basic course content added, more TODO

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---
title: Setting up and Managing Python Environments
author: "[Thomas (Tom) C. Gorordo](https://pages.uoregon.edu/tgorordo) - your TA"
date: 2024-10-01
lang: en
...
To help you get started/possibly avoid at least some tech support/give some advice here's a brief note on Python development environments.
So, welcome to the zoo that is software configuration!
![standards.png](https://imgs.xkcd.com/comics/standards.png)
### POSIX Shells and Environments
It won't come up very often in the course assignments themselves, but for tech support I will generally assume you have access to
a [POSIX](https://en.wikipedia.org/wiki/POSIX) compliant shell (command-line) somewhere on your
machine. If you're using a Linux or Mac operating system
your default shell is likely [`bash`](https://www.gnu.org/software/bash/) or
[`zsh`](https://zsh.sourceforge.io/) (or some variant or equivalent thereof accessible through some kind of 'terminal' program), in which case you should be good-to-go.
If you're on Windows things may be more complicated -
I'm not very up to speed on the current state of [powershell](https://learn.microsoft.com/en-us/powershell/) -
but I can recommend looking into the [Windows Subsystem for Linux (WSL)](https://learn.microsoft.com/en-us/windows/wsl/),
or [`git-bash`](https://gitforwindows.org/), and/or [CygWin](https://www.cygwin.com/)
as ways to get a \*nix-like environment on Windows that I'll be able to help with.
You may also want an editor like [Visual Studio Code](https://code.visualstudio.com/) or [Spyder](https://www.spyder-ide.org/) - though there are many other valid choices for writing/editing your software for this course.
(if you really want to be a shell guru there's always the likes of [neovim](https://neovim.io/);
beware the learning curve.)
You're welcome to set up your technology stack however you'd like, but I can't guarantee I'll be able to debug anything
or replicate your environment faithfully when testing your assignments if you deviate too far from modern Linux dev standards and/or common software (I can help with MATLAB or Julia as well as Python - this guide just anticipates Python will be the most common language choice, and that MATLAB is more self-contained/explanatory).
### Getting and Using Python
If you don't have it already in some form, you should [download and install Python3](https://www.python.org/downloads/) for your system.
You'll also, at a minimum, need to be able to [install packages](https://packaging.python.org/en/latest/tutorials/installing-packages/) (<-- READ THIS LINK if you're at all unsure about what is needed. If you have [`pip`](https://pypi.org/project/pip/) you're good to go with respect to this step).
There are some alternative ways of getting/using python (e.g. [`conda`](https://conda.io/projects/conda/en/latest/user-guide/getting-started.html)) -
but this note will focus on a pretty generic workflow that should be compatible with essentially *any* up-to-date system-level python installation.
Depending on your operating system, it might be more appropriate to use a package manager like
[`apt`](https://ubuntu.com/server/docs/package-management) (for Debian Linux derivatives like Ubuntu - others for other distros),
[homebrew](https://brew.sh/) (for MacOS), or
[winget](https://learn.microsoft.com/en-us/windows/package-manager/winget/install?source=recommendations)/[chocolatey](https://chocolatey.org/) (for Windows)
instead of downloading and running the installer linked above.
Detailed installation instructions will vary a lot by OS, so I won't provide them here - learning how/where to look up system specific ways to do things
(and getting familiar with your machine and customizing it to your liking) is an important skill to develop, but you'll mostly have to find favorite resources and methods yourself over time.
### Dependency Management
We'll often want our code to depend on various external libraries rather than implement *everything* from scratch ourselves (even though that is often necessary or useful - there are situations we won't want to reinvent the wheel and where a better solution than we could write in a reasonable amount of time/effort exists).
The default Python package manager is [`pip`](https://pypi.org/project/pip/) (there are others: [`conda`](https://conda.io/projects/conda/en/latest/user-guide/getting-started.html)
is quite popular and handles some of the virtual environment features mentioned below -
there's also [`poetry`](https://python-poetry.org/), or I am personally partial to [`uv`](https://docs.astral.sh/uv/).
Each work a bit differently, so we'll just cover a barebones python workflow here).
Python projects often list their 'dependencies' in a `requirements.txt` with contents like:
```
jupyter
numpy
matplotlib
pandas
scipy
simpy
```
(some of these are dependencies that will come up in the course - relatively recent versions of each should all work identically well so this list does not specify version numbers [but if you need to lock specific version number down you can do so](https://pip.pypa.io/en/stable/reference/requirements-file-format/)). Given such a file you can install the dependencies for a project into the active environment (usually a venv - see below) via `pip`:
```bash
pip install -r requirements.txt
```
modules can also be installed explicitly by name:
```bash
pip install numpy scipy
```
(Depending on many OS particulars and settings, you may run into permission issues with these commands - let me know if you need help tracking down how to solve them for your particular setup.)
If `pip` is only present in your python installation but not exposed to your commandline you may need to use
```bash
python -m pip <remainder of the pip command goes here...>
```
### Virtual Environments
It can be important to manage dependencies carefully across projects and over time.
For example, suppose you write some code for this course which relies on some specific feature of the current version `numpy1.22` (you might use a particular niche function or rely on a name or shape for some arguments).
Two or three years from now the latest `numpy` version might change the name(s) or interface of the feature you used - and your code will stop working!
If you want to run your old code you'll need to use an older version of `numpy`, but that may be difficult if you have some newer project that wants to rely on the newer version of the library.
While you can ask `pip` to install any version of a library you want at any time (and store a list of required versions in a `requirements.txt`),
uninstalling and re-installing different versions of libraries all the time is messy and liable to break something (especially if you need to manage multiple libraries this way).
![workflow.png](https://imgs.xkcd.com/comics/workflow.png)
The somewhat standard solution to this kind of problem is a "virtual environment" - rather than rely on our global shell environment to keep track of all our projects somehow (hoping nothing winds up incompatible),
we'll manage an independent environment for each project.
Simple dependency management via a virtual environment can be done entirely with `python` and `pip` using the [`venv`](https://docs.python.org/3/library/venv.html) module - in your shell, in some directory relevant to your project(s) invoke:
```bash
# use the python venv module
# to make a new virtual environment stored in the env dir
python -m venv env
```
to create a new virtual environment. You can then activate the environment
(tell your shell it should use the contained version of python and associated libraries) anytime you want to use it by calling:
```bash
source env/bin/activate # run the activation script located in the env dir
```
Your shell will then use a self-contained version of `python` and any libraries you install with `pip` while in this mode.
I recommend using a `venv` of some kind while working on this course -
at the very least it will give you a place to experiment without mucking up your global python installation.
You can leave the virtual environment at any time by calling `exit`.
### All-together: an example
Suppose you want to run a local [`jupyter`](https://jupyter.org/) notebook for yourself - say, to play around a bit and get some ideas ready for an assignment that will require some [`numpy` functions](https://numpy.org/doc/2.1/reference/index.html#reference) and [`matplotlib`](https://matplotlib.org/stable/api/index.html) plotting - but don't yet have anything set up other than your global python installation.
Here's a basic workflow using the methods described above:
1) Set up a working directory along the lines of
```bash
# make a directory for the course and "change directory" (cd) into it
mkdir uoph410-510_image-analysis && cd uoph410-510_image-analysis
# create a virtual environment for the course and activate it
# in the currently open session with your shell (not persistent)
python -m venv env && source ./env/bin/activate
```
2) Install the prerequisite packages (in the venv):
```bash
pip install jupyter numpy matplotlib
```
It can be convenient to append these to a `requirements.txt` in case you want to send anyone else your code (you shouldn't send a `venv` directory - they're not portable between systems).
```bash
# create the .txt, ask pip for its requirements,
# and "pipe" (>>) the text output from pip into the end of the file
touch requirements.txt && pip freeze >> requirements.txt
```
4) Launch `jupyter notebook` & navigate creating a new `.ipynb` in the browser interface.
5) Voila! Notice that installing a new shell command for interacting with python (`jupyter`) could be managed in the same way as a package providing a library you can use in your code. Both are only enabled locally, and temporarily in the current session without polluting your global environment (you won't have any issues in the future anywhere else on your machine because of any software we just installed). If you have dependency issues, just shut down the notebook (`CTRL-C` in the running terminal) and repeat (2), adding any packages that are throwing various "not found" errors.
