List of integrals of exponential functions explained

The following is a list of integrals of exponential functions. For a complete list of integral functions, please see the list of integrals.

Indefinite integral

Indefinite integrals are antiderivative functions. A constant (the constant of integration) may be added to the right hand side of any of these formulas, but has been suppressed here in the interest of brevity.

Integrals of polynomials

\intxecxdx=ecx\left(

cx-1
c2

\right)    forc0;

\intx2ecxdx=ecx\left(

x2-
c
2x+
c2
2
c3

\right)

\begin{align} \intxnecxdx&=

1
c

xnecx-

n
c

\intxn-1ecxdx\\ &=\left(

\partial
\partialc

\right)n

ecx
c

\\ &=ecx

n
\sum
i=0
in!
(n-i)!ci+1
(-1)

xn-i\\ &=ecx

n
\sum
i=0

(-1)n-i

n!
i!cn-i+1

xi \end{align}

\intecx
x

dx=ln|x|

infty(cx)n
nn!
+\sum
n=1
\intecx
xn

dx=

1\left(-
n-1
ecx+c\int
xn-1
ecx
xn-1

dx\right)    (forn1)

Integrals involving only exponential functions

\intf'(x)ef(x)dx=ef(x)

\intecxdx=

1
c

ecx

\intaxdx=

ax
lna

   fora>0,a\ne1

Integrals involving the error function

In the following formulas, is the error function and is the exponential integral.

\intecxlnxdx=

1
c

\left(ecxln|x|-\operatorname{Ei}(cx)\right)

\intx

cx2
e

dx=

1
2c
cx2
e

\int

-cx2
e

dx=\sqrt{

\pi
4c
} \operatorname(\sqrt x)

\int

-cx2
xedx=-
1
2c
-cx2
e

\int
-x2
e
x2

dx=-

-x2
e
x

-\sqrt{\pi}\operatorname{erf}(x)

\int{

1
\sigma\sqrt{2\pi
} e^}\,dx= \frac\operatorname\left(\frac\right)

Other integrals

\int

x2
e

dx=

x2
e

\left(

n-1
\sum
j=0

c2j

1
x2j+1

\right)+(2n-1)c2n-2\int

x2
e
x2n

dxvalidforanyn>0,

where

c2j=

1 ⋅ 3 ⋅ 5 … (2j-1)=
2j+1
(2j)!
j!22j+1

.

(Note that the value of the expression is independent of the value of, which is why it does not appear in the integral.)

{\int

x
x
\underbrace{x
}_mdx= \sum_^m\frac\Gamma(n+1,- \ln x) + \sum_^\infty(-1)^na_\Gamma(n+1,-\ln x) \qquad\textx> 0\text}

where

amn=\begin{cases}1&ifn=0,\\\dfrac{1}{n!}&ifm=1,

n
\\\dfrac{1}{n}\sum
j=1

jam,n-jam-1,j-1&otherwise\end{cases}

and is the upper incomplete gamma function.

\int

1
aeλ+b

dx=

x
b

-

1
bλ

ln\left(aeλ+b\right)

when

b0

,

λ0

, and

aeλ+b>0.

\int

e
aeλ+b

dx=

1
a2λ

\left[aeλ+b-bln\left(aeλ+b\right)\right]

when

a0

,

λ0

, and

aeλ+b>0.

\int

aecx-1dx=
becx-1
(a-b)log(1-becx)
bc

+x.

\int{ex\left(f\left(x\right)+f'\left(x\right)\right)dx

} = e^f\left(x \right) + C

\int{ex\left(f\left(x\right)-\left(-1\right)n

dnf\left(x\right)
dxn

\right)dx}=ex

n
\sum
k=1

{\left(-1\right)k

dkf\left(x\right)
dxk
} + C

\int{e-\left(f\left(x\right)-

dnf\left(x\right)
dxn

\right)dx}=-e-

n
\sum
k=1
dkf\left(x\right)
dxk

+C

\int{eax\left(\left(a\right)nf\left(x\right)-\left(-1\right)n

dnf\left(x\right)
dxn

\right)dx}=eax

n
\sum
k=1

{\left(a\right)n-k\left(-1\right)k

dkf\left(x\right)
dxk
} + C

Definite integrals

1
\begin{align} \int
0

exdx &=

1
\int\left(
0
a
b

\right)xbdx\\ &=

1
\int
0

axb1-xdx\\ &=

a-b
lna-lnb

   fora>0,b>0,ab \end{align}

The last expression is the logarithmic mean.

infty
\int
0

e-axdx=

1
a

(\operatorname{Re}(a)>0)

infty
\int
0
-ax2
edx=
1
2

\sqrt{\pi\overa}(a>0)

