Reynolds stresses from hydrodynamic turbulence with shear and rotation

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Volume 505 / No 3 (October III 2009)

A&A, 505 3 (2009) 955-968

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Table B.1:

Summary of the runs with shear flow only. Here $\tilde{Q}_{ij}=Q_{ij}/u_{\rm rms}^2$ , and brackets around a quantity signify that the number is not statistically significant.
Run	Grid	Re	${\rm Co}$	${\rm Sh}$	$u_{\rm rms}$	$\tilde{Q}_{xx}$	$\tilde{Q}_{yy}$	$\tilde{Q}_{zz}$	$\tilde{Q}_{xy}$	$\tilde{Q}_{xz}$	$\tilde{Q}_{yz}$
A1	64³	5	0	-0.18	0.054	0.295	0.404	0.302	0.075	(-0.000)	(-0.001)
A2	128³	14	0	-0.14	0.069	0.304	0.378	0.319	0.084	(-0.001)	(0.002)
A3	256³	31	0	-0.12	0.079	0.313	0.368	0.320	0.083	(-0.002)	(-0.001)
A4	256³	80	0	-0.12	0.083	0.331	0.342	0.328	0.069	(-0.001)	(-0.001)
A5	512³	164	0	-0.12	0.084	0.318	0.349	0.333	0.058	(-0.003)	(-0.003)
A6	1024³	345	0	-0.11	0.088	0.320	0.343	0.337	0.054	(-0.001)	(-0.003)
B1	64³	8	0	-0.25	0.080	0.198	0.599	0.238	0.146	(0.002)	(0.001)
B2	128³	22	0	-0.18	0.112	0.235	0.491	0.288	0.140	(-0.001)	(-0.000)
B3	256³	44	0	-0.18	0.112	0.262	0.440	0.303	0.124	(-0.002)	(0.000)
B4	512³	99	0	-0.19	0.101	0.282	0.425	0.318	0.110	(0.001)	(0.001)
B5	1024³	196	0	-0.20	0.100	0.300	0.377	0.323	0.101	(-0.003)	(-0.001)
B6	1024³	387	0	-0.20	0.099	0.299	0.375	0.326	0.095	(-0.004)	(-0.005)
C1	128³	27	0	-0.01	0.069	0.335	0.334	0.332	0.010	(-0.003)	(-0.002)
C2	128³	27	0	-0.03	0.069	0.334	0.332	0.335	0.014	(-0.001)	(0.001)
C3	128³	28	0	-0.06	0.070	0.335	0.332	0.333	0.031	(-0.002)	(0.000)
C4	128³	31	0	-0.13	0.078	0.317	0.362	0.321	0.084	(-0.001)	(-0.000)
C5	128³	39	0	-0.20	0.099	0.282	0.392	0.330	0.125	(0.002)	(-0.002)
C6	128³	48	0	-0.24	0.122	0.259	0.396	0.347	0.137	(0.000)	(0.010)
D1	256³	75	0	-0.01	0.076	0.331	0.334	0.335	0.009	(0.002)	(0.002)
D2	256³	75	0	-0.03	0.076	0.335	0.329	0.336	0.015	(0.001)	(0.000)
D3	256³	76	0	-0.05	0.077	0.329	0.334	0.337	0.029	(-0.001)	(-0.000)
D4	256³	81	0	-0.12	0.083	0.331	0.342	0.328	0.069	(0.001)	(-0.000)
D5	256³	99	0	-0.19	0.101	0.297	0.373	0.331	0.108	(-0.000)	(0.001)
D5	256³	123	0	-0.23	0.126	0.267	0.417	0.317	0.129	(0.002)	(0.010)

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