**Note:** `jupyter` is *not* required (nor even really emphasized) in this class - but it can still be a useful tool for quick sanity-checks and pretty-printed tests or document preparation.
Generally this course will prefer you to write your code in a more modular fashion than `jupyter`'s [stateful](https://en.wikipedia.org/wiki/State_(computer_science)) environment encourages, i.e. you should structure and think of your code overall as [module/library development](https://learn.scientific-python.org/development/) rather than each assignment a one-off notebook.
(Though an optional workflow can be to develop your own module, and import it into a notebook for use with particular values).
## Additional Considerations
The guide above covers just a very basic python environment and workflow.
For a more featureful development experience you may want to do your own research on (in addition to some of the things scattered above):
- Linters like [ruff](https://docs.astral.sh/ruff/) or [black](https://black.readthedocs.io/en/stable/), which help you ensure your code is written in a consistent style - to help with readability.
- Unit testing with [pytest](https://docs.pytest.org/en/8.0.x/) or [`unittest`](https://docs.python.org/3/library/unittest.html) (along with *many* plugins for each/either).
In particular, you might find [ipytest](https://jupyter-tutorial.readthedocs.io/en/stable/notebook/testing/ipytest.html) useful for checking that your code is behaving as you expect
while you develop your solutions.
- Type checkers like [mypy](https://www.mypy-lang.org/) or [pyright](https://microsoft.github.io/pyright/#/), while python does not have static typing
(the [interpreter](https://en.wikipedia.org/wiki/Interpreter_(computing)) does not know the [type](https://en.wikipedia.org/wiki/Data_type) of an object [before](https://en.wikipedia.org/wiki/Compile_time) [runtime](https://en.wikipedia.org/wiki/Execution_(computing)#Runtime)) - there is some loose tooling available to help you try to structure your code in a type-safe
(or at least [duck-typed](https://en.wikipedia.org/wiki/Duck_typing)) - and more likely to be correct - way. These tend to integrate well with testing frameworks mentioned in the last bullet.
- You may want to manage a version-controlled [git](https://git-scm.com/) repository for your work on the course. Git and [Github](https://github.com/) are ubiquitous in modern software development.
While we won't cover their use in this course, privately managing your work with these tools would be excellent practice.
Good luck, have fun, don't die!
(page [raw pandoc `.md`](setup.md), [github repo](https://github.com/tgorordo/pages.uoregon.edu))

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# /// script
# requires-python = ">=3.13"
# dependencies = [
# "marimo>=0.19.7",
# ]
# ///
import marimo
__generated_with = "0.19.11"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
return (mo,)
@app.cell
def _():
import numpy as np
return (np,)
@app.cell
def _():
import matplotlib.pyplot as plt
return (plt,)
@app.cell
def _(mo):
from pathlib import Path
mo.pdf(src=Path("Homework0.pdf"), width="100%", height="50vh")
return
@app.cell
def _(np):
def unit_gridcircle_mask(N):
ruler = np.arange(-(N + 1.5), (N + 2.5)) / N
xx, yy = np.meshgrid(ruler, ruler)
mask = np.sqrt(np.square(xx) + np.square(yy)) <= 1
return mask
return (unit_gridcircle_mask,)
@app.cell
def _(np, unit_gridcircle_mask):
def unit_gridcircle_area(N):
area = float(np.sum(unit_gridcircle_mask(N), dtype=float) / N**2)
return area
return (unit_gridcircle_area,)
@app.cell
def _(np, plt, unit_gridcircle_mask):
plt.matshow(unit_gridcircle_mask(5), cmap=plt.cm.gray_r)
plt.grid(visible=True, color="cyan")
plt.xticks(ticks=(np.arange(14) - 0.5))
plt.yticks(ticks=(np.arange(14) - 0.5))
f = plt.gca()
f.axes.xaxis.set_ticklabels([])
f.axes.yaxis.set_ticklabels([])
plt.show()
return
@app.cell
def _(np, plt, unit_gridcircle_area):
Npts = 100
Ns = np.unique(np.floor(np.logspace(np.log10(2), np.log10(2000), Npts)).astype(int))
As = list(map(unit_gridcircle_area, Ns))
plt.figure(figsize=(8,6))
plt.semilogx(Ns, As, 'o-', color='steelblue', markerfacecolor='lightblue', markersize=12)
xlim = plt.gca().get_xlim()
plt.semilogx((xlim[0], xlim[1]), (np.pi, np.pi), ':', linewidth=2.5, color='darkorange')
plt.xlabel('N', fontsize=14)
plt.ylabel('Area', fontsize=14)
plt.xticks(fontsize=12)
plt.yticks(fontsize=12)
plt.show()
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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# /// script
# requires-python = ">=3.13"
# dependencies = [
# "marimo>=0.19.7",
# ]
# ///
import marimo
__generated_with = "0.19.11"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
return (mo,)
@app.cell
def _():
import numpy as np
return (np,)
@app.cell
def _():
import matplotlib.pyplot as plt
return (plt,)
@app.cell
def _(mo):
from pathlib import Path
mo.pdf(src=Path("Homework1.pdf"), width="100%", height="50vh")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Puzzles
### a.
""")
return
@app.cell
def _(plt):
im_A_png = plt.imread("AuLait_gray.png")
im_A_tif = plt.imread("AuLait_gray.tif")
return im_A_png, im_A_tif
@app.cell
def _(im_A_png, plt):
plt.imshow(im_A_png, "gray")
return
@app.cell
def _(im_A_tif):
im_A_tif.shape
return
@app.cell
def _(im_A_png, np):
np.max(im_A_png)
return
@app.cell
def _(im_A_tif, plt):
plt.imshow(im_A_tif, "gray")
return
@app.cell
def _(im_A_tif):
im_A_tif.shape
return
@app.cell
def _(im_A_tif, np):
np.max(im_A_tif)
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## b.
""")
return
@app.cell
def _():
from skimage import io
return (io,)
@app.cell
def _(im_A_png, io):
io.imsave("AuLait_gray_png_skout_unscaled.tif", im_A_png)
return
@app.cell
def _(plt):
im_A_sk_tif_unscaled = plt.imread("AuLait_gray_png_skout_unscaled.tif")
return (im_A_sk_tif_unscaled,)
@app.cell
def _(im_A_sk_tif_unscaled):
im_A_sk_tif_unscaled.shape
return
@app.cell
def _(im_A_sk_tif_unscaled, plt):
plt.imshow(im_A_sk_tif_unscaled)
return
@app.cell
def _(im_A_png, io):
io.imsave("AuLait_gray_png_skout_scaledup.tif", im_A_png * 255)
return
@app.cell
def _(plt):
im_A_sk_tif_scaled = plt.imread("AuLait_gray_png_skout_scaledup.tif")
return (im_A_sk_tif_scaled,)
@app.cell
def _(im_A_sk_tif_scaled):
im_A_sk_tif_scaled.shape
return
@app.cell
def _(im_A_sk_tif_scaled, plt):
plt.imshow(im_A_sk_tif_scaled)
