What is the Taylor series for cosx centered around x = pi?

1 Answer
Apr 6, 2017

The general formula for a Taylor series is:

f(x) = sum_(n=0)^(oo) (f^((n))(a))/(n!)(x-a)^n

where f^((n))(a) is the nth derivative of f defined at x = a. Thus, it makes sense to take some derivatives when finding the Taylor series.

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 x = a is:

= (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 sin(pi) = 0, so for all odd derivatives, the term vanishes. Thus, we get:

= 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 - . . . )