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2,762 results for “Heating”

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zenodo44/100

Dataset of future district heating energy demand in a Finnish municipality

<p>******************* Please view the README.md file for detailed documentation of data. ********************</p> <p>Title: Impact of climate change, energy efficiency and population on long-term heat demand scenarios in districts: Datasets and Supplementary Materials Version: 1.0</p> <p>Date of Release: 28/10/2020&nbsp;Identifier: doi:10.5281/zenodo.4139299 Permalink: http://dx.doi.org/10.5281/zenodo.4139299</p> <p>Associated publication:&nbsp;Hietaharju, P.; Louis, J.-N.; Pulkkinen, J. &amp; Ruusunen, M. Impact of climate change, energy efficiency and population on long-term heat demand scenarios in districts&nbsp;<em>Under Review, </em> <strong>2020</strong></p> <p>Suggested citation: Please reference the associated publication above when using any datasets or materials described in the README file. Contact information: Jean-Nicolas Louis, University of Oulu, Oulu, Finland, jean-nicolas.louis@oulu.fi or jeannicolas.louis@gmail.com</p> <p>Dates of data modelisation: 2013 - 2030 - 2050</p> <p>Geographic location: Jyv&auml;skyl&auml;</p> <p>Time resolution: Hourly, heating season.</p> <p>Types: Input data (all input configuration data are freely available, but dataset related to the district heating network and buildings are not distributed and not shareable&nbsp;for copyright reasons), power, temperature</p> <p>Format: All data are stored in .mat file format (MatLab file).&nbsp;</p> <p>This directory contains the following datasets and supplementary materials: A summary of all the files has been compiled and stored in the &quot;READ ME.md&quot; or&nbsp;&quot;READ ME.html&quot; file</p>

opencc-by-4.0Oct 2020View details →
zenodo44/100

Heat scenarios over Stockholm

<p>A number of heat scenarios studying how green infrastructure would affect the future climate of Stockholm. The dataset consist of a number of scenarios which simulates how building plans could affect heat exposure in Stockholm. The scenarios are:</p> <ul> <li>Stockholm 2014: Baseline scenario simulating the heatwave during the summer of 2014 in Stockholm</li> <li>Stockholm 2030: Simulating the effects of the heatwave 2014 with new building according to plans for city expansion 2030.</li> <li>Stockholm 2050: Simulating the effects of the heatwave 2014 with new buildings according to available plans for city expansion 2050.</li> <li>Grey Scenario: Simulating the effects of the heatwave 2014 in a city where green infrastructure has been minimized.</li> </ul>

opencc-by-4.0May 2020View details →
zenodo44/100

Laboratory dataset on Self-Heating Behavior and Ignition of Shale Rock

<p>The file attached contains a complete set of experimental data from shale rock self-heating ignition cubic basket experiments. The experiments were carried out in a thermostatically controlled oven with thermocouples for measuring the ambient and shale sample temperatures. The data is divided in two parts, one for coarse particles and one for fine particle experiments. The data reported includes the dates of experiments, volume of shale basket being tested, oven ambient temperature, fuel mass of shale, bulk density of the shale, residue mass after the experiment, percentage of residue in respect to initial mass, and if the sample ignited or not. This data is in support of the journal paper:</p> <p>F. Restuccia, N. Ptak, G. Rein, <strong>Self-Heating Behavior and Ignition of Shale Rock</strong>, <em>Combustion and Flame</em>, Vol 176, 2017, pp 213-219. doi: 10.1016/j.combustflame.2016.09.025.</p>

opencc-by-4.0Apr 2017View details →
zenodo44/100

Data, codes for the study "Programmable access to microresonator solitons with modulational sideband heating"

<p>This archive contains the data for figure 2/3/4, codes for simulation in figure 1 and colds for soliton addressing program in figure 3, in the paper "Programmable access to microresonator solitons with modulational sideband heating".</p>

opencc-by-4.0Nov 2023View details →
zenodo44/100

Data of paper "Global supply chains amplify economic costs of future extreme heat risk"