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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@ -0,0 +1,357 @@
import marimo
__generated_with = "0.19.11"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
return (mo,)
@app.cell
def _():
import matplotlib, matplotlib.pyplot as plt
plt.ion()
return (plt,)
@app.cell
def _():
import numpy as np
return (np,)
@app.cell
def _():
from skimage import io
from skimage.filters import threshold_otsu, threshold_local
return io, threshold_local, threshold_otsu
@app.cell
def _(mo):
from pathlib import Path
mo.pdf(src=Path("Homework2.pdf"), width="100%", height="50vh")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## 1. Thresholding
""")
return
@app.cell
def _(io):
robert_mapplethrope_calla_lily_1984_png = io.imread("robert-mapplethrope-calla-lily-1984.png", as_gray=True)
return (robert_mapplethrope_calla_lily_1984_png,)
@app.cell
def _(plt, robert_mapplethrope_calla_lily_1984_png):
fig1, ax1 = plt.subplots()
p1 = ax1.imshow(robert_mapplethrope_calla_lily_1984_png, cmap="gray")
fig1.colorbar(p1, ax=ax1)
fig1
return
@app.cell
def _(robert_mapplethrope_calla_lily_1984_png, threshold_otsu):
robert_mapplethrope_calla_lily_global_threshold = threshold_otsu(robert_mapplethrope_calla_lily_1984_png)
robert_mapplethrope_calla_lily_global_threshold # print
return (robert_mapplethrope_calla_lily_global_threshold,)
@app.cell
def _(
plt,
robert_mapplethrope_calla_lily_1984_png,
robert_mapplethrope_calla_lily_global_threshold,
):
fig2, (ax2a, ax2b) = plt.subplots(1, 2, figsize=(8, 4))
ax2a.hist(robert_mapplethrope_calla_lily_1984_png.flatten(), log=True, bins="auto")
ax2a.vlines(robert_mapplethrope_calla_lily_global_threshold, 0, 80_000, color="r")
p2b = ax2b.imshow(robert_mapplethrope_calla_lily_1984_png > robert_mapplethrope_calla_lily_global_threshold, cmap="gray")
fig2.colorbar(p2b, ax=ax2b)
fig2
return
@app.cell
def _(io, plt):
fig3, ax3 = plt.subplots()
istanbul_arch_museum_gray_crop_png = io.imread("istanbul_arch_museum_gray_crop.png", as_gray=True)
p3 = ax3.imshow(istanbul_arch_museum_gray_crop_png, cmap="gray")
fig3.colorbar(p3, ax=ax3)
fig3
return (istanbul_arch_museum_gray_crop_png,)
@app.cell
def _(istanbul_arch_museum_gray_crop_png, threshold_otsu):
istanbul_global_threshold = threshold_otsu(istanbul_arch_museum_gray_crop_png)
istanbul_global_threshold # print
return (istanbul_global_threshold,)
@app.cell
def _(istanbul_arch_museum_gray_crop_png, istanbul_global_threshold, plt):
fig4, (ax4a, ax4b) = plt.subplots(1, 2, figsize=(8, 4))
ax4a.hist(istanbul_arch_museum_gray_crop_png.flatten(), log=True, bins="auto")
ax4a.vlines(istanbul_global_threshold, 0, 300_000, color='r')
p4b = ax4b.imshow(istanbul_arch_museum_gray_crop_png > istanbul_global_threshold, cmap="gray")
fig4.colorbar(p4b, ax=ax4b)
fig4
return
@app.cell
def _(io):
robert_mapplethrope_calla_lily_1984_crop_png = io.imread("robert-mapplethrope-calla-lily-1984_CROP.png", as_gray=True)
return (robert_mapplethrope_calla_lily_1984_crop_png,)
@app.cell
def _(plt, robert_mapplethrope_calla_lily_1984_crop_png):
fig5, ax5 = plt.subplots()
p5 = ax5.imshow(robert_mapplethrope_calla_lily_1984_crop_png, cmap="gray")
fig5.colorbar(p5, ax=ax5)
fig5
return
@app.cell
def _(robert_mapplethrope_calla_lily_1984_crop_png, threshold_otsu):
robert_mapplethrope_calla_lily_crop_global_threshold = threshold_otsu(robert_mapplethrope_calla_lily_1984_crop_png)
robert_mapplethrope_calla_lily_crop_global_threshold # print
return (robert_mapplethrope_calla_lily_crop_global_threshold,)
@app.cell
def _(
plt,
robert_mapplethrope_calla_lily_1984_crop_png,
robert_mapplethrope_calla_lily_crop_global_threshold,
):
fig6, (ax6a, ax6b) = plt.subplots(1, 2, figsize=(8, 4))
ax6a.hist(robert_mapplethrope_calla_lily_1984_crop_png.flatten(), log=True, bins="auto")
ax6a.vlines(robert_mapplethrope_calla_lily_crop_global_threshold, 0, 80_000, color="r")
p6b = ax6b.imshow(robert_mapplethrope_calla_lily_1984_crop_png > robert_mapplethrope_calla_lily_crop_global_threshold, cmap="gray")
fig6.colorbar(p6b, ax=ax6b)
fig6
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## 2. Thresholding, again
""")
return
@app.cell
def _(
istanbul_arch_museum_gray_crop_png,
plt,
robert_mapplethrope_calla_lily_1984_crop_png,
robert_mapplethrope_calla_lily_1984_png,
threshold_local,
):
fig7, (ax7a, ax7b, ax7c) = plt.subplots(1, 3, figsize=(12, 4))
p7a = ax7a.imshow(robert_mapplethrope_calla_lily_1984_png > threshold_local(robert_mapplethrope_calla_lily_1984_png, block_size=123), cmap="gray")
fig7.colorbar(p7a, ax=ax7a)
p7b = ax7b.imshow(istanbul_arch_museum_gray_crop_png > threshold_local(istanbul_arch_museum_gray_crop_png, block_size=123), cmap="gray")
fig7.colorbar(p7b, ax=ax7b)
p7c = ax7c.imshow(robert_mapplethrope_calla_lily_1984_crop_png > threshold_local(robert_mapplethrope_calla_lily_1984_crop_png, block_size=123), cmap="gray")
fig7.colorbar(p7c, ax=ax7c)
fig7
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## 3. Protein density
""")
return
@app.cell
def _(io, plt):
fig8, ax8 = plt.subplots()
microarray_crop_png = io.imread("microarray_crop.png", as_gray=True)
p8 = ax8.imshow(microarray_crop_png, cmap="gray")
fig8.colorbar(p8, ax=ax8)
fig8
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## 4. Non-uniform background subtraction
""")
return
@app.cell
def _(io, plt):
fig9, ax9 = plt.subplots()
GUV24_bead_crop_png = io.imread("GUV24_bead_Crop.png", as_gray=True)
p9 = ax9.imshow(GUV24_bead_crop_png, cmap="gray")
fig9.colorbar(p9, ax=ax9)
fig9
return (GUV24_bead_crop_png,)
@app.cell
def _(GUV24_bead_crop_png, np):
x = np.arange(GUV24_bead_crop_png.shape[0])
y = np.arange(GUV24_bead_crop_png.shape[1])
xs, ys = np.meshgrid(x, y)
return x, xs, ys
@app.cell
def _(GUV24_bead_crop_png, plt, xs, ys):
fig10, ax10 = plt.subplots()
ax10 = plt.axes(projection ='3d')
p10 = ax10.plot_surface(xs, ys, GUV24_bead_crop_png, cmap="viridis")
fig10
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
### b.
""")
return
@app.cell
def _(GUV24_bead_crop_png, np, xs):
w = np.vstack([xs.ravel(), np.ones(xs.size)]).T
mx, c = np.linalg.lstsq(w, GUV24_bead_crop_png.ravel())[0] # (c-410) 3pt alternative
(mx, c)
return c, mx
@app.cell
def _(GUV24_bead_crop_png, c, mx, plt, x, xs, ys):
fig11, (ax11a, ax11b) = plt.subplots(1, 2, figsize=(8, 4))
ax11a.plot(x, mx * x + c, c='r')
ax11a.scatter(xs.ravel(), GUV24_bead_crop_png.ravel(), s=4)
ax11b.scatter(ys.ravel(), GUV24_bead_crop_png.ravel(), s=4)
