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Hydrodynamic Turbulence: Sweeping Effect and Taylor’s Hypothesis via Correlation Function
We demonstrate the sweeping effect in turbulence using numerical simulations of hydrodynamic turbulence without a mean velocity. The velocity correlation function, C ( k , τ ) , decays with time due to the eddy viscosity. In addition, C ( k , τ ) shows oscillations due to the sweeping effect by “ran...
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Published in: | Transactions of the Indian National Academy of Engineering (Online) 2020-12, Vol.5 (4), p.649-662 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We demonstrate the sweeping effect in turbulence using numerical simulations of hydrodynamic turbulence without a mean velocity. The velocity correlation function,
C
(
k
,
τ
)
, decays with time due to the eddy viscosity. In addition,
C
(
k
,
τ
)
shows oscillations due to the sweeping effect by “random mean velocity field”
U
~
0
. We also perform numerical simulation with mean velocity
U
0
=
10
z
^
(10 times the rms speed) for which
C
(
k
,
τ
)
exhibits damped oscillations with the frequency of
|
U
0
|
k
and decay time scale corresponding to the
U
0
=
0
case. For
U
0
=
10
z
^
, the phase of
C
(
k
,
τ
)
shows the sweeping effect, but it is overshadowed by oscillations caused by
U
0
. We also demonstrate that for
U
0
=
0
and
10
z
^
, the frequency spectra of the velocity fields measured by real-space probes are respectively
f
-
2
and
f
-
5
/
3
; these spectra are related to the Lagrangian and Eulerian space-time correlations respectively. |
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ISSN: | 2662-5423 2662-5423 |
DOI: | 10.1007/s41403-020-00161-3 |