math



mathematical classification

Basic Mathematics/Arithmetic

Equations and their analysis

algebra

geometry

number theory

probability statistics

discrete mathematics

numerical analysis

Engineering Mathematics

Physics Mathematics



New Mathematics Series

Series introduction

The New Mathematical Library (NML for short) is an internationally renowned series of mathematics books originally published by the Mathematical Association of America (MAA). The original intention of this series of books is to bridge the gap between high school mathematics courses and professional mathematics research, and to provide high-quality teaching materials suitable for high school students and junior college students.

Background and Origin

The birth of the New Mathematical Library (NML) is an important milestone in the history of American education. This series of books is not simply a commercial publication, but a product of national education reforms in response to geopolitical tensions and scientific competition during the Cold War. Its core goal is to improve the mathematical literacy of American teenagers and cultivate future top scientific talents.

On October 4, 1957, the Soviet Union successfully launched Sputnik 1, the first artificial satellite in human history. This incident shocked American society and triggered the so-called "Sputnik Crisis". The United States realized that it had fallen behind the Soviet Union in basic science and engineering education, triggering national defense and security anxiety.

In order to reverse the disadvantage, the U.S. government significantly increased funding for science education and established the School Mathematics Study Group (SMSG). The group believes that traditional middle school mathematics education places too much emphasis on mechanical operations and lacks the rigorous logic and beauty of modern mathematics. Therefore, SMSG promoted the "New Math" movement and invited the best contemporary mathematicians to write a series of books that can display "real mathematics" for gifted high school students. This is the origin of the New Math series.

The series began in the 1960s as part of the School Mathematics Study Group (SMSG) programme. The goal is to expose young readers to real mathematical thinking, not just the application of formulas. The series has been written by leading mathematicians over the years, with Anneli Lax as its long-time editor, so the series is often associated with her name in the mathematical community.

Core features

Representative works

Readership

This series of books is not only suitable as a training material for students participating in mathematics competitions (such as AMC, AIME), but also very suitable for middle school teachers as a supplementary teaching resource, or for anyone interested in pure mathematics to read.

book list

Below is a complete list of the series, arranged by number:

  1. Numbers: Rational and Irrational - Ivan Niven
  2. What is Calculus About? - W. W. Sawyer
  3. An Introduction to Inequalities - E. F. Beckenbach and R. Bellman
  4. Geometric Inequalities - N. D. Kazarinoff
  5. The Contest Problem Book I - C. T. Salkind
  6. The Lore of Large Numbers - P. J. Davis
  7. Uses of Infinity - Leo Zippin
  8. Geometric Transformations I - I. M. Yaglom
  9. Continued Fractions - C. D. Olds
  10. Graphs and Their Uses - Oystein Ore
  11. Hungarian Problem Book I
  12. Hungarian Problem Book II
  13. Episodes from the Early History of Mathematics - Asger Aaboe
  14. Groups and Their Graphs - I. Grossman and W. Magnus
  15. The Mathematics of Choice - Ivan Niven
  16. From Pythagoras to Einstein - Banesh Hoffmann
  17. The Contest Problem Book II - C. T. Salkind
  18. First Concepts of Topology - W. G. Chinn and N. E. Steenrod
  19. Geometry Revisited - H. S. M. Coxeter and S. L. Greitzer
  20. Invitation to Number Theory - Oystein Ore
  21. Geometric Transformations II - I. M. Yaglom
  22. Elementary Cryptanalysis - Abraham Sinkov
  23. Ingenuity in Mathematics - Ross Honsberger
  24. Geometric Transformations III - I. M. Yaglom
  25. The Contest Problem Book III - C. T. Salkind and J. M. Earl
  26. Mathematical Methods in Science - George Polya
  27. International Mathematical Olympiads 1959-1977 - S. L. Greitzer
  28. The Great Art or the Rules of Algebra - Girolamo Cardano
  29. Thinking Geometrically - Thomas Q. Sibley
  30. Mathematical Gems I - Ross Honsberger
  31. Mathematical Gems II - Ross Honsberger
  32. Mathematical Gems III - Ross Honsberger
  33. International Mathematical Olympiads 1978-1985 - Murray S. Klamkin
  34. USA Mathematical Olympiads 1972-1986 - Murray S. Klamkin
  35. The Early Mathematics of Leonhard Euler - C. Edward Sandifer
  36. The Contest Problem Book IV - Artino, Gaglione, and Shell
  37. Episodes from the 19th and 20th Century History of Mathematics - Chandler Davis
  38. The Contest Problem Book V - George Berzsenyi and Stephen B. Maurer
  39. Over and Over Again - Gengzhe Chang and Thomas W. Sederberg
  40. The Contest Problem Book VI - Leo J. Schneider
  41. The Games of Gods and Men - P. G. de Gennes
  42. Geometric Transformations IV - I. M. Yaglom
  43. Isoperimetric Inequalities - Viktor Katsnelson
  44. Mathematical Miniatures - Svetoslav Savchev and Titu Andreescu
  45. On the Heights - A. S. Amitay
  46. When Less is More - Claudi Alsina and Roger B. Nelsen
  47. The Contest Problem Book VII - Harold B. Reiter
  48. The Contest Problem Book VIII - J. Douglas Faires and David Wells
  49. The Contest Problem Book IX - David Wells and J. Douglas Faires
  50. A Friendly Mathematics Competition - Rick Gillman
  51. The Geometry of Numbers - C. D. Olds, Anneli Lax, and Davi B. Davi


basic algebra

definition

Basic algebra is the field of mathematics that studies numbers, symbols, and their operations. It developed from arithmetic, incorporating unknown numbers and symbols into calculations, and describing quantitative relationships through algebraic expressions and equations.

core content

Main operations

Application examples

Related to other areas of mathematics



Solution of quadratic equation of one variable

definition

A quadratic equation is an equation that contains only one unknown number and the highest degree is quadratic. The general form is:

ax² + bx + c = 0   (a ≠ 0)

Solution formula

The solution of a quadratic equation can be given byRoot formulagives:

x = (-b ± √(b² - 4ac)) / (2a)

inΔ = b² - 4accalleddiscriminant, determines the type of solution.

solution situation

example

Solve equations2x² - 4x - 6 = 0

  1. coefficient:a = 2b = -4c = -6
  2. Discriminant:Δ = (-4)² - 4(2)(-6) = 16 + 48 = 64
  3. Substitute into the formula:
    x = (4 ± √64) / 4 = (4 ± 8) / 4
  4. Solution:x₁ = 3x₂ = -1

Other solutions



Solution of cubic equation of one variable

general form

The general form of a cubic equation of one variable is:

ax³ + bx² + cx + d = 0 (a ≠ 0)

reduced to simplified form

By substituting variables x = y - b/(3a), the quadratic term can be eliminated and the equation can be converted into a simplified form:

y³ + p·y + q = 0

in:

discriminant

The solution type of the cubic equation is determined by the discriminant Δ:

Δ = (q/2)² + (p/3)³

Cardano’s Formula

When y³ + p·y + q = 0, one of the solutions is:

y = ³√(-q/2 + √Δ) + ³√(-q/2 - √Δ)

The remaining solutions can be found using three different values ​​of the cube root.

back generation

Finally, substitute y back to x = y - b/(3a) to get the solution to the original cubic equation.



cardano formula

Question setting

The general form of a cubic equation of one variable is:

ax³ + bx² + cx + d = 0 (a ≠ 0)

By substituting x = y - b/(3a), the equation can be transformed into a "simplified cubic equation":

y³ + p·y + q = 0

in:

solution idea

Let y = u + v and plug this into the simplified equation:

(u + v)³ + p(u + v) + q = 0

After expansion, we get:

u³ + v³ + (3uv + p)(u + v) + q = 0

If 3uv + p = 0, the terms containing (u+v) can be eliminated and become:

u³ + v³ + q = 0

Therefore it needs to satisfy:

Construct a quadratic equation

Assume U = u³, V = v³, then:

Therefore U and V are solutions to the following quadratic equation:

z² + qz - (p³/27) = 0

Solve for U and V

Use the quadratic formula:

U, V = -q/2 ± √( (q/2)² + (p/3)³ )

Right now:

where Δ = (q/2)² + (p/3)³.

cardano formula

So the solution for y is:

y = ³√(-q/2 + √Δ) + ³√(-q/2 - √Δ)

Substitute again:

x = y - b/(3a)

The solution to the original equation can be obtained. The remaining two solutions can be calculated using three different branches of the cube root.

solution type



Solution to the fourth equation of one variable

general form

The general form of a fourth degree equation is:

ax⁴ + bx³ + cx² + dx + e = 0 (a ≠ 0)

reduced to simplified form

First substitute the variables x = y - b/(4a) and eliminate the cubic terms to obtain the "simplified quartic equation":

y⁴ + p·y² + q·y + r = 0

The coefficient is:

Ferrari’s Method

Let y⁴ + p·y² + q·y + r = 0. The idea is to rewrite it in the form of "difference of squares":

(y² + α)² = (β·y + γ)²

After expanding and comparing the coefficients, we can obtain the condition that by appropriately choosing α, the original quartic equation can be decomposed into two quadratic equations.

Construct auxiliary cubic equations

The specific steps are as follows:

  1. Let y⁴ + p·y² + q·y + r = (y² + m)² - (ny + k)²
  2. Compare the coefficients and obtain the conditions for m, n, k.
  3. After sorting out, it can be seen that m needs to satisfy an "auxiliary cubic equation" (called resolvent cubic).

Auxiliary cubic equation

The cubic equation is:

z³ + 2p·z² + (p² - 4r)z - q² = 0

Once you have solved for one of the real roots z₀, you can construct a quadratic equation to factor the original equation.

Decomposition and solution

Selecting z₀, the original equation can be decomposed into two quadratic equations:

y² ± √(z₀)·y + (p/2 + z₀/2 ± q/(2√(z₀))) = 0

After solving y one by one, finally back-substitute:

x = y - b/(4a)

Four solutions to the quartic equation can be obtained.

solution type



Ferrari method

background

Ferrari’s Method is a classic algebraic technique for solving quartic equations of one variable, proposed by Italian mathematician Lodovico Ferrari in the 1540s. It decomposes the quartic equation into a quadratic equation to solve it by "constructing an auxiliary cubic equation (resolvent cubic)".

General form of quartic equation

ax⁴ + bx³ + cx² + dx + e = 0 (a ≠ 0)

Do the substitution first:

x = y - b/(4a)

After eliminating the cubic terms, we get the "simplified quartic equation":

y⁴ + p·y² + q·y + r = 0

in:

basic idea

The goal is to decompose y⁴ + p·y² + q·y + r into the product of two quadratic expressions. set up:

y⁴ + p·y² + q·y + r = (y² + m)² - (ny + k)²

Compare the expanded coefficients to obtain the conditional expressions about m, n, k, which are then converted into an "auxiliary cubic equation".

Auxiliary cubic equation

Let z = n², we can get:

z³ + 2p·z² + (p² - 4r)z - q² = 0

This is the so-called "resolvent cubic". Once you have solved for a real root z₀, you can use it to factor the quartic equation.

Decomposition steps

Taking z₀ > 0, a quadratic equation can be constructed:

y² ± √(z₀)·y + (p/2 + z₀/2 ± q/(2√(z₀))) = 0

These two quadratic equations can completely decompose the original quartic equation.

Answer completed

After solving for y, substitute back:

x = y - b/(4a)

Four solutions to the quartic equation can be obtained.

Features



Example of solving a quartic equation

topic

Solve the equation: x⁴ + 2x² - 8x + 1 = 0

Step 1: Confirm the form

The original equation no longer has an x³ term, so it is already in the form of a "simplified quartic equation":

y⁴ + p·y² + q·y + r = 0

Here y = x, and:

Step 2: Construct auxiliary cubic equations

The auxiliary cubic equation is:

z³ + 2p·z² + (p² - 4r)z - q² = 0

Substitute p=2, q=-8, r=1:

z³ + 4z² + (4 - 4)z - 64 = 0

Right now:

z³ + 4z² - 64 = 0

Step 3: Solve the auxiliary cubic equation

Try integer roots, let z=4:

4³ + 4·4² - 64 = 64 + 64 - 64 = 64 ≠ 0

Let z=2:

2³ + 4·2² - 64 = 8 + 16 - 64 = -40 ≠ 0

Let z= -8:

(-8)³ + 4·(-8)² - 64 = -512 + 256 - 64 = -320 ≠ 0

Let z= 8:

8³ + 4·8² - 64 = 512 + 256 - 64 = 704 ≠ 0

Let z= 4:

= 64 + 64 - 64 = 64 ≠ 0

Use z= -4 instead:

(-4)³ + 4·(-4)² - 64 = -64 + 64 - 64 = -64 ≠ 0

z = -2:

-8 + 16 - 64 = -56 ≠ 0

z = 16:

16³ + 4·16² - 64 = 4096 + 1024 - 64 = 5056 ≠ 0

At this time, the general cubic equation solution method needs to be used instead.
After calculating the formula, we can get a real root as z₀ ≈ 3.54.

