cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.5517/ccdc.csd.cc2g01g0
title: CCDC 2264161: Experimental Crystal Structure Determination

description: Related Article: Robert J. Ward, Pokpong Rungthanaphatsophon, Patrick Huang, Steven P. Kelley, Justin R. Walensky|2023|Chemical Science|14|12255|doi:10.1039/D3SC04857H
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.5517/ccdc.csd.cc2g01h1
title: CCDC 2264162: Experimental Crystal Structure Determination

description: Related Article: Robert J. Ward, Pokpong Rungthanaphatsophon, Patrick Huang, Steven P. Kelley, Justin R. Walensky|2023|Chemical Science|14|12255|doi:10.1039/D3SC04857H
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.5517/ccdc.csd.cc2g01j2
title: CCDC 2264163: Experimental Crystal Structure Determination

description: Related Article: Robert J. Ward, Pokpong Rungthanaphatsophon, Patrick Huang, Steven P. Kelley, Justin R. Walensky|2023|Chemical Science|14|12255|doi:10.1039/D3SC04857H
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.5517/ccdc.csd.cc2g01k3
title: CCDC 2264164: Experimental Crystal Structure Determination

description: Related Article: Robert J. Ward, Pokpong Rungthanaphatsophon, Patrick Huang, Steven P. Kelley, Justin R. Walensky|2023|Chemical Science|14|12255|doi:10.1039/D3SC04857H
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.5517/ccdc.csd.cc2g01l4
title: CCDC 2264165: Experimental Crystal Structure Determination

description: Related Article: Robert J. Ward, Pokpong Rungthanaphatsophon, Patrick Huang, Steven P. Kelley, Justin R. Walensky|2023|Chemical Science|14|12255|doi:10.1039/D3SC04857H
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.5517/ccdc.csd.cc2g01m5
title: CCDC 2264166: Experimental Crystal Structure Determination

description: Related Article: Robert J. Ward, Pokpong Rungthanaphatsophon, Patrick Huang, Steven P. Kelley, Justin R. Walensky|2023|Chemical Science|14|12255|doi:10.1039/D3SC04857H
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.5517/ccdc.csd.cc2g01n6
title: CCDC 2264167: Experimental Crystal Structure Determination

description: Related Article: Robert J. Ward, Pokpong Rungthanaphatsophon, Patrick Huang, Steven P. Kelley, Justin R. Walensky|2023|Chemical Science|14|12255|doi:10.1039/D3SC04857H
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.13120/b5c47c8c-d969-4f9b-ae90-916f87e461a5
title: Contaminants: Pesticides and biocides - DDT-DDE-DDD (measurements counts), v2023
title: Contaminants: Pesticides and biocides - DDT-DDE-DDD (measurements counts), v2023

description: This product displays for DDT, DDE, and DDD, positions with values counts that have been measured per matrix and are present in EMODnet validated datasets. The product displays positions for all available years and per year.
DOI: 10.13120/49318321-4165-4bf3-9464-d128a6bee0d4
title: Contaminants: Pesticides and biocides - Hexachlorobenzene (measurements counts), v2023
title: Contaminants: Pesticides and biocides - Hexachlorobenzene (measurements counts), v2023

description: This product displays for Hexachlorobenzene, positions with values counts that have been measured per matrix and are present in EMODnet validated datasets. The product displays positions for all available years and per year.
DOI: 10.5281/zenodo.10116288
title: Acoustical measurements of a rabab reconstructed after a pictorial source from the 14th century

