{"id":3375,"date":"2015-02-06T16:12:16","date_gmt":"2015-02-06T07:12:16","guid":{"rendered":"http:\/\/advancae.com\/blog1\/?p=3375"},"modified":"2015-02-06T16:12:16","modified_gmt":"2015-02-06T07:12:16","slug":"lsdyna-r7-1-2-%e3%83%aa%e3%83%aa%e3%83%bc%e3%82%b9","status":"publish","type":"post","link":"https:\/\/www.advancae.com\/blog1\/2015\/02\/06\/lsdyna-r7-1-2-%e3%83%aa%e3%83%aa%e3%83%bc%e3%82%b9\/","title":{"rendered":"lsdyna R7.1.2 \u30ea\u30ea\u30fc\u30b9"},"content":{"rendered":"\r\n<p>\u6628\u65e5\u30012\/5 R7.1.2\u306e\u5168\u30e2\u30b8\u30e5\u30fc\u30eb\u304cLSTC\u30b5\u30a4\u30c8\u306b\u30a2\u30c3\u30d7\u3055\u308c\u3001\u516c\u5f0f\u30ea\u30ea\u30fc\u30b9\u3055\u308c\u305f\u3002<br \/>\u4ee5\u4e0b\u306e\u30ea\u30ea\u30fc\u30b9\u30ce\u30fc\u30c8\u3092\u3055\u3063\u3068\u898b\u3066\u3082\u308f\u304b\u308b\u3088\u3046\u306b\u3001\u65b0\u6a5f\u80fd\u306f\u6b86\u3069\u306a\u304f\u3066\u3001R7.1.1\u306b<br \/>\u5bfe\u3059\u308bFIX=\u30d0\u30b0\u4fee\u6b63\u7248\u3067\u3042\u308b\u3002<br \/><br \/>Windows64 \u3068\u3000Linux64\u7528\u306eSMP\u7248\u3068\u3001MPP\u7248\u3092\uff08IBM Platform\u7248\u306e\u307f\uff09\u3092<br \/>\u5f0a\u793e\u30b5\u30a4\u30c8\u306b\u30a2\u30c3\u30d7\u3057\u305f\u3002LSTC\u306e\u30b5\u30a4\u30c8\u306b\u306f\u3001\u304b\u306a\u308a\u306e\u6570\u306eR8.0\u304c\u30a2\u30c3\u30d7\u3055\u308c\u3066\u3044\u3066<br \/>R7.1.2\u306f\u5fae\u5999\u306a\u6240\u3060\u304c\u3001R7.1.1\u3067\u4e0d\u5177\u5408\u306b\u30d6\u30c1\u5f53\u305f\u3063\u305f\u3089\u3001R7.1.2\u3092\u8a66\u3057\u3066\u304f\u3060\u3055\u3044\u3002<br \/>\u30de\u30cb\u30e5\u30a2\u30eb\u306b\u3064\u3044\u3066\u3082\u30012015\/1\/28\u4ed8\u3051\u306eDRAFT\u7248\u304c\u516c\u958b\u3055\u308c\u3066\u3044\u308b\u3002<br \/><br \/>\u4eca\u56de\u304b\u3089\u3001Linux64 MPP\u7248\u306f\u3001\uff13\u7a2e\u985e\u9078\u629e\u53ef\u80fd\u3068\u306a\u3063\u305f\u3002\u4f8b\u3048\u3070\u500d\u7cbe\u5ea6\u7248\u306e\u5834\u5408<\/p>\r\n<p>ls-dyna_mpp_d_r7_1_2_95028_x64_redhat54_ifort131_avx2_platformmpi.tar.gz<br \/>ls-dyna_mpp_d_r7_1_2_95028_x64_redhat54_ifort131_sse2_platformmpi.tar.gz<br \/>ls-dyna_mpp_d_7_1_2_95028_x64_suse102_pgi105_sse2_platformmpi.tar.gz<\/p>\r\n<p>\u81ea\u5206\u304c\u6301\u3063\u3066\u3044\u308bSUSE 10.2\u3067\u3082\u3001CentOS-6 \u3067\u3082AVX2\u4ee5\u5916\u306f\u5168\u90e8\u52d5\u4f5c\u3057\u305f\u3002<br \/>\u4f55\u304c\u9055\u3046\u304b\u3068\u3044\u3046\u3068\u3001<br \/>\u00a0&#8211; ifort131 : Intel Fortran\u3067\u30b3\u30f3\u30d1\u30a4\u30eb\u3055\u308c\u3066\u304a\u308a\u3001Intel CPU\u3067\u6027\u80fd\u51fa\u308b<br \/>&#8211; pgi105 : PGI Fortran\u3067\u30b3\u30f3\u30d1\u30a4\u30eb\u3055\uff52\u3066\u304a\u308a\u3001AMD CPU\u5411\u3051<br \/>&#8211; avx2 .vs. sse2 : \u6700\u65b0\u306eIntel CPU\u306a\u3089avx2\u304c\u901f\u3044\u306f\u305a\u3002<br \/>\u6027\u80fd\u6bd4\u8f03\u30c6\u30b9\u30c8\u306b\u3064\u3044\u3066\u306f\u3001\u6b21\u306e\u30d6\u30ed\u30b0\u3067\u7d39\u4ecb\u3059\u308b\u4e88\u5b9a\u3002<\/p>\r\n<p>\u30ea\u30ea\u30fc\u30b9\u30ce\u30fc\u30c8<\/p>\r\n<p>&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;-<br \/>This file is revision 0 of the release notes for LS-DYNA version R7.1.2.<br \/>&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;-<br \/><br \/>Herein are summarized enhancements and bug fixes made since the<br \/>release of version R7.1.1.<br \/><br \/>These notes are arranged by topic.\u00a0 Understand that in many cases,<br \/>a particular note may have applicability to multiple topics, but in the<br \/>interest of brevity, each note is listed only under one topic heading.<br \/><br \/>The most recent User&#8217;s Manual (in three volumes) may be downloaded from<br \/>www.lstc.com\/download\/manuals.<br \/><br \/><br \/>________________________ *AIRBAG ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Make VNTOPT in *AIRBAG_HYBRID work for A23.ge.0.<br \/><br \/>*DATABASE_ABSTAT:<br \/>Fix mdot_out for CPM chamber abstat database.<br \/><br \/>Bug fix for *AIRBAG_SIMPLE_AIRBAG_MODEL when using *INCLUDE_TRANSFORM.<br \/>The input parameters MU and A were converted correctly but the<br \/>pre-converted values were written to the dyna.inc file.<br \/><br \/>Implement *DELETE_AIRBAG for small restart.<br \/><br \/><br \/>________________________ *BOUNDARY ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>All *BOUNDARY IDs are offset by idroff when included by *INCLUDE_TRANSFORM.<br \/><br \/>Turn off pore air boundary condition (*BOUNDARY_PAP) during dynamic relaxation.<br \/><br \/>Fix incorrect rigid body velocities when using *BOUNDARY_PRESCRIBED_MOTION_RIGID_LOCAL<br \/>and *INITIAL_VELOCITY_RIGID_BODY.<br \/><br \/>Error terminate if *BOUNDARY_SPC_NODE_BIRTH_DEATH is applied to a node that<br \/>belongs to a rigid body.<br \/><br \/>*BOUNDARY_ACOUSTIC_COUPLING_MISMATCH:<br \/>Fix for spurious automatic coupling<br \/>with faces on free surface of *MAT_ACOUSTIC elements.<br \/><br \/><br \/>________________________ *CONTACT ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>MPP tied contact initialization:<br \/>Change a tolerance in groupable tied contact bucketsort<br \/>to match the non-groupable code, and fix the slave node<br \/>thickness used for beam nodes during initial search in<br \/>non-groupable contact to match groupable contact.<br \/><br \/>MPP groupable tied contact:<br \/>Honor TIEDPRJ in *CONTROL_CONTACT, and output messages about moved<br \/>nodes to match non-groupable tied contact.