<p>This is the database of articles "Global supply chains amplify economic costs of future extreme heat risk". &nbsp;The database contains the number of deaths caused by future heat waves in regions around the world under different SSP scenarios (e.g. SSP119, SSP245, SSP585), as well as global health losses, labor losses, and indirect losses as a percentage of regional or sectoral value added under different SSP scenarios. The regions of the database are aggregated using the GTAP 141 aggregating schema.</p>

opencc-by-4.0Dec 2023View details →
zenodo44/100

2-meter Universal Thermal Climate Index (UTCI) and Human Heat Health Index (H3I) hazard for Austin, Texas

<p>Universal Thermal Climate Index (UTCI) is a physiological temperature that is widely used in biometeorological studies to assess the heat stress felt by humans. UTCI considers the shortwave and longwave radiation incident on humans from the six cubical directions as well as air temperature, humidity, wind speed and clothing. As a part of NOAA National Integrated Heat Health Information System (NIHHIS) and NASA Interdisciplinary Research in Earth Science (IDS) project, we have generated the UTCI data for Austin, Texas and surrounding peri-urban area at 2-meters spatial resolution for the year 2017. Details on data generation and methodology can be found in Kamath et al., (2023) but are summarized here.&nbsp;</p> <p><strong>1. Datasets and model used</strong></p> <p>The solar and longwave environmental irradiance geometry (SOLWEIG) model was used to simulate shadows, mean radiant temperature (T<sub>MRT</sub>) and the UTCI (Lindberg et al., 2008). T<sub>MRT</sub> is the equivalent temperature due to exposure to absorbed shortwave and longwave radiation from all directions in a standing position. SOLWEIG was forced using near-surface ERA-5 data available at a spatial resolution of 0.25&deg;x 0.25&deg;. Building, vegetation heights, and digital terrain model were again derived from 3DEP LiDAR point cloud data.&nbsp; SOLWEIG was run using the urban multi-scale environment predictor (UMEP) (Lindberg et al., 2018) plug-in with QGIS.&nbsp;&nbsp;</p> <p><strong>2. Data availability</strong></p> <p>Diurnal UTCI data were calculated for typical meteorological clear sky days corresponding to Summer and Fall. The typical clear sky day was selected using the 10-year Typical meteorological Year (TMY) for Austin, Texas (30.2672&deg; N, 97.7431&deg; W) provided by National Solar Radiation Database (NSRDB). More details on TMY files can be found at: https://nsrdb.nrel.gov/data-sets/tmy</p> <p>Additionally, data is developed for heat hazard for daytime Human Heat Health Index (H3I) calculation as defined by Kamath et al., (2023). Briefly, this heat hazard is defined as the fraction of the day when the UTCI exceeds certain threshold. The threshold used to calculate heat hazard for Summer and Fall were 35&deg; C and 32&deg;C, respectively that imply strong heat stress (Jendritzky et al., 2012). Note that UTCI is on a different scale compared to air temperature, and could yield different heat stress levels.</p> <p><strong>3. Data format</strong></p> <p>The georeferenced UTCI and heat hazard data are available in the geoTIFF file format. The files can be readily visualized using GIS software such as QGIS and ArcGIS, as well as programing languages such as Python.</p> <p>&nbsp;<strong>4. Companion dataset</strong></p> <p>Based on the calculated UTCI here, the potential locations for tree planting were calculated to increase the shade to reduce heat vulnerability for Austin, Texas. [https://doi.org/10.5281/zenodo.6363494]</p> <p><strong>References</strong></p> <ol> <li>Kamath, H. G., Martilli, A., Singh, M., Brooks, T., Lanza, K., Bixler, R. P., ... &amp; Niyogi, D. (2023). Human heat health index (H3I) for holistic assessment of heat hazard and mitigation strategies beyond urban heat islands. Urban Climate, 52, 101675.</li> <li>Lindberg, F., Holmer, B., &amp; Thorsson, S. (2008). SOLWEIG 1.0&ndash;Modelling spatial variations of 3D radiant fluxes and mean radiant temperature in complex urban settings.&nbsp;<em>International journal of biometeorology</em>,&nbsp;<em>52</em>, 697-713.</li> <li>Lindberg, F., Grimmond, C. S. B., Gabey, A., Huang, B., Kent, C. W., Sun, T., ... &amp; Zhang, Z. (2018). Urban Multi-scale Environmental Predictor (UMEP): An integrated tool for city-based climate services.&nbsp;<em>Environmental modelling &amp; software</em>,&nbsp;<em>99</em>, 70-87.</li> <li>Jendritzky, G., de Dear, R., &amp; Havenith, G. (2012). UTCI&mdash;why another thermal index?.&nbsp;<em>International journal of biometeorology</em>,&nbsp;<em>56</em>, 421-428.</li> <li>Bixler, R. P., Coudert, M., Richter, S. M., Jones, J. M., Llanes Pulido, C., Akhavan, N., ... &amp; Niyogi, D. (2022). Reflexive co-production for urban resilience: Guiding framework and experiences from Austin, Texas. Frontiers in Sustainable Cities, 4, 1015630.</li> <li>Lanza, K., Jones, J., Acu&ntilde;a, F., Coudert, M., Bixler, R. P., Kamath, H., &amp; Niyogi, D. (2023). Heat vulnerability of Latino and Black residents in a low-income community and their recommended adaptation strategies: A qualitative study.&nbsp;<em>Urban Climate</em>,&nbsp;<em>51</em>, 101656.</li> </ol>

