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Feldmann, Daniel; Avila, Marc (2019): Time series of consecutive runs from pipe0028 (vel_friction0001) [dataset]. PANGAEA, https://doi.org/10.1594/PANGAEA.924965, In: Feldmann, D; Avila, M (2019): Overdamped large-eddy simulations of turbulent pipe flow up to Reτ = 1500 [dataset bundled publication]. PANGAEA, https://doi.org/10.1594/PANGAEA.903887

Always quote citation above when using data! You can download the citation in several formats below.

RIS CitationBibTeX Citation

Keyword(s):
Large eddy simulation; Pipe flow; turbulence; Very large scale motion
Related to:
Feldmann, Daniel; Avila, Marc (2018): Overdamped large-eddy simulations of turbulent pipe flow up to Reτ = 1500. Journal of Physics: Conference Series, 1001, 012016, https://doi.org/10.1088/1742-6596/1001/1/012016
Source:
Feldmann, Daniel; Avila, Marc (2019): Raw simulation data, source code and results from all pipe flows [dataset]. (12.1 GiB), raw_simulation_data_of_turbulent_pipe_flow.tar.gz
Event(s):
LES (Large_eddy_simulation) * Method/Device: Computational simulation (SIMUL)
Parameter(s):
#NameShort NameUnitPrincipal InvestigatorMethod/DeviceComment
Dimensionless timetFeldmann, DanielLarge-eddy simulations (LES)
Pressure correction to control constant volume, fluxPress correction control constant vol flFeldmann, DanielLarge-eddy simulations (LES)
Axial velocity component at the pipe center line (r=0)Axial veloc compo pipe center line (r=0)Feldmann, DanielLarge-eddy simulations (LES)
Mean friction velocity at the pipe wallMean friction veloc pipe wallFeldmann, DanielLarge-eddy simulations (LES)
Size:
56004 data points

Data

Download dataset as tab-delimited text — use the following character encoding:


t

Press correction control constant vol fl

Axial veloc compo pipe center line (r=0)

Mean friction veloc pipe wall
0.00E02.02E16.21E-12.67E-2
5.00E-22.05E16.21E-12.69E-2
1.00E-12.08E16.21E-12.70E-2
1.50E-12.09E16.21E-12.71E-2
2.00E-12.11E16.21E-12.72E-2
2.50E-12.11E16.21E-12.73E-2
3.00E-12.12E16.21E-12.73E-2
3.50E-12.13E16.21E-12.73E-2
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7.00E-12.12E16.21E-12.73E-2
7.50E-12.12E16.21E-12.73E-2
8.00E-12.12E16.21E-12.73E-2
8.50E-12.11E16.21E-12.73E-2
9.00E-12.11E16.21E-12.72E-2
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1.00E02.10E16.22E-12.72E-2
1.05E02.10E16.22E-12.71E-2
1.10E02.09E16.22E-12.71E-2
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9.59E11.80E16.14E-12.52E-2
9.59E11.80E16.14E-12.52E-2
9.60E11.80E16.14E-12.52E-2
9.60E11.80E16.14E-12.52E-2
9.61E11.80E16.14E-12.52E-2
9.61E11.80E16.15E-12.52E-2
9.62E11.80E16.15E-12.52E-2
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9.97E11.80E16.16E-12.53E-2
9.97E11.80E16.16E-12.53E-2
9.98E11.80E16.16E-12.53E-2
9.98E11.80E16.16E-12.53E-2
9.99E11.80E16.16E-12.53E-2
9.99E11.80E16.16E-12.53E-2
1.00E21.80E16.16E-12.53E-2

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