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161 results for “Numerical Simulation”

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zenodo32/100

Discrete-continuum numerical simulations of saltation over a rigid, bumpy bed

<p><span><span><span>The data provided here were obtained from discrete-continuum numerical simulations of saltation over a rigid, bumpy bed. The details of the simulation</span></span><span><span>s</span></span><span><span> are reported in the article entitled &ldquo;</span></span><span><span><strong>Collisionless kinetic theory for saltation over a rigid, bumpy bed&rdquo; </strong></span></span><span><span>by D. Berzi, A. Valance and J.T. Jenkins published in 2024 in the Journal of Fluid Mechanics.</span></span></span></p>

opencc-by-4.0May 2024View details →
zenodo32/100

The dataset used in numerical simulations based on the resistivity structure of Kusatsu-Shirane Volcano, Japan

<p>The dataset used in the numerical simulations based on the resistivity structure of Kusatsu-Shirane Volcano, Japan.&nbsp;</p> <p>Descriptions of included files:</p> <p><strong>TOUGH_model.zip</strong></p> <p>The data used in the numerical simulations by the TOUGH3 code. It includes ten cases with different permeability structures considered.</p> <p><strong>HT_model.zip</strong></p> <p>The data used in the numerical simulations by the HYDROTHERM code. It includes seven cases with different permeability structures considered.</p>

opencc-by-sa-4.0Jul 2024View details →
zenodo32/100

'Reconciling Surface Deflections From Simulations of Global Mantle Convection' : Numerical model dataset

<p><strong>Output data from TERRA simulations included in 'Reconciling Surface Deflections From Simulations of Global Mantle Convection'</strong></p> <p>Dataset includes:</p> <ul> <li>Full density field (`NC_visc_dens_037.tar.gz`)</li> <li>Radial stresses (directory `radial_stresses`)</li> <li>Spherical harmonic coefficients for density field (`density_sph.037`)</li> <li>Radial viscosity factors (`visc.dat`)</li> </ul> <p>Radial stresses are calculated at depths of:</p> <ul> <li>0 km (surface)</li> <li>45 km</li> <li>180 km</li> <li>270 km</li> </ul> <p>and with various amounts of shallow structure removed:</p> <ul> <li>NC_DT_rmir0 - No shallow structure removed</li> <li>NC_DT_rmir1 - 45 km removed</li> <li>NC_DT_rmir2 - 90 km removed</li> <li>NC_DT_rmir3 - 135 km removed</li> <li>NC_DT_rmir5 - 225 km removed</li> <li>NC_DT_rmir7 - 270 km removed</li> </ul>

opencc-by-4.0Jul 2024View details →
zenodo32/100

Spatio-temporal Features of Intra-seasonal Oceanic Variability in the Philippine Sea from Mooring Observations and Numerical Simulations

<p>This dataset contains&nbsp;the NPOCE (http://npoce.org.cn) data used in the following submission for Journal of Geophysical Research: Oceans:</p> <p>Hu, S., J. Sprintall, C. Guan, B. Sun, F. Wang, G. Yang, F. Jia, J. Wang, D. Hu, and F. Chai (2018), Spatio-temporal Features of Intra-seasonal Oceanic Variability in the Philippine Sea from Mooring Observations and Numerical Simulations, Journal of Geophysical Research: Oceans.</p> <p>Variables in this dataset are eddy kinetic energy (EKE) observed by the NPOCE moorings, longitudes, latitudes, depths and dates.</p> <p>&nbsp;</p> <p>&nbsp;</p>

opencc-by-4.0May 2018View details →
zenodo32/100

Development of a dense cratonic keel prior to the destruction of the North China Craton: Constraints from sedimentary records and numerical simulation

<p>This file is created for Liu et al. (2019) -- &lsquo;<em>Development of a dense cratonic keel prior to the destruction of the North China Craton: Constraints from sedimentary records and numerical simulation</em>&rsquo;. The folder &#39;mutils-0.2&#39; contains&nbsp;the quick search algorithm tsearch2 (Mutilspackage:http://milamin.sourceforge.net/downloads)</p>

opencc-by-4.0Aug 2019View details →
zenodo32/100

Numerical data pertaining to phase-field simulations of quartz cementation in polycrystalline sandstones

