Blasius–Chaplygin formula: Difference between revisions
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<math>\bar{L}=\frac{ip}2\int_\gamma f^2(z)\,\mathrm dz</math> |
<math>\bar{L}=\frac{ip}2\int_\gamma f^2(z)\,\mathrm dz</math> |
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The ecuation stated above appears from the analysis of the velocity over a body with a boundary <math>\gamma</math>, taking [[Bernoulli's law]] into consideration. |
The ecuation stated above appears from the analysis of the velocity over a body with a boundary <math>\gamma</math>, taking [[Bernoulli's law]] into consideration.<ref>{{cite web|last1=Eremenko|first1=Alexandre|title=Why airplanes fly, and ships sail|url=https://www.math.purdue.edu/~eremenko/dvi/airplanes.pdf|publisher=Purdue University}}</ref> |
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== References == |
== References == |
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{{Reflist}} |
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<ref>{{cite web|last1=Eremenko|first1=Alexandre|title=Why airplanes fly, and ships sail|url=https://www.math.purdue.edu/~eremenko/dvi/airplanes.pdf|publisher=Purdue University}}</ref> |
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Revision as of 15:42, 5 June 2016
The Blasius-Chaplygin formula, deviced by Sergey Chaplygin from the work of Heinrich Blasius relates the force given by a complex velocity field
The ecuation stated above appears from the analysis of the velocity over a body with a boundary , taking Bernoulli's law into consideration.[1]
References
- ^ Eremenko, Alexandre. "Why airplanes fly, and ships sail" (PDF). Purdue University.