標(biāo)題: Titlebook: Generalized Functions Theory and Technique; Theory and Technique Ram P. Kanwal Book 19982nd edition Birkh?user Boston 1998 Boundary value p [打印本頁] 作者: Novice 時(shí)間: 2025-3-21 16:33
書目名稱Generalized Functions Theory and Technique影響因子(影響力)
書目名稱Generalized Functions Theory and Technique影響因子(影響力)學(xué)科排名
書目名稱Generalized Functions Theory and Technique網(wǎng)絡(luò)公開度
書目名稱Generalized Functions Theory and Technique網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Generalized Functions Theory and Technique被引頻次
書目名稱Generalized Functions Theory and Technique被引頻次學(xué)科排名
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書目名稱Generalized Functions Theory and Technique年度引用學(xué)科排名
書目名稱Generalized Functions Theory and Technique讀者反饋
書目名稱Generalized Functions Theory and Technique讀者反饋學(xué)科排名
作者: Valves 時(shí)間: 2025-3-21 23:08 作者: 館長 時(shí)間: 2025-3-22 02:09 作者: 細(xì)微的差異 時(shí)間: 2025-3-22 07:23
Distributions Defined by Divergent Integrals,alue of the singular integral defined by the quantity .. The aim of this chapter is to extend this idea and to regularize various singular integrals and thereby define the coresponding distributions. Let us start with a simple example.作者: 宮殿般 時(shí)間: 2025-3-22 09:43
Distributional Derivatives of Functions with Jump Discontinuities,er derivatives have jumps across .. Classical theory is based on solving such problems on both sides of the boundaries and then attempting to satisfy the boundary conditions or jump conditions across ., as the case may be. There are many problems, however, that cannot be solved by classical techniques.作者: 彈藥 時(shí)間: 2025-3-22 15:11
nce the publication of the first edition, there has been tremendous growth in the subject and I have attempted to incorporate some of these new concepts. Accordingly, almost all the chapters have been revised. The bibliography has been enlarged considerably. Some of the material has been reorganized作者: 彈藥 時(shí)間: 2025-3-22 17:54 作者: HARP 時(shí)間: 2025-3-22 22:42
Congenital Malformations of the Neck,er .; then we define . and . where . = ?/?., . = 1, 2,..., .. For the one-dimensional case . reduces to .. Furthermore, if any component of . is zero, the differentiation with respect to the corresponding variable is omitted. For instance, in ., with . = (3, 0, 4), we have 作者: Incumbent 時(shí)間: 2025-3-23 04:30
https://doi.org/10.1007/978-3-031-59031-3alue of the singular integral defined by the quantity .. The aim of this chapter is to extend this idea and to regularize various singular integrals and thereby define the coresponding distributions. Let us start with a simple example.作者: 油氈 時(shí)間: 2025-3-23 06:00
Special technique in the Poland syndrome,er derivatives have jumps across .. Classical theory is based on solving such problems on both sides of the boundaries and then attempting to satisfy the boundary conditions or jump conditions across ., as the case may be. There are many problems, however, that cannot be solved by classical techniques.作者: Anthology 時(shí)間: 2025-3-23 11:16 作者: 期滿 時(shí)間: 2025-3-23 15:24
https://doi.org/10.1007/978-3-319-44577-9mptotic evaluation of divergent integrals, boundary layer theory and singular perturbations. Our aim in this chapter is to present the basic concepts of their methods and illustrate them with representative examples.作者: FEAT 時(shí)間: 2025-3-23 20:19 作者: 無政府主義者 時(shí)間: 2025-3-23 23:50 作者: Albumin 時(shí)間: 2025-3-24 04:49 作者: lethargy 時(shí)間: 2025-3-24 10:19 作者: entitle 時(shí)間: 2025-3-24 14:44
Congenital Pseudarthrosis of the Clavicleproduct of the distributions .(.) ∈ .′. and .(.) ∈ .′. according to (1),.and check whether the right side of this equation defines a linear continuous functional over .. For this purpose, we prove the following lemma:.(.) = <.(.), .(.)>, . ∈ .′.(.) ∈ ., ., . (., .,..., .) . {.(.)} → .(.) . → ∞, .(.) = {<.(.), .(.)>} → .(.) . → ∞.作者: 展覽 時(shí)間: 2025-3-24 17:42
