Computational Hydraulics Turbulence, Lecture Notes- Physics - , Study notes for Physics. The University of Manchester


Description: Turbulence, momentum transfer, turbulence notation, effect of turbulence on mean flow, generation and transport shear flows
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CFD 7 – 1 David Apsley
7.1 What is turbulence?
7.2 Momentum transfer in laminar and turbulent flow
7.3 Turbulence notation
7.4 Effect of turbulence on the mean flow
7.5 Turbulence generation and transport
7.6 Important shear flows
7.1 What is Turbulence?
Instantaneous Mean
A “random”, 3-d, time-dependent eddying motion with many scales, superposed on an
often drastically simpler mean flow.
A solution of the Navier-Stokes equations.
The natural state at high Reynolds numbers.
An efficient transporter and mixer ... of momentum, energy, constituents.
A major source of energy loss.
A significant influence on drag and boundary-layer separation.
“The last great unsolved problem of classical physics.” (variously attributed to
Sommerfeld, Einstein and Feynman)
CFD 7 – 2 David Apsley
7.2 Momentum Transfer in Laminar and Turbulent Flow
In laminar flow adjacent layers of fluid slide past each other
without mixing. Transfer of momentum occurs between
layers moving at different speeds because of viscous stresses.
In turbulent flow adjacent layers continually mix. A net
transfer of momentum occurs because of the mixing of fluid
elements from layers with different mean velocity. This
mixing is a far more effective means of transferring
momentum than viscous stresses. Consequently, the mean-
velocity profile tends to be more uniform in turbulent flow.
7.3 Turbulence Notation
The instantaneous value of any flow variable can be decomposed into mean + fluctuation.
is decomposed into
mean + fluctuation
Mean and fluctuating parts are denoted by either:
an overbar and prime: uuu
upper case and lower case: uU
The first is useful in deriving theoretical results but becomes cumbersome in general use. The
notation being used is, hopefully, obvious from the context.
By definition, the average fluctuation is zero:
In experimental work and in steady flow the “mean” is usually a time mean, whilst in
theoretical work it is the probabilistic (or “ensemble”) mean. The process of taking the mean
of a turbulent quantity or a product of turbulent quantities is called Reynolds averaging.
The normal averaging rules for products apply:
222 uuu
+= (variance)
+= (covariance)
Thus, in turbulent flow the “mean of a product” is not equal to the “product of the means” but
includes an (often significant) contribution from the net effect of turbulent fluctuations.
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