List of logarithmic identities explained

In mathematics, many logarithmic identities exist. The following is a compilation of the notable of these, many of which are used for computational purposes.

Trivial identities

Trivial mathematical identities are relatively simple (for an experienced mathematician), though not necessarily unimportant. Trivial logarithmic identities are:

logb(1)=0

because

b0=1

logb(b)=1

because

b1=b

Explanations

By definition, we know that:

\color{black}log\color{blue}b\color{black}(\color{green}y\color{black})=\color{red}x\color{black}\iff\color{blue}b\color{black}\color{red}x\color{black}=\color{green}y\color{black}

,where

\color{blue}b\color{black}0

and

\color{blue}b\color{black}1

.

Setting

\color{red}x\color{black}=0

,we can see that:

\color{blue}b\color{black}\color{red}x\color{black}=\color{green}y\color{black} \iff\color{blue}b\color{black}\color{red}(0)\color{black}=\color{green}y\color{black} \iff\color{blue}1\color{black}=\color{green}y\color{black} \iff\color{green}y\color{black}=\color{blue}1\color{black}

. So, substituting these values into the formula, we see that:

\color{black}log\color{blue}b\color{black}(\color{green}y\color{black})=\color{red}x\color{black} \iff\color{black}log\color{blue}b\color{black}(\color{blue}1\color{black})=\color{red}0\color{black}

, which gets us the first property.

Setting

\color{red}x\color{black}=1

,we can see that:

\color{blue}b\color{black}\color{red}x\color{black}=\color{green}y\color{black} \iff\color{blue}b\color{black}\color{red}(1)\color{black}=\color{green}y\color{black} \iff\color{blue}b\color{black}=\color{green}y\color{black} \iff\color{green}y\color{black}=\color{blue}b\color{black}

. So, substituting these values into the formula, we see that:

\color{black}log\color{blue}b\color{black}(\color{green}y\color{black})=\color{red}x\color{black} \iff\color{black}log\color{blue}b\color{black}(\color{blue}b\color{black})=\color{red}1\color{black}

, which gets us the second property.

Cancelling exponentials

Logarithms and exponentials with the same base cancel each other. This is true because logarithms and exponentials are inverse operations—much like the same way multiplication and division are inverse operations, and addition and subtraction are inverse operations.

logb(x)
b

=xbecauseantilogb(logb(x))=x

x)
log
b(b

=xbecauselogb(antilogb(x))=x

[1]

Both of the above are derived from the following two equations that define a logarithm:(note that in this explanation, the variables of

\color{red}x\color{black}

and

x

may not be referring to the same number)

\color{black}log\color{blue}b\color{black}(\color{green}y\color{black})=\color{red}x\color{black}\iff\color{blue}b\color{black}\color{red}x\color{black}=\color{green}y\color{black}

Looking at the equation

\color{blue}b\color{black}\color{red}x\color{black}=\color{green}y\color{black}

, and substituting the value for

\color{red}x\color{black}

of

\color{black}log\color{blue}b\color{black}(\color{green}y\color{black})=\color{red}x\color{black}

, we get the following equation:

\color{blue}b\color{black}\color{red}x\color{black}=\color{green}y\color{black} \iff\color{blue}b\color{black}

logb(y)
\color{red}

\color{black}=\color{green}y\color{black} \iff\color{blue}b\color{black}\color{red}\color{blacklog\color{blue}b\color{black}(\color{green}y\color{black})}\color{black}=\color{green}y\color{black}

, which gets us the first equation.Another more rough way to think about it is that

\color{blue}b\color{black}\color{red}something\color{black}=\color{green}y\color{black}

,and that that "

\color{red}{something

}" is

\color{black}log\color{blue}b\color{black}(\color{green}y\color{black})

.

Looking at the equation

\color{black}log\color{blue}b\color{black}(\color{green}y\color{black})=\color{red}x\color{black}

, and substituting the value for

\color{green}y\color{black}

of

\color{blue}b\color{black}\color{red}x\color{black}=\color{green}y\color{black}

, we get the following equation:

\color{black}log\color{blue}b\color{black}(\color{green}y\color{black})=\color{red}x\color{black} \iff\color{black}log\color{blue}b\color{black}(\color{green}bx\color{black})=\color{red}x\color{black} \iff\color{black}log\color{blue}b\color{black}({\color{blue}b\color{black}\color{red}x\color{black}}\color{black})=\color{red}x\color{black}

, which gets us the second equation.Another more rough way to think about it is that

\color{black}log\color{blue}b\color{black}(\color{green}something\color{black})=\color{red}x\color{black}

,and that that something "

\color{green}something

" is

\color{blue}b\color{black}\color{red}x\color{black}

.

