Known Taylor Series for Common Functions To find Taylor series efficiently, it is often more practical to utilize known series expansions rather than calculating derivatives manually, which can be laborious for many functions. The following standard Taylor series (Maclaurin series, centered at x = 0 x=0 x = 0 ) are fundamental:
Exponential Function: e x = 1 + x + x 2 2 ! + x 3 3 ! + x 4 4 ! + … e^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \frac{x^4}{4!} + \dots e x = 1 + x + 2 ! x 2 + 3 ! x 3 + 4 ! x 4 + …
Sine Function: sin ( x ) = x − x 3 3 ! + x 5 5 ! − x 7 7 ! + … \sin(x) = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \frac{x^7}{7!} + \dots sin ( x ) = x − 3 ! x 3 + 5 ! x 5 − 7 ! x 7 + …
Cosine Function: cos ( x ) = 1 − x 2 2 ! + x 4 4 ! − x 6 6 ! + … \cos(x) = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \frac{x^6}{6!} + \dots cos ( x ) = 1 − 2 ! x 2 + 4 ! x 4 − 6 ! x 6 + …
Natural Logarithm (Shifted): ln ( 1 + x ) = x − x 2 2 + x 3 3 − x 4 4 + … \ln(1+x) = x - \frac{x^2}{2} + \frac{x^3}{3} - \frac{x^4}{4} + \dots ln ( 1 + x ) = x − 2 x 2 + 3 x 3 − 4 x 4 + …
Geometric Series: 1 1 − x = ∑ n = 0 ∞ x n = 1 + x + x 2 + x 3 + … \frac{1}{1-x} = \sum_{n=0}^{\infty} x^n = 1 + x + x^2 + x^3 + \dots 1 − x 1 = ∑ n = 0 ∞ x n = 1 + x + x 2 + x 3 + …
Binomial Series: ( 1 + x ) p = 1 + p x + p ( p − 1 ) 2 ! x 2 + p ( p − 1 ) ( p − 2 ) 3 ! x 3 + … (1+x)^p = 1 + px + \frac{p(p-1)}{2!} x^2 + \frac{p(p-1)(p-2)}{3!} x^3 + \dots ( 1 + x ) p = 1 + p x + 2 ! p ( p − 1 ) x 2 + 3 ! p ( p − 1 ) ( p − 2 ) x 3 + …
Finding Taylor Series via Substitution New Taylor series can be derived by substituting a variable or expression into the standard series listed above.
Example 1: e − x e^{-x} e − x
Start with e x = 1 + x + x 2 2 ! + x 3 3 ! + … e^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \dots e x = 1 + x + 2 ! x 2 + 3 ! x 3 + …
Replace x x x with − x -x − x :
e − x = 1 + ( − x ) + ( − x ) 2 2 ! + ( − x ) 3 3 ! + … e^{-x} = 1 + (-x) + \frac{(-x)^2}{2!} + \frac{(-x)^3}{3!} + \dots e − x = 1 + ( − x ) + 2 ! ( − x ) 2 + 3 ! ( − x ) 3 + …
Result: e − x = 1 − x + x 2 2 ! − x 3 3 ! + … e^{-x} = 1 - x + \frac{x^2}{2!} - \frac{x^3}{3!} + \dots e − x = 1 − x + 2 ! x 2 − 3 ! x 3 + …
Example 2: ln ( 1 − 2 y ) \ln(1-2y) ln ( 1 − 2 y )
