I may have done a poor job of asking this question. You can use the sine function as the Taylor expansion as an example.
As you add more and more terms I can see how the Taylor representation of this function becomes more and more like the sine function! I am OK with that. What I am asking is at the point 0 is the graph any more accurate past the 2nd term?
In other words assuming you are only interested in what the function looked like at the point 0 would an approximation with let us say using a hundred terms be more any more accurate than just using the first few terms. Remember I am only interested at the point 0.
Or is it the case that no matter what point I pick the line through that point becomes more and more accurate as the terms increase?
The reason I ask this is because I am trying to understand why the action in the principle of stationary action uses only the first order terms and the higher order terms vanish! This happens when the Lagrangian is expanded.
All derivation examples end up using the Taylor series to write the expression and then they ignore the higher order terms.
If the Taylor series of $f(x)$ about $x=a$ converges to the function, then we have
$$ f(x)= f(a)+ f'(a)(x-a) + \frac {f''(a)}{2} (x-a)^2 +.....$$
As you see the first term $f(a)$ is a constant whose graph is a horizontal line. The first two terms $f(a) +f'(a)(x-a)$ is a line with the same value and the sme slope as your function at $x=a$
When you add the third term you get a parabola with the same value, the same slope and the same curvature as $f(x)$ at $x=a$
Thus the more terms that you add, the more details you get out of your graph.
For most functions you do not have to go too far to get a reasonable graph which is very similar to the actual graph about $x=a$