Matches in SemOpenAlex for { <https://semopenalex.org/work/W2594842457> ?p ?o ?g. }
Showing items 1 to 90 of
90
with 100 items per page.
- W2594842457 abstract "Selective laser melting (SLM) is an additive manufacturing (AM) technique that is used for metallic products. These products are built in a layer by layer manner by means of selectively melting and hence fusing a layer of metal powder with a laser scanning along a predefined path. The SLM process is able to create products with complex geometries, high accuracy, and within a single manufacturing step. Although SLM presents a number of advantages, the thermal loading causing residual stresses and distortions is an important issue in SLM products. Residual stresses may lead to a limited load resistance and cracks leading to impaired toughness. Distortions may cause the SLM product to be manufactured outside of design tolerances. Therefore, for an SLM product it is essential to accurately predict residual stresses and distortion in the design phase. In literature a great variety of modelling techniques are proposed to capture the physics of the process. Two most widely used approaches to model the process are the melting pool scale and the layer by layer modelling approach. The latter is a computationally efficient way of modelling but does not contain complex process history whereas the former is computationally expensive but can capture the effects of scanning strategy and other process parameters. In this thesis a novel modelling approach is presented which combines the advantages of modelling at the layer scale and the melting pool scale. The general idea is that, the source of strain, giving rise to residual stresses during the SLM process for a given scanning strategy is reconstructed from a detailed simulation and mapped onto a layer. In order to do this the eigenstrain reconstruction method (ERM) is utilised. In this method an equivalent strain source is reconstructed for a residual stress field. The reconstructed equivalent strain source or eigenstrain can be used as a building block to describe the strain source for an entire layer or product. By defining the strain source for an entire product, the residual stresses in the product can be predicted directly. The novelty of the work presented in this thesis lies in the way the residual stress field is predicted. In literature the residual stress field caused by the SLM process is directly mapped to a layer or product. In this approach it is not the stress field that is mapped to the layer or product but the strain source. The advantage of this idea is that the resulting residual stress fields fromthe strain source are continuous in the SLMproduct. Although the ERM is widely used to model 1D and 2D residual stress fields for welding and peening processes, so far no fully 3D ERM has been implemented. In real SLM products the residual stress fields are always multi-axial. Therefore, it is necessary to extend ERMto 3D which is capable of dealing with the multidimensionality of the residual stress fields. One of the requirements of ERMis the input of a reference residual stress field. Therefore an expensive numerical reference model is developed which includes the effect of scanning strategy on the residual stress and warpage of a SLMproduct. The ERM model developed in this thesis is validated by reconstructing the residual stress fields for three geometries; a line, layer and ten layer geometry. The residual stress distributions calculated by the eigenstrain are compared with the results of the expensive numerical reference model. In this model the scanning strategy is incorporated by a point by point modelling approach. The performance of ERM is evaluated by calculating the corresponding residual stress field error between reference and ERM results, which lies within 0.5-4%. It is concluded that the ERMis a suitablemethod to reconstruct equivalent strain sources or eigenstrains for predicting 3D residual stress fields caused by the SLMprocess. The contribution to the field consists of an expansion of ERMto three dimensions and a hybrid model for the SLMprocess which combines the computational efficiency of the global approach with the detail of the local approach." @default.
- W2594842457 created "2017-03-16" @default.
- W2594842457 creator A5032459061 @default.
- W2594842457 date "2016-01-01" @default.
- W2594842457 modified "2023-09-27" @default.
- W2594842457 title "Eigenstrain reconstruction of residual stresses induced by selective laser melting" @default.
- W2594842457 hasPublicationYear "2016" @default.
- W2594842457 type Work @default.
- W2594842457 sameAs 2594842457 @default.
- W2594842457 citedByCount "1" @default.
- W2594842457 countsByYear W25948424572018 @default.
- W2594842457 crossrefType "journal-article" @default.
- W2594842457 hasAuthorship W2594842457A5032459061 @default.
- W2594842457 hasConcept C111919701 @default.
- W2594842457 hasConcept C11413529 @default.
- W2594842457 hasConcept C120665830 @default.
- W2594842457 hasConcept C121332964 @default.
- W2594842457 hasConcept C126780896 @default.
- W2594842457 hasConcept C127413603 @default.
- W2594842457 hasConcept C141349535 @default.
