Exponential and logarithmic functions of a complex variable. Definition and properties. Expressions using complex numbers



Plan:

    Introduction
  • 1 Real logarithm
    • 1.1 Properties
    • 1.2 Logarithmic function
    • 1.3 Natural logarithms
    • 1.4 Decimal logarithms
  • 2 Complex logarithm
    • 2.1 Definition and properties
    • 2.2 Examples
    • 2.3 Analytical continuation
    • 2.4 Riemann surface
  • 3 Historical sketch
    • 3.1 Real logarithm
    • 3.2 Complex logarithm
  • 4 Logarithmic tables
  • 5 Applications
  • Literature
    Notes

Introduction

Rice. 1. Graphs of logarithmic functions

Logarithm of a number b based on a (from Greek λόγος - “word”, “attitude” and ἀριθμός - “number”) is defined as an indicator of the power to which the base must be raised a to get the number b. Designation: . From the definition it follows that the records and are equivalent.

For example, because.


1. Real logarithm

Logarithm of a real number log a b makes sense when . As is known, the exponential function y = a x is monotonic and each value takes only once, and the range of its values ​​contains all positive real numbers. It follows that the value of the real logarithm of a positive number always exists and is uniquely determined.

The most widely used types of logarithms are:


1.1. Properties

Proof

Let's prove that .

(since by condition bc > 0). ■

Proof

Let's prove that

(since by condition ■

Proof

We use the identity to prove it. Let's logarithm both sides of the identity to base c. We get:

Proof

Let's prove that .

(because b p> 0 by condition). ■

Proof

Let's prove that

Proof

Logarithm the left and right sides to the base c :

Left side: Right side:

The equality of expressions is obvious. Since logarithms are equal, then, due to the monotonicity of the logarithmic function, the expressions themselves are equal. ■


1.2. Logarithmic function

If we consider the logarithmic number as a variable, we get logarithmic function y=log a x (see Fig. 1). It is defined at . Range of values: .

The function is strictly increasing at a> 1 and strictly decreasing at 0< a < 1 . График любой логарифмической функции проходит через точку (1;0) . Функция непрерывна и неограниченно дифференцируема всюду в своей области определения.

Straight x= 0 is a left vertical asymptote, since at a> 1 and at 0< a < 1 .

The derivative of the logarithmic function is equal to:

Proof

I. Let us prove that

Let's write down the identity e ln x = x and differentiate its left and right sides

We get that, from which it follows that

II. Let's prove that

The logarithmic function carries out an isomorphism between the multiplicative group of positive real numbers and the additive group of all real numbers.


1.3. Natural logarithms

Relationship with the decimal logarithm: .

As stated above, the derivative of the natural logarithm has a simple formula:

For this reason, natural logarithms are predominantly used in mathematical research. They often appear when solving differential equations, studying statistical dependencies (for example, the distribution of prime numbers), etc.

The indefinite integral of the natural logarithm can be easily found by integrating by parts:

The Taylor series expansion can be represented as follows:
when the equality is true

(1)

In particular,

This series converges faster, and in addition, the left side of the formula can now express the logarithm of any positive number.


1.4. Decimal logarithms

Rice. 2a. Logarithmic scale

Rice. 2b. Logarithmic scale with symbols

Logarithms to base 10 (symbol: lg a) before the invention of calculators were widely used for calculations. The uneven scale of decimal logarithms is usually applied to slide rules. A similar scale is used in many fields of science, for example:

  • Physics - sound intensity (decibels).
  • Astronomy - star brightness scale.
  • Chemistry - hydrogen ion activity (pH).
  • Seismology - Richter scale.
  • Music theory - a scale of notes, in relation to the frequencies of musical notes.
  • History is a logarithmic time scale.

The logarithmic scale is also widely used to identify the exponent in power relations and the coefficient in the exponent. In this case, a graph constructed on a logarithmic scale along one or two axes takes the form of a straight line, which is easier to study.


2. Complex logarithm

2.1. Definition and properties

For complex numbers, the logarithm is defined in the same way as a real one. In practice, the natural complex logarithm is used almost exclusively, which we denote and define as the set of all complex numbers z such that e z = w . The complex logarithm exists for any , and its real part is determined uniquely, while the imaginary part has an infinite number of values. For this reason it is called a multi-valued function. If you imagine w in demonstrative form:

,

then the logarithm is found by the formula:

Here is the real logarithm, r = | w | , k- arbitrary integer. The value obtained when k= 0, called main importance complex natural logarithm; it is customary to take the value of the argument in it in the interval (− π,π]. The corresponding (already single-valued) function is called main branch logarithm and is denoted by . Sometimes they also denote a logarithm value that is not on the main branch.

From the formula it follows:

  • The real part of the logarithm is determined by the formula:
  • The logarithm of a negative number is found by the formula:

Since complex trigonometric functions are related to the exponent (Euler's formula), the complex logarithm, as the inverse function of the exponential, is related to the inverse trigonometric functions. An example of such a connection:


2.2. Examples

Let's give the main value of the logarithm for some arguments:

You should be careful when converting complex logarithms, taking into account that they are multi-valued, and therefore the equality of the logarithms of any expressions does not imply the equality of these expressions. Example of flawed reasoning:

iπ = ln(− 1) = ln((− i) 2) = 2ln(− i) = 2(− iπ / 2) = − iπ - sheer absurdity.

Note that on the left is the main value of the logarithm, and on the right is the value from the underlying branch ( k= − 1 ). The cause of the error is the careless use of the property, which, generally speaking, implies in the complex case the entire infinite set of logarithm values, and not just the main value.


2.3. Analytical continuation

Rice. 3. Complex logarithm (imaginary part)

The logarithm of a complex number can also be defined as the analytic extension of the real logarithm to the entire complex plane. Let the curve Γ begin at unity, not pass through zero, and not intersect the negative part of the real axis. Then the principal value of the logarithm at the end point w curve Γ can be determined by the formula:

If Γ is a simple curve (without self-intersections), then for the numbers lying on it, logarithmic identities can be applied without fear, for example

If the curve Γ is allowed to intersect the negative part of the real axis, then the first such intersection transfers the result from the principal value branch to the adjacent branch, and each subsequent intersection causes a similar shift along the branches of the logarithmic function (see figure).