description: Instrument: rabab Pictorial source: Francesc Comes, Madonna and Child with angel musicians, around 1394, Gold and tempera on wood, Pollença (Mallorca), Museu de Pollença Instrument maker: Thilo Hirsch Year of manufacture: 2022 Location: Basel, property of the ensemble arcimboldo
Dimensions: Total length: 579 mm Max. Body width: 112 mm Body depth: approx. 95 mm 
Vibrating string lengths: d-string: 500 mm G-string: 497 mm
Materials: Body: cherry Pegbox: cherry Fingerboard: serviceberry Bars: spruce Nut/String attachment button: bone Bridge: boxwood Top: goatskin
The main aim of this research was to measure the acoustic effects of the different sound holes. To do this, the instrument was first measured with the upper rosette and the two holes in the body closed, then with both rosettes and the body holes open, and finally only with the body holes closed.
Acoustical measurements: Alexander Mayer, mdw - University of Music and Performing Arts Vienna, Department of Music Acoustics – Wiener Klangstil (IWK), 25.9.2023
Force: Impact hammer exciting at the bass side of the bridge ACC: Acceleration measured on the same side, close to the impact point. Average is the average of all measurements (to be used in the analysis).
Photos of the setup: Thilo Hirsch
Folder comes_rosette_o_loecher_zu Files: comes_rolz_1 to 6 (Description: upper rosette closed with wooden sheet, body-holes closed)
Folder comes_rosette_oO_loecher_offen Files: comes_roo_lo_1 to 6 (Description: rosette open , body-holes open)
Folder comes_rosette_oO_loecher_zu Files: comes_roo_lz_1 to 6 (Description: rosette open , body-holes closed)          
________________________
How to read VIA-Files:
Line 1 to 9: Header, Line 8 holds the number of values
Data is organized as followed: 1st col: Frequency [Hz], 2nd col: Magnitude [as Factor not dB!], 3rd col: Phase [rad], 4th col:  Real part [as Factor not dB!], 5th col: Imaginary part [as Factor not dB!]. So only first 3 columns are needed!
To get dB Value: Amplitude[dB] = 20 log [Magnitude]
Usually the Magnitude was calculated as response/reference (input) in the frequency domain. As for measuring the mechanical admittance the sensor is most likely an accelerometer (capturing the response in m/s2 of the object of interest) and the reference an impact hammer capturing the input force in Newton. As the mechanical admittance is defined as v/F (speed over force) the acceleration signal has to be integrated. The here captured signals are integrated in the frequency domain, what means the magnitude is divided by the corresponding frequency value in s-1. Values coded like: 3.30750000000000E+1 -> 3.3075 * 10 -> 33.075
DOI: 10.5281/zenodo.10116289
title: Acoustical measurements of a rabab reconstructed after a pictorial source from the 14th century

description: Instrument: rabab Pictorial source: Francesc Comes, Madonna and Child with angel musicians, around 1394, Gold and tempera on wood, Pollença (Mallorca), Museu de Pollença Instrument maker: Thilo Hirsch Year of manufacture: 2022 Location: Basel, property of the ensemble arcimboldo
Dimensions: Total length: 579 mm Max. Body width: 112 mm Body depth: approx. 95 mm 
Vibrating string lengths: d-string: 500 mm G-string: 497 mm
Materials: Body: cherry Pegbox: cherry Fingerboard: serviceberry Bars: spruce Nut/String attachment button: bone Bridge: boxwood Top: goatskin
The main aim of this research was to measure the acoustic effects of the different sound holes. To do this, the instrument was first measured with the upper rosette and the two holes in the body closed, then with both rosettes and the body holes open, and finally only with the body holes closed.
Acoustical measurements: Alexander Mayer, mdw - University of Music and Performing Arts Vienna, Department of Music Acoustics – Wiener Klangstil (IWK), 25.9.2023
Force: Impact hammer exciting at the bass side of the bridge ACC: Acceleration measured on the same side, close to the impact point. Average is the average of all measurements (to be used in the analysis).
Photos of the setup: Thilo Hirsch
Folder comes_rosette_o_loecher_zu Files: comes_rolz_1 to 6 (Description: upper rosette closed with wooden sheet, body-holes closed)
Folder comes_rosette_oO_loecher_offen Files: comes_roo_lo_1 to 6 (Description: rosette open , body-holes open)
Folder comes_rosette_oO_loecher_zu Files: comes_roo_lz_1 to 6 (Description: rosette open , body-holes closed)          
________________________
How to read VIA-Files:
Line 1 to 9: Header, Line 8 holds the number of values
Data is organized as followed: 1st col: Frequency [Hz], 2nd col: Magnitude [as Factor not dB!], 3rd col: Phase [rad], 4th col:  Real part [as Factor not dB!], 5th col: Imaginary part [as Factor not dB!]. So only first 3 columns are needed!
To get dB Value: Amplitude[dB] = 20 log [Magnitude]
Usually the Magnitude was calculated as response/reference (input) in the frequency domain. As for measuring the mechanical admittance the sensor is most likely an accelerometer (capturing the response in m/s2 of the object of interest) and the reference an impact hammer capturing the input force in Newton. As the mechanical admittance is defined as v/F (speed over force) the acceleration signal has to be integrated. The here captured signals are integrated in the frequency domain, what means the magnitude is divided by the corresponding frequency value in s-1. Values coded like: 3.30750000000000E+1 -> 3.3075 * 10 -> 33.075
DOI: 10.13120/263054f4-0c11-4e75-8ed1-a4cbe9383e7d
title: Contaminants: Antifoulants - Tributyltin (measurements counts), v2023
title: Contaminants: Antifoulants - Tributyltin (measurements counts), v2023

