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2 Dimensional Ising Model
Simulate the change in energy and magnetization in a ferro magnet
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The commands shown here should be run from the root of this project.
Compiling regular binaries is as easy as running this command:
The binaries will then be inside the **./bin** directory.
If you want to profile the programs (specifically the MPI program), then run this command
The binaries will then be inside the **./prof** directory.
If you want to debug the code, then use this command:
The binaries will then be inside the **./debug** directory.
To run any of the programs, just use the following command:
If you need help with any of the programs, you can use the -h or –help flag to show you how to use the programs. Here is an example:
Before running the scripts, make sure that all libraries are installed. Using pip, you can install all requirements like this:
This recursively install all the packages that are listed in requirements.txt.
For the Python scripts, run them from the root of the project:
If you have any problems running the scripts, you might have to run this instead:
For the phase_transition_mpi program, there are scripts in the **./slurm_scripts** directory that come along with it. This is to be able to run it on a batch system using Slurm if you have access to one. The only program that should be executed by the user is the **./slurm_scripts/execute.script** script. You can see how to use this script by doing:
This is the recommended way to use this program as it takes approximately 90 minutes to complete when using 8 processes where each process has 10 threads.
If you happen to have such a system available to you, then you should clone this repo on that system, then compile the MPI program like this:
After compiling, you can schedule it by using the **./slurm_scripts/execute.script**:
This section aims to give an idea to the time it takes for the phase transition program to run so that you know a bit what to expect if you decide to run it for yourself.
The times mentioned here are times achieved on a computer with these specifications:
Note that all times here are recorded using the OpenMP implementation of the MCMC algorithm.
| lattice size | points | samples | burn-in time | time (seconds) |
|---|---|---|---|---|
| 20 | 20 | 100000 | 0 | 3.20 |
| 20 | 40 | 100000 | 0 | 6.17 |
| 20 | 80 | 100000 | 0 | 12.11 |
| lattice size | points | samples | burn-in time | time (seconds) |
|---|---|---|---|---|
| 20 | 20 | 100000 | 0 | 3.20 |
| 40 | 20 | 100000 | 0 | 11.91 |
| 80 | 20 | 100000 | 0 | 47.88 |
| lattice size | points | samples | burn-in time | time (seconds) |
|---|---|---|---|---|
| 20 | 20 | 100000 | 0 | 3.20 |
| 20 | 20 | 1000000 | 0 | 29.95 |
| 20 | 20 | 10000000 | 0 | 305.849 |
| lattice size | points | samples | burn-in time | time (seconds) |
|---|---|---|---|---|
| 20 | 20 | 100000 | 0 | 3.20 |
| 20 | 20 | 100000 | 5000 | 4.93 |
| 20 | 20 | 100000 | 10000 | 6.58 |
We can see that changing the number of points, samples and burn-in time changes the time in a linear fashion, while changing the size of the lattice changes the time in a square fashion.
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