<br \/><br \/>MPP eroding contact:<br \/>Fix problem of every processor<br \/>participating in every eroding contact, even if they had none of<br \/>the nodes or elements.\u00a0 This caused scaling issues.<br \/><br \/>Fix for MPP contact force summation<br \/>as applied to shells with compressive thickness<br \/>behavior.<br \/><br \/>MPP beam to surface contact: remove &#8220;beam&#8221; node mass<br \/>from the penalty stiffness calculation when soft=1<br \/>is used, which matches SMP behavior.<br \/><br \/>Various fixes to intfor output for MPP contact.<br \/><br \/>MPP tied contact with adaptivity: if any master<br \/>segments get adapted, we were dropping any slave<br \/>nodes.\u00a0 Now flag these, and do a bucketsort for<br \/>just these nodes, to find their new tied location.<br \/>This allows tied contacts to work across adaptive steps.<br \/><br \/>MPP contact: fix routine that updates segment<br \/>Correct update of segment thicknesses for solid elements (every cycle) so that<br \/>it honors the OPTT parameter in *PART_CONTACT.<br \/><br \/>MPP: fix problem with *CONTACT_TIED_&#8230;_BEAM_OFFSET<br \/>and full deck restart: data for this contact type<br \/>was not properly written to the d3full file, making<br \/>full deck restart with this contact type impossible.<br \/><br \/>Fix problem when using *INTERFACE_LINKING together<br \/>with constrained tied interfaces.\u00a0 Nodes involved in<br \/>both are removed from the linking interface, but<br \/>this was leaving some internal structures out of sync,<br \/>sometimes causing nodes to be moved improperly.<br \/><br \/>MPP eroding contact: fix long standing bug that<br \/>might have improperly excluded some nodes from<br \/>contact.<br \/><br \/>Fix for MPP two sided force transducers with erosion:<br \/>shared nodes were only flagged on one processor, so<br \/>some forces along processor boundaries might not have<br \/>been counted to a force transducer.<br \/><br \/>Fix rarely triggered bug for beam thickness\/stiffness<br \/>in MPP CONTACT_AUTOMATIC_GENERAL.<br \/><br \/>Fix for MPP groupable contact and implicit when there<br \/>are both constraint and penalty contact types.<br \/><br \/>Fix segmentation fault when using *CONTACT_GUIDED_CABLE.<br \/><br \/>Fix incorrect contact behavior when using *CONTACT_AUTOMATIC_GENERAL_INTERIOR for<br \/>beams with large differences in thickness and when the thinner beams are<br \/>closer to each other than to the thicker beams. Affects SMP only.<br \/><br \/>Fix incorrect contact thickness used for *CONTACT_ENTITY type 8 and 9 when<br \/>the contact thickness scale factor, g2, is non-zero.<br \/><br \/>Fix *RIGIDWALL_GEOMETRIC_FLAT_DISPLAY which incorrectly displayed the rigidwall<br \/>being penetrated by the slave nodes.<br \/><br \/>Add *CONTROL_CONTACT PENOPT=3 option for *CONTACT_ERODING_NODES_TO_SURFACE<br \/>for SMP.<br \/><br \/>Add contact friction energy to the SLEOUT database file for _2D_AUTOMATIC_SURFACE_TO_SURFACE<br \/>and _2D_AUTOMATIC_SINGLE_SURFACE contact.<br \/><br \/>Fix a 2D automatic contact bug that occurred if a segment has zero length.\u00a0 An<br \/>infinite thickness value was caculated by A\/L\u00a0 causing the bucket sort to fail.<br \/><br \/>Fix an error in 2D automatic contact sliding interface energy reported<br \/>in glstat.\u00a0 The outputted value was about 2x the correct value.<br \/><br \/>Fix both the intersection and initial penetration reporting of segment based<br \/>(soft=2) contact when the shared constraint flag SHAREC is set for the contact.<br \/>The reporting of segment pairs that<br \/>share nodes will not be made when SHAREC=1, but can be reported if neighbor segment<br \/>checking is active.<br \/><br \/>Fix an MPP 2-surface force transducer blunder when segment based contact is used.<br \/>The symptom observed was a change in bucket sort behavior making the contact less<br \/>reliable for contact bewteen segments that are not on the same MPP partition when<br \/>2-surface force transducers were used.<br \/><br \/>Fix a full deck restart error with SMP segment based contact.\u00a0 A segmentation<br \/>fault was likely.<br \/><br \/>Add support for eroding, 2-surface force transducers when used with segment<br \/>based contact.\u00a0 Data is now updated so that when solid element erodes and new<br \/>segments exposed, force on these surfaces will be reported to the force transduders.<br \/><br \/>Stop segment based (soft=2) contact from reporting initial penetrations between segment<br \/>pairs that share nodes.\u00a0 Such segment pairs can only exist when SHAREC=1 as they<br \/>otherwise do not pass the bucket sort so do not make the list.<br \/><br \/>Fix an error with SMP consistency in the segment based (soft=2) contact<br \/>neighbor segment check activated by setting SFNBR&gt;0.<br \/><br \/>Fix MPP full deck restart when using segment based contact.<br \/>It has been broken since rev 64900.<br \/><br \/>Fix the IGAP&gt;2 option on *CONTACT Optional Card C for segment based contact for SMP and MPP,<br \/>and also the regular contact for SMP only.\u00a0 The count of cycles used the cycle number rather<br \/>than equilibrium steps.\u00a0 The problem in using cycle number is that there is no way to know how many<br \/>implicit cycles will occur prior to converging so it almost guarantees that the gap stiffness will switch<br \/>off during iterations.