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436:-Someone changed the Prandtl y-momnentum equation to "0 = dP/dy" from the original true Prandtl momentum expression. This is obviously not the correct Prandtl expression. It is not even a correct momentum balance equation. Setting dP/dy to zero was never invoked by Blasius. It is not a condition that is required to obtain the Blasius solution. I am therefore changing it back to the correct expression.
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305:- It is remarked that the Falkner-Skan equation reduces to the Blasius equation for m=0. However, it does not in the form the presented here. One way to fix this is to add a trivial factor two to the similary parameter (in which case Blasius can be written as:
302:- The boundary layer equations omit the pressure gradient which is essential for Falkner-Skan. I also think that it would be helpful to mention how Bernouilli's equation is used to express the pressure gradient in terms of velocity.
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296:- I find the introduction to Prandtl's boundary layer equations inadequate and superfluous - there already exists a much better description on the Boundary layer page.
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for that content in the latter page, and it must not be deleted as long as the latter page exists.
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on
Knowledge. If you would like to participate, please visit the project page, where you can join
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in the second and it uses partial differentials where is should use ordinary differentials.
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Apart from the lack of citations I find this article lacking in other ways:
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The link to the translation of the
Blasius article is incorrect.
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299:- Mention the application of Falkner-Skan to wedge flows.
293:- The title covers only the first half of the article.
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