Using simpler operations

Logarithms can be used to make calculations easier. For example, two numbers can be multiplied just by using a logarithm table and adding. These are often known as logarithmic properties, which are documented in the table below.[2] The first three operations below assume that and/or, so that and . Derivations also use the log definitions and .

logb(xy)=logb(x)+logb(y)

because

bcbd=bc+d

logb(\tfrac{x}{y})=logb(x)-logb(y)

because

\tfrac{bc}{bd}=bc-d

d)=dlog
log
b(x)
because

(bc)d=bcd

log
b\left(\sqrt[y]{x}\right)=logb(x)
y
because

\sqrt[y]{x}=x1/y

logb(y)
x
logb(x)
=y
because
logb(y)
x
logb(x)logb(y)
=b
logb(y)
=(b
logb(x)
)
logb(x)
=y

clogb(x)+dlogb(y)=log

c
b(x

yd)

because
c
log
b(x
d)
y
b(y

Where

b

,

x

, and

y

are positive real numbers and

b\ne1

, and

c

and

d

are real numbers.

The laws result from canceling exponentials and the appropriate law of indices. Starting with the first law:

xy=

logb(x)
b
logb(y)
b

=

logb(x)+logb(y)
b

logb(xy)=

logb(x)+logb(y)
log
b(b

)=logb(x)+logb(y)

The law for powers exploits another of the laws of indices:

xy=

logb(x)
(b

)y=

ylogb(x)
b

y)
log
b(x

=ylogb(x)

The law relating to quotients then follows:

logb(

x
y

)=logb(xy-1)=logb(x)+

-1
log
b(y

)=logb(x)-logb(y)

logb(

1
y

)=

-1
log
b(y

)=-logb(y)

Similarly, the root law is derived by rewriting the root as a reciprocal power:

logb(\sqrt[y]x)=

1
y
log
b(x

)=

1
y

logb(x)

Derivations of product, quotient, and power rules

These are the three main logarithm laws/rules/principles,[3] from which the other properties listed above can be proven. Each of these logarithm properties correspond to their respective exponent law, and their derivations/proofs will hinge on those facts. There are multiple ways to derive/prove each logarithm law – this is just one possible method.

Logarithm of a product

To state the logarithm of a product law formally:

\forallb\inR+,b1,\forallx,y,\inR+,logb(xy)=logb(x)+logb(y)

Derivation:

Let

b\inR+

, where

b1

,and let

x,y\inR+

. We want to relate the expressions

logb(x)

and

logb(y)

. This can be done more easily by rewriting in terms of exponentials, whose properties we already know. Additionally, since we are going to refer to

logb(x)

and

logb(y)

quite often, we will give them some variable names to make working with them easier: Let

m=logb(x)

, and let

n=logb(y)

.

Rewriting these as exponentials, we see that

\begin{align} m&=logb(x)\iffbm=x,\\ n&=logb(y)\iffbn=y. \end{align}

From here, we can relate

bm

(i.e.

x

) and

bn

(i.e.

y

) using exponent laws as

xy=(bm)(bn)=bmbn=bm

To recover the logarithms, we apply

logb

to both sides of the equality.

logb(xy)=

m+n
log
b(b

)

The right side may be simplified using one of the logarithm properties from before: we know that

m+n
log
b(b

)=m+n

, giving

logb(xy)=m+n

We now resubstitute the values for

m

and

n

into our equation, so our final expression is only in terms of

x

,

y

, and

b

.

logb(xy)=logb(x)+logb(y)

This completes the derivation.

Logarithm of a quotient

To state the logarithm of a quotient law formally:

\forallb\inR+,b1,\forallx,y,\inR+,logb\left(

x
y

\right)=logb(x)-logb(y)

Derivation:

Let

b\inR+

, where

b1

,and let

x,y\inR+

.