\u00a0 Also, the MPP segment based contact was not even working correctly with<br \/>cycles.<br \/><br \/>Fix a problem with segment based contact when used with dynamic relaxation and when the<br \/>solution was switched to implicit after convergence.\u00a0 The contact was scaled too soft causing<br \/>pass through.<br \/><br \/>Fix an error that could occur in segment based contact when some element(s) grow<br \/>very large.\u00a0 Due to a cap on the possible number of sorting buckets, it was possible<br \/>during a bucket sort for the majority of elements to be left in a few buckets<br \/>with most of the buckets remaining empty.\u00a0 This caused the bucket sort to<br \/>become extremely slow.\u00a0 It also had the potential to overrun a buffer causing a<br \/>segmentation fault.\u00a0 With this fix, the buffer will no longer overflow, and<br \/>there is also a fix such that when some elements grow large, the bucket sort<br \/>does not slow down very much.<br \/><br \/>*CONTACT_AUTOMATIC_SINGLE_SURFACE_MORTAR previously did not work<br \/>with beam elements but now works.<br \/><br \/>*CONTACT_FORMING_SURFACE_TO_SURFACE_MORTAR, *CONTROL_ADAPTIVE:<br \/>Look ahead adaptive simulation with forming mortar contact was broken at<br \/>some point, but is now fixed.<br \/><br \/>In initializing *CONTACT_FORMING_SURFACE_TO_SURFACE_MORTAR, reversal of contact segments<br \/>took a long time if slave and master part were far away from each other. This<br \/>algorithm is now improved. The typical situation when this is observed is<br \/>when trimming the blank, some master surfaces are far away so as to not be in play<br \/>but may still be in the contact definition.<br \/><br \/><br \/>________________________ *CONSTRAINED ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Rework MPP support for *CONSTRAINED_MULTIPLE_GLOBAL<br \/>so that it works with more than just solid elements.<br \/><br \/>Fix MPP decomposition for some joint types.<br \/><br \/>Fix bug for *CONSTRAINED_SHELL_TO_SOLID &#8212; MPP only.<br \/><br \/>Fix input error when using large load curve ID for FMPH, FMT, FMPS in card 3<br \/>of *CONSTRAINED_JOINT_STIFFNESS with _GENERALIZED or _TRANSLATIONAL options.<br \/><br \/>Fix seg fault if using tables for FMPH of *CONSTRAINED_JOINT_STIFFNESS and if<br \/>the angle of rotation is less than the the abscissa of the table or load curves.<br \/><br \/>*CONSTRAINED_JOINT:<br \/>Fix for noncoincident joint node error warnings STR+65, STR+67, and<br \/>STR+72.\u00a0 Old data that used to run was error terminating.<br \/>Now, error termination happens only if both the old and new tolerances are exceeded.<br \/><br \/>Improve the precsion of spot weld constraints (*CONSTRAINED_SPOTWELD) to prevent possible<br \/>divide by zeroes when the inertia tensor is inverted.\u00a0 This affect the single precision<br \/>version only.<br \/><br \/>Fix for *CONSTRAINED_SPR2.<br \/>If the resultant normal directions of slave and master sheet<br \/>were not the same, high shear forces could develop initially.<br \/><br \/><br \/>________________________ *CONTROL ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>*CONTROL_TIMESTEP<br \/>Fix a bug whereby selective mass scaling (*CONTROL_TIMESTEP) was not properly initialized<br \/>in a simple restart.<br \/><br \/>________________________ *DATABASE ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>*DATABASE_NCFORC:<br \/>Modify output of ncforc file to support output in<br \/>a local coordinate system.\u00a0 If CID_RCF (field 8<br \/>on optional card C) is defined for a contact interface,<br \/>output the ncforc file in this coordinate system (so<br \/>that it matches the rcforc file).<br \/><br \/>MPP ncforc output: sum forces for slave nodes to fix possible<br \/>problems with shared nodes and symmetric contacts.<br \/><br \/>*CONSTRAINED_INTERPOLATION_SPOTWELD, *DATABASE_SWFORC:<br \/>Fix missing swforc output of spr welds &#8212; MPP only.<br \/><br \/>*DATABASE_BINARY_INTFOR:<br \/>Add support of surface energy output to intfor for contact types 4, 13 and 26<br \/>&#8212; MPP only.<br \/><br \/>*DATABASE_TRACER:<br \/>Fix bug for SPH tracer particle output &#8212; MPP only.<br \/><br \/>Fix incorrect output to disbout for discrete beams (*DATABASE_DISBOUT).<br \/><br \/>Fix stress\/strain output to elout which were in local system instead of global<br \/>when EOCS=2 in *CONTROL_OUTPUT and CMPLG=1 in *DATABASE_EXTENT_BINARY.<br \/>Resolve the conflicting input by giving priority to EOCS.<br \/><br \/>Fix incorrect output 0.0 for history variable #3, bulkq viscosity, of solids to<br \/>d3plot when HYDRO.gt.0 in *DATABASE_EXTENT_BINARY and when equation-of-state is used.<br \/><br \/>Fix non-functioning *DATABASE_SBTOUT and *DATABASE_DISCRETE keywords.<br \/><br \/>Fix incorrect coordinate system used for strains output to d3plot when CMPFLG=1<br \/>in *DATABASE_EXTENT_BINARY and MAXINT&lt;0 for orthotropic and anisotropic materials.<br \/><br \/>Fix inadvertent strain output to d3plot history variables when NODOUT=<br \/>ALL\/ALL_GL\/STRAIN\/STRAIN_GL or INTOUT=ALL\/STRAIN in *DATABASE_EXTENT_BINARY.<br \/><br \/>*DATABASE_ELOUT:<br \/>Fix elout stress output for shell element forms 23 and 24.\u00a0 The in-plane<br \/>averaging was incorrect causing wrong output.