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Fluid displacement data are automatically displayed in real time as both volumetric flux (Jv) and hydraulic conductivity (Lp).
Group of atoms in the simulation constituting cohesive zones which are used to obtain local stress and crack opening displacement data are determined dynamically during the non-planar crack growth as they cannot be determined apriori.
Experiments are done on a small laboratory ball bearing rig on which vibration displacement data are acquired for a baseline condition as well as six different fault conditions that are introduced separately at different subcritical steady state speeds.
Dynamic displacement data are typically displayed as a set of parametric images, including displacement immediately after excitation, maximum displacement, time to peak displacement, and recovery time from peak displacement.
The displacement data are those obtained at 142 continuous GPS stations in Hokkaido and northernmost Tohoku district and two offshore PG stations far off the Pacific coast of Hokkaido.
Illustrative examples of amplitude, coherence and displacement data are from RADARSAT-2 images, while topographic change is derived from the analysis of TanDEM-X data at Reventador volcano, Ecuador (Arnold et al., 2017).
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The resulting load (P) and displacement data were used to calculate the modulus of the sample.
The displacement data is acquired by processing the image from a camera.
Typical load displacement data were obtained for a Berkovich indentor as it was driven into and pulled out of the SU-8 and carbon microstructures.
Hence the experimental displacement data were corrected before calculating the coupon bearing stiffness.
Tests were run until failure and load-optical displacement data was recorded for each test.
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