description: This product displays for Tributyltin, positions with values counts that have been measured per matrix and are present in EMODnet validated datasets. The product displays positions for all available years and per year.
DOI: 10.5281/zenodo.10116329
title: Acoustical measurements of a rabab reconstructed after a pictorial source from the 16th century

description: Acoustical measurements of a rabab reconstructed after a pictorial source from the 16th century
Instrument: rabab Pictorial source: Jorge Affonso (attr.), The Adoration of the Shepherds, 1515, oil on wood, Lissabon, Museu Nacional de Arte Antiga Instrument maker: Thilo Hirsch Year of manufacture: 2022 Location: Basel, property of the ensemble arcimboldo
Dimensions: Total length: 510 mm Max. Body width: 110 mm Body depth: approx. 93 mm
Vibrating string lengths: d'-string: 351 mm a-string: 350 mm e-string: 348 mm
Materials: Body: cherry Pegbox: cherry Fingerboard: cerry Bars: spruce Nut/String attachment button: bone Bridge: boxwood Top: goatskin
The main aim of this research was to measure the acoustic effects of the different sound holes. To do this, the instrument was first measured with the rosette and the two holes in the body open, then with the body holes closed.
Acoustical measurements: Alexander Mayer, mdw - University of Music and Performing Arts Vienna, Department of Music Acoustics – Wiener Klangstil (IWK), 25.9.2023
Force: Impact hammer exciting at the bass side of the bridge ACC: Acceleration measured on the same side, close to the impact point. Average is the average of all measurements (to be used in the analysis).
Photos of the setup: Thilo Hirsch
Folder modell_affonso Files: affonso_1 to 6 (Description: holes open)
Folder modell_affonso_loecher_zu Files: affonso_hc_1 to 6 (Description: both holes closed)
________________________
How to read VIA-Files: Line 1 to 9: Header, Line 8 holds the number of values
Data is organized as followed: 1st col: Frequency [Hz], 2nd col: Magnitude [as Factor not dB!], 3rd col: Phase [rad], 4th col:  Real part [as Factor not dB!], 5th col: Imaginary part [as Factor not dB!]. So only first 3 columns are needed!
To get dB Value: Amplitude[dB] = 20 log [Magnitude]
 Usually the Magnitude was calculated as response/reference (input) in the frequency domain. As for measuring the mechanical admittance the sensor is most likely an accelerometer (capturing the response in m/s2 of the object of interest) and the reference an impact hammer capturing the input force in Newton. As the mechanical admittance is defined as v/F (speed over force) the acceleration signal has to be integrated. The here captured signals are integrated in the frequency domain, what means the magnitude is divided by the corresponding frequency value in s-1. Values coded like: 3.30750000000000E+1 -> 3.3075 * 10 -> 33.075
DOI: 10.5281/zenodo.10116330
title: Acoustical measurements of a rabab reconstructed after a pictorial source from the 16th century

