Skip to content

[B.8-4 Taylor and Maclaurin Series](#page-7-0)

← Back to LINEAR SYSTEMS AND SIGNALS Overview

B.8-4 Taylor and Maclaurin Series

f(x)=f(a)+(xβˆ’a)1!fΛ™(a)+(xβˆ’a)22!fΒ¨(a)+β‹―=βˆ‘k=0∞(xβˆ’a)kk!f(k)(a)f(x) = f(a) + \frac{(x-a)}{1!}\dot{f}(a) + \frac{(x-a)^2}{2!}\ddot{f}(a) + \dots = \sum_{k=0}^{\infty} \frac{(x-a)^k}{k!}f^{(k)}(a) f(x)=f(0)+x1!fΛ™(0)+x22!fΒ¨(0)+β‹―=βˆ‘k=0∞xkk!f(k)(0)f(x) = f(0) + \frac{x}{1!}\dot{f}(0) + \frac{x^2}{2!}\ddot{f}(0) + \dots = \sum_{k=0}^{\infty} \frac{x^k}{k!}f^{(k)}(0)

B.8-5 Power Series

ex=1+x+x22!+x33!+β‹―+xnn!+…e^{x} = 1 + x + \frac{x^{2}}{2!} + \frac{x^{3}}{3!} + \dots + \frac{x^{n}}{n!} + \dots

\n

sin⁑x=xβˆ’x33!+x55!βˆ’x77!+…\sin x = x - \frac{x^{3}}{3!} + \frac{x^{5}}{5!} - \frac{x^{7}}{7!} + \dots

\n

cos⁑x=1βˆ’x22!+x44!βˆ’x66!+x88!βˆ’β€¦\cos x = 1 - \frac{x^{2}}{2!} + \frac{x^{4}}{4!} - \frac{x^{6}}{6!} + \frac{x^{8}}{8!} - \dots

\n

tan⁑x=x+x33+2x515+17x7315+…x2<Ο€2/4\tan x = x + \frac{x^{3}}{3} + \frac{2x^{5}}{15} + \frac{17x^{7}}{315} + \dots \qquad x^{2} < \pi^{2}/4

\n

tanh⁑x=xβˆ’x33+2x515βˆ’17x7315+…x2<Ο€2/4\tanh x = x - \frac{x^{3}}{3} + \frac{2x^{5}}{15} - \frac{17x^{7}}{315} + \dots \qquad x^{2} < \pi^{2}/4

\n

(1+x)n=1+nx+n(nβˆ’1)2!x2+n(nβˆ’1)(nβˆ’2)3!x3+β‹―+(nk)xk+β‹―+xn(1 + x)^{n} = 1 + nx + \frac{n(n-1)}{2!}x^{2} + \frac{n(n-1)(n-2)}{3!}x^{3} + \dots + \binom{n}{k}x^{k} + \dots + x^{n}

\n

(1+x)nβ‰ˆ1+nx∣x∣β‰ͺ1(1 + x)^{n} \approx 1 + nx \qquad |x| \ll 1

\n

11βˆ’x=1+x+x2+x3+β€¦βˆ£x∣<1\frac{1}{1 - x} = 1 + x + x^{2} + x^{3} + \dots \qquad |x| < 1

B.8-6 Trigonometric Identities

e±jx=cos⁑x±jsin⁑xe^{\pm jx} = \cos x \pm j \sin x

\n

cos⁑x=12[ejx+eβˆ’jx]\cos x = \frac{1}{2} [e^{jx} + e^{-jx}]

\n

sin⁑x=12j[ejxβˆ’eβˆ’jx]\sin x = \frac{1}{2j} [e^{jx} - e^{-jx}]

\n

cos⁑(xΒ±Ο€2)=Β±sin⁑x\cos (x \pm \frac{\pi}{2}) = \pm \sin x

\n

sin⁑(xΒ±Ο€2)=Β±cos⁑x\sin (x \pm \frac{\pi}{2}) = \pm \cos x

\n

2sin⁑xcos⁑x=sin⁑2x2 \sin x \cos x = \sin 2x

\n

sin⁑2x+cos⁑2x=1\sin^2 x + \cos^2 x = 1

\n

cos⁑2xβˆ’sin⁑2x=cos⁑2x\cos^2 x - \sin^2 x = \cos 2x

\n

cos⁑2x=12(1+cos⁑2x)\cos^2 x = \frac{1}{2} (1 + \cos 2x)

\n

sin⁑2x=12(1βˆ’cos⁑2x)\sin^2 x = \frac{1}{2} (1 - \cos 2x)

cos⁑3x=14(3cos⁑x+cos⁑3x)\cos^3 x = \frac{1}{4} (3 \cos x + \cos 3x)

\n

sin⁑3x=14(3sin⁑xβˆ’sin⁑3x)\sin^3 x = \frac{1}{4} (3 \sin x - \sin 3x)

