Thermo-mechanical analysis of Wire and Arc Additive Layer Manufacturing process on large multi-layer parts |
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Authors: | J. Ding P. Colegrove J. Mehnen S. Ganguly P.M. Sequeira Almeida F. Wang S. Williams |
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Affiliation: | 1. Manufacturing Department, Cranfield University, Cranfield MK43 0AL, UK;2. Welding Engineering Research Centre, Cranfield University, Cranfield MK43 0AL, UK;1. Department of Mechanical and Nuclear Engineering, The Pennsylvania State University, 127 Reber Building, University Park, PA 16802, USA;2. Department of Mechanical and Nuclear Engineering, The Pennsylvania State University, USA;3. Applied Research Laboratory at The Pennsylvania State University, USA;1. Welding Engineering and Laser Processing Centre (WELPC), Cranfield University, Cranfield, Bedfordshire, MK43 0AL, UK;2. ISIS Facility, Science and Technology Facilities Council, RutherfordAppleton Laboratory, Harwell Oxford, Didcot, Oxfordshire, OX11 0QX, UK |
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Abstract: | Wire and Arc Additive Layer Manufacturing (WAALM) is gaining increasing popularity as the process allows the production of large custom-made metal workpieces with high deposition rates. The high power input of the welding process, causes significant residual stress and distortion of the workpiece. This paper describes the thermo-mechanical behaviour of the multi-layer wall structure made by the WAALM process. A 3D thermo-elastic–plastic transient model and a model based on an advanced steady-state thermal analysis are employed in this study. This modelling approach shows a significant advantage with respect to the computational time. The temperature simulations and distortion predictions are verified by comparing with the experimental results from thermo-couples and laser scanners, while the residual stresses are verified with the neutron diffraction strain scanner ENGIN-X. The stress across the deposited wall is found uniform with very little influence of the preceding layers on the following layers. The stress redistributed after unclamping with a much lower value at the top of the wall than at the interface due to the bending distortion of the sample. |
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