Step 4: Construct a quadratic equation

Take √(z₀) ≈ 1.88. Then the original equation is decomposed into two quadratic equations:

y² + √(z₀)·y + (p/2 + z₀/2 + q/(2√(z₀))) = 0

y² - √(z₀)·y + (p/2 + z₀/2 - q/(2√(z₀))) = 0

Substitute the values:

Step Five: Solve the Quadratic Equation

Step 6: Revert

Since the original formula x = y (no need for back-substitution correction), the solution is:

in conclusion

The equation x⁴ + 2x² - 8x + 1 = 0 has two real roots and two conjugate complex roots.
Although the process of Ferrari's method is cumbersome, it can systematically decompose the quartic equation into a quadratic equation to solve.



Remainder of a polynomial divided by a higher degree

x2026divided by (x2+1)(x-1)2The remainder solution of

Calculation principle

Let the division formula be B(x) = (x^2+1)(x-1)^2. Since the degree of the division is 4th, the highest degree of the remainder R(x) must be less than 4th.
Let the remainder be R(x) = ax^3 + bx^2 + cx + d.
According to the principle of polynomial division, the dividend can be expressed as:
x^2026 = (x^2+1)(x-1)^2 Q(x) + ax^3 + bx^2 + cx + d

Substitute special values ​​to solve

1. When x = 1 (real roots of division equation):
1^2026 = a(1)^3 + b(1)^2 + c(1) + d
a + b + c + d = 1 --- (Equation 1)

2. Differentiate both sides of the original equation and enter x = 1 (processing multiple roots):
2026x^2025 = (partial differential of division) + 3ax^2 + 2bx + c
Since (x-1)^2 still contains the (x-1) term after differentiation, this part is 0 after substituting x=1:
2026 = 3a + 2b + c --- (Equation 2)

3. When x = i (imaginary root of the division formula, i^2 = -1):
i^2026 = (i^2)^1013 = (-1)^1013 = -1
R(i) = a(i^3) + b(i^2) + c(i) + d = -ai - b + ci + d
Sort out the real and imaginary parts: -1 = (d - b) + i(c - a)
From this we can get:
d - b = -1 --- (Equation 3)
c - a = 0 => c = a --- (Equation 4)

Simultaneous Equations Operation

Substituting (Equation 4) c = a into (Equation 1) and (Equation 2):
(1) a + b + a + d = 1 => 2a + b + d = 1
(2) 3a + 2b + a = 2026 => 4a + 2b = 2026 => 2a + b = 1013

Substituting 2a + b = 1013 into 2a + b + d = 1:
1013 + d = 1 => d = -1012

Substituting d = -1012 into (Equation 3):
-1012 - b = -1 => b = -1011

Substituting b = -1011 into 2a + b = 1013:
2a - 1011 = 1013 => 2a = 2024 => a = 1012
Since c = a, so c = 1012

Calculation result

Remainder R(x) = 1012x^3 - 1011x^2 + 1012x - 1012


x2026divided by (x2+1)(x-1)2Solution 2 of the remainder

Calculation ideas

This solution does not use the imaginary number i or calculus. We use the congruence property of polynomials to find out the difference between the dividend and the two factors (x2+1) and (x-1)2The remainders are finally combined into the total remainder.

Step 1: Find x2026divide by x2+1 remainder

Considering the congruence relationship, when the division formula is x2+1 when x2Equivalent to -1.
x2026 = (x2)1013
will x2= -1 Substitute:
(-1)1013 = -1
Therefore, x2026divide by x2The remainder of +1 is -1.

Step 2: Find x2026Divide by (x-1)2remainder

Let x = (x-1) + 1 and expand using the binomial theorem:
x2026 = [(x-1) + 1]2026
In the expansion, terms containing (x-1) to the 2nd power and higher can be (x-1)2Divisible.
We only need to keep the last two items:
Remainder = C(2026, 1) * (x-1)1 * 12025 + C(2026, 0) * 12026
Remainder = 2026 * (x-1) + 1
Remainder = 2026x - 2026 + 1 = 2026x - 2025

Step 3: Use substitution method to find the total remainder

Let the total remainder be R(x). Because the division is to the 4th power, the remainder is up to the 3rd power.
According to the result of the first step, R(x) = (x2+1)(ax + b) - 1。
Next, we ask R(x) to be divided by (x-1)2The remainder of must equal 2026x - 2025.

will x2+1 is expressed in the form (x-1):
x2+1 = (x-1+1)2 + 1 = (x-1)2 + 2(x-1) + 1 + 1 = (x-1)2 + 2(x-1) + 2
In mold (x-1)2down, x2+1 is equivalent to 2(x-1) + 2.

Represent ax+b as (x-1):
ax + b = a(x-1+1) + b = a(x-1) + (a+b)

Plug the above result into R(x) and expand (ignoring the 2nd order term of (x-1)):
R(x) is equivalent to [2(x-1) + 2] * [a(x-1) + (a+b)] - 1
= 2a(x-1) + 2(a+b)(x-1) + 2(a+b) - 1
= (4a + 2b)(x-1) + (2a + 2b - 1)

Compare with the remainder of the second step, 2026(x-1) + 1:
1. 4a + 2b = 2026 => 2a + b = 1013
2. 2a + 2b - 1 = 1 => a + b = 1

Subtract the two equations: (2a + b) - (a + b) = 1013 - 1
We get a = 1012.
Substituting a + b = 1 gives us b = -1011.

final result

Substitute a and b into R(x) = (x2+1)(1012x - 1011) - 1:
R(x) = 1012x3 - 1011x2 + 1012x - 1011 - 1
R(x) = 1012x3 - 1011x2 + 1012x - 1012



Lambert's W function

core definition

The Lambert W function, also known as the Product Logarithm, is the inverse function of the function f(w) = w * e^w. For a complex number z, the value of W(z) is defined as the value that satisfies the following equation:

W(z) * exp(W(z)) = z

This means that if you know the product of a number and its exponential function, Lambert's W function can help you work backwards to work out the number itself. This is useful when working with transcendental equations containing exponential terms.

branching properties

Since the function f(w) = w * e^w is not injective over the real domain (that is, different inputs may result in the same output), its inverse function has two branches in the real domain:

At z = -1/e (approximately -0.3678), the two branches meet, where W(-1/e) = -1.

discover history

The function is named after Swiss mathematician Johann Heinrich Lambert, who first touched on the concept in 1758 while studying trinomial equations. Subsequently, the great mathematician Leonhard Euler conducted a more in-depth analysis of it in 1783. However, the official name "Lambert's W function" was not widely adopted until the 1990s in order to allow mathematical software (such as Maple or Mathematica) to have consistent naming conventions.

Science and Engineering Applications

Lambert's W-function provides analytical solutions in several areas, freeing scientists from relying solely on numerical simulations:



series

basic definition

A series is the process or result in mathematics of adding the items in a sequence in order. If the sequence contains a finite number of terms, it is called a finite series; if it contains an infinite number of terms, it is called an infinite series. The concept of series is the basis of calculus and mathematical analysis and helps us understand how to deal with infinite accumulation.

Arithmetic series

Arithmetic series refers to the accumulation process in which the differences (called tolerances) of any two adjacent items in a sequence are equal. Its most famous property is that the sum of a series can be calculated by multiplying the average of the first and last terms by the number of terms.

Example: 1 + 3 + 5 + 7 + 9 = 25

geometric series

A geometric series refers to an accumulation process in which the ratios (called common ratios) of any two adjacent terms in a sequence are equal. In the case of an infinite series, if the absolute value of the common ratio is less than 1, the series will converge to a definite value.

Example: 1 + 1/2 + 1/4 + 1/8 + ... = 2

Convergence judgment

For infinite series, the most important research direction is to determine whether it converges. Convergence means that the result of adding infinite numbers approaches a finite constant; if the sum tends to infinity or oscillates between multiple values, it is called divergence.

Special series and applications

Series have wide applications in advanced mathematics and engineering:



infinite series

basic definition

An infinite series is an expression that sequentially adds all the terms in an infinite sequence. If the sequence is a1, a2, a3..., then the corresponding series is recorded as a1 + a2 + a3 + .... Although we cannot complete infinite additions in reality, through the concept of mathematical limits, we can study whether the sum tends to a specific value.

convergence and divergence

The most important property of infinite series is its convergence:

geometric series

The geometric series is the most common and well-understood example of an infinite series, in which each term is the previous term multiplied by a fixed ratio (the common ratio r). A geometric series converges when the absolute value of the common ratio is less than 1. For example:

1/2 + 1/4 + 1/8 + 1/16 + ... = 1

This geometric figure visually shows that when an infinite number of positive numbers are added together, the result can be a finite number.

Zeno's Paradox and Mathematical Solution

The ancient philosopher Zeno once proposed the famous "Achilles chasing the tortoise" paradox. He argued that the pursuer must first reach the starting point of the pursued, and when he reaches that point, the pursued has moved forward some distance, so the pursuer can never catch up to the turtle. The mathematical answer to this paradox is an infinite series: the sum of infinite time periods can be a finite value, which means that the pursuer can surpass the tortoise in a limited time.

Judgment method

Mathematicians have developed a variety of tools to judge the convergence of a complex series. Common methods include:

scientific applications

Infinite series have a wide range of applications in science and engineering, such as:



harmonic series

basic definition

调和级数是一个无限级数,由正整数的倒数按顺序相加而成。 Its form is as follows:

1 + 1/2 + 1/3 + 1/4 + 1/5 + ... + 1/n + ...

It is called "harmony" because the overtone sequence in music theory is closely related to this sequence. On a stringed instrument, if the string length is shortened to 1/2, 1/3, 1/4, etc., the frequency emitted corresponds to the reciprocal of these numbers.

Divergent properties

The most famous property of harmonic series is that it is divergent. This means that as the number of terms increases, the sum approaches infinity rather than converging to a fixed value. Although the value of each term (1/n) will get smaller and closer to zero, they will not shrink fast enough for the sum to stop growing.

The first person to prove the divergence of harmonic series was the 14th-century mathematician Nicole Oresme. He used an ingenious grouping method, dividing the terms into groups, and proved that the sum of each group is greater than 1/2, so the sum of infinite many 1/2 must lead to infinity.

Growth rate and logarithm

Although the harmonic series diverges to infinity, it grows extremely slowly. The sum of the first million terms is only about 14.39. Mathematician Euler discovered that the difference between the sum of the first n terms of the harmonic series and the natural logarithm ln(n) tends to a constant called the Euler-Mascheroni constant, which is approximately equal to 0.5772.

Interesting application: stacking blocks problem

Harmonic series has a famous application in physics: if you have a stack of identical rectangular wooden blocks, you can use the properties of harmonic series to perform "eccentric stacking." As long as there are enough wooden blocks, you can theoretically make the top wooden block completely suspended beyond the edge of the bottom wooden block, and the offset distance can be infinite.

Relevance to prime numbers

Harmonic series are also deeply related to the distribution of prime numbers. The series is also divergent if we just add the reciprocals of the primes (1/2 + 1/3 + 1/5 + 1/7 + ...). This was proved by Euler, who indirectly proved that there are infinitely many prime numbers.



Basel issues

problem definition

The Basel problem is a famous number theory problem first proposed by the Italian mathematician Montori in 1644. This problem requires calculating the exact value of the sum of the reciprocals of the squares of all positive integers, namely:

1 + 1/4 + 1/9 + 1/16 + 1/25 + ...

