cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.15468/dl.q4tzcl
title: Occurrence Download

description: A dataset containing 93497 species occurrences available in GBIF matching the query:
{
 "DatasetKey" : [
 "is Déterminations et observations du Forum \"Le Monde des Insectes\" (LMDI)-Données photographiques validées de la galerie du forum \"Le Monde des Insectes\""
 ]
}

 The dataset includes 93497 records from 1 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0024924-200221144449610/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.1594/pangaea.949055
title: Optimal growth (classic, Re=2000,A=1,Wo=15): time series for selected t0

description: The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe flows. In this study, a Newtonian fluid driven by pulsatile and oscillatory flow rate flows in a straight pipe. In pulsatile flow, there are three governing parameters: steady Reynolds number (defined by the steady flow component), pulsation amplitude (ratio of oscillatory and steady flow component) and Womersley number (dimensionless pulsation and oscillation frequency). In oscillatory flow, due to vanishment of steady flow component, oscillatory Reynolds number (defined by the oscillation flow component) and Womersley number. The Reynolds number defined by the thickness of Stokes layer is alternatively used for the oscillatory Reynolds number. The study was carried out in a manner that one governing parameter varies while other governing parameters are fixed.The data file 'time_TG_all.dat' shows the maximum energy amplification over all modes at each time instant.This file includes three columns: the first column indicates dimensionless time; the second column indicates the time normalized by the pulsation period; the third column indicates the energy amplification at a time instant (first column).
description: #(Re,A,Wo)=(2000,1.00,15.00)VARIABLES = VARIABLES = k_z, k_theta, phase, time, G(t)ZONE T="enveloped TG", I=10000, J=1
DOI: 10.1594/pangaea.949057
title: Optimal growth (helical, Re=2000,A=1,Wo=15): time series for selected t0

description: The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe flows. In this study, a Newtonian fluid driven by pulsatile and oscillatory flow rate flows in a straight pipe. In pulsatile flow, there are three governing parameters: steady Reynolds number (defined by the steady flow component), pulsation amplitude (ratio of oscillatory and steady flow component) and Womersley number (dimensionless pulsation and oscillation frequency). In oscillatory flow, due to vanishment of steady flow component, oscillatory Reynolds number (defined by the oscillation flow component) and Womersley number. The Reynolds number defined by the thickness of Stokes layer is alternatively used for the oscillatory Reynolds number. The study was carried out in a manner that one governing parameter varies while other governing parameters are fixed.The data file 'time_TG_helical.dat' shows the time series of the maximum energy amplification of a helical perturbation.This file includes five columns: the first column indicates streamwise wavenumber or axial wavenumber; the second column indicates the azimuthal wavenumber; the third column indicates the phase of the perturbation; the fourth column indicates the dimensionless time; the fifth column indicates the maximum energy amplification at the time instant.
description: #(Re,A,Wo)=(2000,1.00,15.00)VARIABLES = k_z, k_theta, phase, time, G(t)ZONE T= "data", I=26, J=1
DOI: 10.1594/pangaea.949058
title: Optimal wavenumber envelope (Re=2000,A=1,Wo=15)

description: The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe flows. In this study, a Newtonian fluid driven by pulsatile and oscillatory flow rate flows in a straight pipe. In pulsatile flow, there are three governing parameters: steady Reynolds number (defined by the steady flow component), pulsation amplitude (ratio of oscillatory and steady flow component) and Womersley number (dimensionless pulsation and oscillation frequency). In oscillatory flow, due to vanishment of steady flow component, oscillatory Reynolds number (defined by the oscillation flow component) and Womersley number. The Reynolds number defined by the thickness of Stokes layer is alternatively used for the oscillatory Reynolds number. The study was carried out in a manner that one governing parameter varies while other governing parameters are fixed.The data file 'time_wavenumber.dat' shows the optimal wavenumber (corresponding to the maximum energy amplification) at a time instant.This file includes three columns: the first column indicates the dimensionless time normalized by the pulsation period; the second column indicates the optimal axial wavenumber at the time instant; the third column indicates the optimal azimuthal wavenumber at the time instant.
description: #(Re,A,Wo)=(2000,1.00,15.00)VARIABLES = "time/period", "axial wavenumber (k)", "azimuthal wavenumber (m)"ZONE T="data", I=101, J=1
DOI: 10.1594/pangaea.949070
title: Optimal growth (Re=2000,A=1,Wo=15): value of TG as function to and tf (computed)