opencc-by-4.0Mar 2024View details →
zenodo44/100

Probabilistic projections of granular energy technology diffusion at subnational level - solar photovoltaics, heat pumps, and battery electric vehicles in Switzerland

<p>The probabilistic projections are part of the work:&nbsp;<br><em>Nik Zielonka, Xin Wen, Evelina Trutnevyte, Probabilistic projections of granular energy technology diffusion at subnational level, PNAS Nexus, Volume 2, Issue 10, October 2023, pgad321, </em><a href="https://doi.org/10.1093/pnasnexus/pgad321"><em>https://doi.org/10.1093/pnasnexus/pgad321</em></a></p> <p>Please cite the article together with the Zenodo link when you use the data.</p> <p>The provided data files contain the estimated probabilistic projections for all Swiss municipalities on the actual diffusion of solar photovoltaics (PV), heat pumps, and battery electric vehicles (BEVs) in Switzerland for the indicated years:</p> <p>Version 2022-2050: Projections for the years 2022-2050 as presented by Zielonka et. al (2023), PNAS Nexus.<br>Version 2023-2050: Projections for the years 2023-2050, using the latest data of 2022.<br>Version 2024-2050: Projections for the years 2024-2050, using the latest data of 2023.</p> <p>The computations were performed at University of Geneva using Baobab HPC service.</p> <p>This research was carried out with the support of the Swiss Federal Office of Energy SFOE as part of the SWEET project SURE (N.Z., E.T.) and the Swiss National Science Foundation Eccellenza Grant as part of the project "Accuracy of long-range national energy projections" (Grant no. 186834, X.W., E.T.). The authors bear sole responsibility for the conclusions and the results.</p>

opencc-by-4.0Oct 2023View details →
zenodo44/100

Elevated increase in compound extreme heat-precipitation events over China

<p>This file contains the fractions (in percentage) of the compound extreme precipitation events that are preceded by an extreme heat event in China during 1961-2017. The compound events are identified based on the CN05.1 dataset at 0.5x0.5 resolution.&nbsp;Please contact us with any questions or concerns (email: luo.ming@hotmail.com).</p>

opencc-by-4.0Dec 2020View details →
zenodo44/100

European cities with Geothermal District Heating and conventional District Heating - GeoDH project

<p>The dataset includes two shapefiles showing the location data for cities across Europe that use Geothermal District Heating and conventional District Heating.&nbsp;<br><br>This dataset was developed for assessing the potential of Geothermal District Heating in Europe as part of the <strong>GeoDH project</strong> (<a href="http://geodh.eu/" target="_new" rel="noopener">http://geodh.eu/</a>). Please note that this represents the<strong> state of the art as of 2014</strong> and that geological, technological, and regulatory developments may have occurred since its creation, and users should verify if more recent data is available for their purposes. <br><br></p>

opencc-by-4.0Nov 2024View details →
zenodo44/100

Data and code for "Autonomous demon exploiting heat and information at the trajectory level"

