For one sample of each type, poro-elastic experiments show that the variation in normalized matrix bulk modulus (due to confining pressure increase) may be attributed to the closure of portions of the connected pore network.
In the end, the analysis results of NHFMM were verified by a specially designed photo-elastic experiment.
Compared with the photo-elastic experiment of the joint sample, the result shows that the corssfeed mechanical model of the contact bodies is more practical than the traditional model.
One of the central issues in the design and the use of pulsed neutron sources is the control of pulse length in elastic scattering experiments, most significantly diffraction on crystalline matter.
The atomic composition with less than 1 2 atom% uncertainty was measured in ternary BeZnO and quaternary BeMgZnO alloys using a combination of nondestructive Rutherford backscattering spectrometry with 1 MeV He+ analyzing ion beam and non-Rutherford elastic backscattering experiments with 2.53 MeV energy protons.
This was further reflected in elastic recovery experiments, where these materials yielded before completing cycling up to 150% strain.
This setup is designed to reach the nano-eV energy resolution in the case of quasi-elastic scattering experiments.
A commercial elastic phantom experiment on a freehand strain imaging system further validates the superior performance of chirp pulse.
In the present work Monte-Carlo simulations for quasi-elastic MIEZE experiments taking into account beam divergence as well as the sample dimensions are presented.
The crystal sturcture of the high temperature modifications have been determined be elastic neutron scattering experiments on powdered samples.
Utilising the indentation data obtained from the micro-indentation experiments, elastic moduli of each constituent were calculated using a well-established method whereas yield strength and hardening exponent were extracted using the inverse procedure based on finite element analysis.
