convection | A fully generic , modular DSL for AWS CloudFormation | AWS library
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kandi X-RAY | convection Summary
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convection Key Features
convection Examples and Code Snippets
Community Discussions
Trending Discussions on convection
QUESTION
Let me start by saying that I have found similar problems to mine on the NARKIVE FiPy mailing list archive but since the equations won't load, they are not very useful. For example Convection-diffusion problem on a 1D cylindrical grid, or on another mailing list archive Re: FiPy Heat Transfer Solution. In the second linked mail Daniel says:
There are two ways to solve on a cylindrical domain in FiPy. You can either use the standard diffusion equation in Cartesian coordinates (2nd equation below) and with a mesh that is actually cylindrical in shape or you can use the diffusion equation formulated on a cylindrical coordinate system (1st equation below) and use a standard 2D / 1D grid mesh.
And the equations are not there. In this case it is actually fine because I understand the first solution and I want to use that.
I want to solve the following equation on a 1D cylindrical grid (sorry I don't have 10 reputation yet so I cannot post the nice rendered equations):
with boundary conditions:
where rho_core is the left side of the mesh, and rho_edge is the right side of the mesh. rho is the normalized radius, J is the Jacobian:
R is the real radius in meters, so the dimension of the Jacobian is distance. The initial conditions doesn't really matter, but in my code example I will use a numerical Dirac-delta at R=0.8
.
I have a working example without(!) the Jacobian, but it's quite long, and it doesn't use FiPy's Viewers so I'll link a gist: https://gist.github.com/leferi99/142b90bb686cdf5116ef5aee425a4736
The main part in question is the following:
...ANSWER
Answered 2021-Apr-02 at 14:26[cobbling an answer from the discussion in the comments]
The results are similar between a Grid1D
and a CylindricalGrid1D
, particularly in the early steps, but they are not the same. They are quite different as the problem evolves.
FiPy doesn't like things outside the divergence, but you should be able to multiply the equation by J
and put it in the coefficient of the TransientTerm
, e.g.,
or
QUESTION
I modified the examples.convection.exponential1D.mesh1D
example and it gives an error when I run it.
ANSWER
Answered 2021-Feb-11 at 22:30That's a warning, not an error. It just means we're not being very smart about normalizing an equation with zero error.
The PDE still solves (although the solution isn't very interesting).
QUESTION
In Matlab, the [C, ia, ic] = unique(A)
function returns an sorted array C
in which the duplicates in A
are removed, and the ia
and ic
arrays contains the indices such that C = A(ia) and A = C(ic)
. For example:
ANSWER
Answered 2020-Aug-22 at 15:09The answer is very similar to how you calculate ic
. Just swap A
and C
in the transform
call:
QUESTION
I am looking for solutions to:
- Align vertically the tick labels along the colorbar with the center of each color/class.
- Place some tick labels beside both colorbar triangular extensions.
- Change the figure size to see the tick labels completely while keeping the same colorbar width.
I already tried various solutions proposed on stack overflow to center the tick labels, but none seems to work properly with my current code. For exemple, using ax.set_yticks(number_of_classes + 0.5)
or other similiar methods put all the tick labels at the bottom of the colorbar instead of placing them aligned with the center of each color.
This is the colorbar I get with my current code.
Here's the code I used:
...ANSWER
Answered 2020-Jul-23 at 22:54When setting ticklabels, it is important to also set the tick positions. For the colorbar, these positions need to be set with cb.set_ticks
(this is confusing, as the labels need to be set via cb.ax.set_yticklabels
). Tick positions can only be set at the extremes of the main colorbar, not exactly near the extensions.
So, logical positions are: one at the very bottom, one at the very top, and in the middle of the subsequent bounds
. The label at the bottom can be top-aligned to set it closer to the downward triangle (and similar for the upward triangle).
As the labels now indicate a region, the ticks marks could be removed.
QUESTION
I have a video and I need to simulate frames using Optical Flow; i.e. having a frame and the Optical Flow that represents the pixel translation for the next frame simulate this following resulting frame.
