List of Integrals of Exponential Functions With Proofs

#Calculus
TL;DR
Every exponential integral grows from ∫ex,dx=ex+C\int e^{x},dx = e^{x} + C. This list of integrals of exponential functions groups the results by family, with derivations, conditions, common traps and verified examples.
BT
Bhanzu TeamLast updated on October 11, 202617 min read

What Is The List Of Integrals Of Exponential Functions?

The list of integrals of exponential functions is a reference table of antiderivatives for integrands built on exe^{x} or axa^{x}, alone or multiplied by powers of xx, sines, cosines or another exponential. Its anchor entry is

∫ex,dx=ex+C,\int e^{x},dx = e^{x} + C,

which holds because exe^{x} is the only base whose exponential function equals its own derivative. Here CC is the constant of integration, added to every indefinite integral.

The symbols used in every table:

Symbol

Meaning

Condition

xx

variable of integration

real

aa, bb, λ\lambda

constants

a≠0a \neq 0 when it multiplies xx in an exponent; a>0a > 0, a≠1a \neq 1 when it is a base

nn

exponent on xx

a positive integer in the polynomial rows

erf⁡(x)\operatorname{erf}(x)

error function

erf⁡(x)=2π∫0xe−t2,dt\operatorname{erf}(x) = \frac{2}{\sqrt{\pi}}\int_{0}^{x} e^{-t^2},dt

Ei⁡(x)\operatorname{Ei}(x)

exponential integral

a special function, defined for x≠0x \neq 0

CC

constant of integration

added to every indefinite integral

This page is the catalogue. For the step-by-step lesson on the method itself, see integration of exponential functions.

How Do You Read A Table Of Exponential Integrals?

Read every row as a promise you can check: differentiate the result column and you get the integrand back. Three reading rules keep the table honest.

  • Divide only by a constant. The rows for eaxe^{ax} divide by aa because the derivative of axax is the constant aa. When the exponent is x2x^2 or x\sqrt{x}, there is no division rule; the row either has the matching factor outside (like x,ex2x,e^{x^2}) or it belongs to the error-function family.

  • Other bases carry ln⁡a\ln a. Rewrite ax=exln⁡aa^{x} = e^{x\ln a}, and the constant ln⁡a\ln a in the exponent becomes the divisor. That uses the properties of logarithms and nothing else.

  • Two correct answers can look different. Antiderivatives of the same function differ by a constant, so ex+3e^{x+3} and e3exe^{3}e^{x} are the same entry, and so are ln⁡(1+ex)\ln(1+e^{x}) and x+ln⁡(1+e−x)x + \ln(1+e^{-x}).

What Are The Basic Integrals Of exe^x And axa^x?

The basic rows all come from one move: substitute the exponent, then divide by its constant derivative. Brainly's "Evaluate the integral: ∫2e−x,dx\int 2e^{-x},dx" is a typical case; the exponent −x-x has derivative −1-1, so ∫2e−x,dx=−2e−x+C\int 2e^{-x},dx = -2e^{-x} + C.

Integral

Result

Condition

How it is derived

∫ex,dx\int e^{x},dx

ex+Ce^{x} + C

all real xx

ddxex=ex\frac{d}{dx}e^{x} = e^{x}

∫eax,dx\int e^{ax},dx

1aeax+C\frac{1}{a}e^{ax} + C

a≠0a \neq 0

u=axu = ax, du=a,dxdu = a,dx

∫eax+b,dx\int e^{ax+b},dx

1aeax+b+C\frac{1}{a}e^{ax+b} + C

a≠0a \neq 0

u=ax+bu = ax + b

∫e−x,dx\int e^{-x},dx

−e−x+C-e^{-x} + C

all real xx

row 2 with a=−1a = -1

∫ax,dx\int a^{x},dx

axln⁡a+C\frac{a^{x}}{\ln a} + C

a>0a > 0, a≠1a \neq 1

ax=exln⁡aa^{x} = e^{x\ln a}

∫abx,dx\int a^{bx},dx

abxbln⁡a+C\frac{a^{bx}}{b\ln a} + C

a>0a > 0, a≠1a \neq 1, b≠0b \neq 0

abx=ebxln⁡aa^{bx} = e^{bx\ln a}

∫2x,dx\int 2^{x},dx

2xln⁡2+C\frac{2^{x}}{\ln 2} + C

all real xx

row 5 with a=2a = 2

∫10x,dx\int 10^{x},dx

10xln⁡10+C\frac{10^{x}}{\ln 10} + C

all real xx

row 5 with a=10a = 10

∫ef(x)f′(x),dx\int e^{f(x)}f'(x),dx

ef(x)+Ce^{f(x)} + C

ff differentiable

u=f(x)u = f(x)

The last row is the master key for the next table. Whenever the derivative of the exponent sits outside as a factor, integration by substitution with uu equal to the exponent finishes the job in one line.