description: The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe flows. In this study, a Newtonian fluid driven by pulsatile and oscillatory flow rate flows in a straight pipe. In pulsatile flow, there are three governing parameters: steady Reynolds number (defined by the steady flow component), pulsation amplitude (ratio of oscillatory and steady flow component) and Womersley number (dimensionless pulsation and oscillation frequency). In oscillatory flow, due to vanishment of steady flow component, oscillatory Reynolds number (defined by the oscillation flow component) and Womersley number. The Reynolds number defined by the thickness of Stokes layer is alternatively used for the oscillatory Reynolds number. The study was carried out in a manner that one governing parameter varies while other governing parameters are fixed.The data file 't0_TG_contour.dat' shows the maximum energy amplification over modes in the parameter regime of initial time and final time.This file includes three columns: the first column indicates initial time of perturbations normalized by pulsation period; the second column indicates the evolution time of the perturbation normalized by period; the third column indicates the energy amplification corresponding to the initial time (first column) and the evolution time (second column).
description: #t0:initial time; tf:end time; tau:time duration, tau=tf-t0VARIABLES = "t0/period", "(tf-t0)/period", "G(t0,tau)"ZONE T="data", I=21, J=21
DOI: 10.15468/dl.q6qbpf
title: Occurrence Download

description: A dataset containing 180952 species occurrences available in GBIF matching the query:
{
 "and" : [
 {
 "and" : [
 "HasGeospatialIssue is false",
 "HasCoordinate is true",
 {
 "not" : {
 "BasisOfRecord" : [
 "is one of (Fossil, Living Specimen)"
 ]
 }
 }
 ]
 },
 "TaxonKey is one of (Odonata, Ephemeroptera, Insecta, Trichoptera)",
 "Country is one of (Kenya)"
 ]
}

 The dataset includes 180952 records from 281 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0037145-231002084531237/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.1594/pangaea.949072
title: Optimal growth (Re=2000,A=1,Wo=15): value of TG as function to and tf (interpolated to plot)

description: The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe flows. In this study, a Newtonian fluid driven by pulsatile and oscillatory flow rate flows in a straight pipe. In pulsatile flow, there are three governing parameters: steady Reynolds number (defined by the steady flow component), pulsation amplitude (ratio of oscillatory and steady flow component) and Womersley number (dimensionless pulsation and oscillation frequency). In oscillatory flow, due to vanishment of steady flow component, oscillatory Reynolds number (defined by the oscillation flow component) and Womersley number. The Reynolds number defined by the thickness of Stokes layer is alternatively used for the oscillatory Reynolds number. The study was carried out in a manner that one governing parameter varies while other governing parameters are fixed.The data file 't0_TG_contour.dat' shows the maximum energy amplification over modes in the parameter regime of initial time and final time.This file includes three columns: the first column indicates initial time of perturbations normalized by pulsation period; the second column indicates the evolution time of the perturbation normalized by period; the third column indicates the energy amplification corresponding to the initial time (first column) and the evolution time (second column).
description: #t0:initial time; tf:end time; tau:time duration, tau=tf-t0VARIABLES = "t0/period", "(tf-t0)/period", "G(t0,tau)"ZONE T="data, interp2", I=100, J=100
DOI: 10.1594/pangaea.949074
title: Detailed mineral proportion reconstruction for batch experiments simulating hydrothermal troctolite alteration at 300 and 400°C (40 MPa)
DOI: 10.1594/pangaea.948575
title: Optimal growth envelope (Re=2000,A=1,Wo=15)