<br \/><br \/>Redo stress and strain output for thick shells.\u00a0 This should produce slightly different results<br \/>in the output files (not the solution) since some corrections were made to the local to global<br \/>transformation done for thick shell types 2 and 3.\u00a0 Forms 1 and 5 should not change.<br \/><br \/>*DATABASE_SECFORC:<br \/>Correct the sign of secforc data for thick shell forms 2, 3, and 5.<br \/>The force magnitude was correct but the sign wrong.<br \/><br \/>*DATABASE_ELOUT:<br \/>Fix eloutdet stress and strain output for thick shell form 5.\u00a0 It was<br \/>outputting nonsense.<br \/><br \/>Synchronize output time for intfor and d3plot databases.<br \/><br \/>Add *INTEGRATION&#8230; data to d3prop output.<br \/><br \/>Fix bug in d3plot if MSSCL option is defined in *DATABASE_EXTENT_BINARY.<br \/><br \/><br \/>________________________ *ELEMENT ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Fix a bug related to using superelements (*ELEMENT_DIRECT_MATRIX_INPUT) with explicit<br \/>and having null columns in the linear algebra system<br \/>due to improperly constructed model.<br \/><br \/>Output of midside node data to d3xxxx databases was incorrect in MPP.<br \/><br \/>Fix a bug for detailed element output (eloutdet) for 6-node or 4-node solid when ESORT of *control_solid &gt;0,<br \/>and for solid element type 15.<br \/><br \/>Fix &#8220;*** termination due to mass increase ***&#8217; error when using mass scaling with<br \/>*ELEMENT_MASS_PART.<br \/><br \/>Fix fix incorrect output of initial stresses and initial strains to dynain for<br \/>thick shells.<br \/><br \/>Fix incorrect reading of TIME on Card 3 of *ELEMENT_SEATBELT_SENSOR, SBSTYP=3<br \/>when using long=s on the execution line.<br \/><br \/>Error terminate with message, STR+1296, if same node is defined multiple times in<br \/>*ELEMENT_MASS_MATRIX.<br \/><br \/>Fix seg fault when using shell formulation 18,20,21 for implicit eigenvalue<br \/>analysis and when triangular shell elements are present.<br \/><br \/>Fix input error when using *ELEMENT_SHELL_SHL4_TO_SHL8.<br \/><br \/>Fix time step being set to zero after full deck restart for problems with discrete<br \/>elements.<br \/><br \/>Fix input error during adaptivity cycle when using *PART_ANNEAL with adaptivity.<br \/><br \/>Add warning message, STR+1286, when no mid-side nodes are defined for shell<br \/>element type 23 and 24.<br \/><br \/>Fix thick shell form 5 when used in implicit solutions with non isotropic materials.<br \/>The stiffness matrix was wrong due to incorrect transformations.<br \/><br \/>Fix the implicit stiffness of thin and thick shells when used with laminated shell<br \/>theory by assumed strain (LAMSHT=3,4,5 on *CONTROL_SHELL).\u00a0 Elements were either failing<br \/>to converge or converging more slowly due to the failure to adjust the stiffness matrix to<br \/>be consistent with the assumed strains which are the basis for the forces on the right side of<br \/>the equation.<br \/><br \/>Improve the accuracy of the Belytshko-Schwer resultant beam (form 2) in single<br \/>precision.<br \/><br \/>*DATABASE_EXTENT_BINARY, CMPFLG:<br \/>Rework the thick shell stress output routine.<br \/>The 4-point in-plane elements (forms 2 and 3) could not correctly<br \/>average the stress from the 4 points when outputting only 1 and when outputting<br \/>in the composite material direction.\u00a0 Therefore, I changed the order of the output<br \/>calculations to do averaging in the material direction rather than the global system.<br \/>This change has no effect on the solution, and should only affect stress output in<br \/>the material direction, not the global direction.<br \/><br \/>*CONTROL_SOLID, ESORT:<br \/>Suppress sorting of tetrahedral acoustic elements into non-acoustic tets.<br \/><br \/>Fix the NLOC option on *SECTION_SHELL for the BCIZ triangle elements (ELFORM=3)<br \/>and DKT triangles (ELFORM=17).<br \/>The offset was scaled by the solution time step so typically the offset was<br \/>much smaller than expected.<br \/><br \/>Fix implicit thick shell form 2 when used with *MAT_058.\u00a0 Since rev 81390,<br \/>the stiffness matrix has been wrong and convergence impossible.<br \/><br \/>Remove an inappropriate warning message (INI+161) for cable elements with<br \/>*MAT_071.<br \/><br \/>Fix the rigid body inertia calculation for 2D axisymmetric element<br \/>types 14, 15, 44, 46, and 47.\u00a0 While this affects the mass properties reported<br \/>to d3hsp, it likely has no effect on the solution.<br \/><br \/>Modify shell element form 16.\u00a0 The node 1 coordinates are now subracted from the<br \/>other nodal coordinates in double precision so the precision of the element is<br \/>independent of location in space.\u00a0 Some minor recoding of this part of the code<br \/>makes it slightly faster on Xeon64 even though there are 9 additional subtractions<br \/>per element per time step.\u00a0 Single precision results with shell section 16 will be<br \/>slightly different with this change but single precision results should be closer<br \/>to double precision.<br \/><br \/>Fix the long option of *ELEMENT_SHELL_COMPOSITE_LONG.\u00a0 A mistake in<br \/>keyword reading caused an erroneous KEY+157 error message.<br \/><br \/>Fix thick shell form 3 when used with an equation of state.<br \/>The pressure was not properly accounted for in the stress calculation.