<p>The numerical data in this repository pertains to the simulation results of quartz cementation in polycrystalline sandstones. The simulations were performed using&nbsp; the software package named &quot;Pace3D version 2.5.1&quot;.&nbsp; The software license can be purchased at Steinbeis Network (www.steinbeis.de) in the management of Britta Nestler and Michael Selzer under the subject area &lsquo;Material Simulation and Process Optimization&rsquo;. &nbsp;</p> <p>The data is organized, the way it appears in the figures in the manuscript. Thus, the folders are named according to the figure number in the manuscript. Each folder contains a separate ReadMe.dat file, which contains all the information regarding the data present in that folder.</p> <p>&nbsp;</p> <ul> <li>&nbsp;For the sake of convenience, the simulation data that comprises the pictures is converted to .stl and .vtk format, for visualization using open source software packages like Paraview and MeshLab.</li> <li>The original complete output data is in the formats (e.g. *.phiindex.p3s, *.fluiddynamics_velocity.p3v etc.) which can be visualized using the in-house visualization tools GLviewer and XSimview.</li> <li>The data presented in plots is extracted from the simulation output using the post-processing tool chain of &quot;Pace3D&quot;.</li> </ul> <p>&nbsp;</p>

opencc-by-4.0Dec 2019View details →
zenodo32/100

Free surface evolution from numerical wave tank simulations - Experiment W6N5D5

<p>An ensemble of two-dimensional numerical wave tank (NWT) simulations of breaking and non-breaking wave packets. The NWT uses the Gerris software package, a two-phase Navier-Stokes solver that utilises the volume-of-fluid method and explicitly models viscosity and surface tension effects. It is configured in non-dimensional coordinates scaled by the length and time characteristics of a deep-water wave with wavelength 1 m. This dataset contains simulations from experiment W6N5D5 (wind forcing speed equal to 6 times the wave speed, chirped wave packet with 5 waves in the packet signal, deep water) and forms part of an ensemble of experiments available <a href="https://doi.org/10.5281/zenodo.12797829" target="_blank" rel="noopener">here</a>. A full description of the NWT is provided in:</p> <p><a href="https://doi.org/10.1017/jfm.2023.134" target="_blank" rel="noopener">Boettger, D. G., Keating, S. R., Banner, M. L., Morison, R. P., &amp; Barthelemy, X. (2023). An energetic&nbsp;signature for breaking inception in surface gravity waves. Journal of Fluid Mechanics, 959, A33.</a></p> <p><a href="https://doi.org/10.1103/PhysRevFluids.9.054803" target="_blank" rel="noopener">Boettger, D. G., Keating, S. R., Banner, M. L., Morison, R. P., &amp; Barthelemy, X. (2024). Energetic&nbsp;inception of breaking in surface gravity waves under wind forcing. Physical Review Fluids, 9 (5),&nbsp;054803.</a></p>

opencc-by-nc-nd-4.0Jul 2024View details →
zenodo32/100

Free surface evolution from numerical wave tank simulations - Experiment W0N5D2

<p>An ensemble of two-dimensional numerical wave tank (NWT) simulations of breaking and non-breaking wave packets. The NWT uses the Gerris software package, a two-phase Navier-Stokes solver that utilises the volume-of-fluid method and explicitly models viscosity and surface tension effects. It is configured in non-dimensional coordinates scaled by the length and time characteristics of a deep-water wave with wavelength 1 m. This dataset contains simulations from experiment W0N5D2 (Zero wind forcing, chirped wave packet with 5 waves in the packet signal, intermediate water depth)&nbsp;and forms part of an ensemble of experiments available <a href="https://doi.org/10.5281/zenodo.12797829" target="_blank" rel="noopener">here</a>. A full description of the NWT is provided in:</p> <p><a href="https://doi.org/10.1017/jfm.2023.134" target="_blank" rel="noopener">Boettger, D. G., Keating, S. R., Banner, M. L., Morison, R. P., &amp; Barthelemy, X. (2023). An energetic&nbsp;signature for breaking inception in surface gravity waves. Journal of Fluid Mechanics, 959, A33.</a></p> <p><a href="https://doi.org/10.1103/PhysRevFluids.9.054803" target="_blank" rel="noopener">Boettger, D. G., Keating, S. R., Banner, M. L., Morison, R. P., &amp; Barthelemy, X. (2024). Energetic&nbsp;inception of breaking in surface gravity waves under wind forcing. Physical Review Fluids, 9 (5),&nbsp;054803.</a></p>