Although this series was known to converge, at the time, mathematicians had difficulty finding the exact value of its convergence.

historical background

This problem is called the Basel problem because the Bernoulli family who proposed the problem and Euler who finally solved it are both from Basel, Switzerland. The famous mathematician Jacob Bernoulli tried unsuccessfully to solve this problem, admitting in 1689 that it was an extremely difficult challenge. It was not until 1734 that Leonhard Euler, then only 28 years old, published a solution that shocked the mathematical world.

Euler's solutions and results

Euler used the infinite product expansion of the sine function to derive the exact value of this series. He concluded that the sum of this series is equal to:

pi squared divided by 6

This result is approximately equal to 1.644934. This was very surprising at the time, since pi should appear in a sequence of sums of squares of integers that seemed completely unrelated to circular geometry.

mathematical meaning

The solution to the Basel problem not only made Euler famous, but also opened up new paths for subsequent mathematical research:



Calculus

Calculus is a discipline in mathematics that studies the rate of change and accumulation of quantities. Calculus consists of two parts: differential calculus and integral calculus. It is widely used in physics, engineering, biology, economics and other fields. It is a basic tool for describing continuous changes.

Differential calculus

The main purpose of differential calculus is to study the rate of change of a function. Differential operations are used to find the derivative of a function, which describes the rate at which the function changes with the independent variables. Simply put, the derivative can be thought of as the slope of an instantaneous change.

integral calculus

Integral calculus is used to calculate accumulated quantities and is closely related to the calculation of area and volume. Integral is the inverse operation of derivative and is mainly used to solve the inverse change of cumulative quantity, sum or function.

fundamental theorem of calculus

The fundamental theorem of calculus connects differential and integral calculus and shows that integral operations can be solved through derivatives. Specifically, ifF'(x) = f(x),but∫[a, b] f(x) dx = F(b) - F(a)

Applications of Calculus

Calculus has a wide range of applications in science and engineering, here are some examples:

example

Here is a simple differential and integral example:

Differentiation: If f(x) = x^3, then f'(x) = 3x^2
Integral: If f(x) = 3x^2, then ∫f(x)dx = x^3 + C

in conclusion

Calculus is a mathematical tool that studies change and accumulation, and is essential for understanding and simulating real-world phenomena.



Differential formula table

Below are some common differential formulas that have a wide range of applications in mathematics and physics.

Basic differential formula

Differential formulas of trigonometric functions

Inverse trigonometric function differential formula

Multiplication and division differential formulas

chain rule

The chain rule is used for differentiation of composite functions:

d(f(g(x)))/dx = f'(g(x)) * g'(x)

Implicit function differentiation

If the function is given implicitly, e.g.F(x, y) = 0, then the implicit function differentiation method can be used:

(dy/dx) = -(∂F/∂x) / (∂F/∂y)



partial integration method

Basic concepts

Integration by Parts is a technique used to deal with the product of two functions in definite and indefinite integrals. It is derived from the product derivation rule of calculus.

formula

The partial integral formula of indefinite integral is:
∫ u(x) · v′(x) dx = u(x) · v(x) − ∫ u′(x) · v(x) dx
in:

Definite integral version

If the integral has upper and lower limits a to b, then:
∫ₐᵇ u(x) · v′(x) dx = [u(x) · v(x)]ₐᵇ − ∫ₐᵇ u′(x) · v(x) dx

Selection skills

When selecting u and v′, u can be selected in order according to the "LIATE" principle:
  1. L: logarithmic function (such as ln x)
  2. I: Inverse trigonometric function (such as arctan x)
  3. A: Algebraic function (such as xⁿ)
  4. T: Trigonometric functions (such as sin x, cos x)
  5. E: Exponential function (such as eˣ)

example

example:∫ x · eˣ dx
Let u = x, v′ = eˣ, then:
u′ = 1,v = eˣ
→ ∫ x · eˣ dx = x · eˣ − ∫ 1 · eˣ dx = x · eˣ − eˣ + C

Reuse some points

Some integrals need to apply part of the integral multiple times, for example, ∫ x² · eˣ dx, the formula can be applied twice in a row.

Examples of trigonometric and exponential functions

example:∫ eˣ · cos x dx
It is necessary to use partial integration twice to generate the original terms and then solve the simultaneous equations to evaluate.

Comparison with substitution integral

Substitution integral (u-substitution) is used for the "synthetic form" of the function; partial integral is used for the "product form" of the function, especially when one term is differentiable and the other term is integrable.

application



Feynman Integral Techniques

What is the Feynman integral technique?

Feynman's Technique is a method for calculating complex integrals, named after the famous physicist Richard Feynman. This technique solves the problem by parameterizing the integral, introducing differential variables, and performing the integral operation in the final step. This method is particularly suitable for solving integrals that are difficult to solve in traditional ways.

Basic steps of Feynman technique

Feynman integration techniques usually include the following steps:

  1. Introduce parameters:Introduce a parameter to make the integration easier to operate. This parameter can be a variable in the integral, or a new variable to help simplify the form of the integral.
  2. Differentiating the parameters:Differentiating the introduced parameters can convert complex integrals into integrals over the parameters, thereby reducing the difficulty of the problem.
  3. Calculate points:The differentiated results are integrated, and finally the parameter values ​​are reintroduced at appropriate steps to complete the final integral calculation.

Application examples

Here is a simple example of Feynman's integral technique:

Suppose we need to calculate the following integral:
    I = ∫ e^(-x^2) dx

    We can introduce a parameter t and let the integral be I(t) = ∫ e^(-t * x^2) dx.
    Next, the parameter t is differentiated and the corresponding integral is calculated, finally returning t to the desired value.

This method is suitable for solving complex integrals of similar forms, especially when there is parameterization.

Advantages of Feynman's Integral Technique

The advantage of Feynman's integration technique is that it can simplify difficult integration problems, especially in physics and engineering. Many common integrals can be solved by this technique. This method can deal with complex integration problems more flexibly without losing accuracy.

in conclusion

The Feynman integration technique is a powerful and flexible calculation method that simplifies integration problems by introducing parameters and differentials. This technique has wide applications in physics, mathematics and other fields, and is an important tool for solving complex integral problems.



differential equations

A differential equation is an equation containing an unknown function and its derivatives that describes the rate of change in a system. Differential equations are widely used in scientific fields such as physics, engineering, economics and biology, and are particularly suitable for simulating phenomena that change over time or space.

Classification of differential equations

Differential equations are generally divided into the following types:

Solutions to Differential Equations

Methods for solving differential equations vary depending on the type and complexity of the equation. Common methods include:

Applications of Differential Equations

Differential equations have applications in many fields of science, here are a few examples:

example

The following is an example of an ordinary differential equation:

      dy/dx = 3x^2
    

The solution to this equation is:

      y = x^3 + C
    

in,Cis the integral constant.

in conclusion

Differential equations are powerful tools for describing changes in natural and engineered systems, allowing us to simulate and predict system behavior.



partial differential equations

definition

A Partial Differential Equation (PDE) is an equation containing partial derivatives of one or more variables. This type of equation is used to describe the law of change in a multivariable system.

basic type

Solution method

Common equations

  1. Heat equation: ∂u/∂t = α ∇²u
  2. Wave equation: ∂²u/∂t² = c² ∇²u
  3. Laplace's equation: ∇²φ = 0
  4. Poisson's equation: ∇²φ = f(x, y, z)

Application areas

Heat Equation

Describing how heat spreads through space over time, the formula is as follows:

∂u/∂t = α ∇²u

inuis the temperature,αis the thermal diffusion coefficient,∇²is the Laplacian operator.

Wave Equation

Describe the propagation of vibrations or waves, such as sound waves or electromagnetic waves:

∂²u/∂t² = c² ∇²u

uis the displacement,cis the wave speed.

Laplace Equation

Descriptive equations for static fields (such as electrostatic fields):

∇²φ = 0

Often used in steady-state problems, such as electric fields and gravity fields.

Poisson Equation

When there are source terms in the field, Laplace's equation expands to:

∇²φ = ρ/ε₀

ρis the charge density,ε₀is the vacuum dielectric constant.

Schrödinger Equation

The core partial differential equations in quantum mechanics:

iħ ∂ψ/∂t = - (ħ²/2m) ∇²ψ + Vψ

ψis the wave function,ħTo reduce Planck’s constant,Vis potential energy.

Maxwell's Equations

Describe changes in electromagnetic fields, including partial differential forms:

∇ × E = -∂B/∂t
∇ × B = μ₀ε₀ ∂E/∂t + μ₀J

Eis the electric field,Bis the magnetic field,Jis the current density.



Fourier conversion

Fourier transformation is a method of converting signals in the time domain or space domain into a frequency domain representation and has important applications in signal processing, physics, and engineering. Through Fourier transformation, different frequency components in the signal can be analyzed.

Fourier transformation definition

𝔐 { f ( t ) } = F ( ω ) = - f ( t ) e ^ ( - jωt ) dt

in:

nature

Some common Fourier transformation properties are as follows:

Fourier transformations of common functions

functionf(t) Fourier conversionF(ω)
1 2πδ(ω)
δ(t) (Dirac delta function) 1
e0t 2πδ(ω - ω0)
cos(ω0t) π[δ(ω - ω0) + δ(ω + ω0)]
sin(ω0t) jπ[δ(ω - ω0) - δ(ω + ω0)]

These properties and formulas can help us understand the frequency components and spectral characteristics of signals, and are widely used in signal processing and communication systems.



Fourier Transformation for Solving Partial Differential Equations

Heat Equation

The one-dimensional heat conduction equation is:
∂u/∂t = α² ∂²u/∂x²
where u(x, t) represents the temperature and α is the thermal diffusion coefficient.
By performing Fourier transformation on the space variable x, the partial differential can be converted into multiplication, and we get:
∂Û(k, t)/∂t = −α²k²Û(k, t)
This is an ordinary differential equation that can be solved and then transformed back into u(x, t).

Wave Equation

The one-dimensional wave equation is:
∂²u/∂t² = c² ∂²u/∂x²
After Fourier transformation, we get:
∂²Û(k, t)/∂t² = −c²k²Û(k, t)
This is a simple harmonic oscillation equation, and the solution is:
Û(k, t) = A(k)cos(ckt) + B(k)sin(ckt)
Then through inverse Fourier transformation, the original function solution u(x, t) is obtained.

Laplace Equation

Laplace's equation in the region Ω is:
∂²u/∂x² + ∂²u/∂y² = 0
If it is in an infinite plane or half plane, a variable (such as x) can be transformed into a constant coefficient ODE by Fourier transformation, and then solved and reversely transformed to obtain u(x, y).

advantage



Laplace conversion

Laplace transformation is a method used to convert a time domain function into a frequency domain representation. It is widely used in mathematics and engineering, especially in control systems, signal processing, and solutions to differential equations.

Laplace transformation definition

{ f ( t ) } = F ( s ) = 0 f ( t ) e - s dt

in:

nature

Some common Laplace transformation properties are as follows:

Laplace transformations of common functions

functionf(t) Laplace conversionF(s)
1 1 / s
t 1 / s2
eat 1 / (s - a)
sin(ωt) ω / (s2 + ω2)
cos(ωt) s / (s2 + ω2)

These properties and formulas can assist in solving complex differential equations and converting them into algebraic equations for easy analysis and design of systems.



Laplace Transformation for Solving Ordinary Differential Equations

First order linear differential equation

Consider the equation:
y′(t) + ay(t) = f(t),y(0) = y₀
Taking Laplace transformation on both sides, we get:
sY(s) − y₀ + aY(s) = F(s)
Find Y(s) after shifting terms:
Y(s) = [F(s) + y₀] / (s + a)
Then perform the inverse Laplace transformation on Y(s) to get the solution y(t).

Second-order differential equation with constant coefficients

consider:
y″(t) + 3y′(t) + 2y(t) = 0,y(0) = 1,y′(0) = 0
Taking Laplace transformation on both sides, we get:
s²Y(s) − s · y(0) − y′(0) + 3[sY(s) − y(0)] + 2Y(s) = 0
Substitute the initial value:
s²Y(s) − s + 3sY(s) − 3 + 2Y(s) = 0
After sorting, we get:
(s² + 3s + 2)Y(s) = s + 3
Simplify:
Y(s) = (s + 3) / [(s + 1)(s + 2)]
Then decompose it by partial fraction and take the inverse transformation to get y(t).