description: The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe flows. In this study, a Newtonian fluid driven by pulsatile and oscillatory flow rate flows in a straight pipe. In pulsatile flow, there are three governing parameters: steady Reynolds number (defined by the steady flow component), pulsation amplitude (ratio of oscillatory and steady flow component) and Womersley number (dimensionless pulsation and oscillation frequency). In oscillatory flow, due to vanishment of steady flow component, oscillatory Reynolds number (defined by the oscillation flow component) and Womersley number. The Reynolds number defined by the thickness of Stokes layer is alternatively used for the oscillatory Reynolds number. The study was carried out in a manner that one governing parameter varies while other governing parameters are fixed.The data file 'Fig2a_time_TG_all.dat' shows the maximum energy amplification over all perturbations at each time instant.This file includes three columns: the first column indicates dimensionless time; the second column indicates the time normalized by the pulsation period; the third column indicates the energy amplification at a time instant (first column).
description: #(Re,A,Wo)=(2000,1.00,15.00)VARIABLES = "t", "t/T", "TG(t)"ZONE T="enveloped TG", I=10000, J=1
DOI: 10.1594/pangaea.949076
title: Optimal t_f and t_0 as function of Re (A=1,Wo=15)

description: The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe flows. In this study, a Newtonian fluid driven by pulsatile and oscillatory flow rate flows in a straight pipe. In pulsatile flow, there are three governing parameters: steady Reynolds number (defined by the steady flow component), pulsation amplitude (ratio of oscillatory and steady flow component) and Womersley number (dimensionless pulsation and oscillation frequency). In oscillatory flow, due to vanishment of steady flow component, oscillatory Reynolds number (defined by the oscillation flow component) and Womersley number. The Reynolds number defined by the thickness of Stokes layer is alternatively used for the oscillatory Reynolds number. The study was carried out in a manner that one governing parameter varies while other governing parameters are fixed.The data file 't0_tf_Re_Wo15.dat' shows the variation of optimal time (corresponding to the maximum energy amplification) with the Reynolds numbers.This file includes fourth columns: the first column indicates the Reynolds number; the second column indicates the initial time of perturbations normalized by pulsation period; the third column indicates the evolution time of the perturbation normalized by period; the fourth column indicates the final time normalized by the period.
description: #(A,Wo)=(1.00,15.00)#t0:initial time; tf:end time; tf-t0:time durationVARIABLES = "Re", "t0/T", "(tf-t0)/T", "tf/T"ZONE T="data, raw", I=10, J=1
DOI: 10.15468/dl.ba5cz7
title: Occurrence Download

description: A dataset containing 450 species occurrences available in GBIF matching the query:
{
 "DatasetKey" : [
 "is Données papillons en Auvergne, observations de Philippe Bachelard. - Données papillons en Auvergne, observations synthétisées par Philippe Bachelard 2001-2016, espèces déterminantes des ZNIEFF Massif Central."
 ]
}

 The dataset includes 450 records from 1 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0024923-200221144449610/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.qbs8eh
title: Occurrence Download

description: A dataset containing 404 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is one of (Apamea exulis (Lefèbvre, 1836))",
 "Geometry POLYGON((-9.36035 44.71551,-10.59082 42.81152,-11.82129 36.80928,-7.69043 36.17336,-3.38379 35.88905,3.12012 38.13456,9.18457 38.20366,11.7334 37.16032,12.78809 34.74161,17.09473 33.79741, 23.15918 34.23451,30.10254 32.62087,33.2666 32.99024,35.72754 35.03,33.00293 35.53223,28.69629 35.17381,28.34473 36.31513,25.7959 37.50973,24.91699 39.90974,28.78418 40.6473,30.71777 41.17865,36.87012 45.213,38.18848 46.98025,38.71582 47.7541,39.94629 47.93107,40.20996 49.61071,37.0459 50.34546,35.72754 50.40152,33.79395 52.26816,31.68457 51.94426,31.4209 53.27835,32.56348 53.43572,30.98145 54.77535,30.89355 55.52863,28.43262 56.02295,27.20215 57.65716,27.37793 58.30949,27.90527 59.17593,29.66309 59.88894,27.6416 60.58697,31.50879 62.75473,28.78418 69.83962,30.89355 70.28912,29.22363 71.55274,21.75293 71.30079,14.28223 70.14036,11.38184 67.47492,4.87793 63.66576,-5.53711 71.52491,-10.63477 71.69129,-21.5332 67.74276,-28.56445 65.36684,-24.3457 61.35461,-9.36035 44.71551))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "Year is greater than or equal to 1980",
 "Year is less than or equal to 2021"
 ]
}