From the analytic continuation formula it follows that on any branch of the logarithm

For any circle S, covering point 0:

The integral is taken in the positive direction (counterclockwise). This identity underlies the theory of residues.

You can also define the analytical continuation of the complex logarithm using the above series (1), generalized to the case of a complex argument. However, from the type of expansion it follows that at unity it is equal to zero, that is, the series relates only to the main branch of the multivalued function of the complex logarithm.


2.4. Riemann surface

A complex logarithmic function is an example of a Riemann surface; its imaginary part (Fig. 3) consists of an infinite number of branches twisted in the form of a spiral. This surface is simply connected; its only zero (of first order) is obtained at z= 1, singular points: z= 0 and (branch points of infinite order).

The Riemann surface of the logarithm is the universal covering for the complex plane without the point 0.


3. Historical sketch

3.1. Real logarithm

The need for complex calculations grew rapidly in the 16th century, and much of the difficulty involved multiplying and dividing multi-digit numbers and taking roots. At the end of the century, several mathematicians, almost simultaneously, came up with the idea: to replace labor-intensive multiplication with simple addition, using special tables to compare the geometric and arithmetic progressions, with the geometric one being the original one. Then division is automatically replaced by the immeasurably simpler and more reliable subtraction, and extracting the root of the degree n comes down to dividing the logarithm of the radical expression by n. He was the first to publish this idea in his book “ Arithmetica integra"Michael Stiefel, who, however, did not make any serious efforts to implement his idea.

In 1614, the Scottish amateur mathematician John Napier published an essay in Latin entitled " Description of the amazing table of logarithms"(lat. Mirifici Logarithmorum Canonis Descriptio ). It contained a brief description of logarithms and their properties, as well as 8-digit tables of logarithms of sines, cosines and tangents, with a step of 1". Term logarithm, proposed by Napier, has established itself in science. Napier outlined the theory of logarithms in his other book “ Building an Amazing Logarithm Table"(lat. Mirifici Logarithmorum Canonis Constructio ), published posthumously in 1619 by his son.

The concept of function did not yet exist, and Napier defined the logarithm kinematically, comparing uniform and logarithmically slow motion; for example, he defined the logarithm of sine as follows:

The logarithm of a given sine is a number that always increased arithmetically at the same rate at which the total sine began to decrease geometrically.

In modern notation, Napier’s kinematic model can be represented by the differential equation: dx/x = -dy/M, where M is a scale factor introduced to ensure that the value turns out to be an integer with the required number of digits (decimal fractions were not yet widely used). Napier took M = 10000000.

Strictly speaking, Napier tabulated the wrong function, which is now called the logarithm. If we denote its function LogNap(x), then it is related to the natural logarithm as follows:

Obviously, LogNap(M) = 0, that is, the logarithm of the “full sine” is zero - this is what Napier achieved with his definition. .

The main property of the Napier logarithm: if quantities form a geometric progression, then their logarithms form an arithmetic progression. However, the logarithm rules for the neper function differed from the rules for the modern logarithm.

For example, LogNap(ab) = LogNap(a) + LogNap(b) - LogNap(1).

Unfortunately, all the values ​​in Napier's table contained a computational error after the sixth digit. However, this did not prevent the new calculation method from gaining wide popularity, and many European mathematicians, including Kepler, began compiling logarithmic tables. Just 5 years later, in 1619, London mathematics teacher John Spidell ( John Speidell) reissued Napier's tables, transformed so that they effectively became tables of natural logarithms (although Spidell retained the scaling to integers). The term "natural logarithm" was proposed by the Italian mathematician Pietro Mengoli ( Pietro Mengoli)) in the middle of the 16th century.

In the 1620s, Edmund Wingate and William Oughtred invented the first slide rule, before the advent of pocket calculators - an indispensable engineer's tool.

A close to modern understanding of logarithmization - as the inverse operation of raising to a power - first appeared with Wallis and Johann Bernoulli, and was finally legitimized by Euler in the 18th century. In the book “Introduction to the Analysis of Infinites” (1748), Euler gave modern definitions of both exponential and logarithmic functions, expanded them into power series, and especially noted the role of the natural logarithm.

Euler is also credited with extending the logarithmic function to the complex domain.


3.2. Complex logarithm

The first attempts to extend logarithms to complex numbers were made at the turn of the 17th-18th centuries by Leibniz and Johann Bernoulli, but they failed to create a holistic theory, primarily because the very concept of a logarithm was not yet clearly defined. The discussion on this issue took place first between Leibniz and Bernoulli, and in the middle of the 18th century - between d'Alembert and Euler. Bernoulli and d'Alembert believed that it should be determined log(-x) = log(x). The complete theory of logarithms of negative and complex numbers was published by Euler in 1747-1751 and is essentially no different from the modern one.

Although the dispute continued (D'Alembert defended his point of view and argued it in detail in an article in his Encyclopedia and in other works), Euler's point of view quickly gained universal recognition.


4. Logarithmic tables

Logarithmic tables

From the properties of the logarithm it follows that instead of labor-intensive multiplication of multi-digit numbers, it is enough to find (from tables) and add their logarithms, and then, using the same tables, perform potentiation, that is, find the value of the result from its logarithm. Doing division differs only in that logarithms are subtracted. Laplace said that the invention of logarithms “extended the life of astronomers” by greatly speeding up the process of calculations.

When moving the decimal point in a number to n digits, the value of the decimal logarithm of this number changes to n. For example, log8314.63 = log8.31463 + 3. It follows that it is enough to compile a table of decimal logarithms for numbers in the range from 1 to 10.