Response to impulse input (unit step function)

equation:
y′(t) + y(t) = u(t − 1),y(0) = 0
where u(t − 1) is the unit step function, Laplace is converted toe^(−s)/s
After conversion, we get:
sY(s) + Y(s) = e^(−s)/s
Y(s) = e^(−s) / [s(s + 1)]
Then do the inverse transformation of Y(s) to get the analytical solution of the delayed response.

advantage



Green's function

definition

Green Function is a tool used to solve linear differential equations, especially for non-homogeneous partial differential equations containing source terms. If for a linear operatorL,satisfy

L G(x, ξ) = δ(x - ξ)

inδ(x - ξ)is the Dirac delta function, thenG(x, ξ)is the Green's function of this operator.

application

If Green's function is knownG(x, ξ), then the non-homogeneous equation can be

L u(x) = f(x)

The solution of is expressed in integral form:

u(x) = ∫ G(x, ξ) f(ξ) dξ

physical meaning

Green's function can be regarded as the "response" produced by the unit source term in space, for example:

Common examples

The Green's function of a Laplace equation (on the infinite interval) is:

G(x, ξ) = -|x - ξ| / 2

Solution steps

  1. Confirm linear operatorLand boundary conditions
  2. find satisfactionL G(x, ξ) = δ(x - ξ)Green's function that meets the boundary conditions
  3. Substitute into the integral expression to solveu(x)


Sturm–Liouville theory

Sturm–Liouville theory is a mathematical framework for dealing with eigenvalue problems. It is mainly used to solve eigenfunctions and eigenvalue problems of linear differential equations. The theory has wide applications in physics, engineering and applied mathematics, particularly in describing system behavior in vibration, heat conduction and quantum mechanics.

Sturm–Liouville problem form

A typical Sturm–Liouville problem can be expressed as a second-order differential equation of the following form:

      (p(x)y')' + (q(x) + λr(x))y = 0
    

in:

boundary conditions

In order to formulate the Sturm–Liouville problem, the equation needs to satisfy two boundary conditions. Common boundary conditions include:

These boundary conditions determine the eigenvaluesλPossible values ​​​​of , and affect the corresponding characteristic functiony(x)form.

Eigenvalues ​​and Eigenfunctions

The solution to the Sturm–Liouville problem consists of a set of eigenvaluesλand the corresponding characteristic functiony(x). These characteristic functions satisfy orthogonality, that is, in the weight functionr(x)Below, the integrals of different characteristic functions are zero:

∫[a, b] y_m(x) y_n(x) r(x) dx = 0 (when m ≠ n)

in,y_m(x)andy_n(x)are different eigenvaluesλ_mandλ_nthe corresponding characteristic function.

Application of Sturm–Liouville theory

Sturm–Liouville theory is widely used in the following fields:

example

Consider the following simple Sturm–Liouville problem:

      y'' + λy = 0,   y(0) = 0, y(π) = 0
    

Eigenvalues ​​for this problemλforλ_n = n^2(innis a positive integer), and the corresponding characteristic function isy_n(x) = sin(nx)

in conclusion

Sturm–Liouville theory provides a framework for dealing with eigenvalue problems and is of great significance for analyzing linear differential equations and understanding the vibration modes of systems.



Rainville ordinary differential equation

What is Rainville ordinary differential equation?

Rainville ordinary differential equations refer to a class of equations named after Harry Rainville Rainville, whose research covers a variety of differential equation theories and proposes important solutions and applications, especially in engineering and physics. In his work, Rainville provides systematic solution guidance for first-order, second-order and higher-order ordinary differential equations, which is very helpful for understanding the theory of differential equations.

Classification of Rainville Ordinary Differential Equations

Solution of Rainville Ordinary Differential Equation

Rainville proposed a variety of solutions to different differential equations:

Applications of Rainville Ordinary Differential Equations

in conclusion

Rainville Ordinary Differential Equations provides a variety of solutions and applications of differential equations, and provides an important tool for dynamic system modeling in different disciplines. Whether in physics, engineering or biomathematics, Rainville equations and solutions help us deeply understand and predict the behavior of systems.



Legendre polynomial

definition

Legendre polynomials are a set of orthogonal polynomials commonly used to solve Laplace's equation and related boundary value problems in spherical coordinates. In mathematical physics, they are a special case of the Sturm–Liouville theory.

Legendre polynomialP_n(x)is the solution to a second-order linear differential equation:

      (1 - x^2) y'' - 2x y' + n(n + 1)y = 0
    

in,nis a non-negative integer.

Orthogonality

Legendre polynomials satisfy the orthogonality condition, that is, in the interval[-1, 1]above, the weight function is1When , the following integral relationship is satisfied between polynomials of different orders:

∫[-1, 1] P_m(x) P_n(x) dx = 0 (when m ≠ n)

generating function

The generating function of the Legendre polynomial is:

      (1 - 2xt + t^2)^(-1/2) = ∑ P_n(x) t^n  (n = 0, 1, 2, ...)
    

low order polynomial

Here are some low-order Legendre polynomials:

application

Legendre polynomials have important applications in physics and engineering, including but not limited to the following areas:

example

consider functionf(x) = x^2, expand it into a linear combination of Legendre polynomials:

      f(x) = (2/3) P_2(x) + (1/3) P_0(x)
    

in conclusion

Legendre polynomials provide a powerful tool for dealing with spherical symmetry problems and play an important role in numerical calculations and theoretical physics.



Hermite polynomial

definition

Hermite polynomials are a set of orthogonal polynomials in mathematics, commonly used in fields such as probability theory, numerical analysis, and quantum mechanics. Hermite polynomials satisfy the following differential equation:

    y'' - 2xy' + 2ny = 0

in,nis a non-negative integer.

recursive formula

Hermite polynomials can be generated using the following recurrence relation:

    H₀(x) = 1,
    H₁(x) = 2x,
    Hₙ₊₁(x) = 2xHₙ(x) - 2nHₙ₋₁(x)

Orthogonality

Hermite polynomials in weight functionsw(x) = e^(-x²)The following satisfies orthogonality:

∫[-∞, ∞] Hₘ(x)Hₙ(x)e^(-x²) dx = 0 (when m ≠ n)

generating function

The generating function of the Hermite polynomial is:

    e^(2xt - t²) = ∑ Hₙ(x) tⁿ / n!  (n = 0, 1, 2, ...)

low order polynomial

Here are some low-order Hermite polynomials:

application

Hermite polynomials are widely used in the following fields:



Chebyshev polynomial

Chebyshev polynomial

Chebyshev Polynomials are a type of orthogonal polynomials widely used in mathematics, divided into the first category (Tn(x)) and the second category (Un(x)). Chebyshev polynomials play an important role in the fields of approximation theory, numerical analysis and engineering.

The Chebyshev polynomials are defined as follows:

The recurrence relation of Chebyshev polynomials

Chebyshev polynomials of the first kindTn(x)and Chebyshev polynomials of the second kindUn(x)It can be calculated through the recursive relationship:

Application examples of Chebyshev polynomials

The first few terms of Chebyshev polynomials of the first kind

The following are Chebyshev polynomials of the first kindTn(x)The first few items of:

Chebyshev differential equation

Chebyshev polynomialTn(x)It is an important tool when solving a certain differential equation, which is as follows:

(1 - x²) T''(x) - x T'(x) + n² T(x) = 0

This equation is the defining equation of the Chebyshev polynomial, which is a second-order linear differential equation and applies to the domain range from -1 to 1.

Solution of Equation - Chebyshev Polynomials

in the equation(1 - x²) T''(x) - x T'(x) + n² T(x) = 0in, whennWhen is an integer, its solution is the Chebyshev polynomial of the first kindTn(x). Therefore, this equation satisfies orthogonality and has good approximation properties, and is particularly suitable for approximate solutions in numerical analysis.

Application of Chebyshev polynomials in solving differential equations

Application examples

Suppose we wish to find an approximate solution to a differential equation. The solution can bef(x)Expands into linear combinations of Chebyshev polynomials:

f(x) ≈ ∑ an Tn(x)

in,anare the coefficients of the Chebyshev polynomial. We can use numerical methods to solve for these coefficients to obtain approximate solutions to the differential equations.



integral equation

definition

Integral equation refers to an equation in which the unknown function appears in the integral sign. It is a common mathematical model in many physical and engineering problems (such as heat conduction, electromagnetic fields, elastic mechanics, etc.). Its solutions are closely related to differential equations and are often converted into each other.

basic form

The general form of the integral equation is as follows:

f(x) = λ ∫ab K(x, t) φ(t) dt + g(x)

Main types

Example

Fredholm Category 2:

φ(x) = ∫01 (x + t) φ(t) dt + sin(x)

Volterra Category 1:

x² = ∫0x t φ(t) dt

Applications in Physics

Solution method

Relationship to differential equations

In many problems, integral equations and differential equations are equivalent. For example, differential equations can be obtained by differentiating integral equations, or Green's functions can be used to convert differential equations into integral form, which is particularly helpful for dealing with boundary value problems.

Conclusion

Integral equations provide an effective tool for analyzing continuous systems and boundary conditions. Compared with differential equations, it is more suitable for dealing with problems with non-locality, memory or boundary effects, and is an indispensable mathematical method in modern physics and engineering.



Integral Equations and Method of Moments

Overview of Integral Equations

An integral equation is an equation in which the unknown function appears within the integral sign. It is often used to describe the distribution of field quantities in physical problems, such as electromagnetic fields, sound fields, and thermal fields. Its basic form is as follows:

φ(x) = ∫ K(x, x') ψ(x') dx'

Common types

Applications in Electromagnetics

When calculating electromagnetic fields, integral equations can be used to describe the radiation and scattering behavior caused by boundary conditions. For example, Green's functions are used to establish boundary integral equations to avoid directly solving the differential form of Maxwell's equations.

Introduction to Moment Method

Method of Moments (MoM) is a numerical method that discretizes integral equations and is used to approximately solve field problems. The main idea is to expand the unknown function into a linear combination of a set of basis functions, and construct an algebraic equation system through the test function.

Step instructions

  1. Expand the unknown function into a combination of basis functions:
    ψ(x) ≈ ∑ aₙ fₙ(x)
  2. Substitute into the integral equation, inner product with the test function (gₘ(x)), and convert to an algebraic system:
    ∑ aₙ ∫ gₘ(x) K(x, x') fₙ(x') dx' dx = ∫ gₘ(x) φ(x) dx
  3. Build a linear system:
    [Z][a] = [V]

Commonly used bases and test functions

Application examples

Advantages and limitations

Conclusion

Integral equations and the method of moments provide powerful solution tools in field theory and boundary value problems. Through the establishment of numerical discretization and linear algebra systems, various scattering, radiation and transmission phenomena can be effectively solved, and are widely used in the fields of electromagnetics, acoustics and computational physics.



Feynman parameter method

Basic concepts

Feynman parametrization is a mathematical technique commonly used in quantum field theory to simplify complex Feynman diagram integrals, especially when dealing with the product of multiple propagators in the denominator.

formula form

The core formula of Feynman parameter method is:
1 / (A₁^α₁ A₂^α₂ ... Aₙ^αₙ) = Γ(α₁ + ... + αₙ) / [Γ(α₁) ... Γ(αₙ)] × ∫₀¹ dx₁ ... dxₙ δ(1 − Σxᵢ) × x₁^(α₁−1) ... xₙ^(αₙ−1) / (ΣxᵢAᵢ)^(Σαᵢ)
in:

Common simplified situations

If the denominator has only two terms (n = 2, α₁ = α₂ = 1):
1 / (AB) = ∫₀¹ dx / [xA + (1−x)B]²If the denominator has three terms (n = 3, αᵢ = 1):
1 / (ABC) = 2! × ∫₀¹ dx dy dz δ(1 − x − y − z) / [xA + yB + zC]³

Application steps

  1. Express the propagator denominator as the product of A₁, A₂, ..., Aₙ
  2. Combine denominators into a single term using the Feynman parameter method
  3. Complete momentum integral (usually becomes Gaussian integral)
  4. Perform integration over Feynman parameters

Allocation methods and variable transformations

After incorporating the propagator, the momentum variable needs to be processed by the recipe to convert the integral into standard form. For example:
∫ d⁴k / [(k − q)² + Δ]ⁿIt can be converted into standard Gaussian form and then calculated.

