differential equation, which means we must eliminate the arbitrary constant a. Since there is only one constant, we differentiate Equation 1 with respect to x exactly once.
Differentiating x2 gives 2x, and differentiating y2 requires the chain rule, giving 2ydxdy. On the right side, the derivative of 2ax is simply 2a.
So, we have:
This is Equation 2. Now, we have a direct expression for 2a. We can substitute this back into our original Equation 1, which was x2+y2=(2a)x.
Replacing 2a with (2x+2ydxdy), we get:
Distributing the x on the right side, we obtain:
Finally, rearranging the terms to isolate y2 on the left, we subtract x2 from both sides:
This simplifies to the final differential equation:
This is the differential equation that governs our entire family of circles. You have successfully translated a visual family of curves into a precise mathematical law.