<br \/><br \/>Fix thick shell form 5 when used with equations of state.\u00a0 The equation of state pressure was being<br \/>calculated for only the last integration point, creating nonphysical deformation.<br \/>The material models fixed are 8, 9, 10, 11, 15, 17, 65, 88, 155, and 224.<br \/><br \/>*CONTROL_SHELL:<br \/>Fix an initialization problem with laminated shell theory when the data has some<br \/>shell or thick shell parts that use *PART_COMPOSITE or *INTEGRATION_SHELL and some others<br \/>that do not.\u00a0 It was possible for lamatinated shell theory data to be clobbered causing<br \/>unpredictable element behavior.<br \/><br \/>Add z-stress calculation for thick shell forms 1 and 2 for the material types 15, 34, 60, 98, 108, 115, 122,<br \/>125, 130, 137, 165, 170, 172, 203, 204, 214, 222, 234, 235, 244, and 255.\u00a0 Prior to this change,<br \/>strange deformation would likely occur.<br \/>Note: This z-stress is not part of a full 3D stress update as it is for thick shell formulation 3 and 5.<br \/><br \/><br \/>________________________ *FREQUENCY_DOMAIN ___________________\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>*FREQUENCY_DOMAIN_SSD, _RANDOM_VIBRATION, _RESPONSE_SPECTRUM:<br \/>Fix the variable names for beam data written to elout_ssd, elout_psd,<br \/>and elout_spcm.<br \/><br \/>*FREQUENCY_DOMAIN_RANDOM_VIBRATION:<br \/>Fix problem where random vibration analysis was not activated after eigenvalue analysis due to<br \/>mismatch of termination time and time step size specified in *CONTROL_IMPLICIT_GENERAL.<br \/><br \/>*FREQUENCY_DOMAIN_FRF:<br \/>Fix a bug in writing Modal contribution factor.<br \/><br \/>*FREQUENCY_DOMAIN_ACOUSTIC_BEM:<br \/>Fix memory allocation for pressure output array in bem acoustic analysis for the case nfreq=0.<br \/><br \/>*FREQUENCY_DOMAIN_ACOUSTIC_FEM:<br \/>Fix a bug in initialization of the load curve in FEM Acoustics, when the boundary condition<br \/>is given by transient analysis.<br \/><br \/>*FREQUENCY_DOMAIN_RANDOM_VIBRATION:<br \/>Fix a bug in computing rms of displacement, in case the PSD integration provides a negative area.<br \/><br \/>*FREQUENCY_DOMAIN_RANDOM_VIBRATION:<br \/>Fix a bug in running random vibration with time history load.<br \/><br \/>*FREQUENCY_DOMAIN_FRF, *FREQUENCY_DOMAIN_SSD:<br \/>Fix a bug in running frf and ssd with pressure loading.<br \/><br \/>*FREQUENCY_DOMAIN_RESPONSE_SPECTRUM:<br \/>Fix a bug in running response spectrum analysis, related to scaling of modal stresses.<br \/><br \/>Fix a bug in outputing solid types with midside nodes to binary frequency domain databases<br \/>when tet10=1 in *CONTROL_OUTPUT.<br \/><br \/>*FREQUENCY_DOMAIN_FRF:<br \/>Fix bug in running frf with 8-node quadratic quadrilateral shells.<br \/>Fix a bug in running frf when 10-noded tetrahedrons are present.<br \/><br \/><br \/>________________________ *INITIAL ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Fix incorrect initial velocities when using *INITIAL_VELOCITY_GENERATION with<br \/>irigid=1 and *PART_INERTIA with xc=yc=zc=0 and nodeid&gt;0 with *DEFINE_TRANSFORMATION.<br \/><br \/>Fix incorrect initial velocity when using *INITIAL_VELOCITY_GENERATION with<br \/>NX,NY,NZ defined and also *PART_INERTIA is used.<br \/><br \/>Fix incorrect start time for initialization of velocities when PHASE=0 in<br \/>*INITIAL_VELOCITY_GENERATION and *INITIAL_VELOCITY_GENERATION_START_TIME<br \/>is present.<br \/><br \/>Fix stress initialization with *INITIAL_STRESS_SECTION for tetahedron formulation 17.<br \/><br \/>*INITIAL_VELOCITY:<br \/>Fix rigid body velocity initialization for the case of pure translation.<br \/>Nonzero stress could be generated in parts that shared nodes with rigid bodies.\u00a0 The<br \/>problem was that the calculation to initialize rigid body velocities and rotations is<br \/>susceptible to round-off error such that the rigid body has tiny initial rotations which<br \/>lead to stress in the deformable elements.<br \/><br \/>*INITIAL_STRESS<br \/>Fix thick shell stress initialization which was improperly initializing the stress data<br \/>data for for thick shell forms 2 and 3.<br \/>Also correct the warning message for shell and thick shell stress initialization<br \/>when the number or location of thickness integration points in the initialization data does not<br \/>match the elements to be initialized.\u00a0 This is messages INI+143, INI+144, INI+145, INI+146, and<br \/>INI+147.\u00a0 I also made a similar correction for INI+213 which is related to initial failure.<br \/><br \/><br \/>________________________ *LOAD ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Add load curves for dynamic relaxation for *LOAD_THERMAL_VARIABLE.<br \/><br \/>Fix input error when using *LOAD_MOVING_PRESSURE with &gt;100 Card 2&#8217;s.<br \/><br \/>Fix incorrect stress initialization with dynamic relaxation when using<br \/>*LOAD_SEGMENT_SET with AT.ne.0.<br \/><br \/>*LOAD_SEGMENT; *CONTROL_ADAPTIVE:<br \/>Fix bug whereby loads on non-adapting parts were affected when<br \/>3D adaptivity is invoked.