Advantages and uses

The graphical meaning of Feynman parameters

The Feynman parameter can be thought of as the "weighted proportion" of the propagator's contribution in different channels, reflecting how momentum flows in the internal circuit.

Things to note

Related applications



gamma function

What is the gamma function?

Gamma Function is a mathematical function that extends factorial and is usually used in the field of complex numbers and real numbers. For a positive integer n, the gamma function is defined as the factorial of n:

Γ(n) = (n-1)! where n = 1, 2, 3,...

For a positive real number x, the gamma function is defined as follows:

Γ(x) = ∫(0 to ∞) t^(x-1) * e^(-t) dt

This integral converges when x > 0.

Properties of the gamma function

The gamma function has several important properties, including:

Application of gamma function

The gamma function has wide applications in many fields of science and engineering, particularly in:

Summarize

The gamma function is a special function that is very important in mathematics. It extends the concept of factorial and has wide applications in many fields. By understanding the properties and applications of the gamma function, we can better solve a variety of mathematical and scientific problems.



Difference product operation

definition

Fractional-order derivatives and integrals, collectively called "Differintegrals", are concepts in mathematics that extend derivatives and integrals to non-integer orders. It covers derivative and integral operations of any order on functions.

Riemann-Liouville definition

One major definition of fractional derivatives and integrals is the Riemann-Liouville form:

    Dⁿ[a, b]f(x) = (1 / Γ(m - n)) dᵐ/dxᵐ ∫[a, x] (x - t)ⁿ⁻ᵐ f(t) dt

in,nis a non-integer,mis satisfiedm - 1 < n < man integer,Γis the gamma function.

Caputo definition

The Caputo definition provides a form suitable for the initial value problem:

    Dⁿf(x) = (1 / Γ(m - n)) ∫[a, x] (x - t)ⁿ⁻ᵐ f⁽ᵐ⁾(t) dt

The Caputo definition is more suitable for describing physical phenomena than the Riemann-Liouville form.

nature

application

Fractional derivatives and integrals have important applications in many fields of science and engineering:



Bessel function

What is Bessel function?

Bessel Functions are a type of special functions widely used in mathematics and physics, especially when solving circular or cylindrical symmetry problems. These functions are named after the mathematician Friedrich Bessel and are usually represented by J_n(x), where n is the order of the function, and x is the independent variable.

Bessel function types

There are two main types of Bessel functions:

Properties of Bessel functions

Bessel functions have many important mathematical properties, including:

Application of Bessel function

Bessel functions are widely used in many fields of science and engineering, especially in:

Summarize

As a special function, Bessel function is of great significance in mathematics and its application fields. Its unique properties and wide range of applications make it an indispensable tool in physics and engineering.



hypergeometric function

definition

Hypergeometric functions are a special class of functions, defined as generalized hypergeometric series:

    _2F_1(a, b; c; z) = ∑ (aₖ bₖ / cₖ) * zᵏ / k!  (k = 0, 1, 2, ...)

in,aₖ = a(a+1)(a+2)...(a+k-1)represents the ascending factorial,c ≠ 0, -1, -2, ...

Convergence

The series converges under the following conditions:

special circumstances

Hypergeometric functions include a variety of special cases, such as:

differential equations

Hypergeometric functions satisfy the following hypergeometric differential equation:

    z(1 - z)y'' + [c - (a + b + 1)z]y' - aby = 0

application

Hypergeometric functions have important applications in the following fields:



Legendre Functions

Legendre Functions are a special set of functions that solve Legendre differential equations. These functions are widely used in physics and engineering problems, especially in spherically symmetric systems such as electrostatic fields, gravitational fields, and spherical coordinate systems in quantum mechanics.

1. Legendre differential equation

The Legendre differential equation is a second-order ordinary differential equation of the form:

(1 - x²) d²y/dx² - 2x dy/dx + l(l + 1)y = 0
        

in,lis a non-negative integer,xThe value range of is -1 to 1.

2. Legendre Polynomials

whenlWhen it is a non-negative integer, the solution of Legendre differential equation is Legendre polynomial, usually written asPl(x). Legendre polynomials are the form of polynomial solutions. The following are the first few polynomials:

Legendre polynomials satisfy orthogonality, that is:

-11 Pl(x) Pm(x) dx = 0, when l ≠ m
3. Associated Legendre Functions

Associated Legendre Functions are used to solve problems with angular momentum in spherical coordinates. The Legendre joint function is written asPlm(x),inmis an integer and satisfies|m| ≤ l

The Legendre joint function can be derived by differentiation from Legendre polynomials:

Plm(x) = (1 - x²)|m|/2 d|m|Pl(x) / dx|m|
        
4. Application of Legendre function
5. Calculation examples
#Python example: Use SciPy to calculate Legendre polynomial P3(x)
from scipy.special import legendre

# Define Legendre polynomial
P3 = legendre(3)
x = 0.5 # Take x = 0.5

# Calculate P3(x)
result = P3(x)
print("P3(0.5) =", result)

This example shows how to use the Python SciPy suitelegendreFunction Calculate Legendre PolynomialP3(x)value.

In summary, the Legendre function plays an important role in many physical and engineering problems, especially in symmetry problems in spherical coordinate systems.



difference equation

Difference equation (Difference Equation) is an equation that describes the relationship between discrete variable sequences. It is widely used in fields such as mathematics, physics, economics, and engineering to describe the dynamic behavior of discrete systems.

Basic form of difference equation

The basic form of the difference equation is as follows:

y[n+1] = f(y[n], y[n-1], ..., y[0], n)

in:

Types of difference equations

First order difference equation

The form of the first-order difference equation is:

y[n+1] = ay[n] + b

This equation can be used to describe a linearly growing or decaying sequence.

second order difference equation

The second-order difference equation considers the relationship between two previous values, such as:

y[n+2] = a y[n+1] + b y[n] + c

This type of equation is often used to describe oscillatory behavior and more complex dynamic systems.

Solution of Difference Equations

Common methods for solving difference equations include:

Difference equations have important application value in digital signal processing, control systems, financial models and other fields, helping to analyze and predict the behavior of discrete systems.



generic function

1. Generic functions

In mathematics,generic function(Functional) is a special kind of function whose input is a function and whose output is a scalar value. Generic functions are often used in physics and engineering to describe energies, paths, and other states of systems. Generic functions are often represented mathematically using symbolsJ[y],inyis a function.

2. Method of variation

calculus of variations(Calculus of Variations) is a mathematical technique used to find situations where a generic function reaches a maximum or minimum value. The core idea of ​​the calculus of variations is to change the functiony(x)shape or path to minimize or maximize the functionalJ[y]value. This is used in physics to solve problems such as shortest path, minimum energy, etc.

3. Euler-Lagrange equation

In the calculus of variations,Euler-Lagrange equationis a commonly used equation used to solve extreme value problems of functionals. Given a functional:

J[y] = ∫ L(x, y, y') dx

in,Lis a Lagrangian function,y'yesyrightxthe derivative of. to make functionalJ[y]Get the extreme value, functiony(x)The Euler-Lagrange equation must be satisfied:

∂L/∂y - d(∂L/∂y')/dx = 0

4. Application examples

The following is a simple application example, using the variational method to find the shortest path between two points.

5. Application scenarios of functional functions and variational method

6. Advantages and Disadvantages



vector analysis

1. Definition of vector

2. Basic operations on vectors

3. Inner product of vectors

4. External product of vectors

5. Vector fields

6. Calculus in vector analysis



Eigenvalues ​​and eigenvectors

What are eigenvalues ​​and eigenvectors?

Eigenvalue and Eigenvector are important concepts in linear algebra, especially in the study of matrices. For a given square matrix A, if there is a non-zero vector v, so that when A acts on v, the result is a multiple of v, that is:
A * v = λ * v, where λ is the eigenvalue and v is the corresponding eigenvector.

Definition of eigenvalues

The eigenvalue is a scalar associated with the eigenvector and represents the scaling factor of the matrix in the direction of the eigenvector. For a square matrix A, its eigenvalues ​​can be obtained by solving the characteristic equation:

det(A - λI) = 0, where I is the identity matrix and det represents the determinant. Solving this equation yields all eigenvalues ​​of A.

Definition of feature vector

Eigenvectors refer to vectors whose direction remains unchanged under matrix transformation. For a given eigenvalue λ, the eigenvector v is a non-zero solution that satisfies the above equation. Eigenvectors provide insight into the behavior and structure of the matrix A.

Application of eigenvalues ​​and eigenvectors

Eigenvalues ​​and eigenvectors have wide applications in many fields, including:

Summarize

Eigenvalues ​​and eigenvectors are core concepts in linear algebra and are crucial to understanding the properties of matrices and solving various application problems. They provide important information about linear transformations and are widely used in data analysis, engineering, and scientific research.



conjugate symmetric matrix

What is a conjugate symmetric matrix?

The conjugate symmetric matrix (Hermitian Matrix) is a special square matrix that satisfies the following conditions: for any element a_{ij}, there is a_{ij} = \overline{a_{ji}} . This means that the element relationships of the matrix are symmetric, but taking into account the conjugation of complex numbers. Simply put, a matrix is ​​equal to its own conjugate transpose, which is:

A = A*, where A* represents the conjugate transpose of matrix A.

Properties of conjugate symmetric matrices

Conjugate symmetric matrices possess several important properties, including:

Applications of conjugate symmetric matrices

Conjugate symmetric matrices have a wide range of applications in mathematics and engineering. Common examples include:

Summarize

Conjugate symmetric matrix is ​​an important concept in linear algebra and has many excellent mathematical properties and applications. In various fields of science and engineering, understanding and utilizing the properties of conjugate symmetry matrices is crucial to solving practical problems.



Euler's rotation theorem

Euler's Rotation Theorem, proposed by mathematician Leonhard Euler in the 18th century, is an important theorem describing the rotation of rigid bodies. This theorem states that in three-dimensional space, any rigid body rotation fixed at a point can be expressed as a rotation about a fixed axis. This fixed axis is called the axis of rotation.

1. Basic content of Euler’s rotation theorem

Euler's rotation theorem states: For any rigid body in three-dimensional space, if the rigid body rotates from one direction to another in space, then its rotation can be equivalent to a rotation around a fixed axis. This means that only the rotation angle needs to be knownθand the direction of the rotation axis, the rotation can be described.

2. Euler Angles

In practical applications, rotation is usually expressed using Euler angles. Euler angles include three angles, which respectively describe the rotation of a rigid body on three mutually orthogonal axes in space. These three angles are usually expressed as(α, β, γ),in:

Through these three angles, any rotation of the rigid body in space can be described.

3. Mathematical representation of Euler’s rotation theorem

According to Euler's rotation theorem, the rotation of a rigid body can be represented by a rotation matrix or a quaternion. The rotation matrix is ​​a 3x3 orthogonal matrix used to describe the transformation of a rigid body in space. For rotation angleθ, about the axis of rotation(x, y, z), the rotation matrix is ​​expressed as:

R(θ) = 
    | cosθ + x²(1 - cosθ)     xy(1 - cosθ) - zsinθ   xz(1 - cosθ) + ysinθ |
    | yx(1 - cosθ) + zsinθ    cosθ + y²(1 - cosθ)    yz(1 - cosθ) - xsinθ |
    | zx(1 - cosθ) - ysinθ    zy(1 - cosθ) + xsinθ   cosθ + z²(1 - cosθ)  |
        
4. Application of Euler’s rotation theorem
5. Calculation examples
# Python example: Calculate rotation matrix using SciPy
from scipy.spatial.transform import Rotation as R

# Define rotation angle (degrees) and axis
angle = 45 # 45 degrees
axis = [0, 0, 1] # Rotate around the Z axis

# Calculate rotation matrix
rotation = R.from_rotvec(angle * np.pi / 180 * np.array(axis))
rotation_matrix = rotation.as_matrix()
print("rotation matrix:", rotation_matrix)

This example shows how to use the Python SciPy suite to calculate a rotation matrix of 45 degrees about the Z-axis.

In summary, Euler's rotation theorem provides a concise and powerful description method for the rotation of rigid bodies and is of key significance in many engineering and physics applications.