Direct Products and Convolutions of Distributions,product of the distributions .(.) ∈ .′. and .(.) ∈ .′. according to (1),.and check whether the right side of this equation defines a linear continuous functional over .. For this purpose, we prove the following lemma:.(.) = <.(.), .(.)>, . ∈ .′.(.) ∈ ., ., . (., .,..., .) . {.(.)} → .(.) . → ∞, .(.) = {<.(.), .(.)>} → .(.) . → ∞.作者: Institution 時(shí)間: 2025-3-24 19:54
Applications to Wave Propagation,ul method of attacking these problems is to embed them in the whole space. This is achieved by extending the solution to the other side of the surface in some suitable fashion, as we did in deriving the Poisson integral formula in Chapter 10. We then obtain a regular singular function that satisfies作者: linguistics 時(shí)間: 2025-3-25 01:14
https://doi.org/10.1007/978-1-4613-8315-4ul method of attacking these problems is to embed them in the whole space. This is achieved by extending the solution to the other side of the surface in some suitable fashion, as we did in deriving the Poisson integral formula in Chapter 10. We then obtain a regular singular function that satisfies作者: surmount 時(shí)間: 2025-3-25 07:13 作者: 障礙 時(shí)間: 2025-3-25 07:33 作者: Asparagus 時(shí)間: 2025-3-25 13:56 作者: Felicitous 時(shí)間: 2025-3-25 18:49
The Schwartz-Sobolev Theory of Distributions,tance ., of . from the origin, is . = |.| = (. + . + ... + .).. Let . be an .-tuple of nonnegative integers, . = (., .,..., .), the so-called . of order .; then we define . and . where . = ?/?., . = 1, 2,..., .. For the one-dimensional case . reduces to .. Furthermore, if any component of . is zero作者: incredulity 時(shí)間: 2025-3-25 21:02 作者: Affiliation 時(shí)間: 2025-3-26 01:58 作者: landmark 時(shí)間: 2025-3-26 04:42 作者: COLON 時(shí)間: 2025-3-26 08:41
Direct Products and Convolutions of Distributions,spectively. Then a point in the Cartesian product . = . × . is (.) = (.,..., ., .,..., .). Furthermore, let us denote by ., ., and .the spaces of test functions with compact support in ., ., and ., respectively. When . (.) and .(.) are locally integrable functions in the spaces . and ., then the fun作者: lacrimal-gland 時(shí)間: 2025-3-26 16:03
The Laplace Transform,is variable in this chapter. Let .(.) be a complex-valued function of the real variable . such that .(.). is abolutely integrable over 0 < . < ∞, where . is a real number. Then the Laplace transform of .(.), . ≥ 0, is defined as . where . = . + .. The Laplace transform defined by (1) has the followi作者: 變白 時(shí)間: 2025-3-26 19:28 作者: 難管 時(shí)間: 2025-3-26 22:33
Applications to Wave Propagation,undamental solutions and studied moving point, line, and surface sources. In Chapter 5 we considered various kinematic and geometrical aspects of the wave propagation in the context of surface distributions. In this chapter we consider some applications of these results and study partial differentia作者: 花束 時(shí)間: 2025-3-27 04:21
Interplay Between Generalized Functions and the Theory of Moments,the generalized functions and the theory of moments. Thus, they have not only succeeded in presenting a simplified approach to various known aspects of asymptotics but have also found many new results. They have applied their technique to many different branches of asymptotic expansions, such as asy作者: insert 時(shí)間: 2025-3-27 08:50 作者: CARK 時(shí)間: 2025-3-27 13:16 作者: 放大 時(shí)間: 2025-3-27 16:02 作者: 無目標(biāo) 時(shí)間: 2025-3-27 18:23 作者: Amnesty 時(shí)間: 2025-3-27 22:06 作者: 銼屑 時(shí)間: 2025-3-28 03:40 作者: absolve 時(shí)間: 2025-3-28 09:41
Special technique in the Poland syndrome,side or outside some surface . if the surface is closed, and on both sides of it if it is open. However, these functions or their first- or higher-order derivatives have jumps across .. Classical theory is based on solving such problems on both sides of the boundaries and then attempting to satisfy 作者: Evocative 時(shí)間: 2025-3-28 13:03 作者: Agnosia 時(shí)間: 2025-3-28 18:17