We want to relate the expressions

logb(x)

and

logb(y)

. This can be done more easily by rewriting in terms of exponentials, whose properties we already know. Additionally, since we are going to refer to

logb(x)

and

logb(y)

quite often, we will give them some variable names to make working with them easier: Let

m=logb(x)

, and let

n=logb(y)

.

Rewriting these as exponentials, we see that:

\begin{align} m&=logb(x)\iffbm=x,\\ n&=logb(y)\iffbn=y. \end{align}

From here, we can relate

bm

(i.e.

x

) and

bn

(i.e.

y

) using exponent laws as
x
y

=

(bm)
(bn)

=

bm
bn

=bm

To recover the logarithms, we apply

logb

to both sides of the equality.

logb\left(

x
y

\right)=logb\left(bm\right)

The right side may be simplified using one of the logarithm properties from before: we know that

m-n
log
b(b

)=m-n

, giving

logb\left(

x
y

\right)=m-n

We now resubstitute the values for

m

and

n

into our equation, so our final expression is only in terms of

x

,

y

, and

b

.

logb\left(

x
y

\right)=logb(x)-logb(y)

This completes the derivation.

Logarithm of a power

To state the logarithm of a power law formally:

\forallb\inR+,b1,\forallx\inR+,\forallr\inR,

r)
log
b(x

=rlogb(x)

Derivation:

Let

b\inR+

, where

b1

, let

x\inR+

, and let

r\inR

. For this derivation, we want to simplify the expression
r)
log
b(x
. To do this, we begin with the simpler expression

logb(x)

. Since we will be using

logb(x)

often, we will define it as a new variable: Let

m=logb(x)

.

To more easily manipulate the expression, we rewrite it as an exponential. By definition,

m=logb(x)\iffbm=x

, so we have

bm=x

Similar to the derivations above, we take advantage of another exponent law. In order to have

xr

in our final expression, we raise both sides of the equality to the power of

r

:

\begin{align} (bm)r&=(x)r\\ bmr&=xr \end{align}

where we used the exponent law

(bm)r=bmr

.

To recover the logarithms, we apply

logb

to both sides of the equality.
mr
log
b(b

)=

r)
log
b(x

The left side of the equality can be simplified using a logarithm law, which states that

mr
log
b(b

)=mr

.

mr=

r)
log
b(x

Substituting in the original value for

m

, rearranging, and simplifying gives

\begin{align} \left(logb(x)\right)r&=

r)
log
b(x

\\ rlogb(x)&=

r)
log
b(x
r)
\\ log
b(x

&=rlogb(x) \end{align}

This completes the derivation.

Changing the base

To state the change of base logarithm formula formally:\forall a, b \in \mathbb_+, a, b \neq 1, \forall x \in \mathbb_+, \log_b(x) = \frac

This identity is useful to evaluate logarithms on calculators. For instance, most calculators have buttons for ln and for log10, but not all calculators have buttons for the logarithm of an arbitrary base.

Proof/derivation

Let

a,b\inR+

, where

a,b1

Let

x\inR+

. Here,

a

and

b

are the two bases we will be using for the logarithms. They cannot be 1, because the logarithm function is not well defined for the base of 1. The number

x

will be what the logarithm is evaluating, so it must be a positive number. Since we will be dealing with the term

logb(x)

quite frequently, we define it as a new variable: Let

m=logb(x)

.

To more easily manipulate the expression, it can be rewritten as an exponential.b^m = x

Applying

loga

to both sides of the equality,\log_a(b^m) = \log_a(x)

Now, using the logarithm of a power property, which states that

m)
log
a(b

=mloga(b)

,m\log_a(b) = \log_a(x)

Isolating

m

, we get the following:m = \frac

Resubstituting

m=logb(x)

back into the equation,\log_b(x) = \frac

This completes the proof that

logb(x)=

loga(x)
loga(b)
.

This formula has several consequences:

\log_b a = \frac 1

\log_ a =

b^ = d^

-\log_b a = \log_b \left(\right) = \log_ a

\log_a_1 \,\cdots\, \log_a_n= \log_a_1\, \cdots\, \log_a_n,

where \pi is any permutation of the subscripts . For example \log_b w\cdot \log_a x \cdot \log_d c \cdot \log_d z = \log_d w \cdot \log_b x \cdot \log_a c \cdot \log_d z.