opencc-by-nc-nd-4.0Aug 2024View details →
zenodo32/100

Free surface evolution from numerical wave tank simulations - Experiment W0N5D5

<p>An ensemble of two-dimensional numerical wave tank (NWT) simulations of breaking and non-breaking wave packets. The NWT uses the Gerris software package, a two-phase Navier-Stokes solver that utilises the volume-of-fluid method and explicitly models viscosity and surface tension effects. It is configured in non-dimensional coordinates scaled by the length and time characteristics of a deep-water wave with wavelength 1 m. This dataset contains simulations from experiment W0N5D5 (Zero wind forcing, chirped wave packet with 5 waves in the packet signal, deep water)&nbsp;and forms part of an ensemble of experiments available <a href="https://doi.org/10.5281/zenodo.12797829" target="_blank" rel="noopener">here</a>. A full description of the NWT is provided in:</p> <p><a href="https://doi.org/10.1017/jfm.2023.134" target="_blank" rel="noopener">Boettger, D. G., Keating, S. R., Banner, M. L., Morison, R. P., &amp; Barthelemy, X. (2023). An energetic&nbsp;signature for breaking inception in surface gravity waves. Journal of Fluid Mechanics, 959, A33.</a></p> <p><a href="https://doi.org/10.1103/PhysRevFluids.9.054803" target="_blank" rel="noopener">Boettger, D. G., Keating, S. R., Banner, M. L., Morison, R. P., &amp; Barthelemy, X. (2024). Energetic&nbsp;inception of breaking in surface gravity waves under wind forcing. Physical Review Fluids, 9 (5),&nbsp;054803.</a></p>

opencc-by-nc-nd-4.0Aug 2024View details →
zenodo32/100

Free surface evolution from numerical wave tank simulations - Experiment W0N9D5

<p>An ensemble of two-dimensional numerical wave tank (NWT) simulations of breaking and non-breaking wave packets. The NWT uses the Gerris software package, a two-phase Navier-Stokes solver that utilises the volume-of-fluid method and explicitly models viscosity and surface tension effects. It is configured in non-dimensional coordinates scaled by the length and time characteristics of a deep-water wave with wavelength 1 m. This dataset contains simulations from experiment W0N9D5 (Zero wind forcing, chirped wave packet with 9 waves in the packet signal, intermediate water depth)&nbsp;and forms part of an ensemble of experiments available <a href="https://doi.org/10.5281/zenodo.12797829" target="_blank" rel="noopener">here</a>. A full description of the NWT is provided in:</p> <p><a href="https://doi.org/10.1017/jfm.2023.134" target="_blank" rel="noopener">Boettger, D. G., Keating, S. R., Banner, M. L., Morison, R. P., &amp; Barthelemy, X. (2023). An energetic&nbsp;signature for breaking inception in surface gravity waves. Journal of Fluid Mechanics, 959, A33.</a></p> <p><a href="https://doi.org/10.1103/PhysRevFluids.9.054803" target="_blank" rel="noopener">Boettger, D. G., Keating, S. R., Banner, M. L., Morison, R. P., &amp; Barthelemy, X. (2024). Energetic&nbsp;inception of breaking in surface gravity waves under wind forcing. Physical Review Fluids, 9 (5),&nbsp;054803.</a></p>

opencc-by-nc-nd-4.0Aug 2024View details →
zenodo32/100

Free surface evolution from numerical wave tank simulations - Experiment W1N5D5

<p>An ensemble of two-dimensional numerical wave tank (NWT) simulations of breaking and non-breaking wave packets. The NWT uses the Gerris software package, a two-phase Navier-Stokes solver that utilises the volume-of-fluid method and explicitly models viscosity and surface tension effects. It is configured in non-dimensional coordinates scaled by the length and time characteristics of a deep-water wave with wavelength 1 m. This dataset contains simulations from experiment W1N5D5 (wind forcing speed equal to wave speed, chirped wave packet with 5 waves in the packet signal, deep water) and forms part of an ensemble of experiments available&nbsp;<a href="https://doi.org/10.5281/zenodo.12797829" target="_blank" rel="noopener">here</a>. A full description of the NWT is provided in:</p> <p><a href="https://doi.org/10.1017/jfm.2023.134" target="_blank" rel="noopener">Boettger, D. G., Keating, S. R., Banner, M. L., Morison, R. P., &amp; Barthelemy, X. (2023). An energetic&nbsp;signature for breaking inception in surface gravity waves. Journal of Fluid Mechanics, 959, A33.</a></p> <p><a href="https://doi.org/10.1103/PhysRevFluids.9.054803" target="_blank" rel="noopener">Boettger, D. G., Keating, S. R., Banner, M. L., Morison, R. P., &amp; Barthelemy, X. (2024). Energetic&nbsp;inception of breaking in surface gravity waves under wind forcing. Physical Review Fluids, 9 (5),&nbsp;054803.</a></p>