Integral

Result

Condition

Substitution

∫x,ex2,dx\int x,e^{x^2},dx

12ex2+C\frac{1}{2}e^{x^2} + C

all real xx

u=x2u = x^2

∫exx,dx\int \frac{e^{\sqrt{x}}}{\sqrt{x}},dx

2ex+C2e^{\sqrt{x}} + C

x>0x > 0

u=xu = \sqrt{x}

∫e1/xx2,dx\int \frac{e^{1/x}}{x^2},dx

−e1/x+C-e^{1/x} + C

x≠0x \neq 0

u=1xu = \frac{1}{x}

∫ex1+ex,dx\int e^{x}\sqrt{1+e^{x}},dx

23(1+ex)3/2+C\frac{2}{3}(1+e^{x})^{3/2} + C

all real xx

u=1+exu = 1 + e^{x}

∫ex1+ex,dx\int \frac{e^{x}}{1+e^{x}},dx

ln⁡(1+ex)+C\ln(1+e^{x}) + C

all real xx

u=1+exu = 1 + e^{x}

∫dx1+ex\int \frac{dx}{1+e^{x}}

x−ln⁡(1+ex)+Cx - \ln(1+e^{x}) + C

all real xx

write 11+ex=1−ex1+ex\frac{1}{1+e^{x}} = 1 - \frac{e^{x}}{1+e^{x}}

∫e2x1+ex,dx\int \frac{e^{2x}}{1+e^{x}},dx

ex−ln⁡(1+ex)+Ce^{x} - \ln(1+e^{x}) + C

all real xx

u=exu = e^{x}, then divide

∫dxaeλx+b\int \frac{dx}{a e^{\lambda x} + b}

xb−1bλln⁡(aeλx+b)+C\frac{x}{b} - \frac{1}{b\lambda}\ln(a e^{\lambda x} + b) + C

a,b,λ>0a, b, \lambda > 0

multiply by e−λxe^{-\lambda x} top and bottom

∫ex(f(x)+f′(x)),dx\int e^{x}\big(f(x) + f'(x)\big),dx

exf(x)+Ce^{x}f(x) + C

ff differentiable

product rule read backwards

The last row explains two results that look like tricks: ∫ex(x+1),dx=x,ex+C\int e^{x}(x+1),dx = x,e^{x} + C and ∫ex(ln⁡x+1x)dx=exln⁡x+C\int e^{x}\left(\ln x + \frac{1}{x}\right)dx = e^{x}\ln x + C for x>0x > 0. In each, the bracket is a function plus its own derivative.

What Are The Integrals Of Polynomials Times Exponentials?

A power of xx times eaxe^{ax} is integrated by integration by parts, with uu the power of xx and dv=eax,dxdv = e^{ax},dx. Each round lowers the power by one, which gives the reduction formula

∫xneax,dx=xneaxa−na∫xn−1eax,dx,a≠0.\int x^{n}e^{ax},dx = \frac{x^{n}e^{ax}}{a} - \frac{n}{a}\int x^{n-1}e^{ax},dx, \qquad a \neq 0.

Integral

Result

∫x,eax,dx\int x,e^{ax},dx

eax(xa−1a2)+Ce^{ax}\left(\frac{x}{a} - \frac{1}{a^2}\right) + C

∫x2eax,dx\int x^2 e^{ax},dx

eax(x2a−2xa2+2a3)+Ce^{ax}\left(\frac{x^2}{a} - \frac{2x}{a^2} + \frac{2}{a^3}\right) + C

∫x3eax,dx\int x^3 e^{ax},dx

eax(x3a−3x2a2+6xa3−6a4)+Ce^{ax}\left(\frac{x^3}{a} - \frac{3x^2}{a^2} + \frac{6x}{a^3} - \frac{6}{a^4}\right) + C