<br \/><br \/><br \/>________________________ *SENSOR ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Moment of rotational discrete element can be traced by *SENSOR_DEFINE_ELEMENT,<br \/>with ETYPE=DISC-ELE and CTYPE=FORCE<br \/><br \/>SENSOR referred to by *DEFINE_CURVE_FUNCTION returns a value of:<br \/>\u00a0\u00a0\u00a0 &#8211; &#8220;0&#8221; when the status of ctrlid is OFF and TYPE is not FUNCTION,<br \/>\u00a0\u00a0\u00a0 &#8211; &#8220;TYPEID&#8221; when the status of ctrlid is OFF and TYPE is FUNCTION<br \/><br \/>Fix a bug when using *SENSOR_DEFINE_FORCE to trace the pressure of *AIRBAG_ADIABATIC.<br \/><br \/><br \/>________________________ *MAT ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Fix bug in hysteretic behaviour of reinforcement in *MAT_174. Occasionally,<br \/>it was possible for the Bauschinger effect on re-loading to<br \/>be lost &#8211; for that half-cycle, the behaviour would become<br \/>elastic-perfectly-plastic. This bug occurred only rarely.<br \/><br \/>MAT_082_RCDC:<br \/>&#8211;\u00a0 Fix bug where damage from load curves was incorrectly calculated for solid elements.<br \/>&#8211;\u00a0 Fix error in scaling of averaged nodal pressure for solid formulation 13.<br \/><br \/>Check diagonal terms of C-matrix of *MAT_002\/MAT_{OPTION}TROPIC_ELASTIC and<br \/>error terminate with message, STR+1306, if any of them are negative.<br \/><br \/>Fix incorrect stress initialization of *MAT_57\/MAT_LOW_DENSITY_FOAM using dynain<br \/>file with *INITIAL_STRESS_SOLID when NHISV is equal to the number of history<br \/>variables for this mat 57.<br \/><br \/>Fix error when using *MAT_144\/MAT_PITZER_CRUSHABLE_FOAM with solid tetahedrons type 10.<br \/><br \/>Fix incorrect writing of material data to dyna.str for *MAT_SEATBELT when<br \/>using long=s on the execution line.<br \/><br \/>Fix out-of-range forces after dynamic relaxation when using VP=1 for<br \/>*MAT_PIECEWISE_LINEAR_PLASTICITY and non-zero strain rate parameters, C &amp; P, and<br \/>the part goes into plastic deformation during dynamic relaxation.<br \/><br \/>Fix incorrect *MAT_PLASTICITY_COMPRESSION_TENSION\/MAT_124 yield stresses for shells<br \/>when SRFLAG=2.\u00a0 The yield stress was not scaled correctly according to strain rate<br \/>curves, LCSRC and LCSRT.<br \/><br \/>Fix incorrect results when using *DEFINE_TABLE for LCSS of<br \/>*MAT_89\/MAT_PLASTICITY_POLYMER.<br \/><br \/>Fix incorrect results when using *MAT_MUSCLE\/MAT_156 with *PART_AVERAGED for the<br \/>truss elements.<br \/><br \/>Fix seg fault when using *MAT_NONLOCAL with nhv &gt; 16 and also output<br \/>warning message, STR+1291, if the largest history variable # is &gt; than<br \/>the number of stored history variables(including plastic strain).<br \/><br \/>Fix effect of shear correction factor, SHRF, in *SECTION_SHELL and *PART_COMPOSITE<br \/>on *MAT_ORTHO_ELASTIC_PLASTIC\/*MAT_108.<br \/><br \/>Fix incorrect results when using\u00a0 *MAT_JOHNSON_COOK\/*MAT_15 with thick shell<br \/>formulations 3 and 5.<br \/><br \/>Modify *MAT_221 (MAT_ORTHOTROPIC_SIMPLIFIED_DAMAGE) to correct the damage<br \/>behavior.\u00a0 Prior to this fix, damage was applied to new increments of stress, but<br \/>not the stress history, so matrial softening was not possible.\u00a0 Since damage is<br \/>applied to the constitutive matrix, it was necessary to switch the stress update<br \/>from a rate form (rate-of-deformation) to an total strain form.\u00a0 The total strain<br \/>used is the accumulated increments from the rate-of-deformation.\u00a0 Since the material<br \/>behavior is elastic, the results are about the same except when damage occurs.<br \/><br \/>Fix error in inititialization that could cause a problem with *MAT_FABRIC&#8217;s RGBRTH<br \/>parameter.\u00a0 If there was more than one fabric material model, and all data was the<br \/>same except for RGBRTH, the materials could be merged causing the RGBRTH of the<br \/>second material to be ignored.<br \/><br \/>Add support for *MAT_096 for several solid element types including 3, 4, 15, 18, and\u00a0 23.<br \/>Also, reduce the liklihood of numerical overflow in *MAT_096.\u00a0 This is really a bug fix<br \/>because we did not terminate cleanly.<br \/><br \/>Fix the use of uninitialized curve slope values in the implicit element stiffness<br \/>matrix when the 6 DOF spring material (*MAT_119) is used with beam form 6.\u00a0 The slopes<br \/>have now been set to zero for degrees of freedom for which no curve is defined.<br \/><br \/>Enable 5 newer materials and\/or thick shell materials to be used with the<br \/>material angle field of *PART_COMPOSITE or *PART_COMPOSITE_TSHELL.\u00a0 The new<br \/>materials are 5 40, 136, 219, and 253.<br \/><br \/>Fix type 6, 7, 9 hourglass control for *MAT_187 and *MAT_232.<br \/><br \/>Fixed calculation of failed layers in reading SOFT (crashfront) parameter for *MAT_261\/262.<br \/><br \/>Fix keyword reading of *MAT_124 constants EC and RPCT.<br \/>It was not working if they were defined under *PARAMETER.<br \/><br \/>New option for strain rate averaging in *MAT_083.<br \/>Exponential moving average can be invoked by setting SRAF&lt;0,<br \/>where abs(SRAF) represents the degree of weighting decrease.<br \/><br \/>New option for unloading behavior in *MAT_083.<br \/>If TBID&lt;0 or HU&gt;0 (&#8220;damage formulations&#8221;), unloading is rate dependent<br \/>by default. This can now be changed to &#8220;rate independent&#8221; by new<br \/>input parameter RIULD on Card 5, Column 2. This seems to help noise<br \/>reduction in some cases.<br \/><br \/>Added new option to *MAT_106 for shell and solid elements.