Structural Mechanics Of Steam Turbines: Facing Challenges .

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Structural Mechanics of Steam Turbines:Facing challenges in FE-postprocessing withSTARpostDr. Benjamin Kloss-GroteSiemens AG, Energy SectorFossil Power GenerationRheinstr. 100, 45478 Muelheim, GermanyAbstract: In isothermal machine parts, the location of the highest stress can often be regarded asthe critical location regarding the structural integrity. Steam turbines, like many other products inhot turbomachinery possess an inhomogeneous temperature distribution during operation. As therelevant material properties are temperature dependent, the stress level is no longer a sufficientindicator of the mechanical integrity: Low stress levels in high temperature regions can lead tothe same or a higher mechanical utilization than high stress levels in colder regions. This effectposes a challenge for FE post processing because temperatures, material properties and stresslevels need to be considered together for an assessment of the mechanical integrity. Abaqus offersthe user subroutine UVARM to calculate user defined variables that can meet this challenge, but,especially for long lasting creep calculations, a pure post processing approach is much moreconvenient.This paper describes how Siemens Energy large scale steam turbines R&D has faced thischallenge by developing ‘STARpost’ (i.e. Steam Turbine Analysis Routine – postprocessing), anefficient post-processing-plug-in for Abaqus/CAE: ‘STARpost’ automatically reads in the relevanttemperature-dependent material data, assesses the existing stresses against the varying allowablestresses (for components with different materials and different calculation steps), provides manymore field outputs beneficial for hot turbomachinery R&D and an environment for convenientvisualization.Keywords: Creep, Elasticity, Failure, Heat Transfer, Mechanical Integrity, Output Database,Plasticity, Postprocessing, Python Scripting, Plug-In, Strength Assessment, Thermal Stress,Turbines, Visualization.1. Introduction1.1Steam TurbinesLarge scale Siemens Steam Turbines are installed in steam power plants, combined cycle powerplants and nuclear power plants with a power output between 90 MW and 1900 MW per turboset(example see Fig. 1).2012 SIMULIA Community Conference1

Figure 1. Siemens Steam Turbine SST5-6000 (Power Output 600 MW; 1 highpressure steam turbine, 1 intermediate pressure steam turbine, 2 low pressuresteam turbines and 1 generator). Image courtesy of Siemens AG.An essential part in the development of new steam turbines is to ensure the mechanical integrity ofall components. Steam turbines have to withstand a variety of transient and steady-state loadswhich can be divided into primary (i.e. force/pressure based, centrifugal or gravity loads) andsecondary (thermal based; self equilibrating) loads. With main steam parameters of up to 600 Cand 300 bar, reheat steam temperatures of up to 620 C (Siemens AG Energy Sector, 2010) and anoperational lifetime of over 25 years, creep effects have to be taken into account for the long termbehavior of these components. Due to the complexity of geometries and loads, 2D and 3D finiteelement analyses are applied for for example heat transfer, static and creep analyses.This paper is focused on the mechanical integrity of large components like the casings and therotors of high and intermediate pressure steam turbines (also called ‘hot’ steam turbines, i.e.operating at elevated temperatures) under static loads and long-term steady-state loads includingcreep behavior.1.2Standard load cases in scope of this paperStandard load cases to analyze the static and creep behavior of the large ‘hot’ steam turbinecomponents with Abaqus/Standard are for exampleA.Heat Transfer: The steady state temperature distribution in the assembly is derived by a heattransfer analysis with a selection of surface film interactions, thermal conductance contactinteractions, radiation interactions and temperature boundary conditions, see (Abaqus/CAEUser's Manual, 2010).B.Static Primary elastic: For this elastic analysis step, the steady state temperature distributionfrom the heat transfer analysis is read into the structural analysis which contains allmechanical loads (steam pressures, forces, moments etc.). As no secondary (i.e. thermalbased) loads are taken into account, no thermal expansion is considered in the materialmodels for this step.22012 SIMULIA Community Conference