 The dataset includes 404 records from 20 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0231013-210914110416597/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.1594/pangaea.949126
title: Lightchain measurements from radiation station 2020R10

description: Solar radiation over and under sea ice was measured by radiation station 2020R10, an autonomous platform, installed on drifting First-Year-Ice (FYI) in the Arctic Ocean during MOSAiC (Leg 2) 2019/20. The resulting time series describes radiation measurements as a function of place and time between 08 March 2020 and 21 July 2020 in sample intervals of 1 hour. The radiation measurements have been performed with spectral radiometers. All data are given in full spectral resolution interpolated to 1.0 nm, and integrated over the entire wavelength range (broadband, total: 320 to 950 nm). Two sensors, solar irradiance and upward reflected solar irradiance, were mounted on a on a platform about 1 m above the sea ice surface. The third sensor was mounted 0.5 m underneath the sea ice measuring the downward transmitted irradiance. Along with the radiation measurements, this autonomous platform consisted of a lightchain, which measured counts of red, green and blue light at 49 positions at hourly intervals. In addition, the evolution of snow height is measured at hourly intervals. All times are given in UTC.
description: The data set has been processed and contains quality flags for different kinds for erroneous data. Flag values are the sum of individual error codes. The value of 0 refers to no error. Quality flag, position: The geographic position is flagged +1 if the drift velocity, as derived from the GPS longitude and latitude, exceeds a threshold of 10 deg latitude or 50 deg longitude per time step; +2 if the position exceeds extreme values, such as longitude &gt; 360 deg; +4 if the position is exactly 0.0.
DOI: 10.15468/dl.c2mt9a
title: Occurrence Download

description: A dataset containing 320 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Spectrunculus grandis (Günther, 1877)"
 ]
}

 The dataset includes 320 records from 46 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0037149-231002084531237/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.1594/pangaea.950006
title: Raw calculation of error analysis and its statistics of sediment facies from the East Frisian Wadden Sea, Germany
DOI: 10.1594/pangaea.950013
title: Grid search results during the sediment-facies classification model's training from the East Frisian Wadden Sea, Germany
DOI: 10.15468/dl.p7pdih
title: Occurrence Download

description: A dataset containing 2154 species occurrences available in GBIF matching the query:
{
 "DatasetKey" : [
 "is SILENE-FAUNE-PACA - Ecole_pratique_des_hautes_études_2017_12_18"
 ]
}

 The dataset includes 2154 records from 1 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0024949-200221144449610/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.1594/pangaea.949136
title: Optimal growth as function of Re (A=1,Wo=15)

