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Differential equations with applications and historical notes, third

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Tiêu đề Differential Equations With Applications And Historical Notes
Tác giả George F. Simmons
Trường học CRC Press
Chuyên ngành Mathematics
Thể loại textbook
Năm xuất bản 2017
Thành phố Boca Raton
Định dạng
Số trang 763
Dung lượng 4,65 MB

Cấu trúc

  • 1. The Nature of Differential Equations. Separable Equations (20)
  • 2. First Order Equations (20)
  • 3. Second Order Linear Equations (20)
  • 4. Qualitative Properties of Solutions (20)
  • 5. Power Series Solutions and Special Functions (20)
  • 6. Fourier Series and Orthogonal Functions (20)
  • 7. Partial Differential Equations and Boundary Value Problems (20)
  • 8. Some Special Functions of Mathematical Physics (20)
  • 9. Laplace Transforms (20)
  • 10. Systems of First Order Equations (20)
  • 11. Nonlinear Equations (20)
  • 12. The Calculus of Variations (20)
  • 13. The Existence and Uniqueness of Solutions (0)
  • 14. Numerical Methods (20)

Nội dung

Second Order Linear Equations

10 Systems of first- order equations

Qualitative Properties of Solutions

6 Fourier series and orthogonal functions

7 Partial differential equations and boundary value problems

8 Some special functions of mathematical physics

Partial Differential Equations and Boundary Value Problems

10 Systems of first- order equations

6 Fourier series and orthogonal functions

7 Partial differential equations and boundary value problems

Some Special Functions of Mathematical Physics

5 Power series solutions and special functions

Laplace Transforms

1 The nature of differential equations, separable equations

Nonlinear Equations

6 Fourier series and orthogonal functions

7 Partial differential equations and boundary value problems

8 Some special functions of mathematical physics

5 Power series solutions and special functions

The Calculus of Variations

10 Systems of first- order equations

6 Fourier series and orthogonal functions

7 Partial differential equations and boundary value problems

8 Some special functions of mathematical physics

5 Power series solutions and special functions

Scientists are drawn to the study of nature not for its utility, but for the joy and beauty it brings This intrinsic beauty is essential; without it, the pursuit of knowledge would lose its significance, and life itself would lack meaning The beauty referenced here transcends mere sensory appeal; it is a deeper, profound beauty derived from the harmonious order within nature, which can be appreciated through pure intellect.

As a mathematical discipline travels far from its empirical source, or still more, if it is a second or third generation only indirectly inspired by ideas coming from

The increasing aestheticization of reality poses significant risks, particularly when the discipline lacks strong empirical connections or guidance from individuals with refined taste This trend may lead to a dilution of the subject, resulting in a fragmented array of trivial details rather than a cohesive field of study Consequently, when mathematical subjects stray far from their empirical roots or undergo excessive abstraction, they risk degeneration into a chaotic collection of complexities.

Mathematics thrives on the balance between generalization and attention to detail, where individual problems should not merely serve as illustrations of broader theories General theories arise from specific considerations and lose their significance without clarifying particular instances The dynamic relationship between generality and individuality, along with deduction and imagination, defines the essence of mathematics Typically, mathematical development begins with concrete examples, progresses through abstraction, and culminates in practical applications that ground the abstract concepts in reality Thus, the journey into abstract generality must always begin and end with the concrete and specific.

George Simmons has academic degrees from the California Institute of

In 1962, he joined the faculty of Colorado College as a Professor of Mathematics after teaching at various colleges and universities He has also authored significant works in the field of technology, contributing to the academic community alongside prestigious institutions like the University of Chicago and Yale University.

Introduction to Topology and Modern Analysis (McGraw-Hill, 1963), Precalculus Mathematics in a Nutshell (Janson Publications, 1981), and Calculus with Analytic Geometry (McGraw-Hill, 1985).