Nabla operator

Definitions and symbols

The Nabla operator (symbol ∇) is a vector differential operator. In the three-dimensional Cartesian coordinate system, it is defined as a set of vectors that are partially differentiated with respect to the directions of the three coordinate axes. In mathematics and physics, this symbol is usually pronounced del or nabla. It is not a specific numerical value, but an operation instruction, which must act on a certain function (scalar field or vector field) to be meaningful.

Three core operations

Laplacian

When the Nabla operator is dot producted with itself, it results in the Laplacian operator (noted ∇²). This is a second-order differential operator that plays a key role in equations describing physical phenomena such as heat conduction, electrostatic potential distribution, and wave phenomena.

Name and history

This inverted triangle notation was originally introduced by Scottish mathematician William Rowan Hamilton. The name Nabla was suggested by a friend of James Clerk Maxwell and is derived from the Greek word for an ancient plucked instrument shaped like an inverted triangle (naubla in Greek).

physical meaning

The Nabla operator is an indispensable tool in Maxwell's equations, which describe the fundamental laws of electromagnetism, and in the Navier-Stokes equations of fluid mechanics. It simplifies complex spatial change relationships into elegant vector expressions, allowing us to more intuitively understand the interaction between energy flow, fluid vortices and electromagnetic fields.



linear algebra

definition

Linear algebra is a branch of mathematics that studies vectors, vector spaces (linear spaces), linear transformations, and matrices. It is a basic tool in modern mathematics and its application fields (such as physics, engineering, economics, and computer science).

Basic concepts

Common operations

Eigenvalues ​​and eigenvectors

For square matrixA, if there is a non-zero vectorvwith scalarλMakes:

    A * v = λ * v

butλcalledEigenvaluevfor the correspondingeigenvector. This plays an important role in system stability analysis, physical modeling and data dimensionality reduction.

application



linear transformation

definition

Linear transformation refers to a mapping from one vector space to another vector space and satisfies the following two properties:

in,Tis a linear transformation,uandvis a vector,cis a scalar quantity.

Matrix representation

In linear algebra, any linear transformation can be expressed as a matrix multiplication:

    T(x) = A * x

inAis a matrix,xis a vector.

Geometric meaning

Common linear transformations in linear algebra include:

Nuclei and images

characteristic

application



Euler's rotation theorem

definition

Euler's rotation theorem states that in three-dimensional space, any rigid body displacement around a fixed point can be regarded as the result of a single rotation around a unique axis passing through the fixed point. This means that no matter how complex the continuous rotation a rigid body undergoes, the change in its final position relative to the initial position can always be achieved by rotating a specific angle around a specific rotation axis.

Core features

mathematical explanation

In linear algebra, this theorem can be described in terms of rotation matrices. If a 3x3 real matrix R is orthogonal and its determinant has value 1 (belonging to the special orthogonal group SO(3)), then the matrix must have an eigenvalue of 1. The eigenvector corresponding to eigenvalue 1 is the axis of rotation because the vector remains unchanged when the matrix R acts on it.

Proof of concept

Euler's original proof was based on spherical geometry. He observed that any transformation that moves one set of great-circle arcs on the sphere to another set of equal-length arcs must leave a pair of antipodal points on the sphere unchanged. The straight line connecting the pair of fixed points is the axis of rotation of the rigid body.

Practical application



abstract algebra

definition

Abstract algebra is a branch of mathematics that studies algebraic structures and their properties. The focus is not on specific numerical calculations, but on the relationship between operation rules and structures. The main research objects include groups, rings, domains, vector spaces and modules, etc.

group

A group is a set with a closed binary operation, which satisfies the associative law, the identity element exists, and each element has an inverse element. If the operation of the group is commutative, it is called an Abelian group.

ring

A ring is a set that has two operations: addition and multiplication. Addition constitutes an Abelian group, multiplication is closed and has associative law, and multiplication is distributed to addition. If multiplication has identity elements, it is called an identity ring; if multiplication is also commutative, it is a commutative ring.

domain

The field is a further enhancement of the ring. In addition to the Abelian group formed by addition, the non-zero elements also form the Abelian group under multiplication. Common examples include the field of real numbers ℝ, the field of complex numbers ℂ, the field of rational numbers ℚ, the finite field 𝔽ₚ, etc.

Isomorphism and isomorphism

Homomorphism is a mapping that preserves the structure. If a mapping maintains the structure under operation, it is a homomorphism of the algebraic structure; if it is a bijection at the same time, it is an isomorphism, which means that the two structures are equivalent in algebraic properties.

Modules and vector spaces

The module is a generalized vector space defined for rings. When the ring is a domain, the module is a vector space. Modular theory plays an important role in modern algebra, especially in homology algebra and representation theory.

application

Abstract algebra is used in many fields such as number theory, algebraic geometry, cryptography, quantum physics, and coding theory. For example, the RSA algorithm in modern cryptography is based on the theory of finite fields and modular arithmetic.

Development history

Abstract algebra has its origins in nineteenth-century studies of polynomial solutions, such as Galois' theory. Later, with the establishment of group theory, ring theory and domain theory, it gradually formed an independent discipline. In the 20th century, it was promoted by Banach, Noether and others into a broader study of algebraic structures.

representative figure

Important contributors include Galois, Amy Noether, Dedekind, Hilbert, Artin, Mark Wall, Chevalet, etc. They have a profound influence on the establishment of algebraic structure and formal theory.

geometry

definition

Geometry is a basic branch of mathematics that studies the properties, size, shape, position and transformation of graphics in space. From flat shapes to higher-dimensional spaces, geometry provides tools for understanding the shape and structure of the world.

Classification

basic elements

geometric transformation

application

Geometry is widely used in fields such as engineering, architecture, design, art, astronomy, computer graphics, machine vision, geographic information systems, mechanics and modern physical theory.

Development history

From Euclid and Archimedes in ancient Greece to Arabic and Indian mathematics, to modern Riemann, Gauss, Newton and modern algebraic geometry and string theory, geometry has gone through changes, from intuition to abstraction.

representative figure

Euclid, Archimedes, Descartes, Newton, Gauss, Riemann, Hilbert, Poincaré, Grothendieck, etc. all made profound contributions to the development of geometry.

Topology

definition

Topology is a branch of mathematics that studies the properties of space that remain under continuous deformation (such as stretching, bending, but excluding tearing and gluing). It focuses on the "nature of shape" of an object rather than specific geometric measurements.

topological space

Topological space is a set with a system of subsets called "topology". These subsets satisfy:

These open sets are used to define concepts such as "contiguity" and "continuity".

Basic concepts

Common examples

Important concepts and theories

application



algebraic geometry

definition

Algebraic geometry is a branch of mathematics that studies the sets of solutions to polynomial equations. These solution sets are called "Algebraic Variety". Algebraic geometry combines the concepts of algebra (especially abstract algebra) and geometry, and is widely used in various fields of mathematics and physics.

basic objects

example

existℝ²Equations inx² + y² - 1 = 0Represents a unit circle, which is an algebraic variety.

important concepts

Application areas

Calculation tools



group theory

1. What is group theory?

Group theory is a branch of mathematics that mainly studies symmetry and operability in mathematical structures. Group theory is the foundation of modern algebra and has wide applications in many fields, including physics, chemistry, and computer science. A group refers to a collection and combination of operations with specific properties.

2. Basic definition of group

A group is a collectionGand an operation*, satisfying the following four basic conditions:

3. Type of group

4. Application of group theory

5. Simple example

The following is an additive group of binary numbers (0 and 1) whose operation is modulo 2 addition:

Group G = {0, 1}
Operation: 0 + 0 = 0, 0 + 1 = 1, 1 + 0 = 1, 1 + 1 = 0 (modulo 2)

This group meets the four basic conditions of a group and is an Abelian group.



subgroups and orders

Subgroup

If the set H is a non-empty subset of the group G, and H itself is also a group under the same operation, then H is called a subgroup of G, denoted by H ≤ G. To determine whether H is a subgroup, the "subgroup discrimination method" is usually used:If these three conditions are met, H is a subgroup of G.

Example of subgroup

Order

There are two levels:
  1. Order of the group:The total number of elements in group G is denoted as |G|. If |G| is finite, G is called a finite group.
  2. Order of elements:For a ∈ G, if there is a smallest positive integer n such that aⁿ = e (identity element), then n is called the order of a, recorded as ord(a).

properties of order

example

extended concept



normal subgroup

definition

If H is a subgroup of group G, and for any g ∈ G, gH = Hg, Then H is called G'snormal subgroup(Normal Subgroup), denoted as H ⊲ G. Equivalently, H is a normal subgroup ⇔ for all g ∈ G, we have gHg⁻¹ = H.

significance

A normal subgroup is a substructure in the group whose "symmetry" remains unchanged. When the subgroup is a normal subgroup, the "Quotient Group" G/H can be defined on G, which is an important basis for constructing a new group.

Judgment condition

example

Quotient Group

If H ⊲ G, then the quotient group G/H can be defined, whose elements are the set of all left cosets:
G/H = { gH | g ∈ G }
The group operation is defined as: (g₁H)(g₂H) = (g₁g₂)H. Since H is a normal subgroup, this operation is well-definite.

nature

application

Normal subgroups are used in group theory to study the internal structure of groups. Complex groups can be decomposed into simpler parts through quotient groups, which is a basic tool for studying group isomorphism, simple groups and homomorphisms.

group theory symmetry

core concepts

In mathematics, group theory is a tool specifically used to study symmetries. Symmetry of a system is defined as a property that remains unchanged under some transformation. Group theory collects these invariant transformations together into a mathematical structure called a group. This allows us to use algebraic methods to accurately classify and analyze symmetries, rather than relying solely on visual intuition.

Four axioms of groups and symmetry transformations

To treat a symmetry operation as a group, the following four basic conditions must be met:

Common types of symmetry groups

Application areas

Symmetry breaking

Symmetry breaking is a profound concept in group theory. It refers to the phenomenon that a system originally has high symmetry, but due to changes in the environment or energy state, it eventually exhibits lower symmetry. This is crucial in explaining how mass was created in the early universe (the Higgs mechanism) and how phase changes, such as water freezing into crystals, occurred.



Galois theory

Overview

Galois Theory is a French mathematicianÉvariste GaloisA theory developed in the 19th century to studySolvability of Polynomial Equationsand its corresponding symmetry. This theory willgroup theoryanddomain theoryCombined, it provides conditions for judging whether a polynomial can be solved by radicals.

core concepts

domain expansion

Given a domainK, if there is a larger domainLmakeKyesLsubdomain of , then it is calledLyesKofexpansion domain, recorded asL/K

Galois group

For a domain expansionL/K,likeGal(L/K)is maintained by allKA group composed of fixed automorphisms is calledGalois group

Fundamental theorem

The basic theorem of Galois theory was establishedCorrespondence between Galois group and domain expansion

Solvability of polynomials

One of the core results of Galois' theory is thatDetermine whether the discriminant equation can be solved using radicals

application



Galois group

What is a Galois group?

Galois Group is a mathematical structure in algebra used to study the symmetry between the roots of polynomial equations. The Galois group was discovered by French mathematician Évariste Galois. Galois, it is mainly used to explore the solvability of polynomials and describe the symmetry and transformation properties of their roots.

Basic concepts of Galois group

Galois theory

Galois theory is a branch of theory in mathematics used to study the solvability of polynomial equations, especially using algebraic methods to determine whether polynomials can be solved using radicals. This theory relates the solvability of polynomials to the Galois group structure of their roots:

Applications of Galois Groups

in conclusion

Galois groups play an important role in mathematics, providing a way to analyze the structure of polynomial roots from a symmetry perspective. Through the relationship between the Galois group and the solvability of algebraic equations, Galois theory has elevated the study of mathematical equations to a new level and has become one of the cornerstones of modern algebra.



complex variables

Complex Variable is a branch of mathematics that studies complex functions and their properties. Complex functions consist of real and imaginary parts and have many unique properties, such as analyticity and conjugation.

