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| In [[dimensional analysis]], the '''Strouhal number''' ('''St''') is a [[dimensionless number]] describing oscillating flow mechanisms. The parameter is named after [[Vincenc Strouhal]], a Czech physicist who experimented in 1878 with wires experiencing [[vortex shedding]] and singing in the wind.<ref>{{cite book |last=White |first=Frank M. |title=Fluid Mechanics |edition=4th |year=1999 |location= |publisher=McGraw Hill |isbn=0-07-116848-6 }}</ref> The Strouhal number is an integral part of the fundamentals of [[fluid mechanics]].
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| The Strouhal number is often given as
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| :<math> \mathrm{St}= {f L\over V}, </math>
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| where ''f'' is the frequency of [[vortex shedding]], ''L'' is the characteristic length (for example [[hydraulic diameter]], or [[chord]] length) and ''V'' is the velocity of the fluid. In certain cases like heaving (plunging) flight, this characteristic length is the amplitude of oscillation. This selection of characteristic length can be used to present a distinction between Strouhal number and Reduced Frequency.
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| :<math> \mathrm{St}= {k a\over \pi c}, </math>
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| where ''k'' is the [[reduced frequency]] and ''a'' is amplitude of the heaving oscillation.
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| [[Image:Srrrpd.png|thumb|right|300px|Strouhal number as a function of the Reynolds number for a long cylinder]]
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| For large Strouhal numbers (order of 1), viscosity dominates fluid flow, resulting in a collective oscillating movement of the fluid "plug". For low Strouhal numbers (order of 10<sup>−4</sup> and below), the high-speed, quasi steady state portion of the movement dominates the oscillation. Oscillation at intermediate Strouhal numbers is characterized by the buildup and rapidly subsequent shedding of vortices.<ref>{{cite journal |first=Ian J. |last=Sobey |year=1982 |title=Oscillatory flows at intermediate Strouhal number in asymmetry channels |journal=[[Journal of Fluid Mechanics]] |volume=125 |issue= |pages=359–373 |doi=10.1017/S0022112082003371 |bibcode = 1982JFM...125..359S }}</ref>
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| For spheres in uniform flow in the [[Reynolds number]] range of 800 < Re < 200,000 there co-exist two values of the Strouhal number. The lower frequency is attributed to the large-scale instability of the wake and is independent of the [[Reynolds number]] Re and is approximately equal to 0.2. The higher frequency Strouhal number is caused by small-scale instabilities from the separation of the shear layer.<ref name="Kim and Durbin, 1988">{{cite journal |last=Kim |first=K. J. |last2=Durbin |first2=P. A. |year=1988 |title=Observations of the frequencies in a sphere wake and drag increase by acoustic excitation |journal=[[Physics of Fluids]] |volume=31 |issue=11 |pages=3260–3265 |doi=10.1063/1.866937 |bibcode = 1988PhFl...31.3260K }}</ref><ref name="Sakamoto and Haniu, 1990">{{cite journal |last=Sakamoto |first=H. |last2=Haniu |first2=H. |year=1990 |title=A study on vortex shedding from spheres in uniform flow |journal=Journal of Fluids Engineering |volume=112 |issue=December |pages=386–392 |doi= |bibcode=1990ATJFE.112..386S }}</ref>
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| == Applications ==
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| In [[metrology]], specifically axial-flow turbine meters, the '''Strouhal number''' is used in combination with the [[Roshko number]] to give a correlation between flow rate and frequency. The advantage of this method over the freq/viscosity versus K-factor method is that it takes into account temperature effects on the meter.
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| :<math> \mathrm{St}= {f\over U}{C^3} </math> | |
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| f = meter frequency,
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| U = flow rate,
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| C = linear coefficient of expansion for the meter housing material
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| This relationship leaves Strouhal dimensionless, although a dimensionless approximation is often used for C<sup>3</sup>, resulting in units of pulses/volume (same as K-factor).
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| In animal flight or swimming, propulsive efficiency is high over a narrow range of Strouhal constants, generally peaking in the 0.2 < St < 0.4 range.<ref name="tnt">{{Harv|Taylor|Nudds|Thomas|2003}}</ref> This range is used in the swimming of dolphins, sharks, and bony fish, and in the cruising flight of birds, bats and insects.<ref name="tnt" /> However, in other forms of flight other values are found.<ref name="tnt" /> Intuitively the ratio measures the steepness of the strokes, viewed from the side (e.g., assuming movement through a stationary fluid) – ''f'' is the stroke frequency, ''L'' is the amplitude, so the numerator ''fL'' is half the vertical speed of the wing tip, while the denominator ''V'' is the horizontal speed. Thus the graph of the wing tip forms an approximate sinusoid with aspect (maximum slope) twice the Strouhal constant.<ref>See illustrations at {{Harv|Corum|2003}}</ref>
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| == See also ==
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| * [[Froude number]]
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| * [[Mach Number]]
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| * [[Rossby number]]
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| * [[Weber Number]]
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| * [[Aeroelastic_flutter#Flutter|Aeroelastic Flutter]]
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| * [[Kármán vortex street]]
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| ==References==
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| {{Reflist}}
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| {{refbegin}}
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| * {{cite doi|10.1038/nature02000}}
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| * {{cite web|url=http://style.org/strouhalflight/ | title = The Strouhal Number in Cruising Flight | work = ''[http://13pt.com 13pt],'' | first = Jonathan | last = Corum | year = 2003 | postscript = – depiction of Strouhal number for flying and swimming animals | accessdate = 2012-11-13}}
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| {{refend}}
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| ==External links==
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| *[http://www.weltderphysik.de/intern/upload/annalen_der_physik/1878/Band_241_216.pdf Vincenc Strouhal, Ueber eine besondere Art der Tonerregung]
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| {{NonDimFluMech}}
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| [[Category:Dimensionless numbers of fluid mechanics]]
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| [[Category:Fluid dynamics]]
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Hello!
I'm Turkish female :D.
I really love Breaking Bad!
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