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Xu, Duo; Song, Baofang; Avila, Marc (2022): Optimal growth as function of Wo (Re_o=8000,A=infty) [dataset]. PANGAEA, https://doi.org/10.1594/PANGAEA.949208

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Published: 2022-09-29DOI registered: 2023-01-13

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Abstract:
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_Wo_Reo8000.dat' shows the dependence of the maximum energy amplification on the Womersley number for the oscillatory Reynolds number of 8000.
This file includes twelve columns: the first column indicates the Womersley number; the second column indicates the pulsation period; the third column indicates the optimal axial wavenumber; the fourth column indicates the optimal azimuthal wavenumber; the fifth column indicates the initial time of the optimal perturbation; the sixth column indicates the final time of the optimal perturbation; the seventh column indicates the evolution time of the optimal perturbation; the eighth column indicates the initial time of the optimal perturbation normalized by the pulsation period; the nineth column indicates the final time of the optimal perturbation normalized by the pulsation period; the tenth column indicates the evolution time of the optimal perturbation normalized by the pulsation period; the eleventh column indicates the maximum energy amplification; the twelfth column indicates the Reynolds number which is defined with the characteristic length of the thickness of the Stokes layer.
Keyword(s):
nonlinear instability; transition to turbulence
Comment:
#t0:initial time; tf:end time;
VARIABLES = "Wo", "T", "k_z", "k_θ", "t0", "tf", "tf-t0", "t0/T", "tf/T", "(tf-t0)/T", "TG", "Re_delta"
ZONE T="data, all modes, opf", I=11, J=1
Parameter(s):
#NameShort NameUnitPrincipal InvestigatorMethod/DeviceComment
Womersley numberWoXu, Duo
Pulsation periodTXu, Duo
Axial wave numberk_zXu, Duo
Azimuthal wave numberk_θXu, Duo
Time of perturbationt0Xu, Duo
Time of perturbation energy maximumtfXu, Duo
Time of perturbation energy maximum - Time of perturbation (tf-t0)tauXu, Duo
Time of pertubartion by pulsation periodt0/TXu, Duo
Time of pertubartion energy maximum by pulsation periodtf/TXu, Duo
10 Time of perturbation energy maximum - Time of perturbation by pulsation period(tf-t0)/TXu, Duo
11 Transient energy growthTGXu, Duo
12 Reynolds number of the Stokes layerRe_δXu, Duo
Status:
Curation Level: Enhanced curation (CurationLevelC) * Processing Level: PANGAEA data processing level 2 (ProcLevel2)
Size:
132 data points

Data

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


Wo

T

k_z

k_θ

t0

tf

tau

t0/T

tf/T
10 
(tf-t0)/T
11 
TG
12 
Re_δ
5125.662.8156.5486677669.1146677712.5660.450.549997050.0999970517115217.656168101131.37084990
687.272.4130.5432619156.7232619126.1800.350.650000700.30000070462961617.79498280942.80904158
764.113.2122.4399475348.0859475325.6460.350.750005390.400005391581760400.85994050808.12203564
849.093.6117.1805848236.8155848219.6350.350.750000940.40000094997401920.88126840707.10678119
938.794.4113.5747830729.0887830715.5140.350.749999030.39999903226046597.77295940628.53936105
1031.425.0110.9955742923.5615742812.5660.350.749988200.3999882034520129.11188500565.68542495
1318.596.816.5062569713.942256977.4360.350.750014940.40001494259842.11195603435.14263458
1513.968.414.8869219110.471921905.5850.350.749996160.3999961625501.44539324377.12361663
207.8512.002.748893575.104893572.3560.350.649975240.29997524685.76714469282.84271247
303.4919.611.221730481.919730480.6980.350.549962270.1999622726.07568495188.56180832
401.9626.510.687223391.080223390.3930.350.550153260.200153265.47733821141.42135624