The first tables of logarithms were published by John Napier (1614), and they contained only logarithms of trigonometric functions, and with errors. Independently of him, Joost Burgi, a friend of Kepler, published his tables (1620). In 1617, Oxford mathematics professor Henry Briggs published tables that already included decimal logarithms of the numbers themselves, from 1 to 1000, with 8 (later 14) digits. But there were also errors in Briggs' tables. The first error-free edition based on the Vega tables (1783) appeared only in 1857 in Berlin (Bremiwer tables).

In Russia, the first tables of logarithms were published in 1703 with the participation of L. F. Magnitsky. Several collections of logarithm tables were published in the USSR.

  • Bradis V. M. Four-digit math tables. 44th edition, M., 1973.

Bradis tables (1921) were used in educational institutions and in engineering calculations that did not require great accuracy. They contained mantissas of decimal logarithms of numbers and trigonometric functions, natural logarithms, and some other useful calculation tools.

  • Vega G. Tables of seven-digit logarithms, 4th edition, M., 1971.

Professional collection for precise calculations.

  • Five-digit tables of natural values ​​of trigonometric quantities, their logarithms and logarithms of numbers, 6th ed., M.: Nauka, 1972.
  • Tables of natural logarithms, 2nd edition, in 2 volumes, M.: Nauka, 1971.

Nowadays, with the spread of calculators, the need to use tables of logarithms has disappeared.

M, Feature (complex analysis).

(from Greek λόγος - “word”, “relation” and ἀριθμός - “number”) numbers b based on a(log α b) is called such a number c, And b= a c, that is, records log α b=c And b=ac are equivalent. The logarithm makes sense if a > 0, a ≠ 1, b > 0.

In other words logarithm numbers b based on A formulated as an exponent to which a number must be raised a to get the number b(logarithm exists only for positive numbers).

From this formulation it follows that the calculation x= log α b, is equivalent to solving the equation a x =b.

For example:

log 2 8 = 3 because 8 = 2 3 .

Let us emphasize that the indicated formulation of the logarithm makes it possible to immediately determine logarithm value, when the number under the logarithm sign acts as a certain power of the base. Indeed, the formulation of the logarithm makes it possible to justify that if b=a c, then the logarithm of the number b based on a equals With. It is also clear that the topic of logarithms is closely related to the topic powers of a number.

Calculating the logarithm is called logarithm. Logarithm is the mathematical operation of taking a logarithm. When taking logarithms, products of factors are transformed into sums of terms.

Potentiation is the inverse mathematical operation of logarithm. During potentiation, a given base is raised to the degree of expression over which potentiation is performed. In this case, the sums of terms are transformed into a product of factors.

Quite often, real logarithms are used with bases 2 (binary), Euler's number e ≈ 2.718 (natural logarithm) and 10 (decimal).

At this stage it is advisable to consider logarithm samples log 7 2 , ln 5, lg0.0001.

And the entries lg(-3), log -3 3.2, log -1 -4.3 do not make sense, since in the first of them a negative number is placed under the sign of the logarithm, in the second there is a negative number in the base, and in the third there is a negative number under the logarithm sign and unit at the base.

Conditions for determining the logarithm.

It is worth considering separately the conditions a > 0, a ≠ 1, b > 0.under which we get definition of logarithm. Let's consider why these restrictions were taken. An equality of the form x = log α will help us with this b, called the basic logarithmic identity, which directly follows from the definition of logarithm given above.

Let's take the condition a≠1. Since one to any power is equal to one, then the equality x=log α b can only exist when b=1, but log 1 1 will be any real number. To eliminate this ambiguity, we take a≠1.

Let us prove the necessity of the condition a>0. At a=0 according to the formulation of the logarithm can exist only when b=0. And accordingly then log 0 0 can be any non-zero real number, since zero to any non-zero power is zero. This ambiguity can be eliminated by the condition a≠0. And when a<0 we would have to reject the analysis of rational and irrational values ​​of the logarithm, since a degree with a rational and irrational exponent is defined only for non-negative bases. It is for this reason that the condition is stipulated a>0.

And the last condition b>0 follows from inequality a>0, since x=log α b, and the value of the degree with a positive base a always positive.

Features of logarithms.

Logarithms characterized by distinctive features, which led to their widespread use to significantly facilitate painstaking calculations. When moving “into the world of logarithms,” multiplication is transformed into a much easier addition, division is transformed into subtraction, and exponentiation and root extraction are transformed, respectively, into multiplication and division by the exponent.

The formulation of logarithms and a table of their values ​​(for trigonometric functions) was first published in 1614 by the Scottish mathematician John Napier. Logarithmic tables, enlarged and detailed by other scientists, were widely used in scientific and engineering calculations, and remained relevant until the use of electronic calculators and computers.

Proof of the formula .

=

= =

since sine and cosine do not depend on adding an angle that is a multiple of

And this equality is already obvious, since this is the trigonometric form of a complex number.

Thus, the logarithm exists for all points in the plane except zero. For a real positive number, the argument is 0, so this infinite set of points has the form , that is, one of the values, namely, at , will fall on the real axis. If we calculate the logarithm of a negative number, we get , that is, the set of points is shifted upward and none of them falls on the real axis.

It is clear from the formula that only when the argument of the original number is zero, one of the logarithm values ​​falls on the real axis. And this corresponds to the right semi-axis, and that is why in the school mathematics course only logarithms of positive numbers were considered. Logarithms of negative and imaginary numbers also exist, but they do not have a single value on the real axis.

The following drawing shows where all the values ​​of the logarithm of a positive number are located in the plane. One of them is on the real axis, the rest are above and below on , , and so on. For a negative or complex number, the argument is non-zero, so this sequence of points is shifted vertically, resulting in no points on the real axis.

Example. Calculate.

Solution. Let's define the modulus of the number (equal to 2) and the argument 180 0, that is. Then = .


Appendix 1. Questions for evidence (for tickets).

Lecture No. 1

1. Prove the formula for integration by parts.

Lecture No. 2

1. Prove that the replacement , where r = LCM (r 1 ,...,r k) reduces the integral to the integral of a rational fraction.

