The integrated cosine series becomes the sine series because integrating the even-power terms x2n of the cosine series produces odd-power terms x2n+1. Combined with the factorial simplification (2n)!(2n+1)=(2n+1)!, the resulting series exactly matches the standard Maclaurin series for sinx.
Conditions: The starting series is the Maclaurin series for cosx.; Term-by-term integration is justified by the DCT.; The factorial identity (2n)!(2n+1)=(2n+1)! is applied.
The integrated cosine series becomes the sine series because integrating the even-power terms x2n of the cosine series produces odd-power terms x2n+1. Combined with the factorial simplification (2n)!(2n+1)=(2n+1)!, the resulting series exactly matches the standard Maclaurin series for sinx.
Conditions: The starting series is the Maclaurin series for cosx.; Term-by-term integration is justified by the DCT.; The factorial identity (2n)!(2n+1)=(2n+1)! is applied.
The sum and integral can be interchanged because the Dominated Convergence Theorem applies. The terms of the cosine power series are bounded in magnitude by 1 on the interval [0,π/2], making the constant function g(x)=1 a valid dominating function with a finite integral over the interval.
Conditions: The integration interval is [0,π/2].; The series terms are (2n)!(−1)nx2n.; The dominating function is g(x)=1.
The sum and integral can be interchanged because the Dominated Convergence Theorem applies. The terms of the cosine power series are bounded in magnitude by 1 on the interval [0,π/2], making the constant function g(x)=1 a valid dominating function with a finite integral over the interval.
Conditions: The integration interval is [0,π/2].; The series terms are (2n)!(−1)nx2n.; The dominating function is g(x)=1.