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Rotordynamics with ANSYS Mechanical Solutions
Pierre THIEFFRY Product Manager ANSYS, Inc.
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Generalized axisymmetric element Rotordynamics with ANSYS Workbench
Agenda General features Generalized axisymmetric element Rotordynamics with ANSYS Workbench An ANSYS V12.0 example Future plans I’d like to remind everyone that some matters that will be discussed during this presentation may constitute forward-looking statements that involve risks and uncertainties, which could cause actual results to differ from those projected. In addition, I would also like to mention that we will not be able to discuss or answer any questions regarding previously provided guidance, as our Company policy is that we only comment on company guidance in a public forum.
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General features
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Rotordynamics features
Pre-processing: Appropriate element formulation for all geometries Gyroscopic moments generated by rotating parts Bearings Rotor imbalance and other excitation forces (synchronous and asynchronous) Rotational velocities Structural damping Solution: Complex eigensolver for modal analysis Harmonic analysis Transient analysis
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Rotordynamics features
Post-processing Campbell diagrams Orbit plots Mode animation Transient plots and animations User’s guide Advanced features: Component Mode Synthesis for static parts
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Appropriate element formulation
The following elements are supported for rotordynamics analysis (stationary reference frame): Mass MASS21 Beam BEAM4, PIPE16 BEAM188, BEAM189 PIPE 288/289 Solid SOLID45, SOLID95 SOLID185, SOLID186, SOLID187 Shell SHELL63 SHELL181, SHELL281 General axisymmetric elements SOLID272, SOLID273 New in ANSYS 12.0 New in ANSYS 12.0
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Generalized axisymmetric element
The new 272/273 elements: Are computationally efficient when compared to 3D solid Support 3D non-axisymmetric loading Allow a very fast setup of axisymmetric 3D parts: Slice an axisymmetric 3D CAD geometry to get planar model Mesh with 272/273 elements No need to calculate equivalent beam sections Can be combined with full 3D models, including contact 2D axisymmetric mesh 3D representation 3D results (not necessarily axisymmetric)
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Bearings 2D spring/damper with cross-coupling terms: Real constants are stiffness and damping coefficients and can vary with spin velocity w Bearing element choice depends on: Shape (1D, 2D, 3D) Cross terms Nonlinearities Description Stiffness and Damping cross terms Nonlinear stiffness and damping characteristics COMBIN14 Uniaxial spring/damper No COMBI214 2-D spring/damper Unsymmetric Function of the rotational velocity MATRIX27 General stiffness or damping matrix MPC184 Multipoint constraint element Symmetric for linear characteristics - None for nonlinear characteristics Function of the displacement
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Imbalance and other excitation forces
Possible excitations caused by rotation velocity are: Unbalance () Coupling misalignment (2* ) Blade, vane, nozzle, diffusers (s* ) Aerodynamic excitations as in centrifugal compressors (0.5* ) Input made as a force on the model z y r
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Rotating damping structural damping (MP, DAMP or BETAD)
Considered if the rotating structure has: structural damping (MP, DAMP or BETAD) or a localized rotating viscous damper (bearing) The damping forces can induce unstable vibrations. The rotating damping effect is activated along with the Coriolis effect (CORIOLIS command). Damper COMBI214 Beam BEAM4, PIPE16 BEAM188, BEAM189 Solid SOLID45, SOLID95 SOLID185, SOLID186, SOLID187 General axisymmetric SOLID272, SOLID273 (new in V 12.0 ) Elements supporting rotating damping
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Campbell diagrams & whirl
Variation of the rotor natural frequencies with respect to rotor speed w In modal analysis perform multiple load steps at different angular velocities w As frequencies split with increasing spin velocity, ANSYS identifies: forward (FW) and backward (BW) whirl stable / unstable operation critical speeds Also available for multispool models
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Orbit plots In a plane perpendicular to the spin axis, the orbit of a node is an ellipse It is defined by three characteristics: semi axes A , B and phase y in a local coordinate system (x, y, z) where x is the rotation axis Angle j is the initial position of the node with respect to the major semi-axis A. Orbit plots are available for beam models
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Rotordynamics analysis guide
New at release 12.0 Provides a detailed description of capabilities Provides guidelines for rotordynamics model setup
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Sample models available
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Generalized axisymmetric element
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New Element Technology
General Axi-symmetric Element: 272/273 3D elements generated based on 2D mesh Boundary conditions applied in 3D space Nonlinearities, Node to surface contact Benefits Multiple Axis can be defined in any direction Take advantage of axi-symmetry but deformation is general in 3D 1 element in Θ (hoop) direction I L J K A B Y’ Z’ X’ Structural Mechanics Exciting new ‘Generalized 3D Axi-symmetric element’ that can be used for a 3D analysis. SOLID272 is defined by four nodes on the master plane, and nodes created in the circumferential direction based on the four master plane nodes SOLID272 and SOLID273 elements introduce the Fourier series into interpolation functions to describe the change of displacements in the circumferential (theta) direction. Lagrangian polynomial interpolation in r-z plane, Fourier series interpolation in ө dir. The elements can therefore apply to any analysis type, including geometric nonlinear analyses, and can support any load and deformation mode. The element allows a triangle as the degenerated shape on the base plane to simulate irregular areas. The element has plasticity, hyperelasticity, stress stiffening, large deflection, and large strain capabilities. It also has mixed-formulation capability for simulating deformations of nearly incompressible elastoplastic materials, and nearly and fully incompressible hyperelastic materials. The elements can have any axis as the symmetric axis (defined via SECTYPE and SECDATA commands); you need only define quadrilaterals or triangles on a plane. At release 12.0, Node-to Surface contact is supported and only with SOLID272 (lower order). Applications include threaded connections simulations for analyzing piping joints, bio-medical etc. 3D view of shaft