\n

sin⁑(x±y)=sin⁑xcos⁑y±cos⁑xsin⁑y\sin (x \pm y) = \sin x \cos y \pm \cos x \sin y

\n

cos⁑(xΒ±y)=cos⁑xcos⁑yβˆ“sin⁑xsin⁑y\cos (x \pm y) = \cos x \cos y \mp \sin x \sin y

\n

tan⁑(xΒ±y)=tan⁑xΒ±tan⁑y1βˆ“tan⁑xtan⁑y\tan (x \pm y) = \frac{\tan x \pm \tan y}{1 \mp \tan x \tan y}

\n

sin⁑xsin⁑y=12[cos⁑(xβˆ’y)βˆ’cos⁑(x+y)]\sin x \sin y = \frac{1}{2} [\cos (x - y) - \cos (x + y)]

\n

cos⁑xcos⁑y=12[cos⁑(xβˆ’y)+cos⁑(x+y)]\cos x \cos y = \frac{1}{2} [\cos (x - y) + \cos (x + y)]

\n

sin⁑xcos⁑y=12[sin⁑(xβˆ’y)+sin⁑(x+y)]\sin x \cos y = \frac{1}{2} [\sin (x - y) + \sin (x + y)]

\n

sin⁑xcos⁑x+bsin⁑x=Ccos⁑(x+ΞΈ)C=a2+b2,ΞΈ=tanβ‘βˆ’1(βˆ’ba)\sin x \cos x + b \sin x = C \cos (x + \theta) \qquad C = \sqrt{a^2 + b^2}, \theta = \tan^{-1} (\frac{-b}{a})

B.8-7 Common Derivative Formulas

ddxf(u)=dduf(u)dudx\frac{d}{dx}f(u) = \frac{d}{du}f(u)\frac{du}{dx}

\n

ddx(uv)=udvdx+vdudx\frac{d}{dx}(uv) = u\frac{dv}{dx} + v\frac{du}{dx}

\n

ddx(uv)=vdudxβˆ’udvdxv2\frac{d}{dx}\left(\frac{u}{v}\right) = \frac{v\frac{du}{dx} - u\frac{dv}{dx}}{v^2}

\n

dxndx=nxnβˆ’1\frac{dx^n}{dx} = nx^{n-1}

\n

ddxln⁑(ax)=1x\frac{d}{dx}\ln(ax) = \frac{1}{x}

\n

ddxlog⁑(ax)=log⁑ex\frac{d}{dx}\log(ax) = \frac{\log e}{x}

\n

ddxebx=bebx\frac{d}{dx}e^{bx} = be^{bx}

\n

ddxabx=b(ln⁑a)abx\frac{d}{dx}a^{bx} = b(\ln a)a^{bx}

\n

ddxsin⁑ax=acos⁑ax\frac{d}{dx}\sin ax = a\cos ax

\n

ddxcos⁑ax=βˆ’asin⁑ax\frac{d}{dx}\cos ax = -a\sin ax

\n

ddxtan⁑ax=acos⁑2ax\frac{d}{dx}\tan ax = \frac{a}{\cos^2 ax}

\n

ddx(sinβ‘βˆ’1ax)=a1βˆ’a2x2\frac{d}{dx}(\sin^{-1}ax) = \frac{a}{\sqrt{1 - a^2x^2}}

\n

ddx(cosβ‘βˆ’1ax)=βˆ’a1βˆ’a2x2\frac{d}{dx}(\cos^{-1}ax) = \frac{-a}{\sqrt{1 - a^2x^2}}

\n

ddx(tanβ‘βˆ’1ax)=a1+a2x2\frac{d}{dx}(\tan^{-1}ax) = \frac{a}{1 + a^2x^2}

B.8-8 Indefinite Integrals

∫udv=uvβˆ’βˆ«vdu\int u dv = uv - \int v du

\n

∫f(x)gΛ™(x)dx=f(x)g(x)βˆ’βˆ«f(x)g(x)dx\int f(x)\dot{g}(x) dx = f(x)g(x) - \int f(x)g(x) dx

\n

∫sin⁑axdx=βˆ’1acos⁑ax∫cos⁑axdx=1asin⁑ax\int \sin ax dx = -\frac{1}{a} \cos ax \qquad \int \cos ax dx = \frac{1}{a} \sin ax

\n

∫sin⁑2axdx=x2βˆ’sin⁑2ax4a∫cos⁑2axdx=x2+sin⁑2ax4a\int \sin^2 ax dx = \frac{x}{2} - \frac{\sin 2ax}{4a} \qquad \int \cos^2 ax dx = \frac{x}{2} + \frac{\sin 2ax}{4a}

\n

∫xsin⁑axdx=1a2(sin⁑axβˆ’axcos⁑ax)\int x \sin ax dx = \frac{1}{a^2} (\sin ax - ax \cos ax)