description: Acoustical measurements of a rabab reconstructed after a pictorial source from the 16th century
Instrument: rabab Pictorial source: Jorge Affonso (attr.), The Adoration of the Shepherds, 1515, oil on wood, Lissabon, Museu Nacional de Arte Antiga Instrument maker: Thilo Hirsch Year of manufacture: 2022 Location: Basel, property of the ensemble arcimboldo
Dimensions: Total length: 510 mm Max. Body width: 110 mm Body depth: approx. 93 mm
Vibrating string lengths: d'-string: 351 mm a-string: 350 mm e-string: 348 mm
Materials: Body: cherry Pegbox: cherry Fingerboard: cerry Bars: spruce Nut/String attachment button: bone Bridge: boxwood Top: goatskin
The main aim of this research was to measure the acoustic effects of the different sound holes. To do this, the instrument was first measured with the rosette and the two holes in the body open, then with the body holes closed.
Acoustical measurements: Alexander Mayer, mdw - University of Music and Performing Arts Vienna, Department of Music Acoustics – Wiener Klangstil (IWK), 25.9.2023
Force: Impact hammer exciting at the bass side of the bridge ACC: Acceleration measured on the same side, close to the impact point. Average is the average of all measurements (to be used in the analysis).
Photos of the setup: Thilo Hirsch
Folder modell_affonso Files: affonso_1 to 6 (Description: holes open)
Folder modell_affonso_loecher_zu Files: affonso_hc_1 to 6 (Description: both holes closed)
________________________
How to read VIA-Files: Line 1 to 9: Header, Line 8 holds the number of values
Data is organized as followed: 1st col: Frequency [Hz], 2nd col: Magnitude [as Factor not dB!], 3rd col: Phase [rad], 4th col:  Real part [as Factor not dB!], 5th col: Imaginary part [as Factor not dB!]. So only first 3 columns are needed!
To get dB Value: Amplitude[dB] = 20 log [Magnitude]
 Usually the Magnitude was calculated as response/reference (input) in the frequency domain. As for measuring the mechanical admittance the sensor is most likely an accelerometer (capturing the response in m/s2 of the object of interest) and the reference an impact hammer capturing the input force in Newton. As the mechanical admittance is defined as v/F (speed over force) the acceleration signal has to be integrated. The here captured signals are integrated in the frequency domain, what means the magnitude is divided by the corresponding frequency value in s-1. Values coded like: 3.30750000000000E+1 -> 3.3075 * 10 -> 33.075
DOI: 10.13120/e2ec3083-8330-4c40-8491-be8171c0cf9d
title: Contaminants: Antifoulants - Triphenyltin (measurements counts), v2023
title: Contaminants: Antifoulants - Triphenyltin (measurements counts), v2023

description: This product displays for Triphenyltin, positions with values counts that have been measured per matrix and are present in EMODnet validated datasets. The product displays positions for all available years and per year.
DOI: 10.13120/7d2d7fdb-614c-4640-9a8d-09794b20d7ec
title: Contaminants: Heavy metals - Mercury (measurements counts), v2023
title: Contaminants: Heavy metals - Mercury (measurements counts), v2023

description: This product displays for Mercury, positions with values counts that have been measured per matrix and are present in EMODnet validated datasets. The product displays positions for all available years and per year.
DOI: 10.13120/55642314-ca6c-4852-81a4-898a298c441b
title: Contaminants: Heavy metals - Cadmium (measurements counts), v2023
title: Contaminants: Heavy metals - Cadmium (measurements counts), v2023