- W2594842457 hasConcept C155512373 @default.
- W2594842457 hasConcept C159985019 @default.
- W2594842457 hasConcept C192562407 @default.
- W2594842457 hasConcept C194257627 @default.
- W2594842457 hasConcept C21880701 @default.
- W2594842457 hasConcept C26796778 @default.
- W2594842457 hasConcept C2777581544 @default.
- W2594842457 hasConcept C2779227376 @default.
- W2594842457 hasConcept C2780822103 @default.
- W2594842457 hasConcept C37292000 @default.
- W2594842457 hasConcept C41008148 @default.
- W2594842457 hasConcept C46362747 @default.
- W2594842457 hasConcept C49040817 @default.
- W2594842457 hasConcept C520434653 @default.
- W2594842457 hasConcept C54237361 @default.
- W2594842457 hasConcept C78519656 @default.
- W2594842457 hasConcept C87976508 @default.
- W2594842457 hasConcept C98045186 @default.
- W2594842457 hasConceptScore W2594842457C111919701 @default.
- W2594842457 hasConceptScore W2594842457C11413529 @default.
- W2594842457 hasConceptScore W2594842457C120665830 @default.
- W2594842457 hasConceptScore W2594842457C121332964 @default.
- W2594842457 hasConceptScore W2594842457C126780896 @default.
- W2594842457 hasConceptScore W2594842457C127413603 @default.
- W2594842457 hasConceptScore W2594842457C141349535 @default.
- W2594842457 hasConceptScore W2594842457C155512373 @default.
- W2594842457 hasConceptScore W2594842457C159985019 @default.
- W2594842457 hasConceptScore W2594842457C192562407 @default.
- W2594842457 hasConceptScore W2594842457C194257627 @default.
- W2594842457 hasConceptScore W2594842457C21880701 @default.
- W2594842457 hasConceptScore W2594842457C26796778 @default.
- W2594842457 hasConceptScore W2594842457C2777581544 @default.
- W2594842457 hasConceptScore W2594842457C2779227376 @default.
- W2594842457 hasConceptScore W2594842457C2780822103 @default.
- W2594842457 hasConceptScore W2594842457C37292000 @default.
- W2594842457 hasConceptScore W2594842457C41008148 @default.
- W2594842457 hasConceptScore W2594842457C46362747 @default.
- W2594842457 hasConceptScore W2594842457C49040817 @default.
- W2594842457 hasConceptScore W2594842457C520434653 @default.
- W2594842457 hasConceptScore W2594842457C54237361 @default.
- W2594842457 hasConceptScore W2594842457C78519656 @default.
- W2594842457 hasConceptScore W2594842457C87976508 @default.
- W2594842457 hasConceptScore W2594842457C98045186 @default.
- W2594842457 hasLocation W25948424571 @default.
- W2594842457 hasOpenAccess W2594842457 @default.
- W2594842457 hasPrimaryLocation W25948424571 @default.
- W2594842457 hasRelatedWork W1542783270 @default.
- W2594842457 hasRelatedWork W2035361020 @default.
- W2594842457 hasRelatedWork W2044914921 @default.
- W2594842457 hasRelatedWork W2117318505 @default.
- W2594842457 hasRelatedWork W2522615404 @default.
- W2594842457 hasRelatedWork W2623124145 @default.
- W2594842457 hasRelatedWork W2762311902 @default.
- W2594842457 hasRelatedWork W2801305340 @default.
- W2594842457 hasRelatedWork W2887950114 @default.
- W2594842457 hasRelatedWork W2897097186 @default.
- W2594842457 hasRelatedWork W2917919587 @default.
- W2594842457 hasRelatedWork W2930176581 @default.
- W2594842457 hasRelatedWork W2938352174 @default.
- W2594842457 hasRelatedWork W2966602489 @default.
- W2594842457 hasRelatedWork W2988717109 @default.
- W2594842457 hasRelatedWork W3014491654 @default.
- W2594842457 hasRelatedWork W3132743357 @default.
- W2594842457 hasRelatedWork W3175518824 @default.
- W2594842457 hasRelatedWork W641505451 @default.
- W2594842457 hasRelatedWork W2760786292 @default.
- W2594842457 isParatext "false" @default.
- W2594842457 isRetracted "false" @default.
- W2594842457 magId "2594842457" @default.
- W2594842457 workType "article" @default.