What is the Taylor series for #cosx# centered around #x = pi#?
1 Answer
The general formula for a Taylor series is:
#f(x) = sum_(n=0)^(oo) (f^((n))(a))/(n!)(x-a)^n#
where
#f^((0))(x) = f(x) = cosx#
#f'(x) = -sinx#
#f''(x) = -cosx#
#f'''(x) = sinx#
#f''''(x) = cosx#
etc.
Therefore, the Taylor series centered at
#= (f(a))/(0!)(x-a)^0 + (f'(a))/(1!)(x-a)^1 + (f''(a))/(2!)(x-a)^2 + (f'''(a))/(3!)(x-a)^3 + (f''''(a))/(4!)(x-a)^4 + ...#
But
#= cospi + cancel((f'(a))/(1!)(x-a)^1)^(0) + (-cospi)/(2!)(x-pi)^2 + cancel((f'''(a))/(3!)(x-a)^3)^(0) + (cospi)/(4!)(x-pi)^4 + ...#
#= color(blue)(-1 + 1/2(x-pi)^2 - 1/24(x-pi)^4 + . . . )#
Generalizing this...
- We have that the series alternates sign, so we include a
#(-1)^n# term somewhere... - We also have the
#(x-pi)^n# term, obviously, but we specify even#n# to ignore the odd terms (which are zero), so we can use#2n# . - We have a negative sign out front, since the first term in a Taylor series tends to be
#1# . - We would have to specify even
#n# for the factorial terms, so the factorial terms go as#(2n)!# , i.e.#0!# ,#2!# ,#4!# , etc.
So, our instinct gives us a series representation as:
#sum_(n=0)^(oo) -((-1)^(n)(x-pi)^(2n))/((2n)!)#
#= color(blue)(sum_(n=0)^(oo) ((-1)^(n+1)(x-pi)^(2n))/((2n)!))#
#= ((-1)^(0+1)(x-pi)^(2*0))/((2*0)!) + ((-1)^(1+1)(x-pi)^(2*1))/((2*1)!) + ((-1)^(2+1)(x-pi)^(2*2))/((2*2)!) + ((-1)^(3+1)(x-pi)^(2*3))/((2*3)!) + . . . #
#= color(blue)(-1 + 1/2(x-pi)^2 - 1/24(x-pi)^4 + 1/720(x-pi)^6 - . . . )#