For the odd two-periodic extensions, fˉ=∑bnsin(nπx) with bn=2[1+(−1)n]/(nπ), while Fˉ has bn=4[1−(−1)n]/(n3π3). Thus the first has O(n−1) convergence because its periodic extension jumps, while the smoother second extension has O(n−3) coefficients.