transition to turbulence in pipe flow

21
Transition to Turbulence in Pipe Flow T Mullin Manchester Centre for Nonlinear Dynamics with J. Peixinho Support from EPSRC Warwick Dec.'05 O. Reynolds 1883

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with J. Peixinho
O. Reynolds 1883

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Our investigations are concerned with the stability of fully devloped Poiseuille flow.
Introduction • Pipe flow is linearly stable • Finite amplitude perturbation problem • Laminar flow observed at Re =106
Pfenniger(1961) (Re =Ud/ν)
Experimental Setup
• Constant mass flux: Re can be varied in a controlled way
• Accurate in Re better than 1% • Very long pipe: D = 20 mm and 800 D long • Laminar flow can be achieved at Re ~ 23 000
Picture of the Long Pipe
Laminar Profiles Measured In Pipe Using LDV
200
250
300
350
400
.450
500
’R=2170’ ’R=4000’
Perturbation Length (Pipe Diameters)
.
Each point was obtained from 40 runs of experiment
Stability in Long Pipe
Observed that global stability as Re --> 0
Two investigations:
1
10-1
10-2
1600 1620 1640
P
Pipe diameters from Injection Point Pipe diameters from Injection Point
Probability of observing puff.
Decay of Injected Perturbations Below Threshold: Exponential Decay Observed -> Critical Behaviour (40 to 100 runs for each Re)
0
500
1000
1500
2000
2500
Re
tau
Re
Laminar
'Turbulent'
Laminar
'Turbulent'
Push-pull slope -1.4 Azimuthal slope -1.0
Fully turbulent-> Laminar Local reduction in Re by expanding pipe (Laufer 1962, Sibulkin, 1962)
at low Re threshold.
Fewer runs required to obtain good statistics than injection case.
Exponential decay in probability of observing puff downstream ----> Poisson process.
Divergence of timescales ---------> deterministic behaviour.
Qualitatively similar to boundary crisis of attractor Grebogi, Ott & Yorke (1986)
But low-d systems: exponents < 1
Wavy Patterns Puff at Re = 1900
After reduction of Re down to 1750
Re = 1750
Faisst&Eckhardt(2003) Wedin &Kerswell(2004)
C onc lusions
A c lear sc a ling law for t he t ra nsit ion t o
t urbulenc e ha s been est a blished.
S im plest im plic a t ion given by a ba la nc e
of t he inert ia l a nd visc ous t erm s in t he N a vier
S t okes equa t ion.
S lowing down indic a t es c rit ic a l beha viour;
presenc e of wa ves suggest exc it ing prospec t s
lie a hea d.
Phys. Today (2004) Feb.