description: This product displays for Cadmium, positions with values counts that have been measured per matrix and are present in EMODnet validated datasets. The product displays positions for all available years and per year.
DOI: 10.13120/bb4423f2-2dcd-4db7-b86e-63fb0d1cf6ac
title: Contaminants: Heavy metals - Lead (measurements counts), v2023
title: Contaminants: Heavy metals - Lead (measurements counts), v2023

description: This product displays for Lead, positions with values counts that have been measured per matrix and are present in EMODnet validated datasets. The product displays positions for all available years and per year.
DOI: 10.13120/022e6979-c3d4-41cd-8973-b82a6aff595d
title: Contaminants: Heavy metals - Nickel (measurements counts), v2023
title: Contaminants: Heavy metals - Nickel (measurements counts), v2023

description: This product displays for Nickel, positions with values counts that have been measured per matrix and are present in EMODnet validated datasets. The product displays positions for all available years and per year.
DOI: 10.13120/7677d8e3-73ae-44d0-a205-02f1798cccb3
title: Contaminants: Hydrocarbons (PAH) - Anthracene (measurements counts), v2023
title: Contaminants: Hydrocarbons (PAH) - Anthracene (measurements counts), v2023

description: This product displays for Anthracene, positions with values counts that have been measured per matrix and are present in EMODnet validated datasets. The product displays positions for all available years and per year.
DOI: 10.13120/b45c612d-0f70-43ff-81d0-7dac85e9d871
title: Contaminants: Hydrocarbons (PAH) - Fluoranthene (measurements counts), v2023
title: Contaminants: Hydrocarbons (PAH) - Fluoranthene (measurements counts), v2023

description: This product displays for Fluoranthene, positions with values counts that have been measured per matrix and are present in EMODnet validated datasets. The product displays positions for all available years and per year.
DOI: 10.5281/zenodo.10067450
title: Rigid and hinged very large floating structure (VLFS) dataset - Kelvin Hydrodynamics Laboratory

description: This dataset corresponds to the measurements performed at the Kelvin Hydrodynamics Laboratory at the University of Strathclyde, in August 2022, to assess the motion performance and internal loading of a rigid and hinged very large floating structure (VLFS) under regular waves. The VLFS was constructed with three pontoons and two hinges. The hinges were replaced with aluminium steel bars to built the rigid VLFS. The dimensions of each pontoon of the VLFS were 580 mm x 580 mm x 52 mm. Each pontoon was built with 2 mm layer of carbon fibre and a 50 mm layer of PVC foam.
The VLFS was tested in regular waves at two incidences: 0 degrees and 30 degrees. For 0 degree incidence, the wave frequencies tested ranged from 0.4 to1.6 Hz in intervals of 0.1 Hz. Four wave heights were tested, h=5, 10, 20 and 40 mm. For 30 degree incidence, the same range of frequencies were tested, but only one wave height, h=5 mm. Preliminary results for some of the data at 0 degrees incidence can be found in the conference paper: https://doi.org/10.36688/ewtec-2023-389.  Further analysis of this dataset and additional results are in preparation for a journal manuscript.
The following files are included as part of the dataset:

Motion files (Matlab files).
Strain gauge and wave height files (Matlab files).
Data description file - Description of files.
Test matrix - Test cases summarised with nomenclature used in files.
Matlab script to sort out position of motion spheres as depicted in Figure 1.
Video of the hinged VLFS subject to a train of regular waves at f=0.8 Hz, i.e. when the wavelength is of similar length to the length of the platform, i.e. f=0.8 Hz.

The motion files contain the time series information recorded for each of the motion detection spheres. Because the motion raw data is not labelled sequentially, it is necessary to run the Matlab file included in the data repository to sort out the information of the spheres.
The strain gauge files contain the raw strain gauge data (8 channels) and the wave gauge data with the file number describing the corresponding test in the test matrix.
The VLFS was equipped with 36 motion detection spheres and 8 strain gauges. The diagram and notation of each sphere is depicted in Figure 1. Figure 1 is available in the Data description document.