In mathematics, many logarithmicidentities exist. The following is a compilation of the notable of these, many of which are used for computational purposes.
Trivial mathematical identities are relatively simple (for an experienced mathematician), though not necessarily unimportant. The trivial logarithmic identities are as follows:
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.
Both of the above are derived from the following two equations that define a logarithm:
(note that in this explanation, the variables of and may not be referring to the same number)
Looking at the equation , and substituting the value for of
, we get the following equation:
, which gets us the first equation.
Another more rough way to think about it is that ,
and that that "" is .
Looking at the equation
, and substituting the value for of , we get the following equation:
, which gets us the second equation.
Another more rough way to think about it is that ,
and that that something "" is .
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 x = bc and/or y = bd, so that logb(x) = c and logb(y) = d. Derivations also use the log definitions x = blogb(x) and x = logb(bx).
because
because
because
because
because
because
Where , , and are positive real numbers and , and and are real numbers.
The laws result from canceling exponentials and the appropriate law of indices. Starting with the first law:
The law for powers exploits another of the laws of indices:
The law relating to quotients then follows:
Similarly, the root law is derived by rewriting the root as a reciprocal power:
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.
Let , where ,
and let . We want to relate the expressions and . 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 and quite often, we will give them some variable names to make working with them easier: Let , and let .
Rewriting these as exponentials, we see that
From here, we can relate (i.e. ) and (i.e. ) using exponent laws as
To recover the logarithms, we apply to both sides of the equality.
The right side may be simplified using one of the logarithm properties from before: we know that , giving
We now resubstitute the values for and into our equation, so our final expression is only in terms of , , and .
To state the logarithm of a quotient law formally:
Derivation:
Let , where ,
and let .
We want to relate the expressions and . 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 and quite often, we will give them some variable names to make working with them easier: Let , and let .
Rewriting these as exponentials, we see that:
From here, we can relate (i.e. ) and (i.e. ) using exponent laws as
To recover the logarithms, we apply to both sides of the equality.
The right side may be simplified using one of the logarithm properties from before: we know that , giving
We now resubstitute the values for and into our equation, so our final expression is only in terms of , , and .
Let , where , let , and let . For this derivation, we want to simplify the expression . To do this, we begin with the simpler expression . Since we will be using often, we will define it as a new variable: Let .
To more easily manipulate the expression, we rewrite it as an exponential. By definition, , so we have
Similar to the derivations above, we take advantage of another exponent law. In order to have in our final expression, we raise both sides of the equality to the power of :
where we used the exponent law .
To recover the logarithms, we apply to both sides of the equality.
The left side of the equality can be simplified using a logarithm law, which states that .
Substituting in the original value for , rearranging, and simplifying gives
To state the change of base logarithm formula formally:
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.
Let , where Let . Here, and 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.[citation needed] The number will be what the logarithm is evaluating, so it must be a positive number. Since we will be dealing with the term quite frequently, we define it as a new variable: Let .
To more easily manipulate the expression, it can be rewritten as an exponential.
Applying to both sides of the equality,
Now, using the logarithm of a power property, which states that ,
Isolating , we get the following:
Resubstituting back into the equation,
This completes the proof that .
This formula has several consequences:
where is any permutation of the subscripts 1, ..., n. For example
The following summation/subtraction rule is especially useful in probability theory when one is dealing with a sum of log-probabilities:
because
because
Note that the subtraction identity is not defined if , since the logarithm of zero is not defined. Also note that, when programming, and may have to be switched on the right hand side of the equations if to avoid losing the "1 +" due to rounding errors. Many programming languages have a specific log1p(x) function that calculates without underflow (when is small).
Within this interval, for , the series is conditionally convergent, and for all other values, it is absolutely convergent. For or , the series does not converge to . In these cases, different representations[8] or methods must be used to evaluate the logarithm.
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.[9] 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[10]
which characterizes the behavior of harmonic numbers as they grow large. This approximation (which precisely equals 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 denotes the -th harmonic number, defined as
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.[11][9][12] As tends towards infinity, the difference between the harmonic numbers and converges to a non-zero value. This persistent non-zero difference, , precludes the possibility of the harmonic series approaching a finite limit, thus providing a clear mathematical articulation of its divergence.[13][14] 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:
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 to :
This can be estimated using the integral test for convergence, or more directly by comparing it to the integral of from to :
As the window's lower bound begins at and the upper bound extends to , both of which tend toward infinity as , 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 to where the onset implies this minimally discrete region.
which can be generalized as the double series over the residues of :
where is the principle ideal generated by . Subtracting from each term (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 increases. For example:
This method leverages the fine differences between closely related terms to stabilize the series. The sum over all residues ensures that adjustments are uniformly applied across all possible offsets within each block of terms. This uniform distribution of the "correction" across different intervals defined by 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. Note that the structure of the summands of this formula matches those of the interpolated harmonic number when both the domain and range are negated (i.e., ). However, the interpretation and roles of the variables differ.