Start with ln ( 1 + x ) = x − x 2 2 + x 3 3 − x 4 4 + … \ln(1+x) = x - \frac{x^2}{2} + \frac{x^3}{3} - \frac{x^4}{4} + \dots ln ( 1 + x ) = x − 2 x 2 + 3 x 3 − 4 x 4 + …
Substitute x = − 2 y x = -2y x = − 2 y :
ln ( 1 − 2 y ) = ( − 2 y ) − ( − 2 y ) 2 2 + ( − 2 y ) 3 3 − ( − 2 y ) 4 4 + … \ln(1-2y) = (-2y) - \frac{(-2y)^2}{2} + \frac{(-2y)^3}{3} - \frac{(-2y)^4}{4} + \dots ln ( 1 − 2 y ) = ( − 2 y ) − 2 ( − 2 y ) 2 + 3 ( − 2 y ) 3 − 4 ( − 2 y ) 4 + …
Result: ln ( 1 − 2 y ) = − 2 y − 2 y 2 − 8 3 y 3 − 4 y 4 − … \ln(1-2y) = -2y - 2y^2 - \frac{8}{3}y^3 - 4y^4 - \dots ln ( 1 − 2 y ) = − 2 y − 2 y 2 − 3 8 y 3 − 4 y 4 − …
Example 3: z e − z 2 z e^{-z^2} z e − z 2
First, find the series for e − z 2 e^{-z^2} e − z 2 by substituting − z 2 -z^2 − z 2 into the e x e^x e x series:
e − z 2 = 1 + ( − z 2 ) + ( − z 2 ) 2 2 ! + ( − z 2 ) 3 3 ! + ⋯ = 1 − z 2 + z 4 2 ! − z 6 3 ! + … e^{-z^2} = 1 + (-z^2) + \frac{(-z^2)^2}{2!} + \frac{(-z^2)^3}{3!} + \dots = 1 - z^2 + \frac{z^4}{2!} - \frac{z^6}{3!} + \dots e − z 2 = 1 + ( − z 2 ) + 2 ! ( − z 2 ) 2 + 3 ! ( − z 2 ) 3 + ⋯ = 1 − z 2 + 2 ! z 4 − 3 ! z 6 + …
Multiply the entire series by z z z :
z e − z 2 = z ( 1 − z 2 + z 4 2 − z 6 6 + … ) z e^{-z^2} = z(1 - z^2 + \frac{z^4}{2} - \frac{z^6}{6} + \dots) z e − z 2 = z ( 1 − z 2 + 2 z 4 − 6 z 6 + … )
Result: z − z 3 + z 5 2 − z 7 6 + … z - z^3 + \frac{z^5}{2} - \frac{z^7}{6} + \dots z − z 3 + 2 z 5 − 6 z 7 + …
Example 4: t sin ( 3 t ) t \sin(3t) t sin ( 3 t )
Substitute x = 3 t x = 3t x = 3 t into sin ( x ) \sin(x) sin ( x ) .
sin ( 3 t ) = ( 3 t ) − ( 3 t ) 3 3 ! + ( 3 t ) 5 5 ! − ( 3 t ) 7 7 ! + ⋯ = 3 t − 27 t 3 6 + 243 t 5 120 − 2187 t 7 5040 + … \sin(3t) = (3t) - \frac{(3t)^3}{3!} + \frac{(3t)^5}{5!} - \frac{(3t)^7}{7!} + \dots = 3t - \frac{27t^3}{6} + \frac{243t^5}{120} - \frac{2187t^7}{5040} + \dots sin ( 3 t ) = ( 3 t ) − 3 ! ( 3 t ) 3 + 5 ! ( 3 t ) 5 − 7 ! ( 3 t ) 7 + ⋯ = 3 t − 6 27 t 3 + 120 243 t 5 − 5040 2187 t 7 + …
Simplify and multiply by t t t :
t sin ( 3 t ) = 3 t 2 − 9 2 t 4 + 81 40 t 6 − 243 560 t 8 + … t \sin(3t) = 3t^2 - \frac{9}{2}t^4 + \frac{81}{40}t^6 - \frac{243}{560}t^8 + \dots t sin ( 3 t ) = 3 t 2 − 2 9 t 4 + 40 81 t 6 − 560 243 t 8 + …
Example 5: 1 − 2 x \sqrt{1-2x} 1 − 2 x
This uses the Binomial series with p = 1 2 p = \frac{1}{2} p = 2 1 and substituting − 2 x -2x − 2 x for x x x .