fig11
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
### c.
#### 410:
""")
return
@app.cell
def _(GUV24_bead_crop_png, np, xs, ys):
# z = m @ w + c
w2 = np.vstack([xs.ravel(), ys.ravel(), np.ones(GUV24_bead_crop_png.size)]).T
mx2, my2, c2 = np.linalg.lstsq(w2, GUV24_bead_crop_png.ravel())[0]
(mx2, my2, c2)
return c2, mx2, my2
@app.cell
def _(GUV24_bead_crop_png, c2, mx2, my2, plt, xs, ys):
fig12, ax12 = plt.subplots()
ax12 = plt.axes(projection ='3d')
ax12.plot_surface(xs, ys, GUV24_bead_crop_png, cmap="viridis", alpha=0.3)
ax12.plot_surface(xs, ys, mx2 * xs + my2 * ys + c2, cmap="plasma")
fig12
return
@app.cell
def _(GUV24_bead_crop_png, c2, mx2, my2, plt, xs, ys):
fig13, ax13 = plt.subplots()
ax13 = plt.axes(projection ='3d')
ax13.plot_surface(xs, ys, GUV24_bead_crop_png - (mx2 * xs + my2 * ys + c2), cmap="viridis")
fig13
return
@app.cell
def _(GUV24_bead_crop_png, c2, mx2, my2, plt, xs, ys):
fig14, ax14 = plt.subplots()
p14 = ax14.imshow(GUV24_bead_crop_png - (mx2 * xs + my2 * ys + c2), cmap="gray")
fig14.colorbar(p14, ax=ax14)
fig14
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
#### 510:
""")
return
@app.cell
def _(GUV24_bead_crop_png, np, xs, ys):
# z = m @ w + c
w3 = np.vstack([xs.ravel(), np.square(xs.ravel()),
ys.ravel(), np.square(ys.ravel()),
np.ones(GUV24_bead_crop_png.size)]).T
mx3, mx3x, my3, my3y, c3 = np.linalg.lstsq(w3, GUV24_bead_crop_png.ravel())[0]
(mx3, mx3x, my3, my3y, c3)
return c3, mx3, mx3x, my3, my3y
@app.cell
def _(GUV24_bead_crop_png, c3, mx3, mx3x, my3, my3y, np, plt, xs, ys):
fig15, ax15 = plt.subplots()
ax15 = plt.axes(projection ='3d')
ax15.plot_surface(xs, ys, GUV24_bead_crop_png, cmap="viridis", alpha=0.3)
ax15.plot_surface(xs, ys, mx3 * xs + mx3x * np.square(xs) + my3 * ys + my3y * np.square(ys) + c3, cmap="plasma")
return
@app.cell
def _(GUV24_bead_crop_png, c3, mx3, mx3x, my3, my3y, np, plt, xs, ys):
fig16, ax16 = plt.subplots()
p16 = ax16.imshow(GUV24_bead_crop_png - (mx3 * xs + mx3x * np.square(xs) + my3 * ys + my3y * np.square(ys) + c3), cmap="gray")
fig16.colorbar(p16, ax=ax16)
fig16
return
@app.cell
def _(GUV24_bead_crop_png, c3, mx3, mx3x, my3, my3y, np, plt, xs, ys):
fig17, ax17 = plt.subplots()
ax17 = plt.axes(projection ='3d')
ax17.plot_surface(xs, ys, GUV24_bead_crop_png -
(mx3 * xs + mx3x * np.square(xs) + my3 * ys + my3y * np.square(ys) + c3), cmap="viridis")
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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@ -0,0 +1,554 @@
import marimo
__generated_with = "0.19.11"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
return (mo,)
@app.cell
def _():
import matplotlib, matplotlib.pyplot as plt
plt.ion();
return (plt,)
@app.cell
def _():
import numpy as np
return (np,)
@app.cell
def _():
from skimage import io
from skimage.filters import gaussian, median, threshold_otsu
return gaussian, io, median, threshold_otsu
@app.cell
def _():
import scipy.ndimage as ndi
return (ndi,)
@app.cell
def _(mo):
from pathlib import Path
mo.pdf(src=Path("Homework3.pdf"), width="100%", height="50vh")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Convolution and Filtering
""")
return
@app.cell
def _(io):
escher_relativity_png = io.imread("escher-relativity.png", as_gray=True)
return (escher_relativity_png,)
@app.cell
def _(escher_relativity_png, plt):
fig1, ax1 = plt.subplots()
p1 = ax1.imshow(escher_relativity_png, cmap="gray")
cbar1 = fig1.colorbar(p1, ax=ax1)
fig1
return
@app.cell
def _(np):
avgker11 = np.ones((11, 11)) / np.square(11)
return (avgker11,)
@app.cell
def _(avgker11, escher_relativity_png, ndi):
escher_relativity_png_avgd_const = ndi.convolve(escher_relativity_png, avgker11, mode="constant")
escher_relativity_png_avgd_miror = ndi.convolve(escher_relativity_png, avgker11, mode="mirror")
return escher_relativity_png_avgd_const, escher_relativity_png_avgd_miror
@app.cell
def _(escher_relativity_png_avgd_const, escher_relativity_png_avgd_miror, plt):
fig2, (ax2a, ax2b) = plt.subplots(1, 2, figsize=(8, 4))
p2a = ax2a.imshow(escher_relativity_png_avgd_const, cmap="gray")
p2b = ax2b.imshow(escher_relativity_png_avgd_miror, cmap="gray")
fig2.colorbar(p2a, ax=ax2a)
fig2.colorbar(p2b, ax=ax2b)
fig2
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Gaussian Filtering
""")
return
@app.cell
def _(np):
def gaussker(sgm2, shape=(11, 11)):
xs, ys = np.meshgrid(np.arange(shape[0]), np.arange(shape[1]))
r2s = np.square(xs - shape[0] // 2) + np.square(ys - shape[0] // 2)
e = np.exp(- r2s / (2 * sgm2))
return e / np.sum(e) # return normalized kernel
return (gaussker,)
@app.cell
def _(gaussker, plt):
fig3, (ax3a, ax3b) = plt.subplots(1, 2, figsize=(8, 4))
p3a = ax3a.imshow(gaussker(3))
p3b = ax3b.imshow(gaussker(7))
fig3.colorbar(p3a, ax=ax3a)
fig3.colorbar(p3b, ax=ax3b)
fig3
return
@app.cell
def _(escher_relativity_png, gaussker, ndi):
escher_relativity_png_gaussd3 = ndi.convolve(escher_relativity_png, gaussker(3))
escher_relativity_png_gaussd7 = ndi.convolve(escher_relativity_png, gaussker(7))
return escher_relativity_png_gaussd3, escher_relativity_png_gaussd7
@app.cell
def _(escher_relativity_png_gaussd3, escher_relativity_png_gaussd7, plt):
fig4, (ax4a, ax4b) = plt.subplots(1, 2, figsize=(8, 4))
p4a = ax4a.imshow(escher_relativity_png_gaussd3, cmap="gray")
p4b = ax4b.imshow(escher_relativity_png_gaussd7, cmap="gray")
fig4.colorbar(p4a, ax=ax4a)
fig4.colorbar(p4b, ax=ax4b)
fig4
return
@app.cell
def _(escher_relativity_png, gaussian, np):
escher_relativity_png_gaussdsk7 = gaussian(escher_relativity_png, np.sqrt(7))
return (escher_relativity_png_gaussdsk7,)
@app.cell
def _(escher_relativity_png_gaussdsk7, plt):
fig5, ax5 = plt.subplots()
p5 = ax5.imshow(escher_relativity_png_gaussdsk7, cmap="gray")
fig5.colorbar(p5, ax=ax5)
fig5
return
@app.cell
def _(escher_relativity_png_gaussd7, escher_relativity_png_gaussdsk7, np):
escher_relativity_png_skdiff = escher_relativity_png_gaussdsk7 - escher_relativity_png_gaussd7
escher_relativity_png_skdiff = escher_relativity_png_skdiff - np.min(escher_relativity_png_skdiff)
return (escher_relativity_png_skdiff,)
@app.cell
def _(escher_relativity_png_skdiff, plt):
fig6, ax6 = plt.subplots()
p6 = ax6.imshow(escher_relativity_png_skdiff, cmap="gray")
fig6.colorbar(p6, ax=ax6)
fig6
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Median Filtering
""")
return
@app.cell
def _(escher_relativity_png, median, np):
escher_relativity_png_median7 = median(escher_relativity_png, np.ones((7, 7)))
return (escher_relativity_png_median7,)
@app.cell
def _(escher_relativity_png_median7, plt):
fig7, ax7 = plt.subplots()
p7 = ax7.imshow(escher_relativity_png_median7, cmap="gray")
fig7.colorbar(p7, ax=ax7)
fig7
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Filtering and Thresholding
""")
return
@app.cell
def _(io):
makeup_richardprince_1983_gray_png = io.imread("MakeUp_RichardPrince_1983_gray.png", as_gray=True)
return (makeup_richardprince_1983_gray_png,)
@app.cell
def _(makeup_richardprince_1983_gray_png, plt):
fig8, ax8 = plt.subplots()
p8 = ax8.imshow(makeup_richardprince_1983_gray_png, cmap="gray")
fig8.colorbar(p8, ax=ax8)
fig8
return
@app.cell
def _(gaussian, makeup_richardprince_1983_gray_png, np, threshold_otsu):
makeup_richardprince_1983_gray_png_gaussian = 255 * gaussian(makeup_richardprince_1983_gray_png, np.sqrt(51))
makeup_richardprince_1983_gray_png_gaussian_gthreshold = threshold_otsu(makeup_richardprince_1983_gray_png_gaussian)