<br \/>Load curve LCFAIL (Card 4, Column 4) refers to<br \/>plastic failure strain as function of temperature.<br \/><br \/>Fix combination of implicit analysis with *MAT_057<br \/>and solid element types 4, 16, or 17.<br \/><br \/>Add new parameter &#8220;EXPON&#8221; to *MAT_083 on optional card 5, column 1.<br \/>This is an exponent in the damage function for unloading when HU&gt;0:<br \/>\u00a0\u00a0\u00a0 d = (1-HU) * ( 1 &#8211; (Wcur\/Wmax)**SHAPE )**EXPON<br \/><br \/>Add a new failure indicator as history variable #10 to *MAT_123.<br \/>Add triaxiality as history variable #11 to *MAT_123.<br \/><br \/>Fix for combination of standard failure criteria and GISSMO<br \/>with LCREGD&gt;0 in *MAT_ADD_EROSION.<br \/><br \/>Correct internal energy calculation in *MAT_ADD_EROSION<br \/>damage model GISSMO for thin and thick shell elements.<br \/><br \/>Fix for *MAT_ADD_EROSION, damage model GISSMO. Option NUMFIP&lt;0<br \/>was not working correctly for the combination with *MAT_036.<br \/><br \/>Fix for *MAT_083 when unloading is controlled via TBID&lt;0.<br \/>In rare cases it was possible that the lowest curve in the table<br \/>was used for rate dependent stress evaluation, but it should only<br \/>be used for unloading response.<br \/><br \/>Parameter SCLMRR of *DEFINE_CONNECTION_PROPERTIES was not working<br \/>for spotweld assemblies\/clusters. This is now fixed.<br \/><br \/>Correct problem with the number of history variables<br \/>in user materials with solid elements when options INTOUT\/NODOUT<br \/>of *DATABASE_EXTENT_BINARY are set to &#8220;STRAIN&#8221; or &#8220;ALL&#8221;.<br \/><br \/>Fix a bug that prevented *MAT_POWDER from being compressed beyond a certain point.<br \/><br \/><br \/>________________________ ALE ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Fix bug for *ALE_ESSENTIAL_BOUNDARY when defined by parts; wrong surface segments<br \/>generated for pentahedral and tetrahedral elements.<br \/><br \/><br \/>________________________ SPH ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>*DEFINE_ADAPTIVE_SOLID_TO_SPH:<br \/>Fix bug affecting tet and wedge solid elements adaptively transformed into SPH particles.<br \/><br \/><br \/>________________________ *IMPLICIT ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Fix reading of d3kil file to allow for implicit switches<br \/>with more than 4 characters.<br \/><br \/>*CONTROL_IMPLICIT_INERTIA_RELIEF, *CONTROL_DYNAMIC_RELAXATION:<br \/>Allow the case of dynamic relaxation with implicit<br \/>using inertia relief and then switching to explicit.<br \/><br \/>Fix Implicit&#8217;s treatment of rigid bodies after restart of an<br \/>adaptive simulation (*CONTROL_ADAPTIVE).<br \/><br \/>*CONTROL_IMPLICIT_MODAL_DYNAMIC:<br \/>Correct reading of d3eigv database for modal dynamics in the<br \/>presence of higher order elements and tshell elements.<br \/><br \/>*CONTROL_RIGID:<br \/>Turn off LaGrange Multiplier Treatment of joints when Implicit is active.<br \/><br \/>*CONTROL_IMPLICIT_MODES:<br \/>Enhance the computation of the superelement inertia matrix in the presence of<br \/>rigid bodies.\u00a0 The mass matrix multiplication has to involve the mass on the<br \/>slave nodes for this computation which is unlike other applications in LS-DYNA.<br \/><br \/><br \/>________________________ Thermal ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>*CONTROL_ADAPTIVITY:<br \/>MPP fix for possible deadlock<br \/>when using adaptivity together with thermal coupling.<br \/><br \/>Enable thick shells to work with thermal materials.\u00a0 A flaw in the calculation<br \/>of temperatures meant that thermal materials would not behave correctly<br \/>except when done using *MAT_ADD_THERMAL_EXPANSION.<br \/><br \/>Fix thick shell elements when used with thermal materials and there is a variation in<br \/>the temperature field.\u00a0 The temperature variation in the element was not being calculated and<br \/>all integration points were assigned the same temperature.<br \/><br \/>Flux was not being calculated for *MAT_THERMAL_CWM<br \/>when a time function was used for CWM.<br \/><br \/>Fix improper data in d3plot causing problems when using *LOAD_THERMAL_D3PLOT.<br \/><br \/><br \/>________________________ MPP ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Incorporate new element cost routines for purposes of decomposition.<br \/>New pfile options are:<br \/>\u00a0\u00a0 decomp { newcost }\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 = use new element costs<br \/>\u00a0\u00a0 decomp { shellcosts filename }\u00a0 = read shell cost info from &#8216;filename&#8217;<br \/>\u00a0\u00a0 decomp { solidcosts filename }\u00a0 = read solid cost info from &#8216;filename&#8217;<br \/>There is no facility for generating the shellcosts or solidcosts<br \/>data files &#8212; those will have to be done with the R8.0 or later<br \/>versions.<br \/><br \/>Fix issue with full deck restart in case<br \/>some processors do not have any contact interfaces.<br \/><br \/>Fix MPP decomposition issue<br \/>in case there are 2D sliprings.<br \/><br \/>Fix MPP adaptivity for very large models: the<br \/>reading of the adaptive dump file was not<br \/>working properly for files over 8GB.<br \/><br \/>Fix a bug related to *PARAMETER and restart<br \/>that was resulting in parameters not being<br \/>properly redefined on the first restart in MPP<br \/>on processors other than 0, or on the second and<br \/>subsequent restarts in SMP and MPP (all processors).