( 1 − 2 x ) 1 / 2 = 1 + ( 1 2 ) ( − 2 x ) + ( 1 2 ) ( 1 2 − 1 ) 2 ! ( − 2 x ) 2 + ( 1 2 ) ( 1 2 − 1 ) ( 1 2 − 2 ) 3 ! ( − 2 x ) 3 + … (1-2x)^{1/2} = 1 + (\frac{1}{2})(-2x) + \frac{(\frac{1}{2})(\frac{1}{2}-1)}{2!}(-2x)^2 + \frac{(\frac{1}{2})(\frac{1}{2}-1)(\frac{1}{2}-2)}{3!}(-2x)^3 + \dots ( 1 − 2 x ) 1/2 = 1 + ( 2 1 ) ( − 2 x ) + 2 ! ( 2 1 ) ( 2 1 − 1 ) ( − 2 x ) 2 + 3 ! ( 2 1 ) ( 2 1 − 1 ) ( 2 1 − 2 ) ( − 2 x ) 3 + …
= 1 − x + ( 1 2 ) ( − 1 2 ) 2 ( 4 x 2 ) + ( 1 2 ) ( − 1 2 ) ( − 3 2 ) 6 ( − 8 x 3 ) + … = 1 - x + \frac{(\frac{1}{2})(-\frac{1}{2})}{2}(4x^2) + \frac{(\frac{1}{2})(-\frac{1}{2})(-\frac{3}{2})}{6}(-8x^3) + \dots = 1 − x + 2 ( 2 1 ) ( − 2 1 ) ( 4 x 2 ) + 6 ( 2 1 ) ( − 2 1 ) ( − 2 3 ) ( − 8 x 3 ) + …
Result: 1 − x − 1 2 x 2 − 1 2 x 3 − … 1 - x - \frac{1}{2}x^2 - \frac{1}{2}x^3 - \dots 1 − x − 2 1 x 2 − 2 1 x 3 − …
Example 6: t sin ( t 2 ) − t 3 t 7 \frac{t \sin(t^2) - t^3}{t^7} t 7 t s i n ( t 2 ) − t 3
Substitute x = t 2 x = t^2 x = t 2 into sin ( x ) \sin(x) sin ( x ) : sin ( t 2 ) = t 2 − t 6 3 ! + t 10 5 ! − … \sin(t^2) = t^2 - \frac{t^6}{3!} + \frac{t^{10}}{5!} - \dots sin ( t 2 ) = t 2 − 3 ! t 6 + 5 ! t 10 − …
Multiply by t t t : t sin ( t 2 ) = t 3 − t 7 3 ! + t 11 5 ! − … t \sin(t^2) = t^3 - \frac{t^7}{3!} + \frac{t^{11}}{5!} - \dots t sin ( t 2 ) = t 3 − 3 ! t 7 + 5 ! t 11 − …
Subtract t 3 t^3 t 3 : t sin ( t 2 ) − t 3 = − t 7 3 ! + t 11 5 ! − … t \sin(t^2) - t^3 = -\frac{t^7}{3!} + \frac{t^{11}}{5!} - \dots t sin ( t 2 ) − t 3 = − 3 ! t 7 + 5 ! t 11 − …
Divide by t 7 t^7 t 7 :
Result: − 1 3 ! + t 4 5 ! − t 8 7 ! + ⋯ = − 1 6 + 1 120 t 4 − … -\frac{1}{3!} + \frac{t^4}{5!} - \frac{t^{8}}{7!} + \dots = -\frac{1}{6} + \frac{1}{120}t^4 - \dots − 3 ! 1 + 5 ! t 4 − 7 ! t 8 + ⋯ = − 6 1 + 120 1 t 4 − …
Example 7: Hyperbolic Sine (Alternative Construction)
sinh ( x ) = e x − e − x 2 \sinh(x) = \frac{e^x - e^{-x}}{2} sinh ( x ) = 2 e x − e − x
Substitute expansions for e x e^x e x and e − x e^{-x} e − x :
sinh ( x ) = ( 1 + x + x 2 2 ! + x 3 3 ! + … ) − ( 1 − x + x 2 2 ! − x 3 3 ! + … ) 2 \sinh(x) = \frac{(1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \dots) - (1 - x + \frac{x^2}{2!} - \frac{x^3}{3!} + \dots)}{2} sinh ( x ) = 2 ( 1 + x + 2 ! x 2 + 3 ! x 3 + … ) − ( 1 − x + 2 ! x 2 − 3 ! x 3 + … )
sinh ( x ) = 2 x + 2 x 3 3 ! + 2 x 5 5 ! + … 2 \sinh(x) = \frac{2x + \frac{2x^3}{3!} + \frac{2x^5}{5!} + \dots}{2} sinh ( x ) = 2 2 x + 3 ! 2 x 3 + 5 ! 2 x 5 + …
Result: sinh ( x ) = x + x 3 3 ! + x 5 5 ! + … \sinh(x) = x + \frac{x^3}{3!} + \frac{x^5}{5!} + \dots sinh ( x ) = x + 3 ! x 3 + 5 ! x 5 + …
Radius of Convergence Affected by Substitution When substituting an expression into a known Taylor series, the radius of convergence (R R R ) of the original series must be adjusted based on the substitute.
New Series via Differentiation and Integration Just as we can use substitution, we can differentiate or integrate existing series term-by-term to find series for related functions.
Function Expansions in Specific Variables Sometimes functions must be expanded in terms of specific variables by algebraic manipulation to fit standard forms.
