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Samcef ROTORS versus ANSYS V14.0 Patrick Morelle – 4/6/2012 http:WWW.//ablemax.co.kr 5nd floor, Hanho Building, 90-14 SamSung-1 Dong, KangNam-Gu, Seoul, Korea Republic of TEL: 02) 539-5212 FAX: 02) 539-5213 E-mail: info@ablemax.co.kr ableMAX
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LMS Samtech Division Copyright LMS International - 2012 2 Comparison S4R - ANSYSS4R ANSYS Dedicated GUI and integrated solution for rotor dynamics Improved conical beam element (degenerated shell, better taking into account conical shafts) 2D Fourier models without limitations in the number of harmonics (0, 1 and higher orders). Possibility to use them for composite materials. 2D Fourier Lagrangian and Eulerian approach No specific GUI. Rotor dynamics capabilities as part of Work Bench, but needs lots of “epilogue”/scripts (users are complaining), including for the display of results Classical beam element 2D axisym (but with limited number of harmonics). Only 2D Lagrangian approach
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LMS Samtech Division Copyright LMS International - 2012 3 Comparison S4R - ANSYSS4R ANSYS 1D, 2D, 3D, cyclic symmetry, multi stage cyclic symmetry, all exhibiting gyroscopic effect, and possibility to combine all of them Superelement technique for rotating parts AND non rotating parts. The rotating superelement include reduced stiffness, mass, damping, gyroscopic and circulatory forces matrices Specific manoeuver loads available (non rotating) General gear element allowing to take into account coupling between axial, bending and torsion modes NO multi stage cyclic symmetry, no combinations between different types of models Superelement technique ONLY for non rotating parts in inertial frame Only rotating (synchronous or asynchronous) forces No gear
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LMS Samtech Division Copyright LMS International - 2012 4 Comparison S4R - ANSYSS4R ANSYS Large library of specialized bearings (hydrodynamic bearing, rolling element bearing, squeeze-film damper, added mass effect fluid elements), prototype BEARING module for hydrodynamic bearings (normal and thrust) Bearing element with 6X6 matrices (stiffness, damping (viscous or hysteretical), mass) The coefficients are either constant or variables with rotational speed, frequency or time Bi-variable (rotational speed and frequency) bearing element with 6X6 matrices (stiffness, damping, mass) very limited library of bearings (monoaxial spring/damper, general stiffness/damping matrix, 2D spring damper, multi point constraint) General stiffness/Damping matrix (MATRIX27) CONSTANT (no dependency of the speed of rotation) Only constant matrices
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LMS Samtech Division Copyright LMS International - 2012 5 Comparison S4R - ANSYSS4RANSYS Possibility to model transfer function for magnetic bearings including control Local non linearities are taken into account in the frequency domain ( non linear harmonic balance method). Available : bushing (clearances), rolling element bearing, squeeze-film damper, friction element Improved integration schemes in time domain, and on non linear elements available : bushing (clearances), rolling element bearing, squeeze-film damper, friction element, hydrodynamic bearing element No transfer function available for rotor dynamics models Only classical harmonic analysis No specific integration scheme and no specific non linear elements
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LMS Samtech Division Copyright LMS International - 2012 6 Comparison S4R - ANSYSS4R ANSYS Specialized and advanced post- processing included in the GUI Automatic 3D recombination of 2D and cyclic symmetry models including multi stage cyclic symmetry Campbell diagram available for problems in inertial AND rotating frame. Very performant mode tracking process. No specific GUI, use command language to post-process rotor model No automatic 3D recombination No Campbell diagram available for problems in rotating frame. Classical mode tracking process.
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