A fundamental feature of the proof is the accumulation of the subtrahends into a unit fraction, that is, for , thus rather than , where the extrema of are if and otherwise, with the minimum of being implicit in the latter case due to the structural requirements of the proof. Since the cardinality of depends on the selection of one of two possible minima, the integral , as a set-theoretic procedure, is a function of the maximum (which remains consistent across both interpretations) plus , not the cardinality (which is ambiguous[15][16] 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 -tuple—over the harmonic series, advancing the window by positions to select the next -tuple, and offsetting each element of each tuple by relative to the window's absolute position. The sum corresponds to which scales without bound. The sum corresponds to the prefix trimmed from the series to establish the window's moving lower bound , and is the limit of the sliding window (the scaled, truncated[17] series):
The identities of logarithms can be used to approximate large numbers. Note that logb(a) + logb(c) = logb(ac), where a, b, and c are arbitrary constants. Suppose that one wants to approximate the 44th Mersenne prime, 232,582,657 −1. To get the base-10 logarithm, we would multiply 32,582,657 by log10(2), getting 9,808,357.09543 = 9,808,357 + 0.09543. We can then get 109,808,357 × 100.09543 ≈ 1.25 × 109,808,357.
Similarly, factorials can be approximated by summing the logarithms of the terms.
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.
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.
where is the harmonic mean of . This is derived from the fact that the difference between the th harmonic number and asymptotically approaches a small constant, resulting in . This behavior can also be derived from the properties of logarithms: is half of , and this "first half" is the natural log of the root of , which corresponds roughly to the first th of the sum , or . The asymptotic equivalence of the first th of to the latter th of the series is expressed as follows:
which generalizes to:
and:
for fixed . The correspondence sets as a unit magnitude that partitions across powers, where each interval to , to , etc., corresponds to one unit, illustrating that forms a divergent series as .
^Weisstein, Eric W. "Mercator Series". MathWorld--A Wolfram Web Resource. Retrieved 2024-04-24.
^To extend the utility of the Mercator series beyond its conventional bounds one can calculate for and and then negate the result, , to derive . For example, setting yields .
^ abFlajolet, Philippe; Sedgewick, Robert (2009). Analytic Combinatorics. Cambridge University Press. p. 389. ISBN978-0521898065. See page 117, and VI.8 definition of shifted harmonic numbers on page 389
^ abcdDeveci, Sinan (2022). "On a Double Series Representation of the Natural Logarithm, the Asymptotic Behavior of Hölder Means, and an Elementary Estimate for the Prime Counting Function". arXiv:2211.10751 [math.NT]. See Theorem 5.2. on pages 22 - 23
^Graham, Ronald L.; Knuth, Donald E.; Patashnik, Oren (1994). Concrete Mathematics: A Foundation for Computer Science. Addison-Wesley. p. 429. ISBN0-201-55802-5.
^"Harmonic Number". Wolfram MathWorld. Retrieved 2024-04-24. See formula 13.
^Kifowit, Steven J. (2019). More Proofs of Divergence of the Harmonic Series(PDF) (Report). Prairie State College. Retrieved 2024-04-24. See Proofs 23 and 24 for details on the relationship between harmonic numbers and logarithmic functions.
^Harremoës, Peter (2011). "Is Zero a Natural Number?". arXiv:1102.0418 [math.HO]. A synopsis on the nature of 0 which frames the choice of minimum as the dichotomy between ordinals and cardinals.
^The shift is characteristic of the right Riemann sum employed to prevent the integral from degenerating into the harmonic series, thereby averting divergence. Here, functions analogously, serving to regulate the series. The successor operation signals the implicit inclusion of the modulus (the region omitted from ). The importance of this, from an axiomatic perspective, becomes evident when the residues of are formulated as , where is bootstrapped by to produce the residues of modulus . Consequently, represents a limiting value in this context.