opencc-by-nc-nd-4.0Aug 2024View details →
zenodo32/100

DLR AS TEA Configuration B1 Numerical Simulation Database

<p>This database contains the results of the numerical simulations conducted in the framework of WP5.4 by DLR AS TEA. See README file for the description of the cases simulated.</p>

opencc-by-4.0Sep 2024View details →
zenodo32/100

DLR AS TEA Configuration A1 and A2 Numerical Simulation Database

<p>This database contains the results of the numerical simulations conducted in the framework of WP5.2 by DLR AS TEA. See README file for the description of the cases simulated.</p>

opencc-by-4.0Sep 2024View details →
zenodo32/100

Local Time Variations of Quiet Time Meridional Winds during June and December based on ICON Observations and Numerical Simulations

<p>The file named '<a href="../api/records/12139509/draft/files/geomagnetic%20index.mat/content" target="_blank" rel="noopener noreferrer">geomagnetic index</a>' includes Kp, F10.7p, By and Bz indices, AE and Dst indices. The file named '<a href="../api/records/12139509/draft/files/MWjym12.mat/content" target="_blank" rel="noopener noreferrer">MWjym06</a>', &nbsp;'<a href="../api/records/12139509/draft/files/MWjym12.mat/content" target="_blank" rel="noopener noreferrer">MWjym12</a>' are the meridional winds of ICON&nbsp; observations in June and December. The file named '<a href="../api/records/12139509/draft/files/VN_mean06.mat/content" target="_blank" rel="noopener noreferrer">VN_mean06</a>', &nbsp;'<a href="../api/records/12139509/draft/files/VN_mean06.mat/content" target="_blank" rel="noopener noreferrer">VN_mean12</a>' , '<a href="../api/records/12139509/draft/files/VN_mean06.mat/content" target="_blank" rel="noopener noreferrer">VNnotide_mean06</a>','<a href="../api/records/12139509/draft/files/VN_mean06.mat/content" target="_blank" rel="noopener noreferrer">VNnotide_mean12</a>' include the parameters of TIEGCM simulated meridional winds and the forcing terms with and without tides in June and December. The file named 'F107_70' is the simulation in December in F10.7=70.</p>

opencc-by-4.0Jun 2024View details →
zenodo32/100

Deliverable 1.1.1.1 BEL-Float project | Dataset containing the results of numerical simulations (motions, forces) of the operational performance analysis - Part 9: Operational and damaged scenarios in regular waves

<p>This dataset contains the results of OpenFAST simulations performed on the DeepCwind OC4 semi-submersible combined with the 5MW NREL turbine for various wind and wave conditions. The basis of the OpenFAST input files are taken from&nbsp;<a href="https://github.com/OpenFAST/r-test/tree/main/glue-codes/openfast/5MW_OC4Semi_WSt_WavesWN">OpenFAST r-test GitHub repository (5MW_OC4Semi_WSt_WavesWN)</a>&nbsp;and adapted to simulate various wind and wave conditions. The turbulent wind field as the input to the InflowWind module is generated using&nbsp;<a href="https://www.nrel.gov/wind/nwtc/turbsim.html">TurbSim</a>. The simulations are performed on a modified version of OpenFAST v3.5.3 to which adaptation to the code is made to extract additional Morison drag output up to 16 cylindrical members. This adapted code is&nbsp;<a href="https://github.com/abkpribadi/openfast/tree/Morison_additional_output">uploaded on GitHub as a branch from a forked OpenFAST repository</a>. In total there are 1152 simulation results consists of 768 irregular waves and 384 regular waves cases. The complete dataset is divided into 9 sub-datasets to which this is part number 9. A report describing this dataset is available on the BEL-Float project website: https://www.owi-lab.be/bel-float.</p>

opencc-by-4.0Oct 2024View details →
zenodo32/100

3D HDF5 data from numerical relativity simulations

<p>3D HDF5 data from numerical relativity simulations. Test data for visualization purposes.</p>

opencc-by-4.0Jul 2021View details →
zenodo32/100

Dataset from "Numerical gravitational backreaction on cosmic string loops from simulation"

<p>This file contains a data table representing the average power spectrum, P_n, of Nambu-Goto cosmic strings evolved under numerical gravitational backreaction. The power spectra and the methods used to produce them are reported on in "Numerical gravitational backreaction on cosmic string loops from simulation" [to appear], by the same authors as this dataset. See Fig. 5 of that paper for a visualization.</p> <p>The file is organized in three columns:</p> <ol> <li>The fraction of evaporation, chi. The range is from 0.0 to 0.7 in steps of 0.1.</li> <li>The mode number, n. The range is from 2^0 to 2^39 in multiplicative steps of 2.</li> <li>The logarithmically binned elements of the power spectrum, nP_n. Bin edges are 2^i to 2^(i+1)-1 for i from 0 to 39.</li> </ol>

opencc-by-4.0Nov 2024View details →
zenodo32/100

Postprocessed data for "Tracing the rain formation pathways in numerical simulations of deep convection"

