Analyzing the Geometric Constraint
Imagine you are standing on a path defined by a function y=f(x). At any point P(x,y) on this path, you draw a tangent line. This line acts as a mirror, reflecting the local behavior of the curve.
The tangent line strikes the X-axis at point A and the Y-axis at point B. The problem states that P is the midpoint of the segment AB. This geometric constraint implies that the curve is perfectly balanced between its intercepts.
Translating to Calculus
The equation of the tangent line at point P(x,y) with slope y′=dxdy is given by:
To find the intercepts, we set Y=0 to find A and X=0 to find B. This yields the coordinates:
The Master Equation
We apply the midpoint condition, which states that the x-coordinate of P must be the average of the x-coordinates of A and B. This gives us the relation:
Solving this equation, we obtain 2x=x−y′y, which simplifies to:
Rearranging this, we arrive at the fundamental differential equation:
Solving the Differential Equation
This equation indicates that the rate of change of y with respect to x is inversely proportional to x. We separate the variables to integrate:
Integrating both sides, we obtain ln∣y∣=−ln∣x∣+ln∣c∣, which simplifies to ln∣xy∣=ln∣c∣, or:
Final Calculation
Given that the curve passes through the point (1,1), we substitute these values to find the constant:
The resulting curve is xy=1, which is a rectangular hyperbola. Whenever you encounter a problem involving tangents and midpoints, you are likely looking at a hyperbola in disguise.