<p>Code and numerically generated data for the article "Autonomous demon exploiting heat and information at the trajectory level" <a href="https://arxiv.org/abs/2409.05823">arXiv:2409.05823</a>, see README.md for details.</p> <p>Changes: The performance quantifiers X_TUR have been rescaled by a constant factor (see Eq. (20) in the article) compared to the first version.</p>

opencc-by-4.0Sep 2024View details →
zenodo44/100

Characterization of SRF (XRF portable analyser) prepared for an aluminium scrap pre-heating system (REVaMP project)

<p>Open access to experimental data generated by the REVaMP project (GA 869882, Horizon 2020, European Union) along the research of the combustion of a SRF, prepared from ASR, to be used as alternative fuel in a scrap pre-heater at an aluminium refinery plant. Research pertaining to&nbsp;WP1, Deliverable D1.&nbsp;<br> Underlying data for the publication Acha, E.&nbsp;et al. Combustion of a Solid Recovered Fuel (SRF) Produced from the Polymeric Fraction of Automotive Shredder Residue (ASR). Polymers 2021, 13, 3807. https://doi.org/10.3390/polym13213807. Data related to Figure 1 in the article.</p> <p>Subject:&nbsp;Representative samples of SRF were manually sorted into categories of plastics, wood, textile, foam and others, and directly analyzed by the Thermo Fisher Scientific portable analyser Niton&trade;, X-Ray Fluorescence (XRF).</p>

opencc-by-4.0Nov 2021View details →
zenodo44/100

WINTERC-G: a global upper mantle thermochemical model from coupled geophysical–petrological inversion of seismic waveforms, heat flow, surface elevation and gravity satellite data