<p>This dataset is associated with the journal paper &quot;Tracing the rain formation pathways in numerical simulations of deep convection&quot;.</p> <p>There are six .npz files containing data for the 5 simulations (CTRL, CTRLrfix, K13, CTRL800, K13800)<br> and one npz file containing data for constructing the rain pdfs of simulation CTRL (Figure 6).</p> <p>This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52‐07NA27344 IM Release number&nbsp;LLNL-MI-843623</p>

opencc-by-4.0Jan 2022View details →
zenodo32/100

Datasets for numerical Monte Carlo simulations of Diclofenac bio-degradation in a soil-water system

<p>This record contains files and main instructions to repeat the numerical simulations of Diclofenac bio-degradation is a soil-water system. The text file Readme.docx contains a description of the overall content of this record, which is organized in two separate&nbsp;folders.</p>

opencc-by-4.0Jul 2022View details →
zenodo32/100

Numerical simulations reproduce field observations showing transient weakening during shear zone formation by diffusional hydrogen influx and H2O inflow

<p>Abstract of the corresponding paper:</p> <p>Exposures on Holsn&oslash;y island (Bergen Arcs, Norway) indicate fluid infiltration through fractures into a dry, metastable granulite, which triggered a kinetically delayed eclogitization, a transient weakening during fluid-rock interaction, and formation of shear zones that widened during shearing. It remains unclear whether the effects of grain boundary-assisted aqueous fluid inflow on the duration of granulite hydration were influenced by a diffusional hydrogen influx accompanying the fluid inflow. To better estimate the fluid infiltration efficiencies and the parameter interdependencies, a 1D numerical model of a viscous shear zone is utilized and validated using measured mineral phase abundance distributions and H<sub>2</sub>O-contents in nominally anhydrous minerals (NAMs) of the original granulite assemblage to constrain the hydration by aqueous fluid inflow and diffusional hydrogen influx, respectively. Both hydrations are described with a diffusion equation and affect the effective viscosity. Shear zone kinematics are constrained by the observed shear strain and thickness. The model fits the phase abundance and H<sub>2</sub>O-content profiles if the effective hydrogen diffusivity is approximately one order of magnitude higher than the diffusivity for aqueous fluid inflow. The observed shear zone thickness is reproduced if the viscosity ratio between dry granulite and deforming, re-equilibrating eclogite is ~10<sup>4</sup> and that between dry granulite and hydrated granulite is ~10<sup>2</sup>. The results suggest shear velocities &lt;10<sup>-2</sup> cm/a, hydrogen diffusivities of ~10<sup>-13&plusmn;1</sup> m<sup>2</sup>/s, and a shearing duration of &lt;10 years. This study successfully links and validates field data to a shear zone model and highlights the importance of hydrogen diffusion for shear zone widening and eclogitization.</p> <p>&nbsp;</p> <p>The files uploaded here represents the numerical codes and dataset utilized to produce the results presented in the associated paper.<br> Find a description of the single code files ([<em>name</em>].m) in the ST1.doxc file.</p>

opencc-by-4.0Mar 2023View details →

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Allen Brain Atlas

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allen-brain-atlas
neuroscienceopenDocumentation, web resources, and API references are available online.
Last verified 2026-04-30Open record

Annotated Behaviour and Observability Dataset (ABODe)

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abode-home-cage
behavioral-neuroscienceopenThe DataShare record exposes download links for annotations, documentation, license text, and the zipped per-snippet data directory.
Last verified 2026-04-30Open record

DANDI Archive for NWB datasets

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dandi-nwb
electrophysiologyopenPublished Dandiset metadata and archive endpoints are available through the production DANDI API.
Last verified 2026-04-30Open record

International Brain Laboratory public data

The International Brain Laboratory public data releases expose standardized mouse decision-making experiments, including Neuropixels recordings, widefield calcium imaging, behavior, and session metadata accessed through the ONE API.

ibl
behavioral-neuroscienceopenPublic sessions can be searched and loaded from the IBL public data server through ONE.
Last verified 2026-04-29Open record

OpenNeuro

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openneuro
neuroscienceopenPublished datasets are available on demand over the internet.
Last verified 2026-04-29Open record