2. Prove that the replacement reduces the integral of the form to the integral of a rational fraction.

3. Derive formulas for converting sine and cosine

For universal trigonometric substitution.

4. Prove that in the case when the function is odd with respect to the cosine, the replacement reduces the integral to a rational fraction.

5. Prove that in the case when

substitution: reduces the integral to a rational fraction.

6. Prove that for an integral of the form

7. Prove the formula

8. Prove that for an integral of the form the replacement produces an integral to a rational fraction.

9. Prove that for an integral of the form the replacement reduces the integral to a rational fraction.

Lecture No. 3

1. Prove that the function is an antiderivative of the function .

2. Prove the Newton-Leibniz formula: .

3. Prove the formula for the length of an explicitly given curve:

.

4. Prove the formula for the length of a curve given in polar coordinates

Lecture No. 4

Prove the theorem: converges, converges.

Lecture No. 5

1. Derive (prove) the formula for the area of ​​an explicitly given surface .

2. Derivation of formulas for the transition to polar coordinates.

3. Derivation of the Jacobian determinant of polar coordinates.

4. Derivation of formulas for the transition to cylindrical coordinates.

5. Derivation of the Jacobian determinant of cylindrical coordinates.

6. Derivation of formulas for the transition to spherical coordinates:

.

Lecture No. 6

1. Prove that the substitution reduces a homogeneous equation to an equation with separable variables.

2. Derive the general form of the solution to a linear homogeneous equation.

3. Derive the general form of the solution to a linear inhomogeneous equation by the Lagrange method.

4. Prove that the substitution reduces Bernoulli's equation to a linear equation.

Lecture No. 7.

1. Prove that the replacement reduces the order of the equation by k.

2. Prove that the replacement reduces the order of the equation by one .

3. Prove the theorem: The function is a solution to a linear homogeneous differential equation and has a characteristic root.

4. Prove the theorem that a linear combination of solutions to a linear homogeneous diff. the equation is also its solution.

5. Prove the theorem on the imposition of solutions: If is a solution to a linear inhomogeneous differential equation with the right-hand side, and is a solution to the same differential equation, but with the right-hand side, then the sum is a solution to the equation with the right-hand side.

Lecture No. 8.

1. Prove the theorem that the system of functions is linearly dependent.

2. Prove the theorem that there are n linearly independent solutions to a linear homogeneous differential equation of order n.

3. Prove that if 0 is the root of the multiplicity , then the system of solutions corresponding to this root has the form .

Lecture No. 9.

1. Prove using exponential form that when multiplying complex numbers, the modules are multiplied and the arguments are added.

2. Prove Moivre’s formula for degree n

3. Prove the formula for the root of an order n complex number

4. Prove that And

are generalizations of sine and cosine, i.e. for real numbers, these formulas will yield sine (cosine).

5. Prove the formula for the logarithm of a complex number:


Appendix 2.

Minor and oral questions on knowledge of theory (for colloquiums).

Lecture No. 1

1. What are antiderivatives and indefinite integrals, how do they differ?

2. Explain why it is also an antiderivative.

3. Write the formula for integration by parts.

4. What replacement is required in the form integral and how does it eliminate roots?

5. Write down the type of decomposition of the integrand of a rational fraction into simplest ones in the case when all roots are different and real.

6. Write down the type of decomposition of the integrand of a rational fraction into simplest ones in the case when all roots are real and there is one multiple root of multiplicity k.

Lecture No. 2.

1. Write what is the decomposition of a rational fraction into simplest ones in the case when the denominator has a factor of 2 degrees with a negative discriminant.

2. What substitution reduces the integral to a rational fraction?

3. What are universal trigonometric substitutions?

4. What replacements are made in cases where the function under the integral sign is odd with respect to sine (cosine)?

5. What replacements are made if the integrand contains the expressions , , or .

Lecture No. 3.

1. Definition of a definite integral.

2. List some of the basic properties of the definite integral.

3. Write the Newton-Leibniz formula.

4. Write the formula for the volume of a body of rotation.

5. Write a formula for the length of an explicitly given curve.

6. Write the formula for the length of a parametrically defined curve.

Lecture No. 4.

1. Definition of an improper integral (using a limit).

2. What is the difference between improper integrals of the 1st and 2nd kind.

3. Give simple examples of convergent integrals of the 1st and 2nd kind.

4. At what values ​​do the integrals (T1) converge?

5. How is convergence related to the finite limit of the antiderivative (T2)

6. What is a necessary criterion for convergence, its formulation.

7. Comparison test in final form

8. Sign of comparison in extreme form.

9. Definition of multiple integral.

Lecture No. 5.

1. Changing the order of integration, show with a simple example.

2. Write the formula for surface area.

3. What are polar coordinates, write the transition formulas.

4. What is the Jacobian of the polar coordinate system?

5. What are cylindrical and spherical coordinates, what is their difference.

6. What is the Jacobian of cylindrical (spherical) coordinates?

Lecture No. 6.

1. What is a 1st order differential equation (general view).

2. What is a 1st order differential equation resolved with respect to the derivative. Give some example.

3. What is an equation with separable variables.

4. What is a general, particular solution, Cauchy conditions.

5. What is a homogeneous equation, what is the general method for solving it.

6. What is a linear equation, what is the algorithm for solving it, what is the Lagrange method.

7. What is the Bernoulli equation, an algorithm for solving it.

Lecture No. 7.

1. What replacement is necessary for an equation of the form .

2. What replacement is needed for an equation of the form .

3. Show with examples how it can be expressed in the form .

4. What is a linear differential equation of order n.

5. What is a characteristic polynomial, characteristic equation.

6. Formulate a theorem about at what r the function is a solution to a linear homogeneous differential equation.

7. Formulate a theorem that a linear combination of solutions to a linear homogeneous equation is also its solution.

8. Formulate the theorem on the imposition of solutions and its consequences.

9. What are linearly dependent and linearly independent systems of functions, give some examples.

10. What is the Wronski determinant of a system of n functions, give an example of the Wronski determinant for LZS and LNS systems.

