標(biāo)題: Titlebook: An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases; Analysis, Algorithms Francis X. Giraldo Textbook 2020 The Editor [打印本頁] 作者: 正當(dāng)理由 時間: 2025-3-21 19:33
書目名稱An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases影響因子(影響力)
書目名稱An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases影響因子(影響力)學(xué)科排名
書目名稱An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases網(wǎng)絡(luò)公開度
書目名稱An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases被引頻次
書目名稱An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases被引頻次學(xué)科排名
書目名稱An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases年度引用
書目名稱An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases年度引用學(xué)科排名
書目名稱An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases讀者反饋
書目名稱An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases讀者反饋學(xué)科排名
作者: 通知 時間: 2025-3-21 21:49
Overview of Galerkin Methodsthe choices that we have at our disposal. We can categorize the possible methods as follows: .Generally speaking, the most widely used differential form method is the finite difference method while the most widely used integral form method is the Galerkin method (e.g., finite elements).作者: ERUPT 時間: 2025-3-22 01:13 作者: 單調(diào)女 時間: 2025-3-22 04:39 作者: bisphosphonate 時間: 2025-3-22 09:04 作者: 填滿 時間: 2025-3-22 16:00 作者: overshadow 時間: 2025-3-22 20:20
1D Continuous Galerkin Methods for Elliptic Equationsonservation laws for both CG and DG. However, these types of equations are entirely hyperbolic (first order equations in these cases). In this chapter we learn how to use the CG method to discretize second order equations that are elliptic.作者: MEAN 時間: 2025-3-23 00:49
1D Discontinuous Galerkin Methods for Elliptic Equationsw how to compute first derivatives. A judicious use of Green’s first identity then permits a simple discretization of the Laplacian operator. We learn in this chapter that DG cannot use the same representation of the Laplacian operator. Rather, we need to revisit first order derivatives and construc作者: 脫毛 時間: 2025-3-23 05:18 作者: epicondylitis 時間: 2025-3-23 05:32 作者: Fraudulent 時間: 2025-3-23 10:24
2D Continuous Galerkin Methods for Elliptic Equations for the advection and diffusion equations, and by extension the advection-diffusion equation. In addition, in Ch. . we discussed the application of both methods for systems of nonlinear equations in one dimension. In this chapter we now extend the ideas that we have learned so far in one dimension 作者: finite 時間: 2025-3-23 17:09 作者: 磨碎 時間: 2025-3-23 20:31 作者: Postulate 時間: 2025-3-24 00:18 作者: 萬神殿 時間: 2025-3-24 04:40 作者: 極少 時間: 2025-3-24 08:42 作者: obviate 時間: 2025-3-24 13:35 作者: 過份艷麗 時間: 2025-3-24 15:03
,Zehn Regeln für das Risk Assessment,Interpolation is the act of approximating a function .(.) by an .th degree interpolant .. such that . where .. are .?=?0, ..., . specific points where the function is evaluated.作者: Tortuous 時間: 2025-3-24 19:34 作者: 閃光東本 時間: 2025-3-24 23:53 作者: 代理人 時間: 2025-3-25 05:13
978-3-030-55071-4The Editor(s) (if applicable) and The Author(s), under exclusive license to Springer Nature Switzerl作者: 上下倒置 時間: 2025-3-25 09:32
Overview of Galerkin Methodsthe choices that we have at our disposal. We can categorize the possible methods as follows: .Generally speaking, the most widely used differential form method is the finite difference method while the most widely used integral form method is the Galerkin method (e.g., finite elements).作者: incontinence 時間: 2025-3-25 12:26
Numerical Integration in One Dimensionus . and . are element and trace integrals, respectively. By element integrals we mean either area or volume integrals in 2D and 3D, respectively. By trace integrals we mean integrals along the boundary of the element which could be line or surface area integrals in 2D and 3D, respectively.作者: 幸福愉悅感 時間: 2025-3-25 19:28
1D Continuous Galerkin Methods for Elliptic Equationsonservation laws for both CG and DG. However, these types of equations are entirely hyperbolic (first order equations in these cases). In this chapter we learn how to use the CG method to discretize second order equations that are elliptic.作者: 制定法律 時間: 2025-3-25 21:26
Interpolation in Multiple Dimensionso and three dimensions. In one dimension, there is no room to choose the shape of the domain. That is, in the domain .?∈?[?1, +1] we are constrained to line elements. However, in two dimensions this door is flung wide open and we are now free to choose all sorts of polygons as the basic building blocks of our interpolation.作者: 脾氣暴躁的人 時間: 2025-3-26 04:01
2D Continuous Galerkin Methods for Hyperbolic Equationsly. In Ch. . we introduced the extension of the CG method to two dimensions by describing its implementation for elliptic partial differential equations (PDEs). In this chapter we extend the CG method for the application of hyperbolic equations in two dimensions. We also discuss the addition of diffusion operators.作者: Abominate 時間: 2025-3-26 08:24 作者: Hamper 時間: 2025-3-26 10:05 作者: champaign 時間: 2025-3-26 15:22 作者: 沒花的是打擾 時間: 2025-3-26 18:57 作者: 紀(jì)念 時間: 2025-3-26 21:11 作者: 生存環(huán)境 時間: 2025-3-27 03:53 作者: cogitate 時間: 2025-3-27 09:19
https://doi.org/10.1007/978-3-322-87118-3onservation laws for both CG and DG. However, these types of equations are entirely hyperbolic (first order equations in these cases). In this chapter we learn how to use the CG method to discretize second order equations that are elliptic.作者: photophobia 時間: 2025-3-27 09:51