<p>WINTERC-G: A global, temperature and compositional model of the lithosphere<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; and upper mantle.<br> Version:&nbsp; v5.4, December 2020, J. Fullea, S. Lebedev, Z. Martinec, N. Celli<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; &nbsp;<br> Contact:&nbsp; Javier Fullea (jfullea@ucm.es)<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Facultad de Fisica,<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Universidad Complutense de Madrid (UCM),<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Spain<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; ////////<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Geophysics Section,<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Dublin Institute for Advanced Studies<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Dublin, Ireland<br> &nbsp;</p> <p>TYPE:<br> &nbsp;This contains files with:<br> &nbsp;i) the model directly on the triangular grid solved for in the surface wave inversion.</p> <p>&nbsp;ii) an interpolated grid at 0.5 deg lateral resolution for the density and density discontinuities used in the gravity field data inversion<br> &nbsp;</p> <p>If you have any questions regarding the methodology or the construction<br> of the model, please contact the authors. If you use the model, we would<br> request that you cite the reference indicated below, and appreciate<br> your feedback regarding the model and its application.</p> <p>Citation:</p> <p>Fullea, J., Lebedev, S., Martinec, Z., &amp; Celli, N. L. (2021). WINTERC-G: mapping the upper mantle thermochemical heterogeneity from coupled geophysical&ndash;petrological inversion of seismic waveforms, heat flow, surface elevation and gravity satellite data. Geophysical Journal International, 226(1), 146-191.</p> <p>*******************************<br> Summary: construction of the model.<br> WINTERC-G is a Waveform tomography and Gravity (geoid and gravity anomalies and gradiometric measurements<br> from ESA&#39;s GOCE mission) INversion model of the TEmpeRature and Composition of the lithosphere and upper mantle at<br> global scale. WINTERC-G is based on upon the integrated geophysical-petrological<br> approach LitMod (Afonso et al., 2008; Fullea et al. 2009) and, hence, all<br> relevant mantle rock physical properties modelled (seismic velocities and density) are<br> computed within a thermodynamically self-consistent framework allowing for a direct<br> parameterization in terms of the temperature and composition of the lithosphere-upper<br> mantle. The inversion is a two-step procedure. In a first step, we invert surface-wave, Rayleigh and Love<br> fundamental mode dispersion curves from a high resolution global dataset measured using waveform inversion,<br> along with surface heat flow and elevation (isostasy) for temperature and crustal structure<br> using a point-wise, non-linear, gradient-search inversion<br> over a triangular grid with an average 225 km lateral inter-knot spacing. In a second step we<br> use a fully parallelized spherical harmonic formalism to invert satellite gravity field data in<br> order to refine the initial crustal density and mantle composition distributions from the step 1<br> for a fixed temperature field.</p> <p>The parameter space in step 1 includes crust (densities and S-wave velocities for a three-layered crust)<br> &nbsp;and mantle variables (the depth of the thermal Lithosphere-Athenosphere-Boundary,<br> the thickness of the sublithospheric thermal buffer, the sublithospheric temperatures at 3 different<br> equispaced nodes down to 400 km, the lithospheric and sublithospheric mantle compositon, and<br> the the radial anisotropy at the 3 crustal layers and at 56, 80, 110, 150, 200, 260, 330,<br> and 400 km depths.</p> <p>The parameter space in step 2 is defined by the average crustal density, and the<br> mantle composition in the lithosphere and sublithosphere.<br> We use the output crustal density from step 1 as the<br> initial value in step 2 inversion. Mantle densities are derived based on the output temperature<br> field from step 1 (kept fixed) and the bulk mantle composition inversion variables.</p> <p>&nbsp;</p> <p>&nbsp;</p> <p>*******************************</p> <p>This archive contains the following files:<br> &nbsp; README (this file)<br> &nbsp; WINTERC-G_Vp-Vs.lis (triangular grid)<br> &nbsp; WINTERC-G_rad_anis_Vs.lis (triangular grid)<br> &nbsp; WINTERC-G_Temperature.lis (triangular grid)<br> &nbsp; WINTERC-G_Density.lis (triangular grid)<br> &nbsp; WINTERC-G_LAB.lis (triangular grid)<br> &nbsp; WINTERC_T_rho_1D.z (1D average model of temperature and density)<br> &nbsp; rho_*_out.xyz (0.5 deg egular grid for gravity field)<br> &nbsp; ETOPO2_km_continental.xyz (0.5 deg egular grid for gravity field)<br> &nbsp; ETOPO2_km_depth_Ice.xyz (0.5 deg egular grid for gravity field)<br> &nbsp; ETOPO2_km_depth_Bed.xyz (0.5 deg egular grid for gravity field)<br> &nbsp; Global_Moho_WINTERC-G.xyz (0.5 deg egular grid for gravity field)</p> <p><br> Files in the triangular grid with an average 225 km lateral inter-knot spacing (12232 grid points):</p> <p>* WINTERC-G_Vp-Vs.lis: Vp and Vs (in km/s) in all model columns with a vertical grid step of 2 km<br> &nbsp;Format for each column:<br> &nbsp;#Column number longitude latitude depth(km, &lt;0 downwards) Vp (km/s) Vs(km/s)<br> &nbsp;&nbsp;&nbsp;&nbsp; 5640&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 93.72&nbsp;&nbsp;&nbsp;&nbsp; 4.135&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; -5.0&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3.91&nbsp;&nbsp;&nbsp;&nbsp; 2.11</p> <p><br> * WINTERC-G_rad_anis_Vs.lis: radial anisotropy, (Vsh-Vsv)/Vs_iso (in %) in all model columns with a vertical grid step of 2 km<br> &nbsp; Format for each column:<br> &nbsp; #Column number longitude latitude depth(km, &lt;0 downwards) anisotropy (%)</p> <p>* WINTERC-G_Temperature.lis: temperature (in &ordm;C) in all model columns with a vertical grid step of 2 km<br> &nbsp;Format for each column:<br> &nbsp; #Column number longitude latitude depth (km, &lt;0 downwards) T (&ordm;C)&nbsp;&nbsp; dT (%)&nbsp;&nbsp; dT(K)&nbsp; &nbsp;<br> &nbsp;&nbsp;&nbsp;&nbsp; 6437&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 297.20&nbsp;&nbsp;&nbsp; -2.524&nbsp;&nbsp;&nbsp;&nbsp; -259.000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 1431.9&nbsp;&nbsp; -1.91&nbsp;&nbsp;&nbsp;&nbsp; -27.9<br> &nbsp; The anomalies dT are in % and K with respect to the 1D model in WINTERC_T_rho_1D.z (column 2).</p> <p>* WINTERC-G_Density.lis: density (in kg/m3) in all model columns with a vertical grid step of 2 km<br> &nbsp;Format for each column:<br> &nbsp; #Column number longitude latitude depth(km, &lt;0 downwards) rho (kg/m3) drho(%) drho(kg/m3)<br> &nbsp; The anomalies drho are in % and kg/m3 with respect to the 1D model in WINTERC_T_rho_1D.z (column 3).