Fundamentals of Fluid Mechanics B Questions and Answers | |
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OK, this problem will be omitted.
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No, this question will remain because it is a very important problem in fluid dynamics. A fluid dynamicist should know how to derive the integral form from the differential form.
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Keep in mind our polynomial for $u$ is not exact. If it would be exact, $u$ would never reach free stream and $v$ would never become zero even infinitely far from the plate (although $u$ would become very close to freestream and $v$ very close to zero, they would never reach these values). Thus, find the integration constant by specifying $v=0$ at the surface and don't worry about whether $v=0$ at the boundary layer edge.
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If the density is not uniform, then you can not use the polynomial fit expression for $u$ given in the tables.
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Follow the steps shown in class for the displacement thickness and submit revisions to your assignment to get feedback.
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There are a few problems here. The first is that your answer “$\partial_x^2 u \ll \partial_y^2 u$” is not a proper answer to what is asked in the question. If what you meant is that this would occur when $L \gg \delta$, then this should be the answer highlighted. But this is also not what is sought here. You should find a condition based on the freestream flow properties. Another issue is that the length scale you use to approximate the derivative along $x$ is not in practice the length of the plate: it may be much less. Redo this problem so you get rid of these concerns. I gave a hint in class on how to approach this. See the recorded lectures.
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This is not the best way of doing it because it will measure much less than the jet height. The Q&A is finished for this term: the exam is in less than 24 hours. Good luck!
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I added them already more than 1 week ago. Let me check why you can not see them.
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They have to be submitted in class on the due date, not on the D2L.
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There are 2 ways to solve this problem. One which is not exact but close enough (the first answer given) and the other which is exact and does not get rid of any term (the second answer given). However, your expression for $v_\theta$ does not match any of the 2 solutions. The error is thus in the process of finding $v_\theta$.
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You should keep the gravitational effects within the $y$ momentum equation.
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In this case, I would not worry about scale velocities in $x$ and $y$ direction. This will make things more complicated then they need to be. You should rather start this by providing an order of magnitude estimate of the largest viscous terms (in any dimension) close and far from the sphere. So, the direction in which they point is not important here. Then, compare these approximate viscous terms to an approximation of the convection terms. Hint: focus on the length scales.
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$\pi$ |