For , Taylor's theorem after terms, counting the constant term, is
Under the usual hypothesis that is times continuously differentiable on the interval joining and , and times differentiable in its interior, the Taylor theorem with Lagrange remainder gives
This is a finite expansion with a controlled remainder; it does not assume an infinite Taylor series converges. For the remainder is zero.
Let near . The chain rule gives
Substitute into the first three terms of the Taylor expansion:
The quadratic coefficient is , not . The apparent square root creates no local difficulty at the positive expansion point.
Use the Maclaurin series and . Multiplying through the cubic order gives
These are the first three nonzero terms; the constant term vanishes.
Both numerator and denominator vanish quadratically. Factor out before dividing the power series:
The reciprocal of the denominator is . Hence
The expansion describes the continuous extension at the removable singularity , where the original quotient is undefined but its limit is one. Odd powers vanish because the quotient is even.

Articles by others on the same topic (0)

There are currently no matching articles.