<br \/>This is only a problem if there are<br \/>*DEFINE_CURVE_FUNCTION definitions that use<br \/>parameters.<br \/><br \/>Fix MPP problem of creating a pre-decomposition file<br \/>while using a jobid.<br \/><br \/>If a structured output file is being created,<br \/>echo a copy of all pfile data (pfile + internally<br \/>generated from the *CONTROL_MPP keywords) to a file<br \/>named &lt;jobid&gt;pfile.log.\u00a0 This makes it easy for<br \/>decomposition related keywords to be used with<br \/>the structured version of the file.<br \/><br \/>*CONTROL_DYNAMIC_RELAXATION:<br \/>MPP fix for dynamic relaxation<br \/>initialization in polar coordinates.<br \/><br \/>Fix INTERFACE_LINKING in MPP.<br \/><br \/>For small restart job, use the memory size stored in dump file instead<br \/>of memory specificed on command line.<br \/><br \/>*DEFINE_HAZ_PROPERTIES:<br \/>Fix bug for HAZ input deadlock &#8212; MPP only.<br \/><br \/>*DEFINE_SPH_DE_COUPLING:<br \/>Fix bug for SPH + DES coupling &#8212; MPP only.<br \/><br \/>Add support for *DEFINE_DE_BY_PART &#8212; MPP only.<br \/>Overrides *CONTROL_DISCRETE_ELEMENT for specified part IDs.<br \/><br \/>Fix hang up when using *DEFINE_CURVE_FUNCTION with element function<br \/>BEAM(id,jflag,comp,rm) and running MPP with np&gt;1.<br \/><br \/>Fix bug whereby for *CONTROL_MPP_IO under Windows OS, user<br \/>had to have administrative privileges to write tmp file on<br \/>root drive. For Windows only.<br \/><br \/><br \/>________________________ Miscellaneous ___________________\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<br \/><br \/>Fix problem of LOCAL parameters and adaptivity.<br \/>Because the adaptive process merges all the include files,<br \/>the &#8220;locality&#8221; of these was being lost.\u00a0 Two new keywords are<br \/>introduced (*PARAMETER_PUSH and *PARAMETER_POP) and are used<br \/>to work around this issue.<br \/><br \/>When using *INCLUDE_TRANSFORM, offset IDs of sensors, nodes, elements and parts referred<br \/>to in an included *DEFINE_CURVE_FUNCTION by IDROFF, IDNOFF, IDEOFF and IDPOFF,respectively.<br \/><br \/>Fix a bug for *SET_SEGMENT_GENERAL that happens when option=PART is used to<br \/>define segment set of a part of solid element<br \/><br \/>Fix incorrect shell set generated when using *SET_SHELL_GENERAL with OPTION=PART.<br \/><br \/>Fix *NODE_MERGE_SET which gives incorrect set of nodes.<br \/><br \/>Fix input error, KEY+517, for null part set when using *SET_PART_LIST_GENERATE and<br \/>*PART_MOVE together.<br \/><br \/>The delay time, TIME3, in *DEFORMABLE_TO_RIGID_AUTOMATIC is not correctly<br \/>implemented. The TIME3 in the last\u00a0 *DEFORMABLE_TO_RIGID_AUTOMATIC was used<br \/>instead.<br \/><br \/>Fix incorrect sign of result returned from *DEFINE_CURVE_FUNCTION&#8217;s<br \/>JOINT(id,jflag,comp,rm) if jflag=1.<br \/><br \/>Fix input error when using Q=REMAP.<br \/><br \/>Error terminate the input if the abscissa values of *DEFINE_TABLE are the same.<br \/><br \/>Fix input error when parameter is present in cards following *COMMENT<br \/>keyword and before the next &#8216;*&#8217; keyword.<br \/><br \/>Fix NaNs triggered by 100th percentile *COMPONENT_GEBOD.<br \/><br \/>Make improvements and corrections to long format input.<br \/><br \/>Fix bug if *DEFINE_CURVE is used to define adaptivity level.<br \/>See IREFLG in *CONTROL_ADAPTIVITY.<br \/><br \/>If any node\/element is encrypted and PSETID in *DATABASE_BINARY_D3PLOT is set,<br \/>we will disable dynain output.<br \/><br \/>*CONTROL_ADAPTIVE:<br \/>Fix bug whereby element IDs of non-adaptiing parts changed when<br \/>3D adaptivity was invoked.<\/p>\r\n","protected":false},"excerpt":{"rendered":"<p>\u6628\u65e5\u30012\/5 R7.1.2\u306e\u5168\u30e2\u30b8\u30e5\u30fc\u30eb\u304cLSTC\u30b5\u30a4\u30c8\u306b\u30a2\u30c3\u30d7\u3055\u308c\u3001\u516c\u5f0f\u30ea\u30ea\u30fc\u30b9\u3055\u308c\u305f\u3002\u4ee5\u4e0b\u306e\u30ea\u30ea\u30fc\u30b9\u30ce\u30fc\u30c8\u3092\u3055\u3063\u3068\u898b\u3066\u3082\u308f\u304b\u308b\u3088\u3046\u306b\u3001\u65b0\u6a5f\u80fd\u306f\u6b86\u3069\u306a\u304f\u3066\u3001R7.1.1\u306b\u5bfe\u3059\u308bFIX=\u30d0\u30b0\u4fee\u6b63\u7248\u3067\u3042\u308b\u3002Windows6 [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":[],"categories":[5],"tags":[],"_links":{"self":[{"href":"https:\/\/www.advancae.com\/blog1\/wp-json\/wp\/v2\/posts\/3375"}],"collection":[{"href":"https:\/\/www.advancae.com\/blog1\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.advancae.com\/blog1\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.advancae.com\/blog1\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.advancae.com\/blog1\/wp-json\/wp\/v2\/comments?post=3375"}],"version-history":[{"count":1,"href":"https:\/\/www.advancae.com\/blog1\/wp-json\/wp\/v2\/posts\/3375\/revisions"}],"predecessor-version":[{"id":3376,"href":"https:\/\/www.advancae.com\/blog1\/wp-json\/wp\/v2\/posts\/3375\/revisions\/3376"}],"wp:attachment":[{"href":"https:\/\/www.advancae.com\/blog1\/wp-json\/wp\/v2\/media?parent=3375"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.advancae.com\/blog1\/wp-json\/wp\/v2\/categories?post=3375"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.advancae.com\/blog1\/wp-json\/wp\/v2\/tags?post=3375"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}