Lecture No. 8.

1. What property does the Wronski determinant have if the system function is linearly dependent.

2. How many linearly independent solutions exist to a linear homogeneous differential equation of order n.

3. Determination of the FSR (fundamental system of solutions) of a linear homogeneous equation of order n.

4. How many functions does the FSR contain?

5. Write down the form of the system of equations for finding by the Lagrange method for n=2.

6. Write down the type of particular solution in the case when

7. What is a linear system of differential equations, write an example.

8. What is an autonomous system of differential equations.

9. Physical meaning of a system of differential equations.

10. Write down what functions the FSR of the system of equations consists of, if the eigenvalues ​​and eigenvectors of the main matrix of this system are known.

Lecture No. 9.

1. What is an imaginary unit.

2. What is a conjugate number and what happens when you multiply it by the original number.

3. What is the trigonometric, exponential form of a complex number.

4. Write Euler's formula.

5. What is the modulus, the argument of a complex number.

6. what happens to modules and arguments during multiplication (division).

7. Write Moivre’s formula for degree n.

8. Write the formula for a root of order n.

9. Write generalized sine and cosine formulas for a complex argument.

10. Write the formula for the logarithm of a complex number.


Appendix 3. Problems from lectures.

Lecture No. 1

Example. . Example. .

Example. . Example. .

Example. Example. .

Example. . Example. .

Lecture No. 2

Example. . Example. .

Example. . Example. .

Example. . Example.. , where, number .

Example. Divide exponentially.

Example. Find using Moivre's formula.

Example. Find all values ​​of the root.

Definition and properties

Complex zero does not have a logarithm because the complex exponent does not take the value zero. Non-zero texvc can be represented in demonstrative form:

Unable to parse expression (Executable file texvc not found; See math/README - help with setup.): z=r \cdot e^(i (\varphi + 2 \pi k))\;\;, Where Unable to parse expression (Executable file texvc not found; See math/README for setup help.): k- arbitrary integer

Then Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \mathrm(Ln)\,z is found by the formula:

Unable to parse expression (Executable file texvc not found; See math/README - help with setup.): \mathrm(Ln)\,z = \ln r + i \left(\varphi + 2 \pi k \right)

Here Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \ln\,r= \ln\,|z|- real logarithm. It follows from this:

It is clear from the formula that one and only one of the values ​​has an imaginary part in the interval Unable to parse expression (Executable file texvc . This value is called main importance complex natural logarithm. The corresponding (already unambiguous) function is called main branch logarithm and is denoted Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \ln\,z. Sometimes through Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \ln\, z also denote the value of the logarithm that does not lie on the main branch. If Unable to parse expression (Executable file texvc not found; See math/README for setup help.): z is a real number, then the principal value of its logarithm coincides with the ordinary real logarithm.

From the above formula it also follows that the real part of the logarithm is determined as follows through the components of the argument:

Unable to parse expression (Executable file texvc not found; See math/README for help with setup.): \operatorname(Re)(\ln(x+iy)) = \frac(1)(2) \ln(x^2+y^2)

The figure shows that the real part as a function of the components is centrally symmetric and depends only on the distance to the origin. It is obtained by rotating the graph of the real logarithm around the vertical axis. As it approaches zero, the function tends to Unable to parse expression (Executable file texvc not found; See math/README - help with setup.): -\infty.

The logarithm of a negative number is found by the formula:

Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \mathrm(Ln) (-x) = \ln x + i \pi (2 k + 1) \qquad (x>0,\ k = 0, \pm 1 ,\pm 2\dots)

Examples of complex logarithm values

Let us present the main value of the logarithm ( Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \ln) and its general expression ( Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \mathrm(Ln)) for some arguments:

Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \ln (1) = 0;\; \mathrm(Ln) (1) = 2k\pi i Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \ln (-1) = i \pi;\; \mathrm(Ln) (-1) = (2k+1)i \pi Unable to parse expression (Executable file texvc not found; See math/README - help with setup.): \ln (i) = i \frac(\pi) (2);\; \mathrm(Ln) (i) = i \frac(4k+1)(2) \pi

You should be careful when converting complex logarithms, taking into account that they are multi-valued, and therefore the equality of the logarithms of any expressions does not imply the equality of these expressions. Example erroneous reasoning:

Unable to parse expression (Executable file texvc not found; See math/README - help with setup.): i\pi = \ln(-1) = \ln((-i)^2) = 2\ln(-i) = 2(-i\pi/2 ) = -i\pi- an obvious mistake.

Note that on the left is the main value of the logarithm, and on the right is the value from the underlying branch ( Unable to parse expression (Executable file texvc not found; See math/README - help with setup.): k=-1). The cause of the error is careless use of the property Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \log_a((b^p)) = p~\log_a b, which, generally speaking, implies in the complex case the entire infinite set of values ​​of the logarithm, and not just the main value.

Complex logarithmic function and Riemann surface

Due to its simply connectedness, the Riemann surface of the logarithm is a universal covering for the complex plane without a point Unable to parse expression (Executable file texvc .

Analytical continuation

The logarithm of a complex number can also be defined as the analytic continuation of the real logarithm to the entire complex plane. Let the curve Unable to parse expression (Executable file texvc starts at one, does not go through zero and does not cross the negative part of the real axis. Then the principal value of the logarithm at the end point Unable to parse expression (Executable file texvc not found; See math/README for setup help.): w crooked Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \Gamma can be determined by the formula:

Unable to parse expression (Executable file texvc not found; See math/README for help with setting up.): \ln z = \int\limits_\Gamma (du \over u)

If Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \Gamma- a simple curve (without self-intersections), then for numbers lying on it, logarithmic identities can be used without fear, for example:

Unable to parse expression (Executable file texvc not found; See math/README for help with setup.): \ln (wz) = \ln w + \ln z, ~\forall z,w\in\Gamma\colon zw\in \Gamma

The main branch of the logarithmic function is continuous and differentiable on the entire complex plane, except for the negative part of the real axis, on which the imaginary part changes abruptly to Unable to parse expression (Executable file texvc not found; See math/README - help with setup.): 2\pi. But this fact is a consequence of the artificial limitation of the imaginary part of the main value by the interval Unable to parse expression (Executable file texvc not found; See math/README for setup help.): (-\pi, \pi]. If we consider all branches of the function, then continuity occurs at all points except zero, where the function is not defined. If you resolve the curve Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \Gamma cross the negative part of the real axis, then the first such intersection transfers the result from the main value branch to the adjacent branch, and each subsequent intersection causes a similar shift along the branches of the logarithmic function (see figure).

