First, the form of the answer will be: \[ \cos z \approx c_0 + c_1 (z-\pi) + c_2 (z-\pi)^2 + c_3(z-\pi)^3 + c_4(z-\pi)^4\] or \[ \cos z = c_0 + c_1 (z-\pi) + c_2 (z-\pi)^2 + c_3(z-\pi)^3 + c_4(z-\pi)^4+\dots\]
Because I'm asked for the fourth order expansion, I'll keep only terms up to the fourth power. I use the first form (with the \(\approx\) approximation sign and stopping at the fourth order term) when I want to emphasize that I have done an approximation. Ise the second form (with an \(=\) sign and \(\dots\) at the end) when I want to indicate that there are more terms that I am not writing in the exact power series.
Now, to calculate the coefficients: \begin{eqnarray*} c_0 &=& \frac{1}{0!}f(z=z_0) = \cos\pi = -1 \\ c_1 &=& \frac{1}{1!}\left.\frac{df}{dz}\right|_{z=z_0} = -\sin \pi = 0 \\ c_2 &=& \frac{1}{2!}\left.\frac{d^2f}{dz^2}\right|_{z=z_0} = -\frac{1}{2}\cos \pi = \frac{1}{2} \\ c_3 &=& \frac{1}{3!}\left.\frac{d^3f}{dz^3}\right|_{z=z_0} = \frac{1}{6}\sin \pi = 0 \\ c_4 &=& \frac{1}{4!}\left.\frac{d^4f}{dz^4}\right|_{z=z_0} = \frac{1}{24}\cos \pi = -\frac{1}{24} \\ \end{eqnarray*} (Don't forget the \(1/n!\).)
So, the approximation I end up with is:
\[ \cos z \approx -1 + \frac{1}{2} (z-\pi)^2 +-\frac{1}{24}(z-\pi)^4\]
This formula is the correct form of the power serie approximation. Do NOT multiply out and regroup the terms (do Not "FOIL") or you are undoing all the work you did to find the power series.
Here is the code in Mathematica and the graph it produces.
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When I plot this approximation against the cosine function, I see that the expansion approximates the cosine function reasonably well between about \(\pi/2\) and \(3\pi/2\). Inside this region, I can not even distinguish the graphs from each other. Beyond that region, the function and its approximation rapidly start to differ.