Summation/subtraction

The following summation/subtraction rule is especially useful in probability theory when one is dealing with a sum of log-probabilities:

logb(a+c)=logba+logb\left(1+

c
a

\right)

because

\left(a+c\right)=a x \left(1+

c
a

\right)

logb(a-c)=logba+logb\left(1-

c
a

\right)

because

\left(a-c\right)=a x \left(1-

c
a

\right)

Note that the subtraction identity is not defined if

a=c

, since the logarithm of zero is not defined. Also note that, when programming,

a

and

c

may have to be switched on the right hand side of the equations if

c\gga

to avoid losing the "1 +" due to rounding errors. Many programming languages have a specific log1p(x) function that calculates

loge(1+x)

without underflow (when

x

is small).

More generally:\log _b \sum_^N a_i = \log_b a_0 + \log_b \left(1+\sum_^N \frac \right) = \log _b a_0 + \log_b \left(1+\sum_^N b^ \right)

Exponents

A useful identity involving exponents: x^ = \log(x)or more universally: x^ = a

Other/resulting identities

\frac = \log_(a) \frac = \log_(a)

Inequalities

Based on,[4] [5] and [6]

x
1+x

\leqln(1+x) \leq

x(6+x)
6+4x

\leqxforall{-1}<x

\begin{align} 2x&\leq3-\sqrt{
2+x
27
3+2x
}\leq\frac \\[4pt]&\leq \ln(1+x)\leq \frac\leq \frac\frac \\[4pt]&\text 0 \le x \text < x \le 0\end

All are accurate around

x=0

, but not for large numbers.

Calculus identities

\lim
x\to0+

loga(x)=-inftyifa>1

\lim
x\to0+

loga(x)=inftyif0<a<1

\limx\toinftyloga(x)=inftyifa>1

\limx\toinftyloga(x)=-inftyif0<a<1

\lim
x\to0+
blog
x
a(x)=0  

ifb>0

\limx\toinfty

loga(x)
xb

=0   ifb>0

The last limit is often summarized as "logarithms grow more slowly than any power or root of x".

Derivatives of logarithmic functions

{d\overdx}lnx={1\overx},x>0

{d\overdx}ln|x|={1\overx},x0

{d\overdx}logax={1\overxlna},x>0,a>0,anda1

Integral definition

lnx=

x
\int
1
1
t

dt

ln(n+1)=

\limk

k
\sum
i=1
1
xi

\Deltax=

\limk

k
\sum
i=1
1
1+
i-1
k
n

n
k

=

\limk

kn
\sum
x=1
1
1+
x
k

1
k

=

\limk

kn
\sum
x=1
1
k+x

=\limk

kn+k
\sum
x=k+1
1
x

=\limk

k(n+1)
\sum
x=k+1
1
x

for

style\Deltax=

n
k
and

xi

is a sample point in each interval.

Series representation

The natural logarithm

ln(1+x)=

infty
\sum
n=1
(-1)n+1xn
n

=x-

x2
2

+

x3
3

-

x4
4

+

x5
5

-

x6
6

+.

Within this interval, for

x=1

, the series is conditionally convergent, and for all other values, it is absolutely convergent. For

x>1

or

x\leq-1

, the series does not converge to

ln(1+x)

. In these cases, different representations or methods must be used to evaluate the logarithm.

Harmonic number difference

It is not uncommon in advanced mathematics, particularly in analytic number theory and asymptotic analysis, to encounter expressions involving differences or ratios of harmonic numbers at scaled indices.[8] The identity involving the limiting difference between harmonic numbers at scaled indices and its relationship to the logarithmic function provides an intriguing example of how discrete sequences can asymptotically relate to continuous functions. This identity is expressed as[9]

\lim{k

} (H_ - H_k) = \ln(n+1)

which characterizes the behavior of harmonic numbers as they grow large. This approximation (which precisely equals

ln(n+1)

in the limit) reflects how summation over increasing segments of the harmonic series exhibits integral properties, giving insight into the interplay between discrete and continuous analysis. It also illustrates how understanding the behavior of sums and series at large scales can lead to insightful conclusions about their properties. Here