description: The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe flows. In this study, a Newtonian fluid driven by pulsatile and oscillatory flow rate flows in a straight pipe. In pulsatile flow, there are three governing parameters: steady Reynolds number (defined by the steady flow component), pulsation amplitude (ratio of oscillatory and steady flow component) and Womersley number (dimensionless pulsation and oscillation frequency). In oscillatory flow, due to vanishment of steady flow component, oscillatory Reynolds number (defined by the oscillation flow component) and Womersley number. The Reynolds number defined by the thickness of Stokes layer is alternatively used for the oscillatory Reynolds number. The study was carried out in a manner that one governing parameter varies while other governing parameters are fixed.The data file 'TG_Re_Wo15.dat' shows the dependence of the maximum energy amplification on the Reynolds numbers at Womersley number of 15 and pulsation amplitude of 1.This file includes two columns: the first column indicates the Reynolds number; the second column indicates the maximum energy amplifiation.
description: #(A,Wo)=(1.00,15.00)#t0:initial time; tf:end time;VARIABLES = "Re", "TG (max in a Re)"ZONE T="data, raw", I=10, J=1
DOI: 10.1594/pangaea.949619
title: AWI EMR radar data upstream of the northern catchment of the Nioghalvfjerdsbrae (79°North Glacier), Northeast Greenland

description: Here we present AWI EMR radio-echo sounding data in northeast Greenland upstream of the northern catchment of the Nioghalvfjerdsbrae (79°North Glacier; 79NG). The radar data were acquired with AWI's EMR radar system in 1998. The radar lines are located between the central ice divide and the Northeastern glacier outlet region. The radio-echo sounding data was used to decipher the regional ice-flow history of the northeastern Greenland Ice Sheet based on its internal stratigraphy by mapping folds deep below the surface that we then attribute to the deformation caused by now-extinct ice streams. Locally, this ancient ice flow regime was much more focused and reached much further inland than today's and was deactivated when the main drainage system was reconfigured and relocated southwards.
description: Owner/PI: Daniel Steinhage and Olaf Eisen (Alfred Wegener Institute)Email address of the provider:daniel.steinhage@awi.deolaf.eisen@awi.deInstrument used: AWI EMR RadarData Description: We present the radar data and additional variables in the .mat format as well as figures with a radargram plot for each profile.Profile numbers:983518983525983526983529983531Matfile variablesData : Matrix containing the return power values (not in dB)Time : Array containing the time information (two-way traveltime) in range (seconds)Longitude, Latitude : Coordinates of each traceElevation : GPS Elevation of the aircraft (meters above sea level)Surface : Two-way traveltime of the surface reflection (seconds)Surface_idx : Pixel position of the surface reflection
DOI: 10.15468/dl.5jq7sn
title: Occurrence Download

description: A dataset containing 332 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Monopteryx uaucu Spruce ex Benth."
 ]
}

 The dataset includes 332 records from 30 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0021480-231002084531237/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.x6zeu7
title: Occurrence Download

description: A dataset containing 163 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Moho nobilis (Merrem, 1786)"
 ]
}

 The dataset includes 163 records from 21 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0112465-230224095556074/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.nf7zwb
title: Occurrence Download

description: A dataset containing 0 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Telmatobufo ignotus Cuevas, 2010"
 ]
}

 The dataset includes 0 records from 0 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0299308-210914110416597/datasets/export for details.
DOI: 10.1594/pangaea.949138
title: Optimal growth as function of Re (A=1,Wo=25)

description: The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe flows. In this study, a Newtonian fluid driven by pulsatile and oscillatory flow rate flows in a straight pipe. In pulsatile flow, there are three governing parameters: steady Reynolds number (defined by the steady flow component), pulsation amplitude (ratio of oscillatory and steady flow component) and Womersley number (dimensionless pulsation and oscillation frequency). In oscillatory flow, due to vanishment of steady flow component, oscillatory Reynolds number (defined by the oscillation flow component) and Womersley number. The Reynolds number defined by the thickness of Stokes layer is alternatively used for the oscillatory Reynolds number. The study was carried out in a manner that one governing parameter varies while other governing parameters are fixed.The data file 'TG_Re_Wo25.dat' shows the dependence of the maximum energy amplification on the Reynolds numbers at Womersley number of 25 and pulsation amplitude of 1.This file includes two columns: the first column indicates the Reynolds number; the second column indicates the maximum energy amplifiation.
description: #(A,Wo)=(1.00,25.00)#t0:initial time; tf:end time;VARIABLES = "Re", "TG (max in a Re)"ZONE T="data, raw", I=6, J=1