\n

∫xcos⁑axdx=1a2(cos⁑ax+axsin⁑ax)\int x \cos ax dx = \frac{1}{a^2} (\cos ax + ax \sin ax)

\n

∫x2sin⁑axdx=1a3(2axsin⁑ax+2cos⁑axβˆ’a2x2cos⁑ax)\int x^2 \sin ax dx = \frac{1}{a^3} (2ax \sin ax + 2 \cos ax - a^2x^2 \cos ax)

\n

∫x2cos⁑axdx=1a3(2axcos⁑axβˆ’2sin⁑ax+a2x2sin⁑ax)\int x^2 \cos ax dx = \frac{1}{a^3} (2ax \cos ax - 2 \sin ax + a^2x^2 \sin ax)

\n

∫sin⁑axsin⁑bxdx=sin⁑(aβˆ’b)x2(aβˆ’b)βˆ’sin⁑(a+b)x2(a+b)a2β‰ b2\int \sin ax \sin bx dx = \frac{\sin (a - b)x}{2(a - b)} - \frac{\sin (a + b)x}{2(a + b)} \qquad a^2 \neq b^2

\n

∫sin⁑axcos⁑bxdx=βˆ’[cos⁑(aβˆ’b)x2(aβˆ’b)+cos⁑(a+b)x2(a+b)]a2β‰ b2\int \sin ax \cos bx dx = -\left[ \frac{\cos (a - b)x}{2(a - b)} + \frac{\cos (a + b)x}{2(a + b)} \right] \qquad a^2 \neq b^2

\n

∫cos⁑axcos⁑bxdx=sin⁑(aβˆ’b)x2(aβˆ’b)+sin⁑(a+b)x2(a+b)a2β‰ b2\int \cos ax \cos bx dx = \frac{\sin (a - b)x}{2(a - b)} + \frac{\sin (a + b)x}{2(a + b)} \qquad a^2 \neq b^2

\n

∫eaxdx=eaxa2(axβˆ’1)\int e^{ax} dx = \frac{e^{ax}}{a^2} (ax - 1)

\n

∫x2eaxdx=eaxa2(a2x2βˆ’2ax+2)\int x^2 e^{ax} dx = \frac{e^{ax}}{a^2} (a^2x^2 - 2ax + 2)

\n

∫eaxsin⁑bxdx=eaxa2+b2(asin⁑bxβˆ’bcos⁑bx)\int e^{ax} \sin bx dx = \frac{e^{ax}}{a^2 + b^2} (a \sin bx - b \cos bx)

\n

∫eaxcos⁑bxdx=eaxa2+b2(acos⁑bx+bsin⁑bx)\int e^{ax} \cos bx dx = \frac{e^{ax}}{a^2 + b^2} (a \cos bx + b \sin bx)

\n

∫1x2+a2dx=1aln⁑(x\int \frac{1}{x^2 + a^2} dx = \frac{1}{a} \ln(x

B.8-9 L’HΓ΄pital’s Rule

If lim f(x)/g(x) results in the indeterministic form 0/0 or ∞/∞, then

lim⁑f(x)g(x)=lim⁑fΛ™(x)gΛ™(x)\lim \frac{f(x)}{g(x)} = \lim \frac{\dot{f}(x)}{\dot{g}(x)}

B.8-10 Solution of Quadratic and Cubic Equations

Any quadratic equation can be reduced to the form

ax2+bx+c=0ax^2 + bx + c = 0

The solution of this equation is provided by

x=βˆ’bΒ±b2βˆ’4ac2ax = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}

A general cubic equation

y3+py2+qy+r=0y^3 + py^2 + qy + r = 0

may be reduced to the depressed cubic form

x3+ax+b=0x^3 + ax + b = 0

by substituting

y=xβˆ’p3y = x - \frac{p}{3}

This yields

a=13(3qβˆ’p2)b=127(2p3βˆ’9pq+27r)a = \frac{1}{3}(3q - p^2) \qquad b = \frac{1}{27}(2p^3 - 9pq + 27r)

Now let

A=βˆ’b2+b24+a3273B=βˆ’b2βˆ’b24+a3273A = \sqrt[3]{-\frac{b}{2} + \sqrt{\frac{b^2}{4} + \frac{a^3}{27}}} \qquad B = \sqrt[3]{-\frac{b}{2} - \sqrt{\frac{b^2}{4} + \frac{a^3}{27}}}

The solution of the depressed cubic is

x=A+Bx = A + B

, x=βˆ’A+B2+Aβˆ’B2βˆ’3x = -\frac{A+B}{2} + \frac{A-B}{2}\sqrt{-3} , x=βˆ’A+B2βˆ’Aβˆ’B2βˆ’3x = -\frac{A+B}{2} - \frac{A-B}{2}\sqrt{-3}

and

y=xβˆ’p3y = x - \frac{p}{3}