∫x,ex,dx\int x,e^{x},dx

ex(x−1)+Ce^{x}(x - 1) + C

∫x2ex,dx\int x^2 e^{x},dx

ex(x2−2x+2)+Ce^{x}(x^2 - 2x + 2) + C

∫x,e−x,dx\int x,e^{-x},dx

−e−x(x+1)+C-e^{-x}(x + 1) + C

∫x2e−x,dx\int x^2 e^{-x},dx

−e−x(x2+2x+2)+C-e^{-x}(x^2 + 2x + 2) + C

∫x,2x,dx\int x,2^{x},dx

2x(xln⁡2−1(ln⁡2)2)+C2^{x}\left(\frac{x}{\ln 2} - \frac{1}{(\ln 2)^2}\right) + C

The coefficients inside each bracket are successive derivatives of the polynomial, with alternating signs and growing powers of 1a\frac{1}{a}. For x3eaxx^3 e^{ax} the numerators are x3x^3, 3x23x^2, 6x6x and 66, which are x3x^3 and its first three derivatives.

That pattern is the tabular method (often called the DI method). List the polynomial and its derivatives down one column until you reach zero, list eaxe^{ax} and its repeated antiderivatives down the other, then multiply diagonally with alternating signs. For x2exx^2 e^{x} the columns are x2,2x,2,0x^2, 2x, 2, 0 and ex,ex,ex,exe^{x}, e^{x}, e^{x}, e^{x}, giving x2ex−2x,ex+2exx^2e^{x} - 2x,e^{x} + 2e^{x}.

How Do You Integrate eaxsin⁡(bx)e^{ax}\sin(bx) And eaxcos⁡(bx)e^{ax}\cos(bx)?

You integrate by parts twice and then solve for the integral, because the second round brings the original integral back. That answers the Quora question "What is the integration method for e^(ax) sin (bx)?" and the forum request on askIITians to find "Integral e^ax sin(bx)".

Call the integral I=∫eaxsin⁡(bx),dxI = \int e^{ax}\sin(bx),dx. Parts with u=sin⁡(bx)u = \sin(bx) and dv=eax,dxdv = e^{ax},dx, done twice, gives

I=eaxsin⁡(bx)a−ba2eaxcos⁡(bx)−b2a2I.I = \frac{e^{ax}\sin(bx)}{a} - \frac{b}{a^2}e^{ax}\cos(bx) - \frac{b^2}{a^2}I.

Move the II terms to one side and divide by 1+b2a21 + \frac{b^2}{a^2}:

I=eax(asin⁡(bx)−bcos⁡(bx))a2+b2+C.I = \frac{e^{ax}\big(a\sin(bx) - b\cos(bx)\big)}{a^2 + b^2} + C.

A shorter route, for readers who have met Euler's formula, takes the imaginary part of ∫e(a+ib)x,dx=e(a+ib)xa+ib\int e^{(a+ib)x},dx = \frac{e^{(a+ib)x}}{a+ib}. Both routes land on the same rows.

Integral

Result

Condition

∫eaxsin⁡(bx),dx\int e^{ax}\sin(bx),dx

eax(asin⁡(bx)−bcos⁡(bx))a2+b2+C\frac{e^{ax}\big(a\sin(bx) - b\cos(bx)\big)}{a^2+b^2} + C

a2+b2≠0a^2 + b^2 \neq 0

∫eaxcos⁡(bx),dx\int e^{ax}\cos(bx),dx

eax(acos⁡(bx)+bsin⁡(bx))a2+b2+C\frac{e^{ax}\big(a\cos(bx) + b\sin(bx)\big)}{a^2+b^2} + C

a2+b2≠0a^2 + b^2 \neq 0

∫exsin⁡x,dx\int e^{x}\sin x,dx

ex2(sin⁡x−cos⁡x)+C\frac{e^{x}}{2}(\sin x - \cos x) + C

all real xx

∫excos⁡x,dx\int e^{x}\cos x,dx

ex2(sin⁡x+cos⁡x)+C\frac{e^{x}}{2}(\sin x + \cos x) + C

all real xx

∫e−xsin⁡x,dx\int e^{-x}\sin x,dx

−e−x2(sin⁡x+cos⁡x)+C-\frac{e^{-x}}{2}(\sin x + \cos x) + C

all real xx

∫ex(sin⁡x+cos⁡x),dx\int e^{x}(\sin x + \cos x),dx

exsin⁡x+Ce^{x}\sin x + C

all real xx

∫exsin⁡2x,dx\int e^{x}\sin^2 x,dx

ex2−ex10(cos⁡2x+2sin⁡2x)+C\frac{e^{x}}{2} - \frac{e^{x}}{10}\big(\cos 2x + 2\sin 2x\big) + C

all real xx

The sign pattern is the part worth memorising: the sine row has a minus between its terms and the cosine row has a plus. Differentiating the sine row once confirms it, since the bcos⁡b\cos and asin⁡a\sin pieces recombine into (a2+b2)sin⁡(bx)(a^2 + b^2)\sin(bx).