Hk

denotes the

k

-th harmonic number, defined as

Hk=\sum{j=1

}^k \frac

The harmonic numbers are a fundamental sequence in number theory and analysis, known for their logarithmic growth. This result leverages the fact that the sum of the inverses of integers (i.e., harmonic numbers) can be closely approximated by the natural logarithm function, plus a constant, especially when extended over large intervals.[10] [8] [11] As

k

tends towards infinity, the difference between the harmonic numbers

Hk(n+1)

and

Hk

converges to a non-zero value. This persistent non-zero difference,

ln(n+1)

, precludes the possibility of the harmonic series approaching a finite limit, thus providing a clear mathematical articulation of its divergence.[12] [13] The technique of approximating sums by integrals (specifically using the integral test or by direct integral approximation) is fundamental in deriving such results. This specific identity can be a consequence of these approximations, considering:

\sum{j=k+1

}^ \frac \approx \int_k^ \frac

Harmonic limit derivation

The limit explores the growth of the harmonic numbers when indices are multiplied by a scaling factor and then differenced. It specifically captures the sum from

k+1

to

k(n+1)

:

H{k(n+1)

} - H_k = \sum_^ \frac

This can be estimated using the integral test for convergence, or more directly by comparing it to the integral of

1/x

from

k

to

k(n+1)

:

\lim{k

} \sum_^ \frac = \int_k^ \frac = \ln(k(n+1)) - \ln(k) = \ln\left(\frac\right) = \ln(n+1)

As the window's lower bound begins at

k+1

and the upper bound extends to

k(n+1)

, both of which tend toward infinity as

k\toinfty

, the summation window encompasses an increasingly vast portion of the smallest possible terms of the harmonic series (those with astronomically large denominators), creating a discrete sum that stretches towards infinity, which mirrors how continuous integrals accumulate value across an infinitesimally fine partitioning of the domain. In the limit, the interval is effectively from

1

to

n+1

where the onset

k

implies this minimally discrete region.

Double series formula

The harmonic number difference formula for

ln(m)

is an extension[9] of the classic, alternating identity of

ln(2)

:

ln(2)=\limk

k
\sum
n=1

\left(

1
2n-1

-

1
2n

\right)

which can be generalized as the double series over the residues of

m

:

ln(m)=\sumx

\sum
r\inZm\capN

\left(

1
x-r

-

1
x

\right)=\sumx

\sum
r\inZm\capN
r
x(x-r)

where

\langlem\rangle

is the principle ideal generated by

m

. Subtracting
style1
x
from each term
style1
x-r
(i.e., balancing each term with the modulus) reduces the magnitude of each term's contribution, ensuring convergence by controlling the series' tendency toward divergence as

m

increases. For example:

ln(4)=\limk

k
\sum
n=1

\left(

1
4n-3

-

1
4n

\right)+\left(

1
4n-2

-

1
4n

\right)+\left(

1
4n-1

-

1
4n

\right)

This method leverages the fine differences between closely related terms to stabilize the series. The sum over all residues

r\in\N

ensures that adjustments are uniformly applied across all possible offsets within each block of

m

terms. This uniform distribution of the "correction" across different intervals defined by

x-r

functions similarly to telescoping over a very large sequence. It helps to flatten out the discrepancies that might otherwise lead to divergent behavior in a straightforward harmonic series.

Deveci's Proof

style1
x
into a unit fraction, that is,
stylem
x

=

1
n
for

m\midx

, thus

m=\omega+1

rather than

m=|Zm\capN|

, where the extrema of

Zm\capN

are

[0,\omega]

if

N=N0

and

[1,\omega]

otherwise, with the minimum of

0

being implicit in the latter case due to the structural requirements of the proof. Since the cardinality of

Zm\capN

depends on the selection of one of two possible minima, the integral

style\int

1
t

dt

, as a set-theoretic procedure, is a function of the maximum

\omega

(which remains consistent across both interpretations) plus

1

, not the cardinality (which is ambiguous[14] [15] due to varying definitions of the minimum). Whereas the harmonic number difference computes the integral in a global sliding window, the double series, in parallel, computes the sum in a local sliding window—a shifting

m

-tuple—over the harmonic series, advancing the window by

m

positions to select the next

m

-tuple, and offsetting each element of each tuple by
style1
m
relative to the window's absolute position. The sum
k
style\sum
n=1