</p> <p>* WINTERC_T_rho_1D.z: 1D average model of temperature (column 2 in &ordm;C) and density (column 3 in kg/m3) with a vertical grid step of 2 km &nbsp;<br> &nbsp;&nbsp; 5.00000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 0.0000000000000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 6.0259973839110526<br> &nbsp;&nbsp; 3.00000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 0.0000000000000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 38.960571309690394<br> &nbsp;&nbsp; 1.00000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 0.33634006819423840&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 174.42296045978722<br> &nbsp; -1.00000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3.8888495253719624&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 1692.8437489147236<br> &nbsp; -3.00000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 23.974111923225379&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 1863.8834351235944<br> &nbsp; -5.00000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 47.727920701943034&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 2568.2414495590924<br> &nbsp; -7.00000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 89.633398074381162&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 2819.8386016341910<br> &nbsp; -9.00000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 137.01489361657013&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 2839.5325893195904<br> &nbsp; -11.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 182.35233447017222&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 2897.6600872935287<br> &nbsp; -13.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 224.46247069572485&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 2945.2036923862997<br> &nbsp; -15.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 260.63395547331390&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3069.6809340323475<br> &nbsp; -17.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 292.28175449521456&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3132.4574175461721<br> &nbsp; -19.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 322.29571965406632&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3145.5747337463940<br> &nbsp; -21.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 351.58698283375054&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3157.2401512748038<br> &nbsp; -23.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 380.30002225705056&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3177.0000420059773<br> &nbsp; -25.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 408.50259805632055&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3183.6651032398490<br> &nbsp; -27.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 436.22632217636487&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3190.9586785996116<br> &nbsp; -29.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 463.48733903170023&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3198.9369509456310<br> &nbsp; -31.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 490.29841705549831&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3209.7229872383764<br> &nbsp; -33.0000000&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 516.71149258457456&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; 3221.6329506091679<br> &nbsp; ...</p> <p>Files in the interpolated regular grid at 0.5 deg lateral resolution used for gravity field data inversion:</p> <p>&nbsp; * rho_c_out.xyz: average crustal density<br> &nbsp; * rho_submoho_out.xyz: mantle density below the Moho discontinuity<br> &nbsp; * rho_*_out.xyz: mantle density defined at different model depths: 20, 35, 56, 80, 110, 150, 200, 260, 330 and 400 km.</p> <p>&nbsp; Format for the density files:<br> &nbsp; # longitude latitude density (kg/m3)<br> &nbsp;<br> &nbsp; Files containing layer discontinuities:</p> <p>&nbsp;* ETOPO2_km_continental.xyz: surface elevation including ice sheet and 0 in marine areas (km, &lt;0 upwards)</p> <p>&nbsp;* ETOPO2_km_depth_Ice.xyz: surface elevation including ice sheet (km, &gt;0 downwards, &lt;0 above sea level)</p> <p>&nbsp;* ETOPO2_km_depth_Bed.xyz: bedrock surface elevation without ice sheet (km, &gt;0 downwards, &lt;0 above sea level)</p> <p>&nbsp;* Global_Moho_WINTERC-G.xyz: crust-mantle discontinuity depth (km, &gt;0 downwards)</p> <p>&nbsp; Format for the discontinuity files:<br> &nbsp;&nbsp; # longitude latitude depth (km)<br> &nbsp;<br> &nbsp;<br> The gravity field in WINTERC-G is computed using an spherical harmonic formalism and a model discretization<br> in 13 layers with laterally varying density. The first 7 layers are characterized by top and bottom boundaries with laterally varying radius whereas the last 6 layers are defined by top and bottom boundaries with constant radius:</p> <p>1/ Water: from ETOPO2_km_continental.xyz to ETOPO2_km_depth_Ice.xyz with rho=1030 kg/m3 (constant vertically)</p> <p>2/ Ice: from ETOPO2_km_depth_Ice.xyz to ETOPO2_km_depth_Bed.xyz&nbsp; with rho=910 kg/m3 (constant vertically)</p> <p>3/ Crust: from ETOPO2_km_depth_Bed to Global_Moho_WINTERC-G.xyz with rho=rho_c_out.xyz (constant vertically)</p> <p>4/ submoho-20km: from Global_Moho_WINTERC-G.xyz to z_20km (file with 20 km everywhere except where z_moho&gt;20km) with rho=rho_submoho_out.xyz (top) and rho=rho_20km_out.xyz (bottom)</p> <p>5/ 20km-36km: from&nbsp; z_20km (file with 20 km everywhere except where z_moho&gt;20km) to z_36km (file with 36 km everywhere except where z_moho&gt;36km)&nbsp;&nbsp; with rho=rho_20km_out.xyz (top) and rho=rho_36km_out.xyz (bottom)</p> <p>6/ 36km-56km: from&nbsp; z_36km (file with 36 km everywhere except where z_moho&gt;36km) to z_56km (file with 56 km everywhere except where z_moho&gt;56km)&nbsp;&nbsp; with rho=rho_36km_out.xyz (top) and rho=rho_56km_out.xyz (bottom)</p> <p>7/ 56km-80km: from&nbsp; z_56km (file with 56 km everywhere except where z_moho&gt;56km) to 80 km depth with rho=rho_56km_out.xyz (top) and rho=rho_80km_out.xyz (bottom)</p> <p>The next 6 layers are computed using the constant radius option:</p> <p>8/ 80km-110km: from z=80km to z=110 km with rho=rho_80km_out.xyz (top) and rho=rho_110km_out.xyz (bottom)</p> <p>9/ 110km-150km: from z=110km to z=150 km with rho=rho_110km_out.xyz (top) and rho=rho_150km_out.xyz (bottom)</p> <p>10/ 150km-200km: from z=150km to z=200 km with rho=rho_150km_out.xyz (top) and rho=rho_200km_out.xyz (bottom)</p> <p>11/ 200km-260km: from z=200km to z=260 km with rho=rho_200km_out.xyz (top) and rho=rho_260km_out.xyz (bottom)</p> <p>12/ 260km-330km: from z=260km to z=330 km with rho=rho_260km_out.xyz (top) and rho=rho_330km_out.xyz (bottom)</p> <p>13/ 330km-400km: from z=330km to z=400 km with rho=rho_330km_out.xyz (top) and rho=rho_400km_out.xyz (bottom)</p> <p>&nbsp;</p> <p>&nbsp;</p>