Example A: Expand 1 5 − x \frac{1}{5-x} 5 − x 1 in terms of x x x :
Factor out the constant: 1 5 ( 1 − x 5 ) = 1 5 ⋅ 1 1 − ( x 5 ) \frac{1}{5(1 - \frac{x}{5})} = \frac{1}{5} \cdot \frac{1}{1 - (\frac{x}{5})} 5 ( 1 − 5 x ) 1 = 5 1 ⋅ 1 − ( 5 x ) 1 .
Apply geometric series for H = x 5 H = \frac{x}{5} H = 5 x :
Result: 1 5 [ 1 + x 5 + ( x 5 ) 2 + ( x 5 ) 3 + … ] \frac{1}{5} [1 + \frac{x}{5} + (\frac{x}{5})^2 + (\frac{x}{5})^3 + \dots] 5 1 [ 1 + 5 x + ( 5 x ) 2 + ( 5 x ) 3 + … ]
Example B: Expand x 2 + x 2 \frac{x}{2+x^2} 2 + x 2 x in terms of x x x :
Manipulate: x ⋅ 1 2 ( 1 − ( − x 2 2 ) ) = x 2 ⋅ 1 1 − ( − x 2 2 ) x \cdot \frac{1}{2(1 - (-\frac{x^2}{2}))} = \frac{x}{2} \cdot \frac{1}{1 - (-\frac{x^2}{2})} x ⋅ 2 ( 1 − ( − 2 x 2 )) 1 = 2 x ⋅ 1 − ( − 2 x 2 ) 1 .
Apply geometric series: x 2 [ 1 + ( − x 2 2 ) + ( − x 2 2 ) 2 + … ] = x 2 [ 1 − x 2 2 + x 4 4 − … ] \frac{x}{2} [1 + (-\frac{x^2}{2}) + (-\frac{x^2}{2})^2 + \dots] = \frac{x}{2} [1 - \frac{x^2}{2} + \frac{x^4}{4} - \dots] 2 x [ 1 + ( − 2 x 2 ) + ( − 2 x 2 ) 2 + … ] = 2 x [ 1 − 2 x 2 + 4 x 4 − … ]
Result: x 2 − x 3 4 + x 5 8 − … \frac{x}{2} - \frac{x^3}{4} + \frac{x^5}{8} - \dots 2 x − 4 x 3 + 8 x 5 − …
Example C: Expand ( 2 + x ) 3 (2+x)^3 ( 2 + x ) 3 in terms of x x x using the Binomial formula:
Manipulate: [ 2 ( 1 + x 2 ) ] 3 = 8 ( 1 + x 2 ) 3 [2(1 + \frac{x}{2})]^3 = 8(1 + \frac{x}{2})^3 [ 2 ( 1 + 2 x ) ] 3 = 8 ( 1 + 2 x ) 3 .
Substitute p = 3 p=3 p = 3 and H = x 2 H=\frac{x}{2} H = 2 x into ( 1 + H ) p = 1 + p H + p ( p − 1 ) 2 ! H 2 + p ( p − 1 ) ( p − 2 ) 3 ! H 3 (1+H)^p = 1 + pH + \frac{p(p-1)}{2!}H^2 + \frac{p(p-1)(p-2)}{3!}H^3 ( 1 + H ) p = 1 + p H + 2 ! p ( p − 1 ) H 2 + 3 ! p ( p − 1 ) ( p − 2 ) H 3 .
8 [ 1 + 3 ( x 2 ) + 3 ( 2 ) 2 ( x 2 ) 2 + 3 ( 2 ) ( 1 ) 6 ( x 2 ) 3 ] = 8 [ 1 + 3 x 2 + 3 x 2 4 + x 3 8 ] 8 [1 + 3(\frac{x}{2}) + \frac{3(2)}{2}(\frac{x}{2})^2 + \frac{3(2)(1)}{6}(\frac{x}{2})^3] = 8 [1 + \frac{3x}{2} + \frac{3x^2}{4} + \frac{x^3}{8}] 8 [ 1 + 3 ( 2 x ) + 2 3 ( 2 ) ( 2 x ) 2 + 6 3 ( 2 ) ( 1 ) ( 2 x ) 3 ] = 8 [ 1 + 2 3 x + 4 3 x 2 + 8 x 3 ] .
Result: 8 + 12 x + 6 x 2 + x 3 8 + 12x + 6x^2 + x^3 8 + 12 x + 6 x 2 + x 3 .
Ordering and Comparison Near Zero Taylor series allow us to compare the relative magnitudes of different functions for values of y y y near 0 0 0 by looking at the leading terms.