Which Exponential Integrals Need The Error Function?

∫e−x2,dx\int e^{-x^2},dx cannot be written with polynomials, roots, exponentials, logarithms or trig functions, so its antiderivative is a named special function, the error function. That is the honest answer to the Quora question "What is the value of the integral of e^{-x^2} with respect to x?":

∫e−x2,dx=π2erf⁡(x)+C,erf⁡(x)=2π∫0xe−t2,dt.\int e^{-x^2},dx = \frac{\sqrt{\pi}}{2}\operatorname{erf}(x) + C, \qquad \operatorname{erf}(x) = \frac{2}{\sqrt{\pi}}\int_{0}^{x} e^{-t^2},dt.

The definition matches the NIST Digital Library of Mathematical Functions, and erf⁡(1)≈0.8427\operatorname{erf}(1) \approx 0.8427. A related Quora question, "What is the integral of e^(-x)/x?", hits the second special function in this family, the exponential integral Ei⁡\operatorname{Ei}: ∫e−xx,dx=Ei⁡(−x)+C\int \frac{e^{-x}}{x},dx = \operatorname{Ei}(-x) + C for x≠0x \neq 0.

Integral

Result

Elementary?

∫e−x2,dx\int e^{-x^2},dx

π2erf⁡(x)+C\frac{\sqrt{\pi}}{2}\operatorname{erf}(x) + C

no

∫e−ax2,dx\int e^{-ax^2},dx

12πaerf⁡(a,x)+C\frac{1}{2}\sqrt{\frac{\pi}{a}}\operatorname{erf}(\sqrt{a},x) + C, a>0a > 0

no

∫ex2,dx\int e^{x^2},dx

π2erfi⁡(x)+C\frac{\sqrt{\pi}}{2}\operatorname{erfi}(x) + C

no

∫x,e−x2,dx\int x,e^{-x^2},dx

−12e−x2+C-\frac{1}{2}e^{-x^2} + C

yes

∫x2e−x2,dx\int x^2 e^{-x^2},dx

−x2e−x2+π4erf⁡(x)+C-\frac{x}{2}e^{-x^2} + \frac{\sqrt{\pi}}{4}\operatorname{erf}(x) + C

no

∫x3e−x2,dx\int x^3 e^{-x^2},dx

−12(x2+1)e−x2+C-\frac{1}{2}(x^2 + 1)e^{-x^2} + C

yes

∫e−x2x2,dx\int \frac{e^{-x^2}}{x^2},dx

−e−x2x−πerf⁡(x)+C-\frac{e^{-x^2}}{x} - \sqrt{\pi}\operatorname{erf}(x) + C, x≠0x \neq 0

no

∫exx,dx\int \frac{e^{x}}{x},dx

Ei⁡(x)+C\operatorname{Ei}(x) + C, x≠0x \neq 0

no

∫eaxx,dx\int \frac{e^{ax}}{x},dx

Ei⁡(ax)+C\operatorname{Ei}(ax) + C, x≠0x \neq 0

no

Here erfi⁡(x)=−ierf⁡(ix)\operatorname{erfi}(x) = -i\operatorname{erf}(ix) is the imaginary error function, a real-valued function for real xx. Read down the "Elementary?" column and a rule appears that no other table spells out: odd powers of xx times e−x2e^{-x^2} are elementary, even powers are not. An odd power leaves one spare xx to pair with dxdx for the substitution u=x2u = x^2; an even power leaves none.

What Are The Standard Definite Integrals Of Exponential Functions?

Most named definite exponential integrals run from 00 to ∞\infty, so they are improper integrals that converge because e−ax→0e^{-ax} \to 0 faster than any power of xx grows. The Quora question "What is the value of the integral of e-x2 from 0 to infinity, and why?" has a clean answer: π2\frac{\sqrt{\pi}}{2}.

The why is a two-dimensional detour. Square the whole-line integral G=∫−∞∞e−x2,dxG = \int_{-\infty}^{\infty} e^{-x^2},dx and write it as a double integral:

G2=∫−∞∞∫−∞∞e−(x2+y2),dx,dy.G^2 = \int_{-\infty}^{\infty}\int_{-\infty}^{\infty} e^{-(x^2+y^2)},dx,dy.