makeup_richardprince_1983_gray_png_gaussian_threshd = makeup_richardprince_1983_gray_png_gaussian > makeup_richardprince_1983_gray_png_gaussian_gthreshold
return (makeup_richardprince_1983_gray_png_gaussian_threshd,)
@app.cell
def _(makeup_richardprince_1983_gray_png, median, np, threshold_otsu):
makeup_richardprince_1983_gray_png_median = median(makeup_richardprince_1983_gray_png, np.ones((51, 51)))
makeup_richardprince_1983_gray_png_median_gthreshold = threshold_otsu(makeup_richardprince_1983_gray_png_median)
makeup_richardprince_1983_gray_png_median_threshd = makeup_richardprince_1983_gray_png_median > makeup_richardprince_1983_gray_png_median_gthreshold
return (makeup_richardprince_1983_gray_png_median_threshd,)
@app.cell
def _(
makeup_richardprince_1983_gray_png_gaussian_threshd,
makeup_richardprince_1983_gray_png_median_threshd,
plt,
):
fig9, (ax9a, ax9b) = plt.subplots(1, 2, figsize=(8, 4))
p9a = ax9a.imshow(makeup_richardprince_1983_gray_png_gaussian_threshd, cmap="gray")
fig9.colorbar(p9a, ax=ax9a)
p9b = ax9b.imshow(makeup_richardprince_1983_gray_png_median_threshd, cmap="gray")
fig9.colorbar(p9b, ax=ax9b)
fig9
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## High-pass Filtering
""")
return
@app.cell
def _(io):
elevator_to_the_gallows_png = io.imread("Elevator_to_the_gallows.png", as_gray=True)
return (elevator_to_the_gallows_png,)
@app.cell
def _(elevator_to_the_gallows_png, plt):
fig10, ax10 = plt.subplots()
ax10.imshow(elevator_to_the_gallows_png, cmap="gray")
fig10
return
@app.cell
def _(gaussian, np):
def gausshighpass(image, sigma=np.sqrt(7)):
gaussd = (np.max(image) - np.min(image)) * gaussian(image, sigma)
diff = image - gaussd
diff = diff - np.min(diff)
return (255 / np.max(diff)) * diff
return (gausshighpass,)
@app.cell
def _(elevator_to_the_gallows_png, gausshighpass):
elevator_to_the_gallows_png_highpass = gausshighpass(elevator_to_the_gallows_png, sigma=21)
return (elevator_to_the_gallows_png_highpass,)
@app.cell
def _(elevator_to_the_gallows_png_highpass, plt):
fig11, ax11 = plt.subplots()
ax11.imshow(elevator_to_the_gallows_png_highpass, cmap="gray")
fig11
return
@app.cell
def _(elevator_to_the_gallows_png_highpass, threshold_otsu):
elevator_to_the_gallows_png_highpass_threshold = threshold_otsu(elevator_to_the_gallows_png_highpass)
elevator_to_the_gallows_png_highthresh = elevator_to_the_gallows_png_highpass > elevator_to_the_gallows_png_highpass_threshold
return (elevator_to_the_gallows_png_highthresh,)
@app.cell
def _(elevator_to_the_gallows_png_highthresh, plt):
fig12, ax12 = plt.subplots()
ax12.imshow(elevator_to_the_gallows_png_highthresh, cmap="gray")
fig12
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Band-pass Filtering
""")
return
@app.cell
def _(io):
gaussians_s2_to_s50_px_tif = io.imread("gaussians_s2_to_s50_px.tif", as_gray=True)
return (gaussians_s2_to_s50_px_tif,)
@app.cell
def _(gaussians_s2_to_s50_px_tif, plt):
fig13, (ax13a, ax13b) = plt.subplots(1, 2, figsize=(8, 4))
ax13a.imshow(gaussians_s2_to_s50_px_tif, cmap="gray")
ax13a.hlines(1240, 0, 3200, color="magenta")
ax13b.plot(gaussians_s2_to_s50_px_tif[1240, :])
fig13
return
@app.cell
def _(gaussian, np):
def gausslowpass(image, sigma=np.sqrt(7)):
gaussd = (np.max(image) - np.min(image)) * gaussian(image, sigma)
return (255 / np.max(gaussd)) * gaussd
return (gausslowpass,)
@app.cell
def _(gausshighpass, gaussians_s2_to_s50_px_tif, gausslowpass):
gaussians_s2_to_s50_px_tif_bandpassed = gausslowpass(gausshighpass(
gaussians_s2_to_s50_px_tif,
sigma=20), sigma=10)
return (gaussians_s2_to_s50_px_tif_bandpassed,)
@app.cell
def _(gaussians_s2_to_s50_px_tif_bandpassed, plt):
fig14, (ax14a, ax14b) = plt.subplots(1, 2, figsize=(8, 4))
ax14a.imshow(gaussians_s2_to_s50_px_tif_bandpassed, cmap="gray")
ax14a.hlines(1240, 0, 3200, color="magenta")
ax14b.plot(gaussians_s2_to_s50_px_tif_bandpassed[1240, :])
fig14
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Signal to Noise Ratio
""")
return
@app.cell
def _(np):
rng = np.random.default_rng()
def sim_image(r, b=2, t=2, size=(27, 27)):
bg = rng.poisson(lam=b * t, size=size)
sg = np.zeros_like(bg)
sg[sg.shape[0] // 2, sg.shape[1] // 2] = rng.poisson(lam=r*t)
return bg + sg
return (sim_image,)
@app.cell
def _(plt, sim_image):
fig15, (ax15a, ax15b, ax15c) = plt.subplots(1, 3, figsize=(10, 4))
ax15a.imshow(sim_image(2, t=1), cmap="gray")
ax15b.imshow(sim_image(6, t=1), cmap="gray")
ax15c.imshow(sim_image(10, t=1), cmap="gray")
return
@app.cell
def _(np, sim_image):
exposure_sims = [ sim_image(0.5, t=t) for t in range(0, 300) ]
sns = [s[27//2, 27//2] / np.std(s) for s in exposure_sims]
return (sns,)
@app.cell
def _(plt, sns):
fig16, ax16 = plt.subplots()
ax16.scatter(range(0, 300), sns)
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## A little bit of Fourier Transforming
""")
return
@app.cell
def _(io):
Lincoln_Coleman_png = io.imread("Lincoln_Coleman_40-copyright-havecamerawilltravel-com_crop512_gray.png", as_gray=True)
return (Lincoln_Coleman_png,)
@app.cell
def _(Lincoln_Coleman_png, plt):
fig17, ax17 = plt.subplots()
ax17.imshow(Lincoln_Coleman_png, cmap="grey")
return
@app.cell
def _():
# %load fourier_masking_HWproblem.py
return
@app.cell
def _(io, np, plt):
# %load fourier_masking_HWproblem.py
# fourier_masking_HWproblem.py
"""
Author: Raghuveer Parthasarathy
Created on Tue Oct 8 07:25:53 2024
Last modified on Oct. 12, 2024
Description
-----------
For a homework problem on masking Fourier Transforms
"""
#import numpy as np
#import matplotlib.pyplot as plt
import os
#from skimage import io # input output sub-package
# %% Load the image
parentDir = r"./"
fileName = r"Lincoln_Coleman_40-copyright-havecamerawilltravel-com_crop512_gray.png"
im = io.imread(os.path.join(parentDir, fileName))
if im.ndim > 2:
# A bit silly, since I know this is 2D
im = np.mean(im, axis=2, dtype=im.dtype)
print("Image shape: ", im.shape)
# Image size; I'm not checking if it's square!
# The Lincoln Memorial image is 512x512
N = im.shape[0]
plt.figure()
plt.imshow(im, "gray")
plt.title("Original Image")
# %% Fourier Transform
# Perform 2D Fourier transform
F = np.fft.fft2(im) # Fast Fourier Transform
F_shifted = np.fft.fftshift(F) # Shift so zero frequency is in the center
# Calculate the amplitude and phase
amplitude = np.abs(F_shifted)
phase = np.angle(F_shifted)
# Display amplitude as an image
plt.figure()
plt.title("Fourier Transform Amplitude (log scale)")
# Should maybe add an offset to avoid -Inf,
# but I've tested and there are no zeros.
plt.imshow(np.log(amplitude), cmap="gray")
plt.colorbar()
plt.show()
# Display phase as an image
plt.figure()
plt.title("Fourier Transform Phase (radians)")
plt.imshow(phase)
plt.colorbar()
plt.show()
# %% Masking
# "Fundamental frequency" for the mask
f0 = 15 # I determined this "by hand"
# Full width of the mask -- should be an even number
df = 4
# Create a mask array
mask = np.ones((N, N))
for k in range(1, N // (2 * f0)):
center_f = N / 2 + k * f0
mask[:, int(center_f - df / 2) : int(center_f + df / 2)] = 0
center_f = N / 2 - k * f0
mask[:, int(center_f - df / 2) : int(center_f + df / 2)] = 0
# Create a new amplitude array that is the original multiplied by this mask
new_amplitude = amplitude * mask
# new_amplitude = amplitude * (1.0 - mask) # show just the *difference*!
# Display the new amplitude as an image
plt.figure()
plt.title("Amplitude * Mask")
plt.imshow(np.log(new_amplitude + 0.1), cmap="gray") # + 0.1 because of zeros.
