For , Taylor's theorem after terms, counting the constant term, isUnder 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 givesThis 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 givesSubstitute 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 givesThese 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 . HenceThe 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.
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