Switch to polar coordinates, where x2+y2=r2x^2 + y^2 = r^2 and dx,dy=r,dr,dθdx,dy = r,dr,d\theta. The extra rr is the spare factor the one-variable problem lacked:

G2=∫02π∫0∞e−r2,r,dr,dθ=2π⋅12=π.G^2 = \int_{0}^{2\pi}\int_{0}^{\infty} e^{-r^2},r,dr,d\theta = 2\pi \cdot \frac{1}{2} = \pi.

So G=πG = \sqrt{\pi}, and by symmetry the half-line value is π2≈0.8862\frac{\sqrt{\pi}}{2} \approx 0.8862.

Definite integral

Value

Approximate

∫−∞∞e−x2,dx\int_{-\infty}^{\infty} e^{-x^2},dx

π\sqrt{\pi}

1.77251.7725

∫0∞e−x2,dx\int_{0}^{\infty} e^{-x^2},dx

π2\frac{\sqrt{\pi}}{2}

0.88620.8862

∫0∞e−ax2,dx\int_{0}^{\infty} e^{-ax^2},dx

12πa\frac{1}{2}\sqrt{\frac{\pi}{a}}, a>0a > 0

∫0∞x2e−ax2,dx\int_{0}^{\infty} x^2 e^{-ax^2},dx

π4a3/2\frac{\sqrt{\pi}}{4a^{3/2}}, a>0a > 0

∫0∞e−ax,dx\int_{0}^{\infty} e^{-ax},dx

1a\frac{1}{a}, a>0a > 0

∫0∞x,e−ax,dx\int_{0}^{\infty} x,e^{-ax},dx

1a2\frac{1}{a^2}, a>0a > 0

∫0∞xne−x,dx\int_{0}^{\infty} x^{n}e^{-x},dx

Γ(n+1)\Gamma(n+1), which is nn factorial for whole nn

2424 when n=4n = 4

∫0∞e−axsin⁡(bx),dx\int_{0}^{\infty} e^{-ax}\sin(bx),dx

ba2+b2\frac{b}{a^2+b^2}, a>0a > 0

∫0∞e−axcos⁡(bx),dx\int_{0}^{\infty} e^{-ax}\cos(bx),dx

aa2+b2\frac{a}{a^2+b^2}, a>0a > 0

∫0∞e−ax2cos⁡(bx),dx\int_{0}^{\infty} e^{-ax^2}\cos(bx),dx

12πa,e−b2/(4a)\frac{1}{2}\sqrt{\frac{\pi}{a}},e^{-b^2/(4a)}, a>0a > 0

∫0∞dx1+ex\int_{0}^{\infty} \frac{dx}{1+e^{x}}

ln⁡2\ln 2

0.69310.6931

∫01ex,dx\int_{0}^{1} e^{x},dx

e−1e - 1

1.71831.7183

∫01e−x2,dx\int_{0}^{1} e^{-x^2},dx

π2erf⁡(1)\frac{\sqrt{\pi}}{2}\operatorname{erf}(1)

0.74680.7468

The Γ(n+1)\Gamma(n+1) row deserves a second look. ∫0∞xne−x,dx\int_{0}^{\infty} x^{n}e^{-x},dx is the gamma function, the integral that extends factorials to non-integers, and it is where the polynomial-times-exponential family meets the definite table. For more on evaluating with limits, see definite integrals.

Examples Of Integrals Of Exponential Functions

Example 1

Use the list to find ∫5e3x−2,dx\int 5e^{3x-2},dx.

Match the row ∫eax+b,dx\int e^{ax+b},dx with a=3a = 3 and b=−2b = -2:

∫5e3x−2,dx=5⋅13e3x−2+C\int 5e^{3x-2},dx = 5 \cdot \frac{1}{3}e^{3x-2} + C

=53e3x−2+C= \frac{5}{3}e^{3x-2} + C

Final answer: 53e3x−2+C\frac{5}{3}e^{3x-2} + C

Example 2

Evaluate ∫01ex2,dx\int_{0}^{1} e^{x^2},dx.