plt.colorbar()
plt.show()
# Combine new amplitude with original phase
new_F_shifted = new_amplitude * np.exp(1j * phase)
# Perform the inverse Fourier transform
new_F = np.fft.ifftshift(new_F_shifted)
new_im = np.fft.ifft2(new_F)
new_im = np.abs(new_im)
# Display the resulting image
plt.figure()
plt.title("Image based on Inverse FT")
plt.imshow(new_im, cmap="gray")
plt.colorbar()
plt.show()
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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# -*- coding: utf-8 -*-
# frequency_modulation_hw.py
"""
Author: Raghuveer Parthasarathy
Created on Oct. 17, 2024
Last modified on Oct. 18, 2024
Description
-----------
For a homework problem on frequency modulation
"""
import numpy as np
import matplotlib.pyplot as plt
import os
from skimage import io # input output sub-package
#%% Load the image
parentDir = r'C:\Users\Raghu\Documents\Teaching\Image Analysis Course\Images for Class'
fileName = r'Buster_Keaton_General_Train_512.png'
im = io.imread(os.path.join(parentDir, fileName))
print('Image shape: ', im.shape)
N = im.shape[0]
plt.figure()
plt.imshow(im, 'gray')
plt.title('Original Image')
#%% Multiply by sine waves
xc = np.linspace(-N/2, N/2, N)
x, y = np.meshgrid(xc, xc)
Px = 8
Py = 15
sineWave = np.sin(2.0*np.pi*x/Px) # + np.sin(2.0*np.pi*y/Py)
im_mod = im*sineWave
# Rescale to [0, 255]
im_mod = 255.0*(im_mod - np.min(im_mod)) / (np.max(im_mod) - np.min(im_mod))
im_mod = np.clip(im_mod, 0, 255).astype('uint8')
plt.figure()
plt.imshow(im_mod, 'gray')
plt.title('Modified Image')
# Output
outputFileName = r'Buster_Keaton_General_Train_512_sineMod.png'
io.imsave(os.path.join(parentDir, outputFileName), im_mod)
#%% Fourier Transforms
# Perform 2D Fourier transform of the original
F = np.fft.fft2(im) # Fast Fourier Transform
F_shifted = np.fft.fftshift(F) # Shift so zero frequency is in the center
# Calculate the amplitude and phase
amplitude = np.abs(F_shifted)
phase = np.angle(F_shifted)
# Display amplitude as an image
plt.figure()
plt.title("Fourier Transform Amplitude (log scale)")
plt.imshow(np.log(amplitude), cmap='gray')
plt.colorbar()
plt.show()
# Perform 2D Fourier transform of the modified image
F_mod = np.fft.fft2(im_mod) # Fast Fourier Transform
F_shifted_mod = np.fft.fftshift(F_mod) # Shift so zero frequency is in the center
# Calculate the amplitude and phase
amplitude_mod = np.abs(F_shifted_mod)
phase_mod = np.angle(F_shifted_mod)
# Display amplitude as an image
plt.figure()
plt.title("Fourier Transform Amplitude (log scale): modified image")
plt.imshow(np.log(amplitude_mod), cmap='gray')
plt.colorbar()
plt.show()

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import marimo
__generated_with = "0.19.11"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
return (mo,)
@app.cell
def _():
import numpy as np
return (np,)
@app.cell
def _():
from skimage import io, filters
return filters, io
@app.cell
def _():
import scipy as si
import scipy.ndimage as nd
return nd, si
@app.cell
def _():
import matplotlib
import matplotlib.pyplot as plt
plt.ion();
return (plt,)
@app.cell
def _(mo):
from pathlib import Path
mo.pdf(src=Path("Homework4.pdf"), width="100%", height="50vh")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Frequency Modulation
""")
return
@app.cell
def _(io):
buster_keaton_general_train_512_png = io.imread("Buster_Keaton_General_Train_512.png", as_gray=True)
buster_keaton_general_train_512_sinmod_png = io.imread("Buster_Keaton_General_Train_512_sineMod.png", as_gray=True)
return (
buster_keaton_general_train_512_png,
buster_keaton_general_train_512_sinmod_png,
)
@app.cell
def _(
buster_keaton_general_train_512_png,
buster_keaton_general_train_512_sinmod_png,
plt,
):
fig1, (ax1a, ax1b) = plt.subplots(1, 2, figsize=(8, 4))
ax1a.imshow(buster_keaton_general_train_512_png, cmap="gray")
ax1b.imshow(buster_keaton_general_train_512_sinmod_png, cmap="gray")
return
@app.cell
def _(
buster_keaton_general_train_512_png,
buster_keaton_general_train_512_sinmod_png,
np,
):
buster_keaton_general_train_512_fft = np.abs(np.fft.fftshift(np.fft.fft2(buster_keaton_general_train_512_png)))
buster_keaton_general_train_512_sinmod_fft = np.abs(np.fft.fftshift(np.fft.fft2(buster_keaton_general_train_512_sinmod_png)))
return (
buster_keaton_general_train_512_fft,
buster_keaton_general_train_512_sinmod_fft,
)
@app.cell
def _(
buster_keaton_general_train_512_fft,
buster_keaton_general_train_512_sinmod_fft,
np,
plt,
):
fig2, (ax2a, ax2b) = plt.subplots(1, 2, figsize=(8, 4))
ax2a.imshow(np.log(buster_keaton_general_train_512_fft), cmap="gray")
ax2b.imshow(np.log(buster_keaton_general_train_512_sinmod_fft), cmap="gray")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Quantized Aggregates
""")
return
@app.cell
def _(io):
emitters_33px_100ph_png = io.imread("emitters_33px_100ph.png")
return (emitters_33px_100ph_png,)
@app.cell
def _(emitters_33px_100ph_png, plt):
fig3, ax3 = plt.subplots()
ax3.imshow(emitters_33px_100ph_png, cmap="gray")
return
@app.cell
def _(emitters_33px_100ph_png, plt):
fig4, ax4 = plt.subplots()
ax4.hist(emitters_33px_100ph_png.ravel(), bins="auto")
fig4
return
@app.cell
def _(emitters_33px_100ph_png, filters):
emitters_33px_100ph_hflt = emitters_33px_100ph_png - 255 * filters.gaussian(emitters_33px_100ph_png, 8, mode="nearest")
return (emitters_33px_100ph_hflt,)
@app.cell
def _(emitters_33px_100ph_hflt, plt):
fig6, (ax6a, ax6b) = plt.subplots(1, 2, figsize=(8, 4))
ax6a.imshow(emitters_33px_100ph_hflt, cmap="gray")
ax6b.hist(emitters_33px_100ph_hflt.ravel(), bins=20)
fig6
return
@app.cell
def _(emitters_33px_100ph_hflt, np):
ones = np.ones_like(emitters_33px_100ph_hflt, dtype=bool)
zeros = np.zeros_like(ones, dtype=bool)
x, y = np.arange(ones.shape[0]), np.arange(ones.shape[1])
xs, ys = np.meshgrid(x, y)
masks = [np.where((np.abs(xs - 33 * i) <= 2) & (np.abs(ys - 33 * j) <= 2), ones, zeros)
for i in range(1, 11) for j in range(1, 11)]
# mask = np.where((xs % (33 + 4) > (33 - 4)) & (ys % (33 + 4) > (33 - 4)), ones, zeros)
mask = sum(masks)
return mask, masks
@app.cell
def _(emitters_33px_100ph_hflt, masks, np):
intensities = [np.sum(emitters_33px_100ph_hflt, where=m) for m in masks]
return (intensities,)
@app.cell
def _(intensities, mask, plt):
fig7, (ax7a, ax7b) = plt.subplots(1, 2, figsize=(8, 4))
ax7a.imshow(mask, cmap="gray")
counts, edges, _ = ax7b.hist(intensities, bins=25)
fig7
return counts, edges
@app.cell
def _(counts, edges, np):
irange = (np.max(edges) - np.min(edges))
imin = np.min(edges)
(sum(counts[edges[1:] <= (irange/3) + imin]),
sum(counts[((irange/3) + imin < edges[1:]) & (edges[1:] <= (2*irange/3) + imin)]),
