r=K*a
r = nodal force vector
K = stiffness matrix
a = nodal displacement
Implicit Solver
r(i+1) = K(i+1) * a(i+1)
-uses iterative method and needs convergence
-enforces equilibium of internal and external forces
-static or low frequency dynamic analysis
-unconditionally stable, not sensitive to small elements
-more computational expensive
Explicit Solver
r(i+1) = K(i) * a(i+1)
-doesnt enforce equilibium of internal and external forces
-especially dynamic analysis
-conditionally stable, sensitive to small elements
-less computational expensive
Discretization
-domain divided into elements
-connected at nodes
-no empty space
-no overlaps
-quality depends on size and type of elements
Order of interpolation
-interpolation used between mesh nodes
-linear, quadratic, cubic
-higher order needs more nodes
-higher order is more computational expensive
Linear FEM
-linear relation between forces and displacement
-only in elastic range
-K is constant
Nonlinear FEM
-nonlinear relation between forces and displacement
-also large deforrmations
-K is not constant
Reasons for Nonlinearity
-Geometric Nonlinearity (large deformations)
-Material Nonlinearity (material doesnt follow Hooke's law)
-Contact Nonlinearity
FEM (finite element method)
-numerical technique for finding approximate solutions
-divides large problem into smaller parts
-Preprocessor
-Solver
-Postprocessor
Prepocessor
-Definition of geometry
-Discretization
-Definition of material
-Application of boundary conditions
-Setup of simulation
Postprocessor
-view results
-create animations
-plot quantities of time/elements
-create result tables
K (stiffness matrix)
-information about material and geometry
-(#unknowns) = (#DOF per node) * (#nodes)
-global K consists of element Ks of all elements
BEAM188
-standard element for line bodies
-1D
-based on Timeshenko beam theory
-DOF: UX, UY, UZ, ROTX, ROTY, ROTZ
-KEYPOT(3): 0 = linear
1 = quadratic
2 = cubic
When do you use line bodies and why?
Timoshenko beam theory
-extends Euler-Bernoulli beam theory
-accounts for shear deformation and rotational inertia
-especially important for short, thick beams