The first instinct copies the eaxe^{ax} row and divides by the derivative of the exponent, which is 2x2x:

Attempt: ∫ex2,dx=ex22x+C\text{Attempt: } \int e^{x^2},dx = \frac{e^{x^2}}{2x} + C

Differentiate the attempt to check it, using the quotient rule:

ddx[ex22x]=ex2−ex22x2\frac{d}{dx}\left[\frac{e^{x^2}}{2x}\right] = e^{x^2} - \frac{e^{x^2}}{2x^2}

The extra term −ex22x2-\frac{e^{x^2}}{2x^2} means the attempt is wrong. Dividing by the derivative of the exponent only works when that derivative is a constant. Here it is 2x2x, and no spare xx sits outside to absorb it, so ex2e^{x^2} belongs to the error-function family:

∫01ex2,dx=π2erfi⁡(1)\int_{0}^{1} e^{x^2},dx = \frac{\sqrt{\pi}}{2}\operatorname{erfi}(1)

≈0.8862×1.6504≈1.4627\approx 0.8862 \times 1.6504 \approx 1.4627

A numerical method gives the same value, which is how calculators handle it.

Final answer: π2erfi⁡(1)≈1.4627\frac{\sqrt{\pi}}{2}\operatorname{erfi}(1) \approx 1.4627

Example 3

Find ∫x2e−x,dx\int x^2 e^{-x},dx.

This is the Quora question "How to solve this integration ∫x2e−x,dx\int x^2 e^{-x},dx". Use the tabular method with DD column x2,2x,2,0x^2, 2x, 2, 0 and II column e−x,−e−x,e−x,−e−xe^{-x}, -e^{-x}, e^{-x}, -e^{-x}:

∫x2e−x,dx=x2(−e−x)−2x(e−x)+2(−e−x)+C\int x^2 e^{-x},dx = x^2(-e^{-x}) - 2x(e^{-x}) + 2(-e^{-x}) + C

=−e−x(x2+2x+2)+C= -e^{-x}(x^2 + 2x + 2) + C

Check: the derivative is e−x(x2+2x+2)−e−x(2x+2)=x2e−xe^{-x}(x^2 + 2x + 2) - e^{-x}(2x + 2) = x^2 e^{-x}.

Final answer: −e−x(x2+2x+2)+C-e^{-x}(x^2 + 2x + 2) + C

Example 4

Find ∫e2xcos⁡(3x),dx\int e^{2x}\cos(3x),dx.

Match the cosine row with a=2a = 2 and b=3b = 3, so a2+b2=13a^2 + b^2 = 13:

∫e2xcos⁡(3x),dx=e2x(2cos⁡(3x)+3sin⁡(3x))13+C\int e^{2x}\cos(3x),dx = \frac{e^{2x}\big(2\cos(3x) + 3\sin(3x)\big)}{13} + C

Final answer: e2x13(2cos⁡(3x)+3sin⁡(3x))+C\frac{e^{2x}}{13}\big(2\cos(3x) + 3\sin(3x)\big) + C

Example 5

Evaluate ∫0∞x3e−2x,dx\int_{0}^{\infty} x^3 e^{-2x},dx.

Substitute t=2xt = 2x, so x=t2x = \frac{t}{2} and dx=dt2dx = \frac{dt}{2}:

∫0∞x3e−2x,dx=∫0∞t38e−t,dt2\int_{0}^{\infty} x^3 e^{-2x},dx = \int_{0}^{\infty} \frac{t^3}{8}e^{-t},\frac{dt}{2}

=116∫0∞t3e−t,dt=116⋅Γ(4)= \frac{1}{16}\int_{0}^{\infty} t^3 e^{-t},dt = \frac{1}{16} \cdot \Gamma(4)

=616=38= \frac{6}{16} = \frac{3}{8}

Final answer: 38=0.375\frac{3}{8} = 0.375

Example 6

A drug's blood concentration after a dose is c(t)=20e−0.3tc(t) = 20e^{-0.3t} mg/L, with tt in hours. Find the area under the concentration curve from t=0t = 0 to t=10t = 10, and the total area to infinity.

Use the eaxe^{ax} row with a=−0.3a = -0.3:

∫01020e−0.3t,dt=[−200.3e−0.3t]010\int_{0}^{10} 20e^{-0.3t},dt = \left[-\frac{20}{0.3}e^{-0.3t}\right]_{0}^{10}

=2003(1−e−3)≈63.3475= \frac{200}{3}\left(1 - e^{-3}\right) \approx 63.3475

As the upper limit grows without bound, e−0.3t→0e^{-0.3t} \to 0, so the total area is 2003≈66.6667\frac{200}{3} \approx 66.6667.

Final answer: about 63.347563.3475 mg·h/L over 10 hours, and 2003≈66.6667\frac{200}{3} \approx 66.6667 mg·h/L in total

Why Does A Separate List For Exponential Integrals Exist?