From the analytic continuation formula it follows that on any branch of the logarithm:

Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \frac(d)(dz) \ln z = (1\over z)

For any circle Unable to parse expression (Executable file texvc not found; See math/README for setup help.): S, covering the point Unable to parse expression (Executable file texvc not found; See math/README for setup help.): 0 :

Unable to parse expression (Executable file texvc not found; See math/README for help with setting up.): \oint\limits_S (dz \over z) = 2\pi i

The integral is taken in the positive direction (counterclockwise). This identity underlies the theory of residues.

One can also define the analytic continuation of the complex logarithm using series known for the real case:

However, from the form of these series it follows that at one the sum of the series is equal to zero, that is, the series relates only to the main branch of the multivalued function of the complex logarithm. The radius of convergence of both series is 1.

Connection with inverse trigonometric and hyperbolic functions

Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \operatorname(Arcsin) z = -i \operatorname(Ln) (i z + \sqrt(1-z^2)) Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \operatorname(Arccos) z = -i \operatorname(Ln) (z + i\sqrt(1-z^2)) Unable to parse expression (Executable file texvc not found; See math/README - help with setup.): \operatorname(Arctg) z = -\frac(i)(2) \ln \frac(1+z i)(1-z i) + k \pi \; (z \ne \pm i) Unable to parse expression (Executable file texvc not found; See math/README - help with setup.): \operatorname(Arcctg) z = -\frac(i)(2) \ln \frac(z i-1)(z i+1) + k \pi \; (z \ne \pm i) Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \operatorname(Arsh)z = \operatorname(Ln)(z+\sqrt(z^2+1))- inverse hyperbolic sine Unable to parse expression (Executable file texvc not found; See math/README - help with setup.): \operatorname(Arch)z=\operatorname(Ln) \left(z+\sqrt(z^(2)-1) \right)- inverse hyperbolic cosine Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \operatorname(Arth)z=\frac(1)(2)\operatorname(Ln)\left(\frac(1+z)(1-z)\right)- inverse hyperbolic tangent Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \operatorname(Arcth)z=\frac(1)(2)\operatorname(Ln)\left(\frac(z+1)(z-1)\right)- inverse hyperbolic cotangent

Historical sketch

The first attempts to extend logarithms to complex numbers were made at the turn of the 17th-18th centuries by Leibniz and Johann Bernoulli, but they failed to create a holistic theory, primarily because the very concept of logarithm was not yet clearly defined. The discussion on this issue took place first between Leibniz and Bernoulli, and in the middle of the 18th century between D’Alembert and Euler. Bernoulli and D'Alembert believed that it should be determined Unable to parse expression (Executable file texvc not found; See math/README for setup help.): \log(-x) = \log(x), while Leibniz proved that the logarithm of a negative number is an imaginary number. The complete theory of logarithms of negative and complex numbers was published by Euler in 1747-1751 and is essentially no different from the modern one. Although the debate continued (D'Alembert defended his point of view and argued it in detail in an article in his Encyclopedia and in other works), Euler's approach received universal recognition by the end of the 18th century.

Write a review about the article "Complex logarithm"

Literature

Theory of logarithms
  • Korn G., Korn T.. - M.: Nauka, 1973. - 720 p.
  • Sveshnikov A. G., Tikhonov A. N. Theory of functions of a complex variable. - M.: Nauka, 1967. - 304 p.
  • Fikhtengolts G. M. Course of differential and integral calculus. - ed. 6th. - M.: Nauka, 1966. - 680 p.
History of logarithms
  • Mathematics of the 18th century // / Edited by A. P. Yushkevich, in three volumes. - M.: Science, 1972. - T. III.
  • Kolmogorov A. N., Yushkevich A. P. (eds.). Mathematics of the 19th century. Geometry. Theory of analytic functions. - M.: Science, 1981. - T. II.

Notes

  1. Logarithmic function. // . - M.: Soviet Encyclopedia, 1982. - T. 3.
  2. , Volume II, pp. 520-522..
  3. , With. 623..
  4. , With. 92-94..
  5. , With. 45-46, 99-100..
  6. Boltyansky V. G., Efremovich V. A.. - M.: Nauka, 1982. - P. 112. - (Kvant Library, issue 21).
  7. , Volume II, pp. 522-526..
  8. , With. 624..
  9. , With. 325-328..
  10. Rybnikov K. A. History of mathematics. In two volumes. - M.: Publishing house. Moscow State University, 1963. - T. II. - P. 27, 230-231..
  11. , With. 122-123..
  12. Klein F.. - M.: Science, 1987. - T. II. Geometry. - pp. 159-161. - 416 s.