opencc-by-4.0Jul 2021View details →
zenodo44/100

Test and numerical data of a vapour-injection scroll compressor in a heat pump with R1234ze(E)

<p>The dataset contains the experimental results of a water-to-water heat pump tested at the lab for different water temperatures. The refrigerant used is the HFO R1234ze(E). The scroll compressor is equipped with an eco port. The numerical results of a validated semi-empirical model are also included for a standard suction pressure drop model and an improved one.</p>

opencc-by-4.0Dec 2021View details →
zenodo44/100

Within Population Variability of Coral Heat Tolerance - Images

<p>Image dataset used for a colour analysis of coral branches throughout a long-term marine heatwave emulation experiment using machine learning. Article: &quot;Within population variability in coral heat tolerance indicates climate adaptation potential&quot; by Humanes and Lachs et al. Code to analyse the dataset is found at&nbsp;10.5281/zenodo.6256164.</p>

opencc-by-4.0Feb 2022View details →
zenodo44/100

Heat map of Trans-Himalayan languages

<p>This is a modified heat map showing the Trans-Himalayan languages used in the study by Wu, Bodt and Tresoldi (accepted; Supplement, page 11, Figure 4). The map has also been used in the publication&nbsp;Bodt (accepted).</p> <p>Wu, Mei-Shin, Timotheus A. Bodt &amp; Tiago Tresoldi. accepted.&nbsp;Bayesian phylogenetics illuminate shallower relationships among Trans-Himalayan languages in the Tibet-Arunachal area. <em>Linguistics of the Tibeto-Burman Area.</em></p> <p>Bodt, Timotheus Adrianus. accepted.&nbsp;<em>Proto-Western Kho-Bwa: Reconstructing the past of a small indigenous community.</em>&nbsp;Academia Sinica Language and Linguistics monograph series.</p> <p>&nbsp;</p>

