Dynamic Similarity
http://www.typefreediabetes.com/Articles.asp?ID=150
upgDt
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http://www.eosnap.com/?tag=strait-of-gibraltar
Dimensionless Science
Ideas needed to perform Dimensional Analysis
upgDt
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2 All terms in equation must have same dimensions
Terms in equation can be expressed with 3 basic dimensions: Mass, Length, Time
LTMLTMpLMTLu 23
Dimensions of these variables can be arranged in “Dimensional Matrix”
10121311
1101
TLM
up
10121311
1101
TLM
up
Dimensional Matrix
The rank r of a matrix is the size of the largest square submatrix with non-zero determinant
r = 3Most problems in fluid mechanics
Buckingham’s PI theorem: “n variables can be combined to form exactly (n-r) independent non-dimensional variables.”
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21)zu
yu
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xp
zuw
yuv
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tux
2
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2
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21)zu
yu
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xp
zuw
yuv
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tux
Re2
2
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ULLU
LUxu
xuuinertial vs viscous
TtHgpHzLxUu
Reynolds Number
Low Re
High Re
Flow is laminar when Re < 1000
Flow is in transition to turbulence when 100 < Re < 105 to 106
Flow is turbulent when Re > 106, unless the fluid is stratified
UL
Re
Consider an oceanic flow where U = 0.1 m/s; L = 10 km; kinematic viscosity = 10-6 m2/s
610
100001.0Re 910
Is friction negligible in the ocean?
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21)zu
yu
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zuw
yuv
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FrgHULgHLU
xp
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21inertial vs pressure
TtHgpHzLxUu
Froude Number
1 gHUFr
1 gHUFr
http://www.yourlocalweb.co.uk/greater-manchester/city-of-manchester/higher-blackley/pictures/
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21)zu
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21 pressure vs inertial
TtHgpHzLxUu
Euler Number
http://www.freefoto.com/browse/1222-02-0?ffid=1222-02-0
Great Fountain Geyser, Yellowstone National Park, USA
2UpEu
http://ya.astroleague.org/?p=1445
2UpEu
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21)zu
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zuw
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StTULLUTU
xuu
tu
2local vs inertial
TtHgpHzLxUu
Strouhal Number
UAfSt
f = frequency of motion; A = amplitude of motion – for flying or swimming organisms (fin or wing)
Taylor at al. (2003, Nature 425, 707-711(16 )doi:10.1038/nature02000)
http://www.nature.com/nature/journal/v425/n6959/fig_tab/nature02000_F1.html#figure-title
“Left panels, root-flapping motion; right panels, heaving motion. Amplitude, twice wing chord; static angle of attack, 15°; flow speed, 1.5 ms-1; smoke wire visualizations made at end of downstroke.
a, For St < 0.10, flow separates at the sharp leading-edge, but no discrete vortex forms.
b, For 0.10 < St < 0.25, a leading-edge vortex forms but is shed before the downstroke ends.
c, For 0.25 < St < 0.45, the leading-edge vortex is shed as the downstroke ends.
d, For St > 0.45, trailing edge separation produces a characteristic mushroom-shaped wake.
At higher St, the wing collides with shed vorticity on the upstroke, giving an energetically inefficient mode.”
UAfSt
AfAfU 3.33.0
Dynamic Similarity
http://www.typefreediabetes.com/Articles.asp?ID=150
upgDt
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http://www.eosnap.com/?tag=strait-of-gibraltar
UTLStUpEugHUFr
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Re