Functions to compare:
a = 1 + sin ( y ) ≈ 1 + y − y 3 6 a = 1 + \sin(y) \approx 1 + y - \frac{y^3}{6} a = 1 + sin ( y ) ≈ 1 + y − 6 y 3
b = e y ≈ 1 + y + y 2 2 b = e^y \approx 1 + y + \frac{y^2}{2} b = e y ≈ 1 + y + 2 y 2
c = 1 1 − 2 y = ( 1 − 2 y ) − 1 / 2 c = \frac{1}{\sqrt{1-2y}} = (1-2y)^{-1/2} c = 1 − 2 y 1 = ( 1 − 2 y ) − 1/2 . Using Binomial Series with p = − 1 / 2 p=-1/2 p = − 1/2 and substitution − 2 y -2y − 2 y : 1 + ( − 1 2 ) ( − 2 y ) + ( − 1 2 ) ( − 3 2 ) 2 ! ( − 2 y ) 2 = 1 + y + 3 2 y 2 1 + (-\frac{1}{2})(-2y) + \frac{(-\frac{1}{2})(-\frac{3}{2})}{2!}(-2y)^2 = 1 + y + \frac{3}{2}y^2 1 + ( − 2 1 ) ( − 2 y ) + 2 ! ( − 2 1 ) ( − 2 3 ) ( − 2 y ) 2 = 1 + y + 2 3 y 2
Comparison Analysis:
All three series match up to the linear term (all are 1 + y 1+y 1 + y ).
Function (a) has no quadratic term (0 y 2 0y^2 0 y 2 ), while (b) has 1 2 y 2 \frac{1}{2}y^2 2 1 y 2 and (c) has 3 2 y 2 \frac{3}{2}y^2 2 3 y 2 .
Since \frac{3}{2} > \frac{1}{2} > 0, for small positive y y y : Order: 1 + \sin(y) < e^y < \frac{1}{\sqrt{1-2y}}
Applications: Approximations and Graphing Exercise Solutions Problem 1b: First four terms for e x 2 e^{x^2} e x 2 are 1 + x 2 + x 4 2 + x 6 6 1 + x^2 + \frac{x^4}{2} + \frac{x^6}{6} 1 + x 2 + 2 x 4 + 6 x 6 .
Problem 1e: First four terms for e t cos ( t ) e^t \cos(t) e t cos ( t ) .
( 1 + t + t 2 2 + t 3 6 + … ) ( 1 − t 2 2 + t 4 24 − … ) (1 + t + \frac{t^2}{2} + \frac{t^3}{6} + \dots)(1 - \frac{t^2}{2} + \frac{t^4}{24} - \dots) ( 1 + t + 2 t 2 + 6 t 3 + … ) ( 1 − 2 t 2 + 24 t 4 − … )
Multiplying and keeping terms up to t 4 t^4 t 4 : 1 + t − t 3 3 − t 4 6 1 + t - \frac{t^3}{3} - \frac{t^4}{6} 1 + t − 3 t 3 − 6 t 4 .
Problem 2b: Expand r ( a + r ) 2 \frac{r}{(a+r)^2} ( a + r ) 2 r in terms of r r r .
r a 2 ( 1 + r a ) 2 = r a 2 ( 1 + r a ) − 2 \frac{r}{a^2(1+\frac{r}{a})^2} = \frac{r}{a^2}(1+\frac{r}{a})^{-2} a 2 ( 1 + a r ) 2 r = a 2 r ( 1 + a r ) − 2 .
Using Binomial series for p = − 2 p=-2 p = − 2 : r a 2 [ 1 − 2 ( r a ) + 3 ( r a ) 2 − 4 ( r a ) 3 + … ] \frac{r}{a^2} [1 - 2(\frac{r}{a}) + 3(\frac{r}{a})^2 - 4(\frac{r}{a})^3 + \dots] a 2 r [ 1 − 2 ( a r ) + 3 ( a r ) 2 − 4 ( a r ) 3 + … ] .
Problem 3: For g ( x ) = 1 x 2 f ( x ) g(x) = \frac{1}{x^2} f(\sqrt{x}) g ( x ) = x 2 1 f ( x ) with f ( x ) = ∑ n = 0 ∞ ( − 1 ) n x 2 n ( 2 n + 1 ) ! f(x) = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n}}{(2n+1)!} f ( x ) = ∑ n = 0 ∞ ( − 1 ) n ( 2 n + 1 )! x 2 n .