An excerpt characterizing the Complex logarithm

From the wild horror that gripped us, we rushed like bullets across a wide valley, not even thinking that we could quickly go to another “floor”... We simply did not have time to think about it - we were too scared.
The creature flew right above us, loudly clicking its gaping toothy beak, and we rushed as fast as we could, splashing vile slimy splashes to the sides, and mentally praying that something else would suddenly interest this creepy “miracle bird”... It was felt. that she was much faster and we simply had no chance to break away from her. As luck would have it, not a single tree grew nearby, there were no bushes, or even stones behind which one could hide, only an ominous black rock could be seen in the distance.
- There! – Stella shouted, pointing her finger at the same rock.
But suddenly, unexpectedly, right in front of us, a creature appeared from somewhere, the sight of which literally froze our blood in our veins... It appeared as if “straight out of thin air” and was truly terrifying... The huge black carcass was completely covered long, coarse hair, making him look like a pot-bellied bear, only this “bear” was as tall as a three-story house... The monster’s lumpy head was “crowned” with two huge curved horns, and the eerie mouth was decorated with a pair of incredibly long fangs, sharp as knives, just by looking to which, with fright, our legs gave way... And then, incredibly surprising us, the monster easily jumped up and... picked up the flying “muck” on one of its huge fangs... We froze in shock.
- Let's run!!! – Stella squealed. – Let’s run while he’s “busy”!..
And we were ready to rush again without looking back, when suddenly a thin voice sounded behind our backs:
- Girls, wait!!! No need to run away!.. Dean saved you, he is not an enemy!
We turned around sharply - a tiny, very beautiful black-eyed girl was standing behind us... and was calmly stroking the monster that had approached her!.. Our eyes widened in surprise... It was incredible! Certainly - it was a day of surprises!.. The girl, looking at us, smiled welcomingly, not at all afraid of the furry monster standing next to us.
- Please don't be afraid of him. He is very kind. We saw that Ovara was chasing you and decided to help. Dean was great, he made it on time. Really, my dear?
“Good” purred, which sounded like a slight earthquake, and, bending his head, licked the girl’s face.
– Who is Owara, and why did she attack us? – I asked.
“She attacks everyone, she’s a predator.” And very dangerous,” the girl answered calmly. – May I ask what you are doing here? You're not from here, girls?
- No, not from here. We were just walking. But the same question for you - what are you doing here?
“I’m going to see my mother...” the little girl became sad. “We died together, but for some reason she ended up here.” And now I live here, but I don’t tell her this, because she will never agree with it. She thinks I'm just coming...
– Isn’t it better to just come? It’s so terrible here!.. – Stella shrugged her shoulders.
“I can’t leave her here alone, I’m watching her so that nothing happens to her.” And here Dean is with me... He helps me.
I just couldn’t believe it... This little brave girl voluntarily left her beautiful and kind “floor” to live in this cold, terrible and alien world, protecting her mother, who was very “guilty” in some way! I don’t think there would be many people so brave and selfless (even adults!) who would dare to undertake such a feat... And I immediately thought - maybe she just didn’t understand what she was going to doom herself to?!
– How long have you been here, girl, if it’s not a secret?
“Recently...” the black-eyed baby answered sadly, tugging at a black lock of her curly hair with her fingers. – I found myself in such a beautiful world when I died!.. He was so kind and bright!.. And then I saw that my mother was not with me and rushed to look for her. It was so scary at first! For some reason she was nowhere to be found... And then I fell into this terrible world... And then I found her. I was so scared here... So lonely... Mom told me to leave, she even scolded me. But I can’t leave her... Now I have a friend, my good Dean, and I can already somehow exist here.
Her “good friend” growled again, which gave Stella and me huge “lower astral” goosebumps... Having collected myself, I tried to calm down a little and began to take a closer look at this furry miracle... And he, immediately feeling that he was noticed, he terribly bared his fanged mouth... I jumped back.
- Oh, don't be afraid, please! “He’s smiling at you,” the girl “reassured.”
Yeah... You'll learn to run fast from such a smile... - I thought to myself.
- How did it happen that you became friends with him? – Stella asked.
– When I first came here, I was very scared, especially when such monsters as you were attacking today. And then one day, when I almost died, Dean saved me from a whole bunch of creepy flying “birds”. I was also scared of him at first, but then I realized what a heart of gold he has... He is the best friend! I never had anything like this, even when I lived on Earth.
- How did you get used to it so quickly? His appearance is not quite, let’s say, familiar...
– And here I understood one very simple truth, which for some reason I did not notice on Earth - appearance does not matter if a person or creature has a good heart... My mother was very beautiful, but at times she was very angry too. And then all her beauty disappeared somewhere... And Dean, although scary, is always very kind, and always protects me, I feel his kindness and am not afraid of anything. But you can get used to the appearance...
– Do you know that you will be here for a very long time, much longer than people live on Earth? Do you really want to stay here?..
“My mother is here, so I have to help her.” And when she “leaves” to live on Earth again, I will also leave... To where there is more goodness. In this terrible world, people are very strange - as if they don’t live at all. Why is that? Do you know anything about this?
– Who told you that your mother would leave to live again? – Stella became interested.
- Dean, of course. He knows a lot, he’s lived here for a very long time. He also said that when we (my mother and I) live again, our families will be different. And then I won’t have this mother anymore... That’s why I want to be with her now.
- How do you talk to him, your Dean? – Stella asked. – And why don’t you want to tell us your name?
But it’s true – we still didn’t know her name! And they didn’t know where she came from either...
– My name was Maria... But does that really matter here?
- Surely! – Stella laughed. - How can I communicate with you? When you leave, they will give you a new name, but while you are here, you will have to live with the old one. Did you talk to anyone else here, girl Maria? – Stella asked, jumping from topic to topic out of habit.
“Yes, I talked...” the little girl said hesitantly. “But they are so strange here.” And so unhappy... Why are they so unhappy?
– Is what you see here conducive to happiness? – I was surprised by her question. – Even the local “reality” itself kills any hopes in advance!.. How can you be happy here?
- Don't know. When I’m with my mother, it seems to me that I could be happy here too... True, it’s very scary here, and she really doesn’t like it here... When I said that I agreed to stay with her, she yelled at me and said that I’m her “brainless misfortune”... But I’m not offended... I know that she’s just scared. Just like me...
– Perhaps she just wanted to protect you from your “extreme” decision, and only wanted you to go back to your “floor”? – Stella asked carefully, so as not to offend.
– No, of course... But thank you for the good words. Mom often called me not very good names, even on Earth... But I know that this was not out of anger. She was simply unhappy that I was born, and often told me that I ruined her life. But it wasn't my fault, was it? I always tried to make her happy, but for some reason I wasn’t very successful... And I never had a dad. – Maria was very sad, and her voice was trembling, as if she was about to cry.
Stella and I looked at each other, and I was almost sure that similar thoughts visited her... I already really didn’t like this spoiled, selfish “mother”, who, instead of worrying about her child herself, did not care about his heroic sacrifice at all I understood and, in addition, I also hurt her painfully.
“But Dean says that I’m good, and that I make him very happy!” – the little girl babbled more cheerfully. “And he wants to be friends with me.” And others I've met here are very cold and indifferent, and sometimes even evil... Especially those who have monsters attached...
“Monsters—what?..” we didn’t understand.
- Well, they have terrible monsters sitting on their backs and telling them what they must do. And if they don’t listen, the monsters mock them terribly... I tried to talk to them, but these monsters won’t allow me.
We understood absolutely nothing from this “explanation,” but the very fact that some astral beings were torturing people could not remain “explored” by us, so we immediately asked her how we could see this amazing phenomenon.
- Oh, yes everywhere! Especially at the “black mountain”. There he is, behind the trees. Do you want us to go with you too?
- Of course, we will be only too happy! – the delighted Stella immediately answered.
To be honest, I also didn’t really smile at the prospect of dating someone else, “creepy and incomprehensible,” especially alone. But interest overcame fear, and we, of course, would have gone, despite the fact that we were a little afraid... But when such a defender as Dean walked with us, it immediately became more fun...
And then, after a short moment, real Hell unfolded before our eyes, wide open with amazement... The vision was reminiscent of the paintings of Bosch (or Bosc, depending on what language you translate it into), a “crazy” artist who once shocked the whole world with his art world... He, of course, was not crazy, but was simply a seer who for some reason could only see the lower Astral. But we must give him his due - he portrayed him superbly... I saw his paintings in a book that was in my dad’s library, and I still remembered the eerie feeling that most of his paintings carried...
“What a horror!..” whispered the shocked Stella.
One could probably say that we have already seen a lot here, on the “floors”... But even we were not able to imagine this in our most terrible nightmare!.. Behind the “black rock” something completely opened up unthinkable... It looked like a huge, flat “cauldron” carved into the rock, at the bottom of which crimson “lava” was bubbling... The hot air “burst” everywhere with strange flashing reddish bubbles, from which scalding steam burst out and fell in large drops to the ground, or to the people who fell under it at that moment... Heartbreaking screams were heard, but immediately fell silent, as the most disgusting creatures sat on the backs of the same people, who with a contented look “controlled” their victims, not paying the slightest attention to their suffering... Under the naked feet of people, hot stones turned red, the crimson earth, bursting with heat, bubbled and “melted”... Splashes of hot steam burst through huge cracks and, burning the feet of human beings sobbing in pain, were carried into the heights, evaporating with a light smoke ... And in the very middle of the “pit” flowed a bright red, wide fiery river, into which, from time to time, the same disgusting monsters unexpectedly threw one or another tormented entity, which, falling, caused only a short splash of orange sparks, and then but, turning for a moment into a fluffy white cloud, it disappeared... forever... It was real Hell, and Stella and I wanted to “disappear” from there as soon as possible...
“What are we going to do?” Stella whispered in quiet horror. - Do you want to go down there? Is there anything we can do to help them? Look how many there are!..
We stood on a black-brown, heat-dried cliff, observing the “mash” of pain, hopelessness, and violence that stretched below, filled with horror, and felt so childishly powerless that even my militant Stella this time categorically folded her ruffled “wings.” “and was ready at the first call to rush off to her own, so dear and reliable, upper “floor”...