https://doi.org/10.1007/978-3-663-08415-0w how to compute first derivatives. A judicious use of Green’s first identity then permits a simple discretization of the Laplacian operator. We learn in this chapter that DG cannot use the same representation of the Laplacian operator. Rather, we need to revisit first order derivatives and construc作者: 和平 時間: 2025-3-27 13:51
Strategien in organisierten Sozialsystemeno and three dimensions. In one dimension, there is no room to choose the shape of the domain. That is, in the domain .?∈?[?1, +1] we are constrained to line elements. However, in two dimensions this door is flung wide open and we are now free to choose all sorts of polygons as the basic building blo作者: 銀版照相 時間: 2025-3-27 21:34 作者: Sigmoidoscopy 時間: 2025-3-27 23:39 作者: 犬儒主義者 時間: 2025-3-28 02:57
Analyse der Markt- und Positionssituation, of two-dimensional elliptic problems with the discontinuous Galerkin method. Although the extension to multi-dimensions is straightforward, to simplify the discussion we focus on two dimensions. This chapter focuses on the discretization of scalar elliptic problems (e.g., Poisson problem) using the作者: acrimony 時間: 2025-3-28 06:50
Analyse der Markt- und Positionssituation,ow how to compute first derivatives. As in the 1D case, a judicious use of Green’s first identity allows for a simple discretization of the Laplacian operator using the so-called .. In Chs. . and . for the DG method we did not use the simpler primal formulation but rather wrote the second order oper作者: 不能妥協(xié) 時間: 2025-3-28 12:57
Strategische Ausrichtung als Erfolgsbasis,ly. In Ch. . we introduced the extension of the CG method to two dimensions by describing its implementation for elliptic partial differential equations (PDEs). In this chapter we extend the CG method for the application of hyperbolic equations in two dimensions. We also discuss the addition of diff作者: 來就得意 時間: 2025-3-28 16:15 作者: 言外之意 時間: 2025-3-28 22:01
An Introduction to Element-Based Galerkin Methods on Tensor-Product Bases978-3-030-55069-1Series ISSN 1611-0994 Series E-ISSN 2197-179X 作者: 去掉 時間: 2025-3-29 01:36
https://doi.org/10.1007/978-3-662-26063-0the choices that we have at our disposal. We can categorize the possible methods as follows: .Generally speaking, the most widely used differential form method is the finite difference method while the most widely used integral form method is the Galerkin method (e.g., finite elements).作者: Inculcate 時間: 2025-3-29 03:12 作者: 果仁 時間: 2025-3-29 08:07
https://doi.org/10.1007/978-3-322-87118-3onservation laws for both CG and DG. However, these types of equations are entirely hyperbolic (first order equations in these cases). In this chapter we learn how to use the CG method to discretize second order equations that are elliptic.作者: Legion 時間: 2025-3-29 14:30 作者: 的’ 時間: 2025-3-29 16:18 作者: 憂傷 時間: 2025-3-29 21:51
1611-0994 s. In addition, examples are included (which can also serve as student projects) for solving hyperbolic and elliptic partial differential equations, includingboth scalar PDEs and systems of equations..978-3-030-55071-4978-3-030-55069-1Series ISSN 1611-0994 Series E-ISSN 2197-179X 作者: Palter 時間: 2025-3-30 00:37 作者: Customary 時間: 2025-3-30 04:18
1611-0994 r understand the material clearly and assists them in buildi.This book introduces the reader to solving partial differential equations (PDEs) numerically using element-based Galerkin methods. Although it draws on a solid theoretical foundation (e.g. the theory of interpolation, numerical integration作者: TIA742 時間: 2025-3-30 09:43
https://doi.org/10.1007/978-3-322-83873-5c equations. We rely heavily on the theory that we have already presented in Ch. . on interpolation and in Ch. . on numerical integration. We only consider scalar equations in this chapter and extend the implementation of the DG method to systems of nonlinear partial differential equations in Ch. ..作者: 樣式 時間: 2025-3-30 15:11 作者: 編輯才信任 時間: 2025-3-30 18:23
Analyse der Markt- und Positionssituation,fy the discussion we focus on two dimensions. This chapter focuses on the discretization of scalar elliptic problems (e.g., Poisson problem) using the local discontinuous Galerkin (LDG) method. We reserve the symmetric interior penalty Galerkin (SIPG) method for Ch. ..作者: paroxysm 時間: 2025-3-30 21:56 作者: Stress-Fracture 時間: 2025-3-31 02:26
1D Discontinuous Galerkin Methods for Hyperbolic Equationsc equations. We rely heavily on the theory that we have already presented in Ch. . on interpolation and in Ch. . on numerical integration. We only consider scalar equations in this chapter and extend the implementation of the DG method to systems of nonlinear partial differential equations in Ch. ..作者: 修剪過的樹籬 時間: 2025-3-31 06:23
1D Unified Continuous and Discontinuous Galerkin Methods for Systems of Hyperbolic Equationse observed. In this chapter, we construct these methods in a unified way so that they can co-exist within the same piece of software. In order to achieve this unification of CG and DG requires analyzing the storage of the methods; this is the objective of Sec. 7.2.作者: 淺灘 時間: 2025-3-31 09:44
2D Discontinuous Galerkin Methods for Elliptic Equationsfy the discussion we focus on two dimensions. This chapter focuses on the discretization of scalar elliptic problems (e.g., Poisson problem) using the local discontinuous Galerkin (LDG) method. We reserve the symmetric interior penalty Galerkin (SIPG) method for Ch. ..作者: ethnology 時間: 2025-3-31 17:18
2D Unified Continuous and Discontinuous Galerkin Methods for Elliptic Equationsoperator using the so-called .. In Chs. . and . for the DG method we did not use the simpler primal formulation but rather wrote the second order operator as a system of first order operators and then used the local discontinuous Galerkin (LDG) method.