\sum

1
x-r
corresponds to

Hkm

which scales

Hm

without bound. The sum
k
style\sum-
n=1
1
n
corresponds to the prefix

Hk

trimmed from the series to establish the window's moving lower bound

k+1

, and

ln(m)

is the limit of the sliding window (the scaled, truncated[16] series):
k
\sum
n=1
\omega
\sum
r=1

\left(

1
mn-r

-

1
mn

\right)=

k
\sum
n=1
\omega
\sum
r=0

\left(

1
mn-r

-

1
mn

\right)

=

k
\sum
n=1

\left(-

1
n

+

\omega
\sum
r=0
1
mn-r

\right)

=-Hk+

k
\sum
n=1
\omega
\sum
r=0
1
mn-r

=-Hk+

k
\sum
n=1
\omega
\sum
r=0
1
(n-1)m+m-r

=-Hk+

k
\sum
n=1
m
\sum
j=1
1
(n-1)m+j

=-Hk+

k
\sum
n=1

\left(Hnm-Hm(n-1)\right)

=-Hk+Hmk

\limk=Hkm-Hk=\sumx

\sum
r\inZm\capN

\left(

1
x-r

-

1
x

\right)=ln(\omega+1)=ln(m)

Integrals of logarithmic functions

\intlnxdx=xlnx-x+C=x(lnx-1)+C

\intlogaxdx=xlogax-

x
lna

+C=

x(lnx-1)
lna

+C

To remember higher integrals, it is convenient to define

x\left=xn(log(x)-Hn)

where

Hn

is the nth harmonic number:

x\left=logx

x\left=xlog(x)-x

x\left=x2log(x)-\begin{matrix}

3
2

\end{matrix}x2

x\left=x3log(x)-\begin{matrix}

11
6

\end{matrix}x3

Then

d
dx

x\left[=nx\left[

\intx\left[dx=

x\left
n+1

+C

Approximating large numbers

The identities of logarithms can be used to approximate large numbers. Note that, where a, b, and c are arbitrary constants. Suppose that one wants to approximate the 44th Mersenne prime, . To get the base-10 logarithm, we would multiply 32,582,657 by, getting . We can then get .

Similarly, factorials can be approximated by summing the logarithms of the terms.

Complex logarithm identities

The complex logarithm is the complex number analogue of the logarithm function. No single valued function on the complex plane can satisfy the normal rules for logarithms. However, a multivalued function can be defined which satisfies most of the identities. It is usual to consider this as a function defined on a Riemann surface. A single valued version, called the principal value of the logarithm, can be defined which is discontinuous on the negative x axis, and is equal to the multivalued version on a single branch cut.

Definitions

In what follows, a capital first letter is used for the principal value of functions, and the lower case version is used for the multivalued function. The single valued version of definitions and identities is always given first, followed by a separate section for the multiple valued versions.

\operatorname{Log}(z)=ln(|z|)+i\operatorname{Arg}(z)

e\operatorname{Log(z)}=z

The multiple valued version of is a set, but it is easier to write it without braces and using it in formulas follows obvious rules.

When k is any integer:

log(z)=ln(|z|)+i\arg(z)

log(z)=\operatorname{Log}(z)+2\piik

elog(z)=z

Constants

Principal value forms:

\operatorname{Log}(1)=0

\operatorname{Log}(e)=1

Multiple value forms, for any k an integer:

log(1)=0+2\piik

log(e)=1+2\piik

Summation

Principal value forms:

\operatorname{Log}(z1)+\operatorname{Log}(z2)=\operatorname{Log}(z1z2)\pmod{2\pii}

\operatorname{Log}(z1)+\operatorname{Log}(z2)=\operatorname{Log}(z1z2)(-\pi<\operatorname{Arg}(z1)+\operatorname{Arg}(z2)\leq\pi;e.g.,\operatorname{Re}z1\geq0and\operatorname{Re}z2>0)

[17]

\operatorname{Log}(z1)-\operatorname{Log}(z2)=\operatorname{Log}(z1/z2)\pmod{2\pii}

\operatorname{Log}(z1)-\operatorname{Log}(z2)=\operatorname{Log}(z1/z2)(-\pi<\operatorname{Arg}(z1)-\operatorname{Arg}(z2)\leq\pi;e.g.,\operatorname{Re}z1\geq0and\operatorname{Re}z2>0)

[17]

Multiple value forms:

log(z1)+log(z2)=log(z1z2)

log(z1)-log(z2)=log(z1/z2)

Powers

A complex power of a complex number can have many possible values.

