Weak Form, Exact, and Approximate Solutions

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  1. Sarah Hankins
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Weak Form, Exact, 0:12:16

Weak Form, Exact, and Approximate Solutions

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FEA Subdomain 0:07:04

FEA Subdomain method Non weak Form Approximate solutions

Exact and Approximate 0:07:45

Exact and Approximate Solutions

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Galerkin Weak Form Example 1

Governing Equations: Weak 0:16:34

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Approximate Solutions - 0:27:07

Approximate Solutions - The Ritz Method

FEA Point 0:07:16

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Approximate Solutions - 0:34:57

Approximate Solutions - The Galerkin Method

26. Energy Methods 0:50:09

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3.7 Approximate solution 0:09:30

3.7 Approximate solution

Understanding the Finite 0:18:36

Understanding the Finite Element Method

3.6 Weak form 0:13:27

3.6 Weak form Part 2

Finite Element Method: 1:25:32

Finite Element Method: Lecture 6A - Weak Form Galerkin Approximation Method

1-1: Linear Elastic 0:25:45

1-1: Linear Elastic Finite Element Analysis (Weak Form of Governing Differential Equation)

Lecture 15 - 1:35:08

Lecture 15 - 1D FEM (vii) ... Strong to Weak Form (vi) ... Approximation by Shape Functions (iii)

Weak Forms-2 0:07:38

Weak Forms-2

MECH413 Strong And 0:13:06

MECH413 Strong And Weak Form Example2

Finite Element Method: 0:20:51

Finite Element Method: Lecture 6B - Weak Form Galerkin Example Advection-Diffusion Equation

25. Energy Methods 0:41:34

25. Energy Methods and Computational Mechanics - Strong Form Galerkin Approximation Method

Weak forms-1 0:06:37

Weak forms-1

Комментарии
Автор

Good presentation, however you do not need the partial sign here since this is a function of one variable.

Also these are both boundary conditions once they refer to space.

nicolabombace
Автор

I don't understand how a PDQ with partial derivatives in only a single variable isn't de facto an ODQ.

swampwiz
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