C.Static Primary Secondary elastic: The same conditions as for B apply – now including thethermal expansion in the material model.D.1 Static Primary Secondary elastic-plastic: The same conditions as for C apply – nowincluding elastic-plastic material behavior.D.2 Creep Primary Secondary elastic-plastic-creep: The creep step follows step D.1 with timepoints or intermediate steps at interesting times (for example maintenance intervals). Thetotal creep time is the required operational lifetime of the steam turbine.1.3Creep basics(Naumenko and Altenbach, 2007) define creep in the context of uniaxial homogenous stress statesin material testing as ‘the progressive time-dependent deformation under constant load andtemperature’. For creep in structures, they offer a broader definition: i.e. ‘time-dependent changesof strain and stress taking place in structural components as a consequence of external loading andtemperature’. For further general creep basics see for example (Betten, 2008).For the strength assessment of mechanical designs, two temperature ranges have to be considered:In the ‘non creep range’, the nominal design stresses can be determined using time independentmaterial characteristics. In the (high temperature) creep range, this is no longer the case (DIN EN13445-3, 2010) and the creep behavior has to be taken into account. These two ranges can beseparated by the intersection temperature Ti – at the intersection of the yield strength Rp0.2,T andthe creep rupture strength for 1e5h of creep Rm,1e5h,T (see Figure 2):Figure 2. Determination of the creep range with the intersection temperature Ti(Example: high chromium cast steel; explanations in the text).Several approaches exist for modeling the viscoplastic material behavior during creep. Dependingon the problem and the required accuracy of the results, different approaches are used in steamturbine structural mechanics: A simple approach is the Norton-Bailey-law (Bailey, 1930; Norton,1929) for (secondary) steady-state creep (Equation 0, sometimes called power law creep law) in itstime-hardening formulation cr A1 A t A23,(0)with the (uniaxial) creep strain , stress , creep time t and the three temperature dependent,material specific creep constants A1, A2 and A3 (Naumenko and Altenbach, 2007). More advancedapproaches include for example the Garofalo creep law (Garofalo, 1963) and many others (see forexample (Gorash, 2008)).cr2012 SIMULIA Community Conference1

1.4Terminology for the strength assessmentIn a standard assessment of the mechanical integrity of an assembly, existing stresses (orexisting strains) are assessed against allowable stresses (or allowable strains)! existing allowable Material Strength,SFallowable(1)whereby the allowable stresses can be derived from the material strength (for example yieldstrength Rp0.2,T, ultimate tensile strength Rm,T, creep rupture strength Rm,t,T etc., with temperature Tand creep time t), divided by the allowable safety factor SFallowable (see Equation 1). The allowablesafety factor, sometimes called required safety factor, design safety factor or design factor, is ingeneral specified for different stress categories like membrane or bending stresses by experience,company regulations or external standards. To confirm the mechanical integrity, the inequalityrelation in Equation 1 has to be fulfilled.Often, it is not only necessary to confirm Equation 1 to be true, but to determine the degree inwhich the existing stress in the assessed design ‘uses up’ the allowable stress. In this paper, thismetric is called (existing) safety utilization SU and defined as (Equation 2)SU SU existing existing SFallowable existing. allowable Material Strength(2)The safety utilization has the dimension of 1. A safety utilization of 0% implies that there is noload present. The mechanical integrity according to Equation 1 is confirmed if the safetyutilization shows values between 0% and 100%. For safety utilizations greater than 100%, thestructure fails under the given circumstances.With the definition of the existing safety factor SFexisting, (sometimes also called realized safetyfactor) (Equation 3)SFexisting Material Strength existing,(3)the strength assessment in Equation 1 can be written as (Equation 4)!SFexisting SFallowable .(4)(Be aware of the changed inequality sign in comparison to Equation 1.)Especially for non-isothermal FE post processing, it is very effective to define the reciprocal valueof the existing safety factorMU MU existing 1SFexisting existingMaterial Strength(5)and call it (existing) material utilization MU. Safety utilization and material utilization depend oneach other according to Equation 6, derived from Equation 5 and 2:42012 SIMULIA Community Conference