I am using Python and OpenCV as follows:
- Generate flow between two consecutive grayscale frames
ANSWER
Answered 2020-Jun-07 at 15:32The issue was solved slightly updating the code as follows:
QUESTION
So my goal is to scrape a list from a CSV file (I have that part figured out) but when I try running my program on a test URL, that URL is scraped several times and returning the results I want once. I'll clarify with my code and some screen shots.
...ANSWER
Answered 2020-Apr-22 at 22:01The two URLs you are scraping are single product pages, so you shouldn't need the for product in items
loop.
QUESTION
I am writing a CFD solver in C++ but I am in the very beginning. Now I am coding a solver for the linear convection. The math is ok, working well, but I need to write also a code for reading variables from a .txt file. My code is:
...ANSWER
Answered 2020-Mar-14 at 15:53Using only standard features:
QUESTION
I have the following issue: I am trying to parallelize a very simple PDE solver in c++ with openMP but the performance does not improve if I increase the number of threads. The equation is a simple 1D heat equation with convection. Since I need the solution at each timestep I have decided to work with a 2D array
...ANSWER
Answered 2020-Feb-26 at 21:00First of all, you are working on a too small granularity for the multi-threading to be very efficient. Indeed, your sequential time is 9.6 ms and there is 999 time-step. As a result, each time-step take roughly 9.6 us which is rather small.
Additionally, memory accesses are not efficient:
- On one hand using
std::vector>>
produces internally an array that contains pointers to arrays that contains pointers to double-precision arrays (all dynamically allocated). Arrays will probably not be contiguous in memory and could also be badly aligned. This can significantly slow down the execution as it is more difficult for the processor to prefetch data from memory. Consider allocating one big array rather than many small one (eg. one big flatten std::vector). - On the other hand, using padding the way you do result in a very inefficient memory access pattern. Indeed, you only use 1 double over 8, so 7/8 of the memory usage is wasted (probably more since std::vector can allocate additional memory). Additionally, the one read/written are not contiguous due to the added padding and it is hard for the processor to prefetch data and also use the memory efficiently (since reads/writes are performed per the cache line, ie. multiple double-precision scalars). Consider applying padding rows or chunks of your matrix (not scalar).
Finally, using a schedule with blocks of size 8 seems too small. Specifying just schedule(static)
should be probably better here for both the parallel-for and the reduction (the schedule should be the same and static for both if you are using nowait and you want correct results I think).
Consequently, you are probably measuring latency and memory overheads.
Improved versionHere is the corrected code with the most important fixes (false-sharing effects are ignored):
QUESTION
My code below is working properly but I have an issue in the final plot where my schematic is not beginning from the common origin, but instead it is starting from (0,0) but as a point not as the common origin. How to fix it?
...ANSWER
Answered 2020-Feb-08 at 12:04You can set the X and Y limits of the plot with:
QUESTION
I'm using FiPy to model convection/diffusion of a chemical in a given velocity field, and I'm having problems setting this field as ConvectionTerm coefficient.
My velocity field is expressed by two bidimensional arrays, let's say Ugrid
for horizontal velocities and Vgrid
for vertical ones, representing the values at the faces of each cell. For this reason, I'd say that the proper way to set this field as coeff
parameter for the ConvectionTerm would be assigning it to a FaceVariable.
However, I don't get how to pass these two arrays as value
for the FaceVariable. Apparently, I have no problems in setting the field as CellVariable by using value = [np.ravel(Ugrid),np.ravel(Vgrid)]
and the convection simulation appears to make sense as well, but I don't think this is correct, as I briefly mentioned above.
Any suggestions?
...ANSWER
Answered 2019-Nov-14 at 15:23An important consideration with FiPy is that the mesh indexing is not based on grid indexing so mapping from a grid array to cell values should not assume that the mesh is ordered in any particular way. This makes it necessary to use some form of interpolation. Let's first construct a velocity field with grid indexing where the points lie on the grid points (not cell centers).
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