pat328, section 3, march 2001 s7-1 mar120, lecture 4, march 2001mar120, section 7, december 2001...
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PAT328, Section 3, March 2001 S7-1MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
SECTION 7
CHOICE OF ELEMENTS:TOPOLOGY AND RESTARTING
PAT328, Section 3, March 2001 S7-2MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
TABLE OF CONTENTS
Section Page
7.0 Choice of Elements: Topology and Restarting GeometricOverview……………………………………………………………………………………………………………..
7-3Element Topology…………………………………………………………………………………………………..7-4Structural Element Types In MSC.Marc………………………………………………………………………….7-51d (Bar) Elements…………………………………………………………………………………………………..7-6Beam Section Orientation Vector………………………………………………………………………………… 7-72d Solid (Continuum) Elements…………………………………………………………………………………...
7-8 2d Shell Elements (Thin Shell: 5 DOF @ Nodes)……………………………………………………………….
7-102d Shell Elements (Thick Shell: 6 DOF @ Nodes)……………………………………………………………...
7-113d Shell Elements (3 DOF @ Nodes)…………………………………………………………………………….
7-121st And 2nd Order Elements………………………………………………………………………………………...
7-13 Choice Of Elements………………………………………………………………………………………………...
7-15 Connecting Elements Of Different Types………………………………………………………………………...
7-17Choice Of Integration Method……………………………………………………………………………………..7-18
PAT328, Section 3, March 2001 S7-3MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
OVERVIEW
Selecting and Using Finite Elements
Element Topology Versus Element Property
Dimensions of Structural Space versus Dimensions of Finite Element
Connecting Elements of Different Topology
Methods of Numerical Integration
Plane Elements Plane Strain Plane Stress Axisymmetry
Orientation of Beam Cross Sections in Space
Thin Shells Versus Thick Shells
PAT328, Section 3, March 2001 S7-4MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
0-D Elements
1-D Elements
Element Types in MSC.MARC
2-D Elements
3-D Elements
ELEMENT TOPOLOGY
PAT328, Section 3, March 2001 S7-5MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
Example: First modal shape of beam model combining element types
STRUCTURAL ELEMENT TYPES IN MSC.MARC
0-D Point Masses 1D (Bar) Elements 2D Solid (Continuum)
Elements 2D Shell Elements 3D Solid (Continuum)
Elements
PAT328, Section 3, March 2001 S7-6MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
1D (BAR) ELEMENTS Beam Elements (Standard, Euler-
Bernoulli) Truss (Spar) Elements Axisymmetric Shell Elements Springs Dashpots (Use Springs Options
These elements may have nonlinear properties
Example : Snap-through of Bottom of a Soft-Drink Can
Simulated with quadratic (3-node) 1D Axisymmetric elements
Aluminum can –plasticity included When pressure increases the bottom
of the can “snaps” thus increasing the volume inside the can –relieving the pressure- and preventing the rupture and spilling of contents.
Because of plasticity the bottom cannot return back to the original shape thus protecting the consumer from spoilage.
PAT328, Section 3, March 2001 S7-7MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
XZ Plane
Node 1
Node 2
Y
X
Z
1”
2”
J
Izz
Ixx
Z
Global CS
X
Y
BEAM SECTION ORIENTATION VECTOR
PAT328, Section 3, March 2001 S7-8MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
Plane Stress
Plane Strain
2D SOLID (CONTINUUM) ELEMENTS
Plane Stress Elements (2 DOF @ nodes: Ux, Uy)
Planar structures, All out-of-plane stresses zero
Typical: Flat panels subject to inplane loads
Plane Strain Elements (2 DOF @ nodes: Ux, Uy)
Planar model, All out-of-plane strains constant or zero
Typical: Slice of car’s door rubber seal
Membrane Elements (3 DOF @ nodes: Ux, Uy, Uz)
Curved, very thin structures unable to sustain bending
PAT328, Section 3, March 2001 S7-9MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
Axisymmetric Elements (2 DOF @ nodes: Ux, Uy)
Axisymmetric structures with axisymmetric loadings
2D SOLID (CONTINUUM) ELEMENTS (CONT.)
X = Axial Y = Radial !
