Analyzing the Setup
Imagine you are standing before the graph of a quadratic function, f(x)=x2+bx+c. It is a classic parabola, sweeping gracefully across the Cartesian plane.
The problem states that α and β are its distinct roots. Geometrically, this means the parabola intersects the x-axis at exactly two points: α and β. At these precise locations, the function's value is zero.
By the Factor Theorem, we can express this quadratic not just as a sum of terms, but as a product of its roots:
f(x)=(x−α)(x−β)
This form is powerful because it allows us to see exactly what happens to the function as x approaches one of its roots.
The Limit's Anatomy
Unveiling the Taylor Series
Now, let us turn our attention to the limit:
x→βlim(x−β)2e2f(x)−1−2f(x)
As x slides along the x-axis toward β, the value of f(x) drops toward zero. This means the exponent 2f(x) is also approaching zero.
This is a classic setup for a Taylor series expansion. Whenever you see
eu−1−u where
u→0, you should recall the Maclaurin series for
eu:
eu=1+u+2!u2+3!u3+…
By setting t=2f(x), we can rewrite our numerator. As x→β, t also approaches zero. The expansion becomes et≈1+t+2t2.
The Elegant Cancellation
Let us substitute this back into our numerator:
e2f(x)−1−2f(x)≈(1+2f(x)+2(2f(x))2)−1−2f(x)
Notice the magic: the 1 and the 2f(x) terms cancel out perfectly with the −1 and −2f(x) already present. We are left with 2(2f(x))2, which simplifies to 2(f(x))2.
Our limit has now reduced to a much friendlier form:
x→βlim(x−β)22(f(x))2
The Bridge to Coefficients
Now, we bring back our factorized form:
f(x)=(x−α)(x−β). Substituting this into our limit, we get:
x→βlim(x−β)22(x−α)2(x−β)2
Since x is approaching β but is not equal to β, we can safely cancel the (x−β)2 terms. We are left with limx→β2(x−α)2, which evaluates simply to 2(β−α)2.
Finally, we connect this back to the coefficients b and c. Using Vieta's formulas, we know α+β=−b and αβ=c.
The identity
(β−α)2=(α+β)2−4αβ allows us to write this as
b2−4c. Multiplying by the
2 we had outside, our
final answer is:
2(b2−4c)