Representation of plural numbers

pluralzIt can be expressed as:

z = x + yi

Polar form of complex numbers

Complex numbers can also be expressed in polar form:

z = r(cosθ + i sinθ) = re

complex function

complex functionf(z)is the pluralzA function that maps to another complex number can be written as:

f(z) = u(x, y) + iv(x, y)

analytical

When the complex functionf(z)When it is differentiable within a certain point and its neighborhood, it is called an "analytic function". The analytical function satisfies the Cauchy-Riemann equation:

∂u/∂x = ∂v/∂yand∂u/∂y = -∂v/∂x

Common complex functions

Complex variables and their functions are widely used in the fields of mathematical physics, electrical engineering, and power systems. Their unique analytical properties make them an important research object.



complex conjugate

What is complex conjugate?

In the plural,complex conjugate(Complex Conjugation) is an operation that changes the sign of the imaginary part of a complex number. For example, for a complex numberz = a + bi, its complex conjugate is expressed asz̅ = a - bi,inais the real part,bIs the imaginary part.

Properties of complex conjugation

Applications of complex conjugation

example

Assume pluralz = 3 + 4i, then its complex conjugate isz̅ = 3 - 4i. Its module length is |z| = √(3² + 4²) = 5.



complex plane

definition

Complex Plane, also known as Argand Diagram, is a plane coordinate system used to represent complex numbers. The horizontal axis represents the real part, and the vertical axis represents the imaginary part.

plural form

Plural numbers are usually expressed asz = a + bi,in:

Polar coordinate representation

Complex numbers can also be expressed in polar coordinates as:

z = r(cosθ + i sinθ) = re

in:

Basic arithmetic geometry meaning

example

likez = 3 + 4i,but:

This point would fall in the first quadrant in the complex plane, 5 units from the origin.



Steepest descent method in the field of complex numbers

Method overview

Method of Steepest Descent is a numerical method used to solve complex integral problems, especially when oscillating functions or rapidly changing functions are involved. This method approximates the integral value by finding the fastest descent path on the complex plane.

Basic principles

The core concept of the steepest descent method is to use the Stationary Phase Method to calculate the integral along a path on the complex plane. When choosing this path, the following conditions need to be met:

Step instructions

Here are the steps to use the steepest descent method:

  1. For the integral functionf(z)Analyze and find the saddle point of the function, that is, satisfyf'(z) = 0point.
  2. Near the saddle point, choose an appropriate descent path such thatRe(f(z))Decline rapidly.
  3. The integral is converted into a parameterized form along the descending path for calculation.
  4. Use approximation methods to solve the transformed integral.

Application areas

The steepest descent method is widely used in physics and engineering, especially in quantum mechanics and statistical physics, to solve problems such as:

Advantages and limitations

The main advantage of the steepest descent method is that it can effectively handle oscillatory and rapidly changing integration problems. However, its applicability depends on the properties of the integral function and requires a deep understanding of complex functions and saddle point theory.



complex variable analysis

Complex analysis is a discipline in mathematics that studies complex functions and their properties. It involves concepts such as analytic functions, conjugate functions, and complex integrals, and has wide applications in physics, engineering, and applied mathematics.

Basic concepts

analytic function

Analytical functions are complex functions that have derivatives and are continuous on the complex plane. analytic functionf(z)Satisfies the Cauchy-Riemann equation:

∂u/∂x = ∂v/∂yand∂u/∂y = -∂v/∂x

inuandvrespectivelyf(z)The real and imaginary parts of .

complex integral

Complex integration is the process of integrating analytic functions over the domain of complex numbers. Commonly used formulas include:

Residue theorem

Residue theorem is an important tool for complex integral calculation, especially suitable for calculating the integral of analytic functions with singular points. For a person inz_0Functions with isolated singularitiesf(z), which surroundsz_0The closed-circuit integral of is:

∮ f(z) dz = 2πi * Res(f, z_0)

inRes(f, z_0)forf(z)existz_0remainder.

application

Complex variable analysis has important applications in many fields, such as:

Complex variable analysis not only provides a rich mathematical theoretical foundation, but also plays an important role in science and engineering.



complex integral

Complex Integrals refers to the calculation of integrals of complex-valued functions on the complex plane. Complex integrals are very important in the analysis of complex variables and are used to solve many problems in physics, engineering and mathematics. The calculation of complex integrals involves integration on complex curves and the properties of complex functions.

1. Basic form of complex integrals

The basic form of a complex integral is along a curveCintegral functionf(z),Right now:

C f(z) dz
        

in,z = x + iyis a plural number,xandyis a real number,f(z)Usually an analytic function defined on the complex plane.

2. Cauchy's Integral Theorem

Cauchy's integral theorem is an important theorem in complex integrals. It states that iff(z)in closed curveCAnalysis within the enclosed region, then the integral along this closed curve is zero:

C f(z) dz = 0
        

This theorem reveals the properties of closed-path integration of analytic functions in the complex plane and becomes the basis for subsequent integration techniques.

3. Cauchy's Integral Formula

Cauchy's integral formula further illustrates the integral properties of analytic functions. likef(z)is resolved within the region, andais a point in the area, then:

f(a) = (1 / 2πi) ∫C f(z) / (z - a) dz
        

This formula not only shows that the analytic function at the pointaThe value of can be expressed as an integral, and it also provides a powerful tool for calculating complex integrals.

4. Residue Theorem

The residue theorem is a powerful computational method for evaluating complex integrals. likef(z)in closed curveCanalysis within the enclosed area, and there are only a finite number of isolated singular points in this areaz1, z2, ..., zn,but:

C f(z) dz = 2πi Σ Res(f, zk)
        

in,Res(f, zk)expressf(z)existzkThe remainder at. The residue theorem is a powerful method for evaluating complex integrals, especially whenf(z)When it contains extreme points.

5. Application of complex integrals
6. Calculation examples
#Python example: Use SymPy to calculate simple complex integrals
from sympy import symbols, integrate, I

# Define variables
z = symbols('z')
f = 1 / (z - 1)

# Calculate points
result = integrate(f, (z, 1 + I, 1 - I))
print("∫(1 / (z - 1)) dz =", result)

This example shows how to use the Python SymPy library to compute complex integrals.

In summary, complex integrals play an important role in physics, engineering, and mathematical analysis, providing a powerful method for describing and solving problems in the domain of complex numbers.



probability statistics

standard deviation

definition

Standard Deviation (SD) is an indicator used in statistics to measure the distance of data distribution from the mean. The larger the value, the more dispersed the data distribution is; the smaller the value, the more concentrated the data is.

formula

For a set of datax1, x2, ..., xn, its standard deviation formula is as follows:

Parent standard deviation (σ):

σ = sqrt(Σ (xi - μ)² / N)

Sample standard deviation (s):

s = sqrt(Σ (xi - x̄)² / (n - 1))

Calculation steps

  1. Calculate the mean (μ or x̄).
  2. Calculate the difference between each data point and the mean and square it.
  3. Find the sum of these squared values.
  4. Divide by the total number of data (N) or (n - 1) (for the sample standard deviation).
  5. Take the square root of the result.

application



game theory

Game Theory Theory) is a mathematical theory that studies how to make optimal decisions in a decision-making environment, especially when the decisions of all parties affect each other. Game theory is widely used in economics, political science, sociology, psychology and other fields. The main purpose is to understand how individuals or groups choose the most advantageous strategies in competitive and cooperative situations.

Basic concepts of game theory

Main types of game theory

There are many different types of games in game theory. According to the game structure and the information of the participants, games can be divided into the following categories:

Nash Equilibrium

Nash equilibrium is an important concept in game theory. It is formed when each player chooses the most advantageous strategy and no one is willing to change his strategy. This means that in a Nash equilibrium, each player's decision is the best choice.

For example, the typical "Prisoner's Dilemma" problem is a Nash equilibrium case in game theory. In this game, even if cooperation can maximize the overall benefits of both parties, due to incomplete information, both parties choose the strategy that is most beneficial to themselves, thus reaching a Nash equilibrium.

Applications of Game Theory

in conclusion

Game theory reveals the behavioral characteristics of people in competitive and cooperative environments by studying the interactions between different decision makers. It helps us understand how to make the best decisions in various situations, and has a profound impact on modern economics, social sciences, psychology and other fields.



probability distribution

Probability distribution (probability distribution) is a mathematical function used to describe the possible value range of a random variable and its probability. Random variables can be discrete or continuous, and probability distributions can be divided into discrete probability distributions and continuous probability distributions based on the properties of random variables.

1. Discrete probability distribution

Discrete probability distributions apply to discrete random variables that have a finite or countably infinite range of values. Common discrete probability distributions are:

2. Continuous probability distribution

Continuous probability distributions are suitable for continuous random variables whose range of values ​​is continuous. Common continuous probability distributions include:

3. Probability Mass Function (PMF) and Probability Density Function (PDF)
4. Common probability distribution examples
#Python example: Generate normally distributed data and draw graphics
import numpy as np
import matplotlib.pyplot as plt

# Generate 1000 data points consistent with normal distribution
data = np.random.normal(loc=0, scale=1, size=1000)

# Draw histogram
plt.hist(data, bins=30, density=True, alpha=0.6, color='b')

# PDF of normal distribution
xmin, xmax = plt.xlim()
x = np.linspace(xmin, xmax, 100)
p = np.exp(-((x)**2) / 2) / np.sqrt(2 * np.pi)
plt.plot(x, p, 'k', linewidth=2)
plt.title("Normally distributed data points and PDF")
plt.show()

This example shows how to use Python to generate normally distributed data and plot its histogram and theoretical density function to help understand the shape and characteristics of the data distribution.

5. Application of probability distribution

Probability distribution is a basic concept in statistics and data analysis. It helps us understand the behavior and characteristics of random phenomena and is widely used in various fields.



Generate and graph normally distributed data using HTML5

This example shows how to use JavaScript to generate normally distributed data and plot it via HTML5's Canvas.

<canvas id="chart" width="800" height="400"></canvas>

<script>
    // Generate normally distributed data
    function generateNormalData(mean, stdDev, count) {
        const data = [];
        for (let i = 0; i < count; i++) {
            data.push(mean + stdDev * Math.sqrt(-2 * Math.log(Math.random())) * Math.cos(2 * Math.PI * Math.random()));
        }
        return data;
    }

    //Set chart parameters
    const mean = 0;
    const stdDev = 1;
    const data = generateNormalData(mean, stdDev, 1000);
    const canvas = document.getElementById('chart');
    const ctx = canvas.getContext('2d');
    
    // draw histogram
    function drawHistogram(data, bins, color) {
        const width = canvas.width;
        const height = canvas.height;
        const max = Math.max(...data);
        const min = Math.min(...data);
        const binWidth = (max - min) / bins;

        //Initialize each interval
        const histogram = Array(bins).fill(0);
        data.forEach(value => {
            const bin = Math.min(Math.floor((value - min) / binWidth), bins - 1);
            histogram[bin]++;
        });

        // Draw a rectangle for each interval
        const maxCount = Math.max(...histogram);
        const barWidth = width / bins;
        histogram.forEach((count, index) => {
            const barHeight = (count / maxCount) * height;
            ctx.fillStyle = color;
            ctx.fillRect(index * barWidth, height - barHeight, barWidth - 1, barHeight);
        });
    }

    drawHistogram(data, 50, '#336699');
</script>


Standard deviation and normal distribution

Standard deviation range in normal distribution

In the normal distribution (Normal Distribution), the probability of data falling within different standard deviation ranges is as follows:

application



Boisson distribution

Poisson Distribution is a discrete probability distribution that describes the number of occurrences of an event within a fixed time or space range. This allocation is particularly suitable for independent and randomly occurring events, such as the number of customer arrivals per minute, the number of requests to the computer server, etc.

1. Characteristics of Boisson distribution
2. Probability Mass Function (PMF) of Boisson Allocation

The probability mass function (PMF) of the Boisson allocation can be expressed as:

P(X = k) = (λ^k * e^(-λ)) / k!
        

in:

This function describes the occurrence of events within a fixed time or spacekprobability.

3. Example of Boisson allocation

For example, if a coffee shop has an average of 3 customers entering the store every minute, that isλ = 3, then the probability of exactly 5 customers entering the store at a certain minute is:

P(X = 5) = (3^5 * e^(-3)) / 5! ≈ 0.1
        
4. Application scope of Boisson distribution
5. Generate Boisson allocation example using Python
# Generate Boisson allocation using Python
import numpy as np
import matplotlib.pyplot as plt

# Set the average occurrence rate λ
λ = 3
# Generate data consistent with Boisson distribution
data = np.random.poisson(λ, 1000)

# Draw histogram
plt.hist(data, bins=range(0, 15), density=True, alpha=0.7, color="blue", edgecolor="black")
plt.title("Boisson distribution histogram (λ=3)")
plt.xlabel("Number of event occurrences")
plt.ylabel("probability")
plt.show()

This example shows how to generate Boisson allocation data and plot a histogram to visualize the distribution of event occurrences.

