The following static analysis topics are available:
The static analysis (ANTYPE,STATIC) solution method is valid for all degrees of freedom (DOFs). Inertial and damping effects are ignored, except for static acceleration fields.
The overall equilibrium equations for linear structural static analysis are:
(15–1) |
or
(15–2) |
where:
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, the total applied load vector, is defined by:
(15–3) |
where:
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To illustrate the load vectors in Equation 15–2, consider a one element column model, loaded only by its own weight, as shown in Figure 15.1: Applied and Reaction Load Vectors. Note that the lower applied gravity load is applied directly to the imposed displacement, and therefore causes no strain; nevertheless, it contributes to the reaction load vector just as much as the upper applied gravity load. Also, if the stiffness for a certain DOF is zero, any applied loads on that DOF are ignored.
Solving for Unknowns and Reactions discusses the solution of Equation 15–2 and the computation of the reaction loads. Newton-Raphson Procedure describes the global equation for a nonlinear analysis. Inertia relief is discussed in Inertia Relief.
The overall equations for linear 1st order systems are the same as for a linear structural
static analysis, Equation 15–1 and Equation 15–2.
, though, is the total coefficient matrix (for example, the conductivity
matrix in a thermal analysis) and
is the nodal DOF values.
, the total applied load vector, is defined by:
(15–4) |
Table 15.1: Nomenclature relates the nomenclature used in Derivation of Heat Flow Matrices and Derivation of Electromagnetic Matrices for thermal, magnetic and electrical analyses to Equation 15–2 and Equation 15–4. See Table 10.3: Nomenclature of Coefficient Matrices for a more detailed nomenclature description.
Table 15.1: Nomenclature
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Thermal |
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Scalar Magnetic |
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Vector Magnetic |
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Electrical |
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Solving for Unknowns and Reactions discusses the solution of Equation 15–2 and Newton-Raphson Procedure describes the global equation for a nonlinear analysis.