Exponential integrals get their own list because exe^{x} survives integration unchanged, so every entry is "the same exponential, plus bookkeeping". The bookkeeping is what the list records.

  • Constants to divide by. eaxe^{ax} needs 1a\frac{1}{a} and axa^{x} needs 1ln⁡a\frac{1}{\ln a}; nothing else changes.

  • Polynomials to peel off. Each power of xx in front costs one round of parts, which is why the polynomial rows grow by one term per power.

  • A visible boundary. x,e−x2x,e^{-x^2} integrates in one line while e−x2e^{-x^2} needs a new function. The list shows exactly where closed forms stop, and that boundary is the bell curve at the centre of statistics, whose areas are tabulated through erf⁡\operatorname{erf} (the Gaussian integral is the reason the normal curve's total area works out).

Where Do Exponential Integrals Show Up In Real Life?

Exponential integrals appear wherever a quantity decays or grows at a rate proportional to its size, because the area under that curve is a total.

  • Medicine. The area under a drug-concentration curve (Example 6) measures total exposure, and with first-order elimination that curve is c0e−ktc_0e^{-kt}.

  • Radioactivity. The total number of decays over a time window is an integral of N0e−λtN_0e^{-\lambda t}, the same model behind exponential growth and decay.

  • Electric circuits. The charge that flows while a capacitor discharges is the integral of a current I0e−t/RCI_0e^{-t/RC}.

  • Statistics. Every normal-distribution probability is an area under e−x2/2e^{-x^2/2}, evaluated through erf⁡\operatorname{erf}.

  • Damped vibrations. Bridges, car suspensions and guitar strings settle with motion like e−atsin⁡(bt)e^{-at}\sin(bt), the family in the trig table.

Where Do Students Trip Up On Integrals Of Exponential Functions?

Mistake 1: Dividing By A Non-Constant Exponent Derivative

Where it slips in: Integrating ex2e^{x^2}, exe^{\sqrt{x}} or esin⁡xe^{\sin x} by copying the eaxe^{ax} row.

Don't do this: Writing ∫ex2,dx=ex22x+C\int e^{x^2},dx = \frac{e^{x^2}}{2x} + C.

The correct way: Divide only by a constant; with no matching factor outside, the integral belongs to the error-function family or needs numerical methods.

The rusher makes this one most often, because ∫e3x,dx=e3x3\int e^{3x},dx = \frac{e^{3x}}{3} feels like a rule about exponents rather than a rule about constants. The first instinct is always to divide by the derivative of whatever sits upstairs, so the habit worth building is to ask "is that derivative a number?" before dividing.

Mistake 2: Using The Power Rule On axa^x

Where it slips in: Integrating 2x2^{x} or 10x10^{x} right after a page of power-rule practice.

Don't do this: Writing ∫2x,dx=2x+1x+1+C\int 2^{x},dx = \frac{2^{x+1}}{x+1} + C.

The correct way: The variable is in the exponent, not the base, so rewrite 2x=exln⁡22^{x} = e^{x\ln 2} and get 2xln⁡2+C\frac{2^{x}}{\ln 2} + C.

The memorizer knows both rules perfectly and still swaps them, since x2x^2 and 2x2^x use the same two symbols. Reading the integrand aloud ("two to the x" versus "x squared") separates them.

Mistake 3: Dropping The Minus Sign In e−xe^{-x}

Where it slips in: Integrating e−xe^{-x}, x,e−xx,e^{-x} or e−xsin⁡xe^{-x}\sin x, where the inner derivative is −1-1.

Don't do this: Writing ∫e−x,dx=e−x+C\int e^{-x},dx = e^{-x} + C.

The correct way: Carry the −1-1: ∫e−x,dx=−e−x+C\int e^{-x},dx = -e^{-x} + C. In the trig rows, substitute a=−1a = -1 into the formula rather than reworking signs by hand.

Mistake 4: Losing The Circular Integral

Where it slips in: The second round of parts on eaxsin⁡(bx)e^{ax}\sin(bx), when the original integral reappears.

Don't do this: Starting a third round of parts, which cycles forever.

The correct way: Name the integral II, collect both II terms on one side and divide by 1+b2a21 + \frac{b^2}{a^2}.

The sign in Mistake 3 is not cosmetic. e−atsin⁡(bt)e^{-at}\sin(bt) is a vibration that dies out, while eatsin⁡(bt)e^{at}\sin(bt) is one that grows without bound. The 1940 Tacoma Narrows Bridge tore apart because wind produced a negative damping effect, so its twisting oscillation grew in amplitude instead of decaying, the real-world version of a flipped sign in the exponent.

