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2011-08-11T04:40:44Z

Mathematical formulations: mostly units

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The '''Womersley number''' ('''α''') is a [[dimensionless number]] in [[biofluid mechanics]]. It is a dimensionless expression of the [[pulsatile flow]] [[frequency]] in relation to [[viscosity|viscous effects]]. It is named after [[John R. Womersley]] (1907–1958) for his work with bloodflow in [[arteries]].<ref>{{Cite journal
|author=Womersley, J.R.
|title=Method for the calculation of velocity, rate of flow and viscous drag in arteries when the pressure gradient is known
|journal=J Physiol.
|volume=127
|issue=3
|pages=553–563
|date=March 1955
|pmid=14368548
|pmc=1365740
|url=http://jp.physoc.org/cgi/reprint/127/3/553.pdf}}</ref> The Womersley number is important in keeping [[dynamic similarity]] when scaling an experiment. An example of this is scaling up the vascular system for experimental study. The Womersley number is also important in determining the thickness of the [[boundary layer]] to see if entrance effects can be ignored.

== Derivation ==

The Womersley number, usually denoted <math>\alpha</math>, is defined by the relation

<math>\alpha^2 = \frac{\text{transient inertial force}}{\text{viscous force}} = \frac{ \rho \omega U}{\mu U R^{-2} } = \frac{ \omega R^{2} }{\mu \rho^{-1} } = \frac{ \omega R^{2} }{\nu} \, ,</math>

where ''R'' is an appropriate [[length scale]] (for example the radius of a pipe), ''ω'' is the [[angular frequency]] of the oscillations, and ''ν'', ''ρ'', ''μ'' are the [[kinematic viscosity]], density, and [[dynamic viscosity]] of the fluid, respectively.<ref>{{cite book
|author=Fung, Y. C.
|title=Biomechanics - Motion, flow, stress and growth
|year=1990
|pages=569
|publisher=Springer-Verlag
|place=New York (USA)
|url=http://books.google.ie/books?id=33qbOEKAWIwC&printsec=frontcover&dq=Biomechanics+-+Motion,+flow,+stress+and+growth&hl=en&sa=X&ei=bpKiT7jKGMi0hAevo4n-CA&ved=0CDkQ6AEwAA#v=onepage&q=Biomechanics%20-%20Motion%2C%20flow%2C%20stress%20and%20growth&f=false}}</ref> The Womersley number is normally written in the powerless form

<math>\alpha = R \left( \frac{\omega}{\nu} \right)^\frac{1}{2} \ = R \left( \frac{\omega \rho}{\mu} \right)^\frac{1}{2} \, .</math>

It can also be written in terms of the dimensionless [[Reynolds number]] (Re) and [[Strouhal number]] (Sr):

<math>\alpha = \left( 2\pi\, \mathrm{Re} \, \mathrm{Sr} \right)^{1/2}\, .</math>

The Womersley number arises in the solution of the linearized [[Navier Stokes equations]] for oscillatory flow (presumed to be laminar and incompressible) in a tube. It expresses the ratio of the transient or oscillatory inertia force to the shear force. When <math>\alpha</math> is small (1 or less), it means the frequency of pulsations is sufficiently low that a parabolic velocity profile has time to develop during each cycle, and the flow will be very nearly in phase with the pressure gradient, and will be given to a good approximation by [[Poiseuille's law]], using the instantaneous pressure gradient. When <math>\alpha</math> is large (10 or more), it means the frequency of pulsations is sufficiently large that the velocity profile is relatively flat or plug-like, and the mean flow lags the pressure gradient by about 90 degrees. Along with the Reynolds number, the Womersley number governs dynamic similarity.<ref>{{Cite book
|author=Nichols, W.W., O'Rourke, M.F.
|title=McDonald's Blood Flow in Arteries
|publisher=Hodder-Arnold
|location=London (England)
|year=2005
|isbn=0-340-80941-8
|edition=5th}}</ref>

The boundary layer thickness <math>\delta</math> that is associated with the transient acceleration is related to the Womersley number. It is equal to inverse of the Womersley number. The Womersley number is also equal to the square root of the [[Stokes number]].<ref name="BiomechanicsCirculation">{{cite book
|author=Fung, Y.C.
|title=Biomechanics Circulation
|year=1996
|publisher=Springer Verlag
|pages=571
|url=http://books.google.ie/books?id=TlbXtdbT6D8C&dq=Biomechanics%20-%20Motion%2C%20flow%2C%20stress%20and%20growth&source=gbs_similarbooks}}</ref>

<math>\delta = \left( L/\alpha \right)= \left( \frac{L}{\sqrt{\mathrm{Stk}}}\right), </math>

where ''L'' is a characteristic length.

== Biofluid mechanics ==

In a flow distribution network that progresses from a large tube to many small tubes (e.g. a blood vessel network), the frequency, density, and dynamic viscosity are (usually) the same throughout the network, but the tube radii change. Therefore the Womersley number is large in large vessels and small in small vessels. As the vessel diameter decreases with each division the Womersley number soon becomes quite small. The Womersley numbers tend to 1 at the level of the terminal arteries. In the arterioles, capillaries, and venules the Womersley numbers are less than one. In these regions the inertia force becomes less important and the flow is determined by the balance of viscous stresses and the pressure gradient. This is called [[microcirculation]].<ref name="BiomechanicsCirculation" />

Some typical values for the Womersley number in the cardiovascular system for a canine at a heart rate of 2 Hz are:<ref name="BiomechanicsCirculation" />
*Ascending Aorta — 13.2
*Descending Aorta — 11.5
*Abdominal Aorta — 8
*Femoral Artery — 3.5
*Carotid Artery — 4.4
*Arterioles —0.04
*Capillaries — 0.005
*Venules — 0.035
*Inferior Vena Cava — 8.8
*Main Pulmonary Artery — 15

It has been argued that universal biological scaling laws (power-law relationships that describe variation of quantities such as metabolic rate, lifespan, length, etc., with body mass) are a consequence of the need for energy minimization, the [[fractal]] nature of vascular networks, and the crossover from high to low Womersley number flow as one progresses from large to small vessels.<ref>{{Cite journal
|doi=10.1126/science.276.5309.122
|author=West GB, Brown JH, Enquist BJ
|title=A general model for the origin of allometric scaling laws in biology
|journal=Science
|volume=276
|issue=5309
|pages=122–6
|date=4 April 1997
|pmid=9082983
|url=http://www.sciencemag.org/cgi/pmidlookup?view=long&pmid=9082983}}</ref>

==References==
{{reflist}}

{{NonDimFluMech}}

{{Use dmy dates|date=September 2010}}

{{DEFAULTSORT:Womersley Number}}
[[Category:Biomechanics]]
[[Category:Dimensionless numbers of fluid mechanics]]
[[Category:Fluid dynamics]]

Single Vegetative Obstruction Model - Revision history

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