sum(counts[((2*irange/3) + imin < edges[1:])])
)
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## A High-Resolution PSF
""")
return
@app.cell
def _(np, si):
def psfker(l, NA=0.9, side=1.0, N=101, center=(0.0, 0.0)):
xs, ys = np.meshgrid(np.linspace(0.0, side, N), np.linspace(0.0, side, N))
r2s = np.square(xs - side / 2 - center[0]) + np.square(ys - side / 2 - center[1])
v = 2 * np.pi * NA * np.sqrt(r2s) / l
psf = 4 * np.square(si.special.j1(v) / v)
nans = np.isnan(psf)
psf[nans] = 1
return psf / np.sum(psf)
return (psfker,)
@app.cell
def _(plt, psfker):
fig8, (ax8a, ax8b, ax8c) = plt.subplots(1, 3, figsize=(8, 2))
ax8a.imshow(psfker(0.5), cmap="gray")
ax8b.imshow(psfker(0.4), cmap="gray")
ax8c.imshow(psfker(0.4, NA=0.5), cmap="gray")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## A Worse Worm Image
""")
return
@app.cell
def _(io):
fetter_celegans_cellfig10_png = io.imread("fetter_Celegans_cellfig10.jpg", as_gray=True)
return (fetter_celegans_cellfig10_png,)
@app.cell
def _(fetter_celegans_cellfig10_png, plt):
fig9, ax9 = plt.subplots()
ax9.imshow(fetter_celegans_cellfig10_png, cmap="gray")
return
@app.cell
def _(fetter_celegans_cellfig10_png, nd, psfker):
fetter_celegans_cellfig10_psf = nd.convolve(fetter_celegans_cellfig10_png, psfker(0.53, NA=0.7))
return (fetter_celegans_cellfig10_psf,)
@app.cell
def _(fetter_celegans_cellfig10_psf, plt):
fig10, ax10 = plt.subplots()
ax10.imshow(fetter_celegans_cellfig10_psf, cmap="gray")
return
@app.cell
def _(mo):
mo.md(r"""
## SNR and Poisson Noise
$$ N_\text{photon} \sim SNR^2 $$
""")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Simulated Point Sources
""")
return
@app.cell
def _(np):
def pixelate(image, inscale, shape=(15, 15)):
outscale = image.shape[0] * inscale / shape[0]
assert outscale == image.shape[1] * inscale / shape[1]
assert outscale.is_integer()
ii, jj = np.indices(image.shape)
ones = np.ones_like(image, dtype=bool)
zeros = np.zeros_like(image, dtype=bool)
masks = [np.where((i * outscale <= ii * inscale) &
(ii * inscale < (i + 1) * outscale)
& (j * outscale <= jj * inscale) &
(jj * inscale < (j + 1) * outscale),
ones, zeros)
for i in range(shape[0]) for j in range(shape[1])]
outage = np.array([np.sum(image, where=m) for m in masks]).reshape(shape)
return outage, outscale
return (pixelate,)
@app.cell
def _(pixelate, psfker):
simpoint, _ = pixelate(psfker(0.5, NA=0.9, side=15 * 0.1, N = 150), 0.1)
return (simpoint,)
@app.cell
def _(plt, simpoint):
fig11, ax11 = plt.subplots()
ax11.imshow(simpoint, cmap="gray")
return
@app.cell
def _(np):
def fishify(image, N=1, rng=np.random.default_rng()):
return rng.poisson(lam=N * (image / np.sum(image)))
return (fishify,)
@app.cell
def _(fishify, pixelate, psfker):
simpoint50 = fishify(pixelate(psfker(0.5, NA=0.9, side=15 * 0.1, N = 150), 0.1)[0], N=50)
simpoint500 = fishify(pixelate(psfker(0.5, NA=0.9, side=15 * 0.1, N = 150), 0.1)[0], N=500)
return simpoint50, simpoint500
@app.cell
def _(plt, simpoint50, simpoint500):
fig12, (ax12a, ax12b) = plt.subplots(1, 2, figsize=(8, 4))
ax12a.imshow(simpoint50, cmap="gray")
ax12b.imshow(simpoint500, cmap="gray")
return
@app.cell
def _(fishify, pixelate, psfker):
simpoint50_shifted = fishify(pixelate(psfker(0.5, NA=0.9, side=15 * 0.1, N = 150, center=(0.3, 0.3)), 0.1)[0], N=50)
simpoint500_shifted = fishify(pixelate(psfker(0.5, NA=0.9, side=15 * 0.1, N = 150, center=(0.3, 0.3)), 0.1)[0], N=500)
return simpoint500_shifted, simpoint50_shifted
@app.cell
def _(plt, simpoint500_shifted, simpoint50_shifted):
fig13, (ax13a, ax13b) = plt.subplots(1, 2, figsize=(8, 4))
ax13a.imshow(simpoint50_shifted, cmap="gray")
ax13b.imshow(simpoint500_shifted, cmap="gray")
return
@app.cell
def _(fishify, np, pixelate, psfker):
uniform = np.ones((15, 15)) / np.sum(np.ones((15, 15)))
simpoint_i = fishify(pixelate(psfker(0.5, NA=0.9, side=15 * 0.1, N = 150), 0.1)[0], N=50) + fishify(np.ones((15, 15)), N=2 * 15**2)
simpoint_ii = fishify(pixelate(psfker(0.5, NA=0.9, side=15 * 0.1, N = 150, center=(0.03, 0.03)), 0.1)[0], N=50) + fishify(np.ones((15, 15)), N=2 * 15**2)
simpoint_iii = fishify(pixelate(psfker(0.5, NA=0.9, side=15 * 0.1, N = 150, center=(0.03, 0.03)), 0.1)[0], N=500) + fishify(np.ones((15, 15)), N=2 * 15**2)
return simpoint_i, simpoint_ii, simpoint_iii
@app.cell
def _(plt, simpoint_i, simpoint_ii, simpoint_iii):
fig14, (ax14a, ax14b, ax14c) = plt.subplots(1, 3, figsize=(8, 2))
ax14a.imshow(simpoint_i, cmap="gray")
ax14b.imshow(simpoint_ii, cmap="gray")
ax14c.imshow(simpoint_iii, cmap="gray")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Simulating a Ring
""")
return
@app.cell
def _(np):
def ring(inner, outer, center=(0, 0), scale=1, shape=(150, 150), rtol=1e-02, atol=1e-02):
ii, jj = np.indices(shape)
r2s = np.square((ii - shape[0] / 2) * scale - center[0]) + np.square((jj - shape[1] / 2) * scale - center[1])
return ((r2s < np.square(outer)) & (r2s >= np.square(inner))).astype(np.float32)
return (ring,)
@app.cell
def _(fishify, nd, plt, psfker, ring):
fig15, (ax15a, ax15b, ax15c) = plt.subplots(1, 3, figsize=(8, 4))
ax15a.imshow(ring(0.5, 0.6, scale=0.01), cmap="gray")
ax15b.imshow(nd.convolve(ring(0.5, 0.6, scale=0.01), psfker(0.1), mode="nearest"), cmap="gray")
ax15c.imshow(fishify(nd.convolve(ring(0.5, 0.6, scale=0.01), psfker(0.1), mode="nearest"), N=10_000), cmap="gray")
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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import marimo
__generated_with = "0.19.11"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
return (mo,)
@app.cell
def _():
import numpy as np
rng = np.random.default_rng()
return np, rng
@app.cell
def _():
import scipy as si
return (si,)
@app.cell
def _():
import matplotlib
import matplotlib.pyplot as plt
plt.ion();
return (plt,)
@app.cell
def _(mo):
from pathlib import Path
mo.pdf(src=Path("Homework5.pdf"), width="100%", height="50vh")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## The Signal-to-Noise Ratio in Images
""")
return
@app.cell
def _(rng):
xs = rng.poisson(lam=200, size=1000 * 500).reshape(1000, 500)
xs.shape
return (xs,)
@app.cell
def _(np, xs):
np.mean(np.mean(xs, axis=0) / np.std(xs, axis=0))
return
@app.cell
def _(np):
As = np.logspace(-6, 6, 500)
As.shape
return (As,)
@app.cell
def _(As, np, xs):
np.mean(np.mean(As * xs, axis=0) / np.std(As * xs, axis=0))
return
@app.cell
def _(As, np, xs):
ras = np.mean(xs, axis=0) / np.std(xs, axis=0) - np.mean(As * xs, axis=0) / np.std(As * xs, axis=0)
np.mean(ras)
return (ras,)
@app.cell
def _(plt, ras):
fig, ax = plt.subplots()
ax.hist(ras, bins="auto")
fig
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
Zero! To within typical machine error.