When not engaged in professional activities, Professor Simmons enjoys traveling across Western and Southern Europe, Turkey, Israel, Egypt, Russia, China, and Southeast Asia He also finds time for trout fishing in the Rocky Mountain states, playing pocket billiards, and indulging in a diverse range of reading, including literature, history, biography, science, and thrillers that provide enjoyment without guilt.

A differential equation is defined as an equation that includes one dependent variable and its derivatives concerning one or more independent variables This mathematical framework is essential for expressing many fundamental laws of nature across various disciplines, including physics, chemistry, biology, and astronomy Additionally, differential equations play a crucial role in mathematics, particularly in geometry, and are widely applied in engineering, economics, and numerous fields of applied science.

Differential equations are widely utilized due to their ability to represent the relationship between variables and their rates of change When a function y = f(x) is considered, its derivative dy/dx signifies how y changes in relation to x In natural processes, the interconnectedness of variables and their rates of change is dictated by fundamental scientific principles, which can be mathematically expressed as differential equations.

Newton's second law of motion states that the acceleration (a) of an object is directly proportional to the total force (F) applied to it and inversely proportional to its mass (m) This relationship can be expressed mathematically as a = F/m or equivalently, ma = F.

When a body of mass m falls freely under the influence of gravity, the only force acting on it is mg, where g represents the acceleration due to gravity If we define y as the distance from a fixed height to the body, its velocity v can be expressed as the rate of change of position (dy/dt), while its acceleration a is the rate of change of velocity (dv/dt or d²y/dt²) This relationship allows us to derive the fundamental equations of motion for freely falling objects.

On the surface of the Earth, the acceleration due to gravity is approximately 9.81 meters per second squared, or 32 feet per second squared, and can be considered constant for most practical applications This relationship can be expressed mathematically as \( \frac{d^2y}{dt^2} = g \), where \( g \) represents the acceleration due to gravity.

When considering the scenario where air resistance is proportional to velocity, the total force acting on the body can be expressed as mg - k(dy/dt) This modifies the original equation to md(dy/dt) = mg - k(dy/dt).

Equations (2) and (3) are the differential equations that express the essential attributes of the physical processes under consideration.

As further examples of differential equations, we list the following: dy dt =–ky; (4) md y dt 2 2 =–ky; (5) dy dx+2xy e= – x 2 ; (6) d y dx dy dx y

(1-x 2 )d y 2 2 -2 + ( +1) =0 dx xdy dx p p y ; (8) x d y dx xdy dx x p y

In the context of differential equations, the dependent variable is represented by y, while the independent variables are either t or x, with constants denoted by k, m, and p An ordinary differential equation features a single independent variable, ensuring that all derivatives are ordinary derivatives The order of a differential equation is determined by the highest derivative present; for instance, equations (4) and (6) are classified as first order, whereas the others are second order Notably, equations (8) and (9) are recognized as classical equations, specifically Legendre’s equation and Bessel’s equation, both of which have extensive literature and a rich historical background spanning centuries A detailed study of these equations will be conducted later.

A partial differential equation (PDE) involves multiple independent variables, utilizing partial derivatives in its formulation For instance, if w = f(x,y,z,t) represents a function dependent on time and three spatial coordinates, it can be expressed through second-order partial differential equations.

Laplace's equation, the heat equation, and the wave equation are classical equations of great significance in theoretical physics, driving the advancement of important mathematical concepts Partial differential equations commonly appear in the study of continuous media, addressing issues related to electric fields, fluid dynamics, diffusion, and wave motion Their theory is notably distinct and more complex than that of ordinary differential equations For the foreseeable future, our focus will remain solely on ordinary differential equations.

J B S Haldane, the English biologist, emphasized the importance of simplicity in scientific theories, stating that we should adopt the simplest theory that can explain all relevant facts and predict new ones He noted that the term "simplest" is subjective, akin to aesthetic judgments in art and poetry, highlighting the nuanced nature of scientific reasoning.

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