SU MU SFallowable ,(6)To derive allowable values for the safety utilization, the remarks below Equation 2 lead toEquation 7:SU allowable 100% .(7)The allowable material utilization can be derived from Equation 7 and 6 (Equation 8):MU allowable 1SFallowable,(8)The strength assessment Equation 1, written for the safety utilization, reads (Equation 9)!SU existing SU allowable 100% ,(9)and for the material utilization (Equation 10)!MU existing MU allowable 1SFallowable.(10)The respective definitions have been added in Equations 11 and 12 in order to provide a twoequation-summary of the utilization-based strength assessments:SU existing MU existing existing SFallowable!Material Strength existingMaterial Strength! SU allowable 100% , MU allowable 1SFallowable(11).(12)For the strength assessment of isothermal assemblies, Equations 9 to 12 (i.e. the utilization basedformulation) do not present any significant advantage in comparison to Equation 1 (the stressbased formulation) other than a scaling of the results, because the material strength is a constantfor one material over the whole assembly. The great advantages for non-isothermal assemblies inFE post processing will be presented in Chapter 2.2. The ChallengeThe structural analyst who wants to perform strength assessments for steam turbines at elevatedtemperatures (for example with load cases according to Chapter 1.2) faces several challengesduring his or her FE analysis:The illustration example selected for this paper represents the upper part of an inner casing of aSiemens intermediate pressure (IP) steam turbine with operational temperatures below and withinthe creep range (the blading is not part of this analysis).2012 SIMULIA Community Conference1

2.1Inhomogeneous temperature distribution prevents stress basedassessmentsFor an isothermal assembly, the (existing) stress results can be assessed against one single value ofthe allowable stress (Equation 13, with the assumption of a constant safety factor):! existing ( x, y, z ) allowable Material Strength const ,SFallowable(13)This can be easily performed in Abaqus/CAE during post processing for example by setting theupper limit of the contour plot options to the allowable stress and/or using isosurface view cuts(see (Abaqus/CAE User's Manual, 2010)): Grey/displayed areas exceed the allowable stress limit.Critical locations can be therefore easily identified.For assemblies with a non-uniform temperature distribution, the allowable stress varies over thewhole assembly with the temperature, because the material strength varies with the temperature.! existing ( x, y, z ) allowable ( x, y, z ) Material Strength(x, y, z ),SFallowable(13)In Figure 3, the contour plot of the equivalent stress (von Mises stress) is shown for the illustratedexample with an inner casing of an intermediate pressure (IP) Siemens Steam Turbine.Figure 3. Equivalent stress distribution during steady-state operation in the upperpart of the inner casing of an intermediate pressure (IP) steam turbine [left: outsideview, right: inside view].Inside the turbine at the bladepath, the equivalent stresses remain almost constant.The steady-state temperature distribution (NT11) of the assembly, derived from the heat transferanalysis, is pictured in Figure 4: This temperature distribution is clearly non-isothermal, so thematerial strength of Equation 13 varies spatially according to Figure 2 and Figure 4.62012 SIMULIA Community Conference

Figure 4. Non-isothermal temperature distribution in steady-state operation of theinner casing of an IP steam turbine.Therefore, the stress level is no longer a sufficient indicator of the mechanical integrity: Lowstress levels in high temperature regions can lead to the same or a higher mechanical utilizationthan high stress levels in colder regions. In addition, stress redistribution may also change themechanical utilization along a critical cross section.The only effective way to assess the mechanical integrity of these assemblies is to apply aprocedure that automatically calculates the temperature dependent allowable stress (or materialstrength) for every node (or integration point) of the assembly and assesses the existing stressagainst it. Here, the definitions of the safety utilization SU or the material utilization MU (seeChapter 1.4) come in very handy for a strength assessment (Equation 14 and 15)SU existing ( x, y, z ) MU existing ( x, y, z ) existing ( x, y, z ) SFallowable!Material Strength( x, y, z ) existing ( x, y, z )Material Strength( x, y, z ) SU allowable 100% ,! MU allowable 1SFallowable(14),(15)because the spatial dependency is contained in one single expression on the left side of theequation. The allowable value on the right side has become a constant in this formulation(assumption for Equation 14 and 15: SFallowable const). This allows for easy visualization of criticallocations by using the limits in contour plot options and isosurface view cuts.To conclude it can be stated that for strength assessments of non-isothermal assemblies, new fieldoutputs need to be created, the SU or MU.2.2Material strength is not contained in inp and ODBFor strength assessments in the creep range, one relevant material strength is the creep rupturestrength Rm,t,T. This material property is not part of the common material models in Abaqus.Therefore it cannot be included in the input file and it is subsequently not available for the solverand finally not in the ODB for post processing.Hence the creep rupture strength needs to be made available to the algorithm that calculates theSU or the MU by a different way than the input file. (This applies as well for rupture strains instrain assessments, which have not been mentioned before.)2012 SIMULIA Community Conference1