Practice Problems On The List Of Integrals Of Exponential Functions

  1. Find ∫4e−2x,dx\int 4e^{-2x},dx.

  2. Find ∫5x,dx\int 5^{x},dx.

  3. Find ∫x,e3x,dx\int x,e^{3x},dx.

  4. Find ∫e−xcos⁡(2x),dx\int e^{-x}\cos(2x),dx.

  5. Evaluate ∫0∞e−4x2,dx\int_{0}^{\infty} e^{-4x^2},dx.

  6. Evaluate ∫0∞x2e−3x,dx\int_{0}^{\infty} x^2 e^{-3x},dx.

Answer to Question 1: −2e−2x+C-2e^{-2x} + C

Answer to Question 2: 5xln⁡5+C\frac{5^{x}}{\ln 5} + C

Answer to Question 3: e3x(x3−19)+Ce^{3x}\left(\frac{x}{3} - \frac{1}{9}\right) + C

Answer to Question 4: e−x5(2sin⁡(2x)−cos⁡(2x))+C\frac{e^{-x}}{5}\big(2\sin(2x) - \cos(2x)\big) + C

Answer to Question 5: π4≈0.4431\frac{\sqrt{\pi}}{4} \approx 0.4431

Answer to Question 6: 227≈0.0741\frac{2}{27} \approx 0.0741

The Short Version

  • The list of integrals of exponential functions grows from ∫ex,dx=ex+C\int e^{x},dx = e^{x} + C.

  • eaxe^{ax} divides by aa, axa^{x} divides by ln⁡a\ln a, and the division works only when the exponent's derivative is a constant.

  • Polynomials times exponentials use repeated parts, best organised with the tabular method.

  • eaxsin⁡(bx)e^{ax}\sin(bx) and eaxcos⁡(bx)e^{ax}\cos(bx) need parts twice and a solve for the repeated integral.

  • e−x2e^{-x^2} has no elementary antiderivative, yet its whole-line integral is exactly π\sqrt{\pi}.

Your Next Move

Work through practice problems 1 to 6; if you divide by something that contains xx, return to "How Do You Read A Table Of Exponential Integrals?" and check whether the exponent's derivative is a constant. Want a live Bhanzu trainer to help you build table-reading speed? Book a free demo class.

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Frequently Asked Questions

What is the integral of x^2e^x in the list of integrals of exponential functions?
ex(x2−2x+2)+Ce^{x}(x^2 - 2x + 2) + C. It is the n=2n = 2 polynomial row with a=1a = 1.
Can integration by parts be used to integrate e^(ax) sin(bx) dx?
Yes. Parts applied twice brings the original integral back, and solving for it gives eax(asin⁡bx−bcos⁡bx)a2+b2+C\frac{e^{ax}(a\sin bx - b\cos bx)}{a^2+b^2} + C. The tabular method also works if you stop after two rows and collect the repeated integral.
Write a value of ∫eaxsin⁡(bx),dx\int e^{ax}\sin(bx),dx from the list of integrals of exponential functions.
We derived it in the sine and cosine section: eax(asin⁡(bx)−bcos⁡(bx))a2+b2+C\frac{e^{ax}\big(a\sin(bx) - b\cos(bx)\big)}{a^2+b^2} + C.
What is the integral of e^(-x)/x?
It has no elementary formula. The antiderivative is Ei⁡(−x)+C\operatorname{Ei}(-x) + C for x≠0x \neq 0, where Ei⁡\operatorname{Ei} is the exponential integral; for x>0x > 0 this equals −E1(x)+C-E_1(x) + C, another common notation for the same function.
How to integrate e^x^2 sinx dx?
Read as ex2sin⁡xe^{x^2}\sin x, it has no elementary antiderivative, because even ex2e^{x^2} alone does not. Definite versions are evaluated numerically, for example with Simpson's rule or a calculator's integration function.
How to integrate x e^(-x^2) dx from 0 to infinity?
Substitute u=x2u = x^2, so x,dx=du2x,dx = \frac{du}{2}. The integral becomes 12∫0∞e−u,du=12\frac{1}{2}\int_{0}^{\infty} e^{-u},du = \frac{1}{2}. The spare xx is what makes this one elementary, unlike ∫e−x2,dx\int e^{-x^2},dx.
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