Principal value form:

z2
{z
1}

=

z2\operatorname{Log
e

(z1)}

z2
\operatorname{Log}{\left({z
1}

\right)}=z2\operatorname{Log}(z1)\pmod{2\pii}

Multiple value forms:

z2
{z
1}

=

z2log(z1)
e

Where, are any integers:

z2
log{\left({z
1}

\right)}=z2log(z1)+2\piik2

z2
log{\left({z
1}

\right)}=z2\operatorname{Log}(z1)+z22\piik1+2\piik2

External links

Notes and References

  1. Web site: Weisstein. Eric W.. Logarithm. 2020-08-29. mathworld.wolfram.com. en.
  2. Web site: 4.3 - Properties of Logarithms. 2020-08-29. people.richland.edu.
  3. Web site: Properties and Laws of Logarithms. courseware.cemc.uwaterloo.ca/8. 2022-04-23.
  4. Web site: Archived copy . 2016-12-20 . 2016-10-20 . https://web.archive.org/web/20161020123226/http://ajmaa.org/RGMIA/papers/v7n2/pade.pdf . dead .
  5. http://www.lkozma.net/inequalities_cheat_sheet/ineq.pdf
  6. http://downloads.hindawi.com/archive/2013/412958.pdf
  7. Web site: Weisstein . Eric W. . Mercator Series . MathWorld--A Wolfram Web Resource . 2024-04-24.
  8. Book: Flajolet . Philippe . Sedgewick . Robert . Analytic Combinatorics . 2009 . Cambridge University Press . 978-0521898065 . 389. See page 117, and VI.8 definition of shifted harmonic numbers on page 389
  9. Deveci. Sinan. On a Double Series Representation of the Natural Logarithm, the Asymptotic Behavior of Hölder Means, and an Elementary Estimate for the Prime Counting Function. 2022. 2211.10751. math.NT. See Theorem 5.2. on pages 22 - 23
  10. Book: Graham . Ronald L. . Knuth . Donald E. . Patashnik . Oren . Concrete Mathematics: A Foundation for Computer Science . 1994 . Addison-Wesley . 0-201-55802-5 . 429.
  11. Web site: Harmonic Number . Wolfram MathWorld . 2024-04-24. See formula 13.
  12. Kifowit . Steven J. . More Proofs of Divergence of the Harmonic Series . Prairie State College . 2019 . 2024-04-24. See Proofs 23 and 24 for details on the relationship between harmonic numbers and logarithmic functions.
  13. Bell . Jordan . Blåsjö . Viktor . Pietro Mengoli's 1650 Proof That the Harmonic Series Diverges . Mathematics Magazine . 91 . 5 . 2018 . 341–347 . 10.1080/0025570X.2018.1506656 . 48665556 . 1874/407528 . 2024-04-24. free .
  14. 1102.0418 . Peter . Harremoës . Is Zero a Natural Number? . 2011. math.HO . A synopsis on the nature of 0 which frames the choice of minimum as the dichotomy between ordinals and cardinals.
  15. Barton . N. . 2020 . Absence perception and the philosophy of zero . Synthese . 197 . 9 . 3823–3850 . 10.1007/s11229-019-02220-x . 7437648 . 32848285. See section 3.1
  16. The

    k+1

    shift is characteristic of the right Riemann sum employed to prevent the integral from degenerating into the harmonic series, thereby averting divergence. Here,
    style-1
    n
    functions analogously, serving to regulate the series. The successor operation

    m=\omega+1

    signals the implicit inclusion of the modulus

    m

    (the region omitted from

    N1

    ). The importance of this, from an axiomatic perspective, becomes evident when the residues of

    m

    are formulated as

    eln(\omega

    , where

    \omega+1

    is bootstrapped by

    \omega=0

    to produce the residues of modulus

    m=\omega=\omega0+1=1

    . Consequently,

    \omega

    represents a limiting value in this context.
  17. Book: Abramowitz, Milton. Handbook of mathematical functions, with formulas, graphs, and mathematical tables. 1965. Dover Publications. Irene A. Stegun. 0-486-61272-4. New York. 429082.