The basic properties of the logarithm, logarithm graph, domain of definition, set of values, basic formulas, increasing and decreasing are given. Finding the derivative of a logarithm is considered. As well as integral, power series expansion and representation using complex numbers.

Content

Domain, set of values, increasing, decreasing

The logarithm is a monotonic function, so it has no extrema. The main properties of the logarithm are presented in the table.

Domain 0 < x < + ∞ 0 < x < + ∞
Range of values - ∞ < y < + ∞ - ∞ < y < + ∞
Monotone monotonically increases monotonically decreases
Zeros, y = 0 x = 1 x = 1
Intercept points with the ordinate axis, x = 0 No No
+ ∞ - ∞
- ∞ + ∞

Private values


The logarithm to base 10 is called decimal logarithm and is denoted as follows:

Logarithm to base e called natural logarithm:

Basic formulas for logarithms

Properties of the logarithm arising from the definition of the inverse function:

The main property of logarithms and its consequences

Base replacement formula

Logarithm is the mathematical operation of taking a logarithm. When taking logarithms, products of factors are converted into sums of terms.
Potentiation is the mathematical operation inverse to logarithm. During potentiation, a given base is raised to the degree of expression over which potentiation is performed. In this case, the sums of terms are transformed into products of factors.

Proof of basic formulas for logarithms

Formulas related to logarithms follow from formulas for exponential functions and from the definition of an inverse function.

Consider the property of the exponential function
.
Then
.
Let's apply the property of the exponential function
:
.

Let us prove the base replacement formula.
;
.
Assuming c = b, we have:

Inverse function

The inverse of a logarithm to base a is an exponential function with exponent a.

If , then

If , then

Derivative of logarithm

Derivative of the logarithm of modulus x:
.
Derivative of nth order:
.
Deriving formulas > > >

To find the derivative of a logarithm, it must be reduced to the base e.
;
.

Integral

The integral of the logarithm is calculated by integrating by parts: .
So,

Expressions using complex numbers

Consider the complex number function z:
.
Let's express a complex number z via module r and argument φ :
.
Then, using the properties of the logarithm, we have:
.
Or

However, the argument φ not uniquely defined. If you put
, where n is an integer,
then it will be the same number for different n.

Therefore, the logarithm, as a function of a complex variable, is not a single-valued function.

Power series expansion

When the expansion takes place:

References:
I.N. Bronstein, K.A. Semendyaev, Handbook of mathematics for engineers and college students, “Lan”, 2009.

See also: