A Taylor series rebuilds a complicated function as a polynomial, the easiest thing in maths to work with, by copying its value, slope and bend at one point. Exams ask for a second-order expansion, a limit, an approximation or a growth rate, and all of them come from one table. This guide teaches that table, the shortcuts that skip it, and shows the polynomial hugging the curve as you add terms.
Stand at one point on a curve, x = a. How would you build a polynomial that looks as much like the curve as possible near that point? Match it one feature at a time:
Same height. A flat line: right at a, useless anywhere else.
Same height and slope: the tangent line, or linear approximation.
Same bend too. A parabola that curves the way the function curves.
Each new term matches one more derivative, and the fit spreads further from a.
A Taylor polynomial of degree n is the one polynomial that agrees with f at a in value and in its first n derivatives. Let n run to infinity and you get the Taylor series; about a = 0 it is called the Maclaurin series.
Why divide by k!? Differentiate k times and you get k! (the power comes down as k, then k − 1, and so on). So the k-th derivative of the term at a is , and every other term contributes 0 there. For that to equal we need .
If a series is , then . That turns “find the 6th derivative at 0” into “find one coefficient”, often with no differentiating at all (chapter 6).
Never write the formula out in one go. Build a table with four columns and fill it row by row:
| k | f⁽ᵏ⁾(x) | at x = 1 | ÷ k! |
|---|---|---|---|
| 0 | 0 | 0 | |
| 1 | 1 | 1 | |
| 2 | −1 | −1/2 | |
| 3 | 2 | 1/3 |
Pick a function and press play: terms are added one at a time and the blue polynomial wraps itself around the black curve. Move the centre to get a Taylor series about a different point. The green band is where the series converges; outside it, extra terms make things worse. The table under the graph is the table method, filled in live.
True value 2.7183, polynomial gives 2.6667: an error of 0.0516. Add terms and the error shrinks: each new term fixes one more derivative at the centre.
| k | k-th derivative | Value at a = 0 | ÷ k! | Term |
|---|---|---|---|---|
| 0 | 1 | ÷ 1 | 1 | |
| 1 | 1 | ÷ 1 | 1 | |
| 2 | 1 | ÷ 2 | 0.5 | |
| 3 | 1 | ÷ 6 | 0.1667 |
These converge everywhere. However far out you go, enough terms will catch the curve.
These only converge for |x| < 1 about 0. Past x = 1 the polynomial flaps wildly however many terms you add.
No change from 1 to 2: sin is odd, so its even-power terms are all zero. The same happens to cos with odd powers.
| Function | Maclaurin series | Valid for |
|---|---|---|
| all x | ||
| all x | ||
| all x | ||
| (any real m) |
eˣ has every power with k! underneath. sin takes the odd powers and cos the even ones, both with alternating signs. ln(1 + x) has no factorials, just 1/k with alternating signs. The last row is the binomial theorem, which also works for fractional and negative m: put m = −1 and replace x by −x to get 1/(1 − x).
Differentiating four times is miserable. You don't need to: a Maclaurin series stays valid when you substitute something else for x, multiply two series together, or differentiate and integrate term by term.
(x → −x). (x → 2x).
. Multiply each term of the series by x.
The first-order series for small g is used all the time. It is why a growth rate can be computed as , why the growth rate of a product is the sum of growth rates, and where the rule of 70 comes from:
1.1 × 0.9 = 0.99. In logs: . The first-order terms cancel; the second-order terms don't. Volatility drags down compound growth, here by about 0.5% a year.
Expanding a utility function to second order around expected wealth gives the Arrow–Pratt result: the risk premium is about . Curvature (u″) is exactly what the second Taylor term measures.
The error behaves like . Halve the distance from the centre and a second-order approximation becomes about 8 times more accurate.
The underneath grows very fast, which is why eˣ, sin and cos converge everywhere.
Some series only converge within a distance R of the centre. For ln(1 + x) and 1/(1 − x) about 0, R = 1: the distance to the nearest point where the function breaks.
Decimals or fractions (like 4/3) are both fine.
One attempt each. Read the explanation even when you get it right.
. About a = 0 it is the Maclaurin series.
Differentiate → plug in a → divide by k! → attach (x − a)^k → add.
(coefficient of ). A missing power means that derivative is 0.
eˣ, sin x, cos x, ln(1 + x) (−1 < x ≤ 1), 1/(1 − x) and (1 + x)ᵐ (|x| < 1).
Substitute (x → −x², 2x, …), multiply by powers of x, differentiate or integrate term by term.
Limits (expand the top), approximations (write as 1 + small), ln(1 + g) ≈ g, rule of 70, second-order risk.
From CUET-PG, JNU, IIT JAM and the University of Hyderabad: second-order Taylor expansions, limits that fall straight out of a series, e as a limit, and a growth-rate approximation.
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