Left Ventricular Outflow Obstructive Lesionsis variable in this chapter. Let .(.) be a complex-valued function of the real variable . such that .(.). is abolutely integrable over 0 < . < ∞, where . is a real number. Then the Laplace transform of .(.), . ≥ 0, is defined as . where . = . + .. The Laplace transform defined by (1) has the followi作者: nephritis 時(shí)間: 2025-3-28 20:59 作者: insurgent 時(shí)間: 2025-3-29 01:53
https://doi.org/10.1007/978-1-4613-8315-4undamental solutions and studied moving point, line, and surface sources. In Chapter 5 we considered various kinematic and geometrical aspects of the wave propagation in the context of surface distributions. In this chapter we consider some applications of these results and study partial differentia作者: aptitude 時(shí)間: 2025-3-29 06:59 作者: BLANC 時(shí)間: 2025-3-29 11:02 作者: 裂隙 時(shí)間: 2025-3-29 12:38
Jamie Stanhiser M.D.,Marjan Attaran M.D.on to certain curvilinear coordinates. For this purpose we devote an entire section to this topic. Let us first study the meaning of the function .[. (.)] and prove the result . where . runs through the simple zeros of . (.).作者: 繁重 時(shí)間: 2025-3-29 18:00
Left Ventricular Outflow Obstructive Lesionsis variable in this chapter. Let .(.) be a complex-valued function of the real variable . such that .(.). is abolutely integrable over 0 < . < ∞, where . is a real number. Then the Laplace transform of .(.), . ≥ 0, is defined as . where . = . + .. The Laplace transform defined by (1) has the following basic properties.作者: FLIRT 時(shí)間: 2025-3-29 21:52
Additional Properties of Distributions,on to certain curvilinear coordinates. For this purpose we devote an entire section to this topic. Let us first study the meaning of the function .[. (.)] and prove the result . where . runs through the simple zeros of . (.).作者: 發(fā)現(xiàn) 時(shí)間: 2025-3-30 01:07
The Laplace Transform,is variable in this chapter. Let .(.) be a complex-valued function of the real variable . such that .(.). is abolutely integrable over 0 < . < ∞, where . is a real number. Then the Laplace transform of .(.), . ≥ 0, is defined as . where . = . + .. The Laplace transform defined by (1) has the following basic properties.作者: arabesque 時(shí)間: 2025-3-30 07:15
Congenital Vascular MalformationsIn attempting to define the Fourier transform of a distribution . (.), we would like to use the formula (in .)作者: 審問 時(shí)間: 2025-3-30 10:35
Ravi Jhaveri MD,Yvonne Bryson MDIn Section 2.6 we defined the differential operator .,.and its formal adjoint .,.where the coefficients a.. are infinitely differentiable functions, . is a distribution, and . is a test function. These operators are related by the equation.This means that the action of . on φ is equivalent to the action of . on the test function . =.*..作者: gout109 時(shí)間: 2025-3-30 13:58 作者: 調(diào)整 時(shí)間: 2025-3-30 18:06 作者: Expostulate 時(shí)間: 2025-3-30 23:31
Tempered Distributions and the Fourier Transform,In attempting to define the Fourier transform of a distribution . (.), we would like to use the formula (in .)作者: 翅膀拍動 時(shí)間: 2025-3-31 02:36
Applications to Ordinary Differential Equations,In Section 2.6 we defined the differential operator .,.and its formal adjoint .,.where the coefficients a.. are infinitely differentiable functions, . is a distribution, and . is a test function. These operators are related by the equation.This means that the action of . on φ is equivalent to the action of . on the test function . =.*..作者: 天賦 時(shí)間: 2025-3-31 06:10
Applications to Partial Differential Equations,Recall from Chapter 2 that the differential operator . of order . in n independent variables ., .,...,.,is.where the coefficients . have partial derivatives of all orders. Its formal adjoint .* is defined as .Here . and . are functions having derivatives of order . in ..作者: 大炮 時(shí)間: 2025-3-31 12:31
Miscellaneous Topics,In order to present the applications of generalized functions to the theories of probability and random processes let us start with some basic concepts.