opencc-by-4.0Apr 2022View details →
zenodo44/100

FAIR raw data and heat maps of ARAP deposition modeling

<p>FAIR Supplementary Information and Raw Data for <a href="https://www.plus.ac.at/biowissenschaften/der-fachbereich/arbeitsgruppen/duschl/members/martin-himly/list-of-publications/">Hofer S. et al., 2021, SARS-CoV-2-Laden Respiratory Aerosol Deposition in the Lung Alveolar-Interstitial Region Is a Potential Risk Factor for Severe Disease: A Modeling Study, Journal of Personalized Medicine 11(5):431</a>, DOI: <a href="https://doi.org/10.3390/jpm11050431">https://doi.org/10.3390/jpm11050431</a></p> <p>1. pdf/A of deposition heat maps (incl probability values) for 5 different ARAP modes</p> <p>2. xls-formatted file of MPPD v3.04-derived deposition raw data sets for 5 different ARAP modes</p> <p>3.-7. rpt-formatted MPPD v3.04 files of deposition raw data sets for 5 different ARAP modes</p> <p>8.-12. csv-formatted files of MPPD v3.04-derived deposition raw data sets for 5 different ARAP modes</p> <p>13. pdf/A of deposition heat maps (incl probability values) for 5 different ERAP modes (upon rehydration of ARAPs)</p> <p>14. txt-formatted README file for Hofer et al 2021</p>

opencc-by-4.0Dec 2020View details →
zenodo44/100

video_heating

This is the process of making a carafe Bontemps. The step depicted is called "Annealing"(from the Mingei project).

opencc-by-sa-4.0Aug 2022View details →
zenodo44/100

Planktonic Mg/Ca-derived IPWP upper ocean temperature, heat content and sea water δ18O over the last 360 ka

<p>This dataset contains planktonic foraminifera Mg/Ca-derived temperature estimates, age control points and sea water &delta;18O (&delta;18Osw) of cores ODP807, KX21-2, MD10-3340, SO18480-3 and MD98-2162 from the Indo-Pacific Warm Pool (IPWP) over the last 360 ka. It also includes reconstructed IPWP stacks of SST, TWT, upper OHC and &delta;18Osw, and numerical simulated upper OHC, &delta;18Osw (sea water) and &delta;18Op (rainfall) from the CESM model and GISS-ModelE2-R model.</p>

opencc-by-4.0Aug 2022View details →
zenodo44/100

VirgoA M87 Heat Transfer

<p>The research continued from the white hole observation experiment with data analysis. The math- ematical method derived before the observation is supplemented with the heat transfer method. The research took an empirical boundary approach on heat flux for the heat transfer between a black hole and white hole, without considering the Big Bang theory. The heat transfer in the system material boundary is seen as a gravitational indicator from asymptotic decay. Albeit the numerical results are instrumentation specific, the conceptualization of the method can be applied to other data imaging apparatus. However, this method is material dependent, and the estimation of the imaginary time di- mension depends on the chemical components of incident light and detection plate. It puts the cosmic microwave background to the account of instrumentation noise, and conceptualized cosmic background radiation for asymptotic safety. The convergence and divergence can be further corrected by different bias factors.</p>

opencc-by-4.0Aug 2021View details →
zenodo44/100

video_heating

This is the process of making a carafe Bontemps. The step depicted is called "Annealing"(from the Mingei project).

opencc-by-sa-4.0Aug 2022View details →

ScienceDex guides

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These curated guides explain access requirements, typical timelines, costs, and reuse considerations for widely used research datasets.

Compare curated datasets

Allen Brain Atlas

Allen Brain Atlas is an Allen Institute collection of brain map atlases, datasets, APIs, and analysis tools covering mouse, human, and non-human primate brain resources.

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

Annotated Behaviour and Observability Dataset (ABODe)

ABODe is a University of Edinburgh DataShare dataset for behavior classification in group-housed mice using home-cage video, identities, bounding boxes, ground-plate positions, and annotator labels.

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

DANDI is a BRAIN Initiative archive for publishing and sharing neurophysiology data, including electrophysiology, optophysiology, and behavioral data packaged as NWB and related standards.

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

OpenNeuro is a free, open platform for sharing neuroimaging datasets, with public search, dataset pages, and download paths for web, S3, DataLad, and the OpenNeuro CLI.

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