Please use this identifier to cite or link to this item: https://doi.org/10.48441/4427.266
License: 
Publisher DOI: 10.5281/zenodo.1257872
Title: Transverse and torsional vibration on bowed cello G steel string
Language: English
Authors: Mores, Robert  
Keywords: bowed strings; transverse vibration; torsional vibration
Issue Date: 2-Jun-2018
Is supplement to: https://doi.org/10.1371/journal.pone.0211217
Abstract: 
Transverse and torsional vibrations from a cello G string made of steel, product name "Pirastro Chromcor medium".

Transverse signal taken electrodynamically below bow contact point,while string is mounted on a monochord and tuned to 98 Hz.

Torsional signal taken electrodynamically at either 10 mm from the bow contact point towards the bridge side, or close string termination (all file names containing *_torsion zum steg_*.mat) or at 10 mm from the bow contact point towards the nut side, or more distant string termination (all file names containing *_torsion zum sattel_*.mat). The number in the filename indicates the distance of the bow contact point from the bridge in cm, while the string has a free length of 68 cm, e.g. the file *_11_*.mat contains data for bowstrokes at 11 cm distance from the bridge. Upstrokes/downstrokes are indicated by *_u.mat and *_d.mat in the file name. Dates of recording indicated in the file name by session_yyyymmdd_*.mat.

Manual bowing by experienced player, while each individual stroke covers a wide range for bow velocity and bow pressure, however, always exciting regular Helmholtz motion on the string. Only the file session_*_doppelzahn represents data for a non-Helmholtz case. Statistical analyses cover the wide dynamic range, and structural analyses use smaller windows of comparable levels, the position of which are indicated in the files startpunkte_*.m.

File formats are MATLAB files. For all *.mat files: column 1 of table Y is the transverse time signal (0.1 per mm), column 2 the torsional time signal (0.004 per 1°). Sampling frequency is 48 kHz.

Raw data for the Mores R (2019) Further empirical data for torsion on bowed strings. PLOS ONE 14(2): e0211217. https://doi.org/10.1371/journal.pone.0211217
URI: http://hdl.handle.net/20.500.12738/12255
DOI: 10.48441/4427.266
Review status: Unknown / not specified
Institute: Department Medientechnik 
Fakultät Design, Medien und Information 
Type: Dataset
Appears in Collections:Research Data (with datasets)

Files in This Item:
File Description SizeFormat
session_20171120_torsion_zum_steg_10_d.mat1.65 MBUnknownView/Open
session_20171120_torsion_zum_steg_10_u.mat1.5 MBUnknownView/Open
session_20171120_torsion_zum_steg_11_d.mat1.59 MBUnknownView/Open
session_20171120_torsion_zum_steg_11_u.mat1.63 MBUnknownView/Open
session_20171120_torsion_zum_steg_12_d.mat1.62 MBUnknownView/Open
session_20171120_torsion_zum_steg_12_u.mat1.87 MBUnknownView/Open
session_20171120_torsion_zum_steg_13_d.mat1.53 MBUnknownView/Open
session_20171120_torsion_zum_steg_13_u.mat1.69 MBUnknownView/Open
session_20171120_torsion_zum_steg_14_d.mat1.88 MBUnknownView/Open
session_20171120_torsion_zum_steg_14_u.mat1.44 MBUnknownView/Open
session_20171120_torsion_zum_steg_15_d.mat1.64 MBUnknownView/Open
session_20171120_torsion_zum_steg_15_u.mat1.43 MBUnknownView/Open
session_20171120_torsion_zum_steg_16_d.mat1.36 MBUnknownView/Open
session_20171120_torsion_zum_steg_16_u.mat1.23 MBUnknownView/Open
session_20171120_torsion_zum_steg_4_u.mat1.92 MBUnknownView/Open
session_20171120_torsion_zum_steg_4_d.mat2.15 MBUnknownView/Open
session_20171120_torsion_zum_steg_5_d.mat1.5 MBUnknownView/Open
session_20171120_torsion_zum_steg_5_u.mat1.66 MBUnknownView/Open
session_20171120_torsion_zum_steg_6_d.mat1.75 MBUnknownView/Open
session_20171120_torsion_zum_steg_6_u.mat1.57 MBUnknownView/Open
session_20171120_torsion_zum_steg_7_d.mat1.87 MBUnknownView/Open
session_20171120_torsion_zum_steg_7_u.mat1.74 MBUnknownView/Open
session_20171120_torsion_zum_steg_8_d.mat1.94 MBUnknownView/Open
session_20171120_torsion_zum_steg_8_u.mat1.97 MBUnknownView/Open
session_20171120_torsion_zum_steg_9_d.mat1.55 MBUnknownView/Open
session_20171120_torsion_zum_steg_9_u.mat1.62 MBUnknownView/Open
session_20171121_torsion_zum_sattel_10_d.mat1.28 MBUnknownView/Open
session_20171121_torsion_zum_sattel_10_d_doppelzahn.mat1.35 MBUnknownView/Open
session_20171121_torsion_zum_sattel_10_u.mat1.6 MBUnknownView/Open
session_20171121_torsion_zum_sattel_11_d.mat1.59 MBUnknownView/Open
session_20171121_torsion_zum_sattel_11_u.mat1.45 MBUnknownView/Open
session_20171121_torsion_zum_sattel_12_d.mat1.47 MBUnknownView/Open
session_20171121_torsion_zum_sattel_12_u.mat1.58 MBUnknownView/Open
session_20171121_torsion_zum_sattel_13_d.mat1.44 MBUnknownView/Open
session_20171121_torsion_zum_sattel_13_u.mat1.46 MBUnknownView/Open
session_20171121_torsion_zum_sattel_14_d.mat1.84 MBUnknownView/Open
session_20171121_torsion_zum_sattel_14_u.mat1.32 MBUnknownView/Open
session_20171121_torsion_zum_sattel_15_d.mat1.86 MBUnknownView/Open
session_20171121_torsion_zum_sattel_15_u.mat1.44 MBUnknownView/Open
session_20171121_torsion_zum_sattel_16_d.mat1.68 MBUnknownView/Open
session_20171121_torsion_zum_sattel_16_u.mat1.36 MBUnknownView/Open
session_20171121_torsion_zum_sattel_4_d.mat1.54 MBUnknownView/Open
session_20171121_torsion_zum_sattel_4_u.mat1.54 MBUnknownView/Open
session_20171121_torsion_zum_sattel_5_d.mat1.56 MBUnknownView/Open
session_20171121_torsion_zum_sattel_5_u.mat1.67 MBUnknownView/Open
session_20171121_torsion_zum_sattel_6_d.mat1.5 MBUnknownView/Open
session_20171121_torsion_zum_sattel_6_u.mat1.69 MBUnknownView/Open
session_20171121_torsion_zum_sattel_7_d.mat1.66 MBUnknownView/Open
session_20171121_torsion_zum_sattel_7_u.mat1.42 MBUnknownView/Open
session_20171121_torsion_zum_sattel_8_d.mat1.56 MBUnknownView/Open
session_20171121_torsion_zum_sattel_8_u.mat1.29 MBUnknownView/Open
session_20171121_torsion_zum_sattel_9_d.mat1.42 MBUnknownView/Open
session_20171121_torsion_zum_sattel_9_u.mat1.65 MBUnknownView/Open
startpunkte_20171121.m739 BUnknownView/Open
startpunkte_20171120.m563 BUnknownView/Open
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