Analyzing the Symmetry of the Parabola
Imagine you are standing before a perfectly symmetric parabola defined by the second-degree polynomial f(x)=Ax2+Bx+C. We are given the condition f(1)=f(−1).
Geometrically, this means the height of the parabola at x=1 is identical to its height at x=−1. This is the hallmark of symmetry.
Algebraically, substituting these values into the equation yields:
A(1)2+B(1)+C=A(−1)2+B(−1)+C
Simplifying this expression, we get A+B+C=A−B+C. This leads us directly to 2B=0, which implies B=0.
Our polynomial simplifies to the elegant form f(x)=Ax2+C. The linear term vanishes, leaving us with a pure, symmetric quadratic.
The Derivative as a Linear Operator
Now, we consider the derivatives
f′(a),
f′(b), and
f′(c). Applying the power rule to our simplified polynomial, we find:
f′(x)=2Ax
Notice how the derivative is a linear function passing through the origin. It is a straight line.
This is a powerful realization. We are no longer dealing with a curve; we are dealing with a linear transformation of the points a, b, and c.
The Beauty of Arithmetic Progressions
We are given that
a,b,c are in an Arithmetic Progression (A.P.). This implies that the common difference is constant:
b−a=c−b
Now, let us evaluate the derivative values at these points:
f′(a)=2Aa,f′(b)=2Ab,f′(c)=2Ac
To check if these values form an A.P., we examine the differences between consecutive terms:
f′(b)−f′(a)=2Ab−2Aa=2A(b−a)
f′(c)−f′(b)=2Ac−2Ab=2A(c−b)
The Final Conclusion
Since b−a=c−b, it follows that 2A(b−a)=2A(c−b). The common difference is preserved under the linear transformation 2Ax.
We have taken a journey from the symmetry of a parabola to the linear nature of its derivative, and finally to the preservation of an A.P. under linear scaling.
Because the common difference remains constant, we can confidently conclude that f′(a),f′(b),f′(c) are in an A.P.