research
The reality of English living rooms – A comparison of internal temperatures against common model assumptions
Highlights of this open access article published in Energy and Buildings:
finite strain in ABAQUS
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'Innovative solutions please, as long as they have been proved elsewhere: the case of a polished lime-pozzolan concrete floor'
Highlights of this open access article published in Case Studies in Construction Materials:
Heating patterns in English homes: national survey vs common model assumptions
Hightlights of this open access article published in Building and Environment:
• Building stock models need to revise some of their assumptions on space heating.
• Weekends and weekdays are similar in their heating pattern and duration.
• Estimated heating demand temperature is slightly lower than the assumed 21 °C.
• Homes differ widely in their hours of heating and their demand temperature.
Crack length measurement
I am trying to measure J - integral from experiment. " Let my initial fatigue crack length is 6mm, then i did single specimen unloading compliance test on it. The crack legth increased to 8mm" If i want to model the same geometry in FEA. Now my doubt is that "what carck length should i take 1) Initial fatigue crack = 6mm 2) final crack length = 8 mm.................... Note: I need to model my CT specimen in FEA to correct my experiments :-)
Parallel Multiscale modeling in ABAQUS using UMAT
Hello everyone,
I am currently in the process of implementing a multiscale modeling approach in ABAQUS/Standard.
Here is what I am doing.
Macroscale ABAQUS model <--> UMAT <--> Python script <--> Microscale ABAQUS model
So basically the microscale model is being called at every macroscale integration point. The UMAT passes the required data to python as command line arguments and the python script returns the stress and tangent modulus in a text file.
Scaling theory of continuum dislocation dynamics in three dimensions: Self-organized fractal pattern formation
Y. S. Chen, W. Choi, S. Papanikolaou, M. Bierbaum, J. P. Sethna
instability induced by incoherent twin boundary in nanotwinned copper
1. Strain hardening and softening in nanotwinned Cu:
Nanotwinned Cu foils with about 99% coherent twin boundaries (TBs) among all the boundaries were made. These coherent
TBs, with an average spacing of 25 nm, were engineered approximately parallel to foil surfaces. Low plane-strain deformation
enhances the hardness by refining microstructure and introducing dislocations. High plane-strain deformation results in crystallographic
lattice rotation and reaction between dislocations and coherent TBs, and induces incoherent TBs, thus twin coarsening and
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