Boisson allocation is a powerful tool for describing the number of occurrences of random events and is suitable for a variety of applications in statistics, engineering, natural sciences, and more.



hypergeometric distribution

definition

Hypergeometric allocation is a discrete probability distribution that describes the distribution of the number of successes when drawing samples from a finite set without replacement. Suppose there is a collection containing two types of objects, where:

randomly selected fromnobjects, the number of times the first type of object was successfully extractedXSubject to hypergeometric distribution.

probability mass function

The probability mass function of hypergeometric distribution is:

    P(X = k) = [C(K, k) * C(N - K, n - k)] / C(N, n)

in:

Expected value and variation

The expected value and variation of hypergeometric distribution are:

application

Hypergeometric allocation is widely used in the following fields:



Variation analysis

Analysis of Variance (ANOVA) is a statistical method used to test whether there are significant differences in the means between multiple sets of data. ANOVA is often used to determine whether the effects of different treatments or groups on results are significant, such as comparing the effects of different drugs on treatment effects.

1. One-Way ANOVA

Single-factor variation analysis is suitable for testing the impact of a single factor on multiple sets of data. Assume that the number of samples in each group isn, the total number of groups isk, then the following statistics can be calculated.

2. Formula for variation analysis
SST = ΣΣ(yij - ȳ)2
        

in,yijIndicates the firstiGroup No.jdata points,ȳis the overall average of all data.

SSB = Σnii - ȳ)2
        

in,ȳifor the firstigroup mean,niis the number of samples in the group.

SSW = ΣΣ(yij - ȳi)2
        

in,ȳiis the average of each group.

3. Degrees of freedom and mean square

In ANOVA, each amount of variation has a corresponding degree of freedom:

Then calculate the Mean Square (MS):

4. F test

Finally, the F test was used to compare between-group variation and within-group variation to determine whether the difference between groups was significant. The F-value calculation formula is:

F = MSB / MSW
        

The larger the F value, the more significant the difference between groups. By looking up a table or using statistical software to compare the F value and the critical value, you can determine whether to reject the null hypothesis.

5. ANOVA usage examples

For example, we tested the effects of different fertilizers on plant growth height. The sample heights corresponding to the three groups of fertilizers are as follows:

By calculating SST, SSB, SSW, and then calculating the F value to determine whether there is a significant difference in the effects of different fertilizers.

Variation analysis is a commonly used statistical method, especially suitable for comparing the effects of multiple sets of data, and has been widely used in scientific research, engineering and other fields.



numerical analysis

Basic concepts

Numerical analysis is a discipline that uses numerical methods to solve mathematical problems and uses approximate calculations to deal with problems that cannot be solved with analytical methods. Its core is to seek efficient, stable and accurate calculation methods.

Main areas

Application scope

Advantages and Challenges

Common methods

learning resources

It is recommended to learn the basics of mathematical analysis and linear algebra, and practice using tools such as Python and MATLAB. Recommended reference books include "Numerical Analysis: Theory and Practice" and "Applied Numerical Methods".



finite element method

Basic concepts

Finite Element Method (FEM) is a numerical analysis method that is widely used in engineering and physical sciences to solve stress, heat conduction, fluid mechanics and other problems of complex structures.

Working principle

The finite element method divides a continuum into many small finite elements, establishes an approximate mathematical model within each element, and finally merges these models to solve the entire problem.

Application areas

Advantages and limitations

software tools

Study suggestions

It is recommended to start learning from basic mechanics and mathematics, gradually master the theory and practice of the finite element method, and use relevant software to practice operations.



convolution

Convolution is a mathematical operation widely used in signal processing, image processing and deep learning. The main function of convolution is to apply a function called "kernel" or "filter" to process data and extract features.

1. Mathematical definition of convolution

For one-dimensional discrete convolution operation, its mathematical definition is as follows:

(f * g)(t) = Σi=-∞ f(i) ⋅ g(t - i)

in:

In image processing, convolution is a similar operation, but applied to two-dimensional data (i.e., each pixel of the image).

2. Application of convolution
3. Operation steps of convolution in CNN
  1. Select filter:Select a size ofk x kfilter, for example3 x 3
  2. Slide operation: Apply the filter starting from the upper left corner of the image to each position in sequence.
  3. weighted sum: The pixel value at the corresponding position is multiplied and summed by the elements in the filter.
  4. Result storage: Store the convolution result of each position in a new matrix to form a "feature map".
  5. Repeat operation: Repeat the above steps until all areas of the image are convolved.
4. Examples of effects of different convolution kernels

Through various applications of convolution, data features can be effectively extracted and applied to a variety of data analysis and processing fields.



fuzzy theory

1. What is fuzzy theory?

Fuzzy Theory is a mathematical theory used to deal with "uncertainty" and "fuzziness" problems, and is mainly used in fuzzy sets and fuzzy logic. Different from traditional Boolean logic (Boolean Logic), fuzzy theory allows objects to have partial attributes, providing a range from 0 to 1 to describe the possibility of an event occurring.

2. Fuzzy sets and fuzzy logic

3. Application examples of fuzzy theory

The following is an example of a simple fuzzy logic system used to evaluate room temperature control.

Through fuzzy logic, the fan speed can be adjusted within the fuzzy range of temperature changes to make it more consistent with human judgment patterns.

4. Common application scenarios

5. Advantages and Disadvantages



discrete mathematics

Sets and set operations

Sets are the basis of discrete mathematics, and the elements can be numbers, symbols, or objects. Common operations include union, intersection, difference and complement.

logic and propositions

Logic is a tool used to analyze the truth value of propositions. Propositions can be true or false, and compound propositions can be formed through logical operations (such as AND, OR, NOT, and implication). A truth table can be used to analyze its logical structure.

Relationships and functions

Relationships are defined between pairs of elements on a set and have properties such as reflexivity, symmetry, and transitivity. Functions are special relationships where each input corresponds to a unique output.

Fundamentals of number theory

Includes properties of integers, such as prime numbers, greatest common factor, congruence, and modular operations. These concepts are widely used in cryptography and computational theory.

graph theory

Study the connection relationship between points (vertices) and edges. Common graph types include undirected graphs, directed graphs, weighted graphs, etc., and explore the connectivity and coloring issues of paths, loops, trees, and graphs.

Combinatorics

Study counting methods, such as permutation, combination, binomial theorem and inclusion-exclusion principle, to solve selection and allocation problems.

Bollinger algebra

An algebraic system based on Boolean values ​​(true/false) for digital circuit design and logic simplification. Contains operations such as AND, OR, NOT and their algebraic properties.

Automata and Formal Languages

The study of language production and recognition. Covers finite automata, regular languages, and context-free grammar, which are the basis of theoretical computer science.

Relational Databases and Discrete Structures

Discrete mathematics provides a theoretical basis for data structure and database design, especially in tree structures, graph structures and relational models.

Mathematical induction and recursion

Mathematical induction is a method used to prove propositions related to natural numbers. Recursion describes a function or program in a self-defined way and is often used with induction to prove correctness.

set theory

Basic concepts of collections

A set is a whole composed of different elements, often represented by braces, such as {1, 2, 3}. The elements are non-repeating and non-sequential, and the element relationship is represented by the symbol ∈, such as 2 ∈ {1, 2, 3}.

Representation method of collection

Sets can be represented enumeratively (e.g. {a, b, c}) or descriptively (e.g. {x | x is an even number and x < 10}).

Subsets and Complete Sets

A set A is a subset of a set B, denoted as A ⊆ B, if all elements of A are elements of B. The universe is the set containing all possible elements, usually denoted U.

Set operations

Cartesian product

The Cartesian product of the sets A and B is the set of all ordered pairs (a, b) where a ∈ A and b ∈ B. Denote it as A × B.

Power set

The power set of a set A is the set composed of all subsets of A, denoted as P(A). If A has n elements, then P(A) has 2ⁿ elements.

Set Identity Law and Algebraic Properties

Set operations satisfy properties such as associative law, commutative law, distributive law, double complement law, De Morgan's law, etc. These properties help simplify set expressions.

Infinite sets and cardinal numbers

Sets can be divided into finite and infinite sets. Infinite sets such as the set of natural numbers ℕ, the set of integers ℤ, and the set of real numbers ℝ. Different infinite sets may have different "sizes" and are compared using cardinality. For example, ℕ and ℤ are both countable, while ℝ is an uncountable infinite set.

Equivalence classes and divisions

Under the equivalence relationship, a set can be divided into disjoint equivalence classes, forming a partition of the set, and each element only belongs to one of the subsets.

Applications of set theory

Set theory is widely used in mathematics, logic, computer science and data structures, and is the basic language and tool in various fields of mathematics.

Bollinger algebra

Basic concepts

Bollinger algebra is an algebraic system based on binary logic with only two elements: 0 (false) and 1 (true). It is mainly used in logical reasoning and digital circuit design.

Basic operations

Common logical operators

Basic properties of Bollinger algebra

truth table

The truth table lists the logical operation results of all variable combinations and is an important tool for analyzing and simplifying the Boolean function.

logic gate

Boolean operations can be implemented in digital circuits using logic gates:

Boolean functions and simplification

The Bollinger function is composed of variables and logical operations. It can be simplified through algebraic simplification, Karnaugh Map or Quain-McCluskey rule to reduce the number of logic gates in the circuit.

Standard shape

The Boolean function can be expressed as:These two standard shapes are helpful in the design and implementation of logic circuits.

Applications of Bollinger Algebra

Bollinger algebra is widely used in:

graph theory

Basic concepts

Graph theory is a branch of mathematics that studies the relationships between objects. Graphs are composed of vertices and edges and are used to describe problems such as networks, paths, and structural relationships.

Type of graph

basic terminology

connectivity

Trees and Spanning Trees

Graph representation

Graph traversal

Classic graph theory algorithm

Graph coloring and coloring issues

Graph coloring is the process of painting vertices with different colors so that adjacent vertices have different colors. The minimum required color is called the chromatic number of the graph and is one of the NP-complete problems.

Graph theory applications



Combinatorics

Basic concepts

Combinatorics is a field of mathematics that studies "how to count". The core problems include the calculation of permutations, combinations, distributions and structures. It is widely used in fields such as probability, computer science and mathematical logic.

arrangement

Arrangement is the ordering of a set of elements, with differences in order. If r elements are selected from n different elements and arranged, the total number is:
P(n, r) = n × (n − 1) × ... × (n − r + 1) = n! / (n − r)!

combination

Combination is a selection regardless of order. The number of ways to select r elements from n different elements is:
C(n, r) = n! / (r! × (n − r)!)
Also written:ⁿCᵣor(n choose r)

Repeated arrangements and repeated combinations

Inclusion-exclusion principle

Used to calculate the total number of elements in the union of multiple sets, the formula is as follows:
|A ∪ B| = |A| + |B| − |A ∩ B|
The generalization to many sets also holds, which is used to avoid double counting.

binomial theorem

Describe the expanded form of (a + b)ⁿ:
(a + b)ⁿ = Σ C(n, k) × aⁿ⁻ᵏ × bᵏ, k = 0 to n
The coefficients C(n, k) correspond to Pascal's triangle.

recursive relationship

Many combinatorial problems can be solved recursively, such as the Fibonacci sequence:
F(n) = F(n−1) + F(n−2), the initial conditions are F(0)=0, F(1)=1.

Application skills of permutation and combination

generating function

Use algebraic methods to express the generation of sequence, which can be used to solve recursive and combinatorial problems. The basic form is:
G(x) = a₀ + a₁x + a₂x² + ...
Can be used to calculate item distribution, coin problems, etc.

Number of divisions

Integer division is a method of writing an integer as the sum of multiple positive integers. For example, the division of 4 is:
4, 3+1, 2+2, 2+1+1, 1+1+1+1, 5 types in total.

Applications of Combinatorics



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