(the Gaussian integral)
infty
\int
-infty
-ax2
e

dx=\sqrt{\pi\overa}(a>0)

infty
\int
-infty
-ax2
e
-b
x2
edx=\sqrt{
\pi
a
}e^ \quad (a,b>0)
infty
\int
-infty
-(ax2+bx)
e

dx=\sqrt{\pi\over

\tfrac{b2
a}e

{4a}}(a>0)

infty
\int
-infty
-(ax2+bx+c)
e

dx=\sqrt{\pi\over

\tfrac{b2
a}e

{4a}-c}(a>0)

infty
\int
-infty
-ax2
e

e-2bxdx=\sqrt{

\pi
a
}e^ \quad (a>0) (see Integral of a Gaussian function)
infty
\int
-infty

x

-a(x-b)2
e

dx=b\sqrt{

\pi
a
} \quad (\operatorname(a)>0)
infty
\int
-infty

x

-ax2+bx
e

dx=

\sqrt{\pi
b

}{2a3/2

} e^ \quad (\operatorname(a)>0)
infty
\int
-infty

x2

-ax2
edx=
1
2

\sqrt{\pi\overa3}(a>0)

infty
\int
-infty

x2

-(ax2+bx)
edx=
\sqrt{\pi
(2a+b

2)}{4a5/2

} e^ \quad (\operatorname(a)>0)
infty
\int
-infty

x3

-(ax2+bx)
edx=
\sqrt{\pi
(6a+b

2)b}{8a7/2

} e^ \quad (\operatorname(a)>0)
infty
\int
0

xn

-ax2
e

dx=\begin{cases} \dfrac{\Gamma\left(

n+1
2
n+1
2
\right)}{2\left(a

\right)}&(n>-1,a>0)\\ \dfrac{(2k-1)!!}{2k+1ak}\sqrt{\dfrac{\pi}{a}}&(n=2k,kinteger,a>0)\\ \dfrac{k!}{2(ak+1)}&(n=2k+1,kinteger,a>0) \end{cases}

(the operator

!!

is the Double factorial)

infty
\int
0

xne-axdx=\begin{cases} \dfrac{\Gamma(n+1)}{an+1

} & (n>-1,\ \operatorname(a)>0) \\ \\ \dfrac & (n=0,1,2,\ldots,\ \operatorname(a)>0) \end
1
\int
0

xne-axdx=

n!
an+1

\left[1-e-a

n
\sum
i=0
ai
i!

\right]

b
\int
0

xne-axdx=

n!
an+1

\left[1-e-ab

n
\sum
i=0
(ab)i
i!

\right]

infty
\int
0
-axb
e

dx=

1
b
-1
b
a\Gamma\left(
1
b

\right)

infty
\int
0

xn

-axb
e

dx=

1
b
-n+1
b
a\Gamma\left(
n+1
b

\right)

infty
\int
0

e-ax\sinbxdx=

b
a2+b2

(a>0)

infty
\int
0

e-ax\cosbxdx=

a
a2+b2

(a>0)

infty
\int
0

xe-ax\sinbxdx=

2ab
(a2+b2)2

(a>0)

infty
\int
0

xe-ax\cosbxdx=

a2-b2
(a2+b2)2

(a>0)

infty
\int
0
e-ax\sinbx
x

dx=\arctan

b
a
infty
\int
0
e-ax-e-bx
x

dx=ln

b
a
infty
\int
0
e-ax-e-bx
x

\sinpxdx=\arctan

b
p

-\arctan

a
p
infty
\int
0
e-ax-e-bx
x

\cospxdx=

1
2

ln

b2+p2
a2+p2
infty
\int
0
e-ax(1-\cosx)
x2

dx=\arccota-

a
2

ln(

1
a2

+1)

infty
\int
-infty
ax4+bx3+cx2+dx+f
e

dx =ef

infty
\sum
n,m,p=0
b4n
(4n)!
c2m
(2m)!
d4p
(4p)!
\Gamma(3n+m+p+14)
3n+m+p+14
a

(appears in several models of extended superstring theory in higher dimensions)
2\pi
\int
0

exd\theta=2\piI0(x)

(is the modified Bessel function of the first kind)
2\pi
\int
0

exd\theta=2\piI0\left(\sqrt{x2+y2}\right)

inftyxs-1
ex/z-1
\int
0

dx=\operatorname{Li}s(z)\Gamma(s),

where

\operatorname{Li}s(z)

is the Polylogarithm.

infty\sinmx
e2-1
\int
0

dx=

1
4

\coth

m
2

-

1
2m

infty
\int
0

e-xlnxdx=-\gamma,

where

\gamma

is the Euler–Mascheroni constant which equals the value of a number of definite integrals.

Finally, a well known result,\int_0^ e^ d\phi = 2 \pi \delta_ \qquad\textm,n\in\mathbbwhere

\deltam,n

is the Kronecker delta.

See also

References

Toyesh Prakash Sharma, Etisha Sharma, "Putting Forward Another Generalization Of The Class Of Exponential Integrals And Their Applications.," International Journal of Scientific Research in Mathematical and Statistical Sciences, Vol.10, Issue.2, pp.1-8, 2023.https://www.isroset.org/pdf_paper_view.php?paper_id=3100&1-ISROSET-IJSRMSS-08692.pdf

Further reading

External links