2.3Assemblies with more than one materialIf more than one material is used in the assembly, the complexity increases. The calculation of theSU or the MU requires the knowledge of the material association for each element. Simple postprocessing approaches could involve the use of display groups for each material. This approach a)becomes very tedious with an increasing number of materials. In addition, it is b) always apossible quality threat for the assessment if the assembly is not evaluated with a completeoverview but only in individual pieces of the whole puzzle: There is the risk that important effectsat the intersection of two materials can be overlooked or not properly understood.2.4Many frames need to be evaluatedIt can be concluded from Chapter 1.2, that the strength assessment of ‘hot’ steam turbines requirestaking many analysis frames into account. An automatic evaluation procedure has to support that.2.5Many different output variables necessaryMany different stress outputs (for example equivalent stress, principal stresses, shear stresses etc.)need to be able to be taken into account – depending on the expected failure mechanism. Anautomatic evaluation procedure has to support that.2.6Varying allowable safety factorsStandards relevant for the mechanical design of steam turbines provide different safety factors fordifferent materials (e.g. ductile vs. brittle), for different material models (e.g. elastic vs. elasticplastic), for different load cases (e.g. primary vs. primary secondary loads), for different locationsin an assembly (e.g. local vs. global location), for different temperatures in an assembly (e.g. creepvs. no creep range), for different categories of linearized stresses (e.g. membrane vs. bending vs.peak stresses) etc.Therefore, not only the existing stresses and material strength vary spatially, but also the allowablesafety factor. The utilization based strength assessment equations with varying safety factors looklike this (Equations 16 and 17):SU existing ( x, y, z ) MU existing ( x, y, z ) existing ( x, y, z ) SFallowable ( x, y, z )Material Strength( x, y, z )! SU allowable 100% , (16) existing ( x, y, z )Material Strength( x, y, z )! MU allowable ( x, y, z ) 1, (17)SFallowable ( x, y, z )It is obvious at first glance, that with varying safety factors, an effective strength assessmentwould require the use of the SU formulation (Equation 16), because the right side of the equationis still a constant. The MU formulation (Equation 17) would still need to work with display groupsor other different views.82012 SIMULIA Community Conference

3. Existing solutions in AbaqusThe user subroutine UVARM (Abaqus User Subroutines Reference Manual, 2010) is provided forAbaqus/Standard to generate element output. With UVARM, the safety utilizations and materialutilizations can be calculated during the solver process. The limitations of the application ofUVARM in regard to the challenges mentioned in Chapter 2 are: a) no self-explanatory outputvariable names can be used, which can lead to significant confusion and quality issues, b)Calculation of user output variables with UVARM require a solver run. If a user output has notbeen requested before the solver run and should be added afterwards to the ODB – a new solverrun is required. This is especially inconvenient for long lasting creep calculations that may take upto several weeks. c) Many material properties need to be hard coded into the subroutine, which isespecially tedious when using many materials and if material properties are updated.To conclude it can be stated that it is possible to calculate the utilizations with UVARM, althoughthe limitations regarding effectiveness and possible quality concerns apply.4. Siemens Energy’s solution: STARpost4.1IntroductionTo face the challenges mentioned in Chapter 2 and to compensate the limitations of a strengthassessment based on UVARM mentioned in Chapter 3, Siemens Energy large scale steam turbineR&D have developed a customized strength assessment post processing approach as Python PlugIns for the visualization module of Abaqus/CAE: STARpost.STARpostSteam Turbine Analysis Routines Post Processing t. materialfilesCalculation of strengthassessment output variablesUserinput(GUI)STARvisSTARvisODBODBwith added user variablesEffective Visualization ofSTARmech‘s user variablesEffective strength assessmentcontour plots in Abaqus/CAEFigure 5. Structure of STARpost, the post processing suite for static and creepanalyses, including relevant inputs and outputs.2012 SIMULIA Community Conference1

As can be seen in Figure 5, STARpost consists of two modules: STARmech, the plug-in for thecalculation of strength assessment output variables, and STARvis, the plug-in for effectivevisualization of STARmech‘s user variables:The workflow of a strength assessment with STARpost (including Figure 5) will be described onthe basis of

pressure steam turbine, 1 intermediate pressure steam turbine, 2 low pressure steam turbines and 1 generator). Image courtesy of Siemens AG. An essential part in the development of new steam turbines is to ensure the mechanical integrity of all components. Steam turbines have t

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