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Application to rotordynamics
The new 272/273 elements: Are computationally efficient when compared to 3D solid Support rotordynamics analysis Support 3D non-axisymmetric loading Allow a very fast setup of axisymmetric 3D parts: Slice an axisymmetric 3D CAD geometry to get planar model Mesh with 272/273 elements No need to calculate equivalent beam sections Can be combined with full 3D models, including contact 2D axisymmetric mesh 3D representation 3D results (not necessarily axisymmetric)
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Rotordynamics with ANSYS Workbench An example
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Storyboard The geometry is provided in form of a Parasolid file Part of the shaft must be reparametrized to allow for diameter variations A disk must be added to the geometry Simulation will be performed using the generalized axisymmetric elements, mixing WB features and APDL scripting Design analysis will be made with variations of bearings properties and geometry
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Project view Upper part of the schematics defines the simulation process (geometry to mesh to simulation) Parameters of the model are gathered in one location (geometry, bearing stiffness) Lower part of the schematics contains the design exploration tools
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Geometry setup Geometry is imported in Design Modeler
A part of the shaft is redesigned with parametric dimensions Model is sliced to be used with axisymmetric elements Bearing locations are defined A disc is added to the geometry Initial 3D geometry Final axisymmetric model Additional disk Bearings location
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Geometry details 3D Model sliced to create axisymmetric model
Part of the original shaft is removed and recreated with parametric radius Additional disk created with parameters (the outer diameter will be used for design analysis) Bearing locations and named selections are created (named selections will be transferred as node components for the simulation)
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Mesh The model is meshed using the WB meshing tools
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Simulation Simulation is performed using an APDL script that defines:
Element types Bearings Boundary conditions Solutions settings (Qrdamp solver…) Post-processing (Campbell plots and extraction of critical speeds) Axisymmetric model with boundary conditions Expanded view
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APDL script Mesh transferred as mesh200 elements, converted to solid272 Spring1 component comes from named selection
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Simulation results The APDL scripts can create plots and animations
The results can also be analyzed within the Mechanical APDL interface Results are extracted using *get commands and exposed as WB parameters (showing the performance of the design)
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Mode animation (expanded view)
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Design exploration The model has 2 geometry parameters (disc and shaft radius) as well as a stiffness parameters (bearings stiffness) 4 output parameters are investigated: first and second critical speeds at 2xRPM and 4xRPM (obtained from theCampbell diagrams and *get commands)
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Sample results Sensitivity plots: the bearing stiffness has no influence on the first and second critical speeds, the disc radius is the key parameter A response surface of the model is created using a Design of Experiments Curves, surfaces and sensitivity plots are created and the design can be investigated Optimization tools are also available Evolution of critical speed with shaft and disc radius
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Optimization A multi-objective optimization is described and possible candidates are found (usually, there are multiple acceptable configurations) Trade-off plots give an indication about the achievable performance
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Future plans (V13 and beyond)
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Campbell diagrams Multiple steps (modal) X axis is rotational velocity
Rotational velocity scoped on bodies( (multispool analysis) available in modal analysis Output Quantities:frequencies or stability values
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Additional enhancements
Provide modal solver choice (QRDAMP, LANB…) The connection folder hosting bearings: Location Damping and stiffness (as functions of w) Coriolis option available from the Analysis settings (like the large deflection or inertia relief) Orbit plots for beam models Exposure of generalized axisymmetric elements
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Modal post-processing (already available at V12)
Complex eigenshapes Mode animation similar to ANHARM For complex modes, tabular data display both imaginary and real parts
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Results parameterization
The user will probably want to be able to parameterize frequencies (real and/or imaginary part) but also the critical frequencies (from Campbell results) Doing so, he will be able to perform DX analyses : to examine the variations of critical frequencies To examine the evolution of the stability of a mode wrt various parameters
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