Modeling of 3D Beams
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1 Modeling of 3D Beams Friday, July 11 th, (1 Hour) Goran Golo Goran Golo
2 Preliminaries Goran Golo
3 Preliminaries Limitations of liner beam theory Large deviations Equilibrium is not a straight line 3
4 Preliminaries Non-linear beam theory Geometrically exact beam theory (Reissner 72 ; Simo vu-quoc 86 ) Virtual work Port-Hamiltonian framework Modeling and simulation Analysis Control 4
5 Contents Model derivation Notation Interconnection structure Elastic domain Kinetic domain Discretization (network) Examples Open problem 5
6 Goran Golo
7 Notation Centroid curve Cross-sectional sectional area Arc-length coordinate Centroid curve length 7
8 Spatial manifold If then the spatial manifold is 8
9 Remark If then the flexible body can be described by using either shell theory of general flexible theory. 9
10 10
11 Position of a slice of the beam is completely determined by an element of. Thus, the position of the whole beam is a curve laying in. 11
12 Mathematical intermezzo group is six dimensional matrix group. Elements of this group are represented by where (i) (ii) 12
13 Choice of initial body frame 13
14 Elastic energy Kinetic energy Interconnection structure 14
15 Interconnection structure Internal relations Boundary relations 15
16 There exists such that 16
17 Mathematical intermezzo is Lie algebra corresponding to. It is a six dimensional vector space. Elements of this space are represented by where (i) (ii) 17
18 Equivalently, Therefore If where 18
19 then where 19
20 Remark The position of the beam is completely determined by a point and. 20
21 Meaning of Since is orthogonal is skew-symmetric and thus is -valued 1-form on. 21
22 Example (straight beam) 22
23 Example (straight beam) 23
24 Expression for in non-stressed position 24
25 Strain measure Strain measure is intrinsically defined quantity i.e. it is invariant under a superposed rigid-body motion. Indeed, let then 25
26 Beam in motion The position of the beam in motion is specified by 26
27 Velocity of a point of the beam is defined as is -valued 0-form on. 27
28 Kinematic relation describes the relation between the strain measure and velocity. In the sequel we show that Where Here stands for the space of -valued -forms. 28
29 Based on relation we have that Since, it follows that The term can be rewritten as 29
30 Hence Using the equality The following is obtained 30
31 Consequently, Since the previous equality becomes 31
32 Matrix representation Vector representation 32
33 The matrix equality has the following vector representation Obviously is a linear transformation. 33
34 Elastic forces,, and the strain rate,,are power-conjugate variables. is the dual space of. One-forms are dual to zero-forms. is -valued 0-form on. 34
35 Duality product (elastic domain power) 35
36 Velocity,, and the momenta rate,,are powerconjugate variables. is -valued 1-form on. 36
37 Duality product (kinetic domain power) 37
38 Relation between forces 38
39 Boundary relations 39
40 Interconnection structure 40
41 Remark Expression can be rewritten as 41
42 42
43 Elastic energy Constitutive relations for elastic domain 43
44 Torsion in direction Energy Constitutive relation 44
45 Bending in direction Energy Constitutive relation 45
46 Bending in direction Energy Constitutive relation 46
47 Longitudinal elongation in direction Energy Constitutive relation 47
48 Shear deflection in direction Energy Constitutive relation 48
49 49
50 Total elastic energy Constitutive relation 50
51 Kinetic energy Constitutive relations for kinetic domain 51
52 Total kinetic energy where is ij th element of the matrix 52
53 The constitutive relation is or in vector notation 53
54 54
55 Discretization Goran Golo
56 Discretization 56
57 Discretization 57
58 Example Goran Golo
59 Examples We consider the beam whose motion takes place in XY plane only. This means that Elastic energy 59
60 Examples Kinetic energy where 60
61 Examples Beam parameters 61
62 Examples 62
63 Examples 63
64 Open problem Goran Golo
65 Open problem If then there exists such that Find expression for as a function of 65
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