PAT328, Section 3, March 2001 S7-10MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
1
Z
Y
X
n4 3
2n 3
2
1
Top
Bottom
2D SHELL ELEMENTS (THIN SHELL: 5 DOF @ NODES)
In-plane/out-of-plane loadings in planar and curved surfaces
Ignores out-of-plane normal stress Ignores out-of-plane transverse
shear stresses (Normals remain normals)
Thickness very small (<5%) compared to typical surface
PAT328, Section 3, March 2001 S7-11MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
2D SHELL ELEMENTS (THICK SHELL: 6 DOF @ NODES)
In-plane/out-of-plane loadings in planar and curved surfaces
Ignores out-of-plane normal stress Considers out-of-plane transverse
shear stresses (Plane Sections remain Plane)
Thickness small (>5%, but <10%, ) compared to typical surface dimensions
PAT328, Section 3, March 2001 S7-12MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
3D SHELL ELEMENTS (3 DOF @ NODES)
Considers all 6 components of stresses and strains
Suitable for 3D solid bodies
Although valid, 3D Solid Elements are neither efficient, nor very accurate for thin surfaces, or long and slender parts.
PAT328, Section 3, March 2001 S7-13MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
Linear
Quadratic
Herrmann - extra node carries compressibility degree of
freedom typically GUI handles this in an automated fashion.
1ST AND 2ND ORDER ELEMENTS
PAT328, Section 3, March 2001 S7-14MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
Truss/SparBeam (2D)
Beam (3D)
Axysym. Shell
9,51 5,1613,14,25,31,52,78,
79,981,15
Elem 31 is a curved pipe (Elbow)/Straight Beam ElementElem 98 is a Thick (Timoshenko) Beam Element
1D (2-Node Line) Structural Elements:
Shape/Type Shell
ShellPlane Stress
Plane Strain Azysym. SolidMembrane Shear
Tri3 8, 138 6 2 2Quad4 75, 139, 4, 24 3 11 11 10 18Quad4 (RI) 140 114 115 116 116 68Tri6 49 124 125 126 126Quad8 22, 72 26 27 28 28 30Quad8 (RI) 53 54 54 55
2D (Surface) Structural Elements:
Elem 3, 11 can be used with/without assumed strainElem 22, 75, 140 are Thick shell Elements
ShapeElement Number
Tet4 134Hex8 7Hex8 (RI) 117Tet10 127Hwx20 21Hex20 (RI) 57
3D (Solid) Structural Elements:
HEX8 (Elem 7) can be used with/without assumed strain
Springs, Dashpots: SPRINGS for both springs and dashpots
Point MASS: MASSES for concentrated (point) Masses
1ST AND 2ND ORDER ELEMENTS (Cont.)
PAT328, Section 3, March 2001 S7-15MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
CHOICE OF ELEMENTS
Use beam elements to model beam-like structures, if possible and appropriate.
They are economical and give very good answers within the assumptions of beam theory.
Also very useful to represent stiffeners on shells
Example:Pantograph
Including beam-to-beam contact
PAT328, Section 3, March 2001 S7-16MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
CHOICE OF ELEMENTS (Cont.)
For bending problems with solid elements (2D or 3D), element type and meshing can greatly affect the results.
Solid elements may be necessary in bending problems where beam theory is not sufficient if thickness is too large or stresses in the thickness direction are important.
How shall we choose the element type?
How fine a mesh do we need?
PAT328, Section 3, March 2001 S7-17MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
CONNECTING ELEMENTS OF DIFFERENT TYPES
Part of the structure may be represented by shell elements and part by solid elements
The number of degrees of freedom is different for solid elements than for shell element
How to prevent the free rotation of the shell at the interface with the solid
PAT328, Section 3, March 2001 S7-18MAR120, Lecture 4, March 2001MAR120, Section 7, December 2001
CHOICE OF INTEGRATION METHOD
Different methods of integration are available. Their performance is discussed in further detail in the next chapter
Standard Elements provide full integration
Materials with incompressible behavior (such as rubber) require special options such as Reduced Integration or Herrmann formulation. The reason for this is that a Poisson’s ratio of 0.5 will have an indeterminate stiffness coefficient Integration Points for Standard
8-Node Membrane Element