""")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Centroid Warmup
""")
return
@app.cell
def _(np):
i = np.arange(0, 1000)
I = 0.2 * np.sqrt(i)
float(np.sum(i * I) / np.sum(I))
return (i,)
@app.cell
def _(i, np, rng):
J = 30 / (i + 20) + 0.05 * rng.poisson(lam=10, size=i.size)
float(np.sum(i * J) / np.sum(J))
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Centroid Localization
""")
return
@app.cell
def _(np, si):
def psfker(l, NA=0.9, side=1.0, N=210, center=(0.0, 0.0)):
xs, ys = np.meshgrid(np.linspace(- side / 2, side / 2, N),
np.linspace(- side / 2, side / 2, N))
r2s = np.square(xs - center[0]) + np.square(ys - center[1])
v = 2 * np.pi * NA * np.sqrt(r2s) / l
psf = 4 * np.square(si.special.j1(v) / v)
psf[np.isnan(psf)] = 1
scale = side / N
return psf / np.sum(psf), scale
return (psfker,)
@app.cell
def _(np):
def pixelate(image, inscale, shape=(7, 7)):
outscale = image.shape[0] * inscale / shape[0]
out = np.sum(image.reshape(shape[0], int(image.shape[0] / shape[0]),
shape[1], int(image.shape[1] / shape[1])),
axis=(1, 3))
return out, outscale
return (pixelate,)
@app.cell
def _(np):
def fishify(image, N=1, rng=np.random.default_rng()):
return rng.poisson(lam=N * (image / np.sum(image)))
return (fishify,)
@app.cell
def _(fishify, np, pixelate, psfker):
def sim(l=0.51, NA=0.9, side=0.7, center=(0.0, 0.0), Nphoton=500, Nfine=280, bgavg=10, shape=(7, 7)):
point, scale = psfker(l, NA=NA, side=side, N=Nfine, center=center)
pxpt, scale = pixelate(point, scale, shape=shape)
fg = fishify(pxpt, N=Nphoton)
bg = fishify(np.ones(shape), N=bgavg * np.prod(shape))
return fg + bg, scale
return (sim,)
@app.cell
def _(np):
def centroid(im, scale=None):
ys, xs = np.indices(im.shape)
c = np.hstack([np.sum(xs * im), np.sum(ys * im)]) / np.sum(im)
c = (im * np.mgrid[0:im.shape[0], 0:im.shape[1]]).sum(1).sum(1)/im.sum()
return c if scale is None else scale * (c - np.array(im.shape) // 2)
return (centroid,)
@app.cell
def _(np):
def rms(cs, center=(0.0, 0.0)):
return float(np.sqrt(np.mean(np.square(cs[:,0] - center[0]) + np.square(cs[:,1] - center[1]))))
return (rms,)
@app.cell
def _(centroid, np, sim):
sims1 = [sim(center=(0.0, 0.0)) for m in range(100)]
cs1 = np.array([centroid(s, scale=scale) for (s, scale) in sims1])
return cs1, sims1
@app.cell
def _(centroid, cs1, plt, sims1):
fig1, (ax1a, ax1b) = plt.subplots(1, 2, figsize=(8, 4))
ax1a.imshow(sims1[0][0], cmap="gray")
cx, cy = centroid(sims1[0][0])
ax1a.vlines(cx, 0, 6, color="red")
ax1a.hlines(cy, 0, 6, color="red")
ax1b.hist(cs1[:,0], bins="auto")
fig1.tight_layout()
fig1
return
@app.cell
def _(cs1, rms):
rms(cs1)
return
@app.cell
def _(centroid, np, rms, sim):
rmss = []
for n in np.logspace(0, 5, 15):
sims = [sim(Nphoton=n) for m in range(100)]
cs = np.array([centroid(s, scale=sc) for (s, sc) in sims])
rmss.append(rms(cs))
return (rmss,)
@app.cell
def _(np, plt, rmss):
fig2, ax2 = plt.subplots()
ax2.scatter(np.logspace(0, 5, 15), rmss)
ax2.loglog(np.logspace(0, 5, 10), 1 / np.sqrt(np.logspace(0, 5, 10)), color="orange")
ax2.set_aspect('equal', 'box')
fig2.tight_layout()
fig2
return
@app.cell
def _(centroid, np, sim):
sims3a = [sim(Nphoton=1000) for m in range(100)]
cs3a = np.array([centroid(s, scale=sc) for (s, sc) in sims3a])
sims3b = [sim(Nphoton=1000, center=(0.3, 0.0)) for m in range(100)]
cs3b = np.array([centroid(s, scale=sc) for (s, sc) in sims3b])
sims3c = [sim(Nphoton=1000, center=(-0.3, 0.0)) for m in range(100)]
cs3c = np.array([centroid(s, scale=sc) for (s, sc) in sims3c])
return cs3a, cs3b, cs3c
@app.cell
def _(cs3a, cs3b, cs3c, plt):
fig3, (ax3a, ax3b, ax3c) = plt.subplots(1, 3, figsize=(9, 3))
ax3a.hist(cs3a[:, 0] - 0.0, bins="auto")
ax3b.hist(cs3b[:, 0] - 0.3, bins="auto")
ax3c.hist(cs3c[:, 0] - (-0.3), bins="auto")
fig3.tight_layout()
fig3
return
@app.cell
def _(centroid, np, sim):
Dxs = []
for p in np.linspace(-7, 7, 10):
sms = [sim(Nphoton=1000) for m in range(100)]
Dxs.append(np.mean([centroid(s, scale=sc)[0] - p for (s, sc) in sms]))
return (Dxs,)
@app.cell
def _(Dxs, np, plt):
fig4, ax4 = plt.subplots()
ax4.scatter(np.linspace(-0.5, 0.5, 10), Dxs)
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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import marimo
__generated_with = "0.19.11"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
return (mo,)
@app.cell
def _():
import numpy as np
rng = np.random.default_rng()
return np, rng
@app.cell
def _():
import matplotlib
import matplotlib.pyplot as plt
plt.ion();
return (plt,)
@app.cell
def _():
from skimage import io
import scipy.ndimage as nd
return (io,)
@app.cell
def _():
import scipy as si
import scipy.optimize as sio
return si, sio
@app.cell
def _():
import timeit
return (timeit,)
@app.cell
def _(mo):
from pathlib import Path
mo.pdf(src=Path("Homework6.pdf"), width="100%", height="50vh")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Cilia and temporal filtering
""")
return
@app.cell
def _(io):
cilia_movie_crop = io.imread("cilia_movie_crop.tif", plugin="tifffile")
cilia_movie_crop_nframes = cilia_movie_crop.shape[0]
return cilia_movie_crop, cilia_movie_crop_nframes
@app.cell
def _(cilia_movie_crop_nframes, mo):
i = mo.ui.slider(0, cilia_movie_crop_nframes - 1, 1)
i
return (i,)
@app.cell
def _(cilia_movie_crop, i, plt):
figi, axi = plt.subplots()
axi.imshow(cilia_movie_crop[0,:,:], cmap="gray")
axi.imshow(cilia_movie_crop[i.value,:,:], cmap="gray")
return
@app.cell
def _(cilia_movie_crop, np):
cilia_movie_crop_med = np.median(cilia_movie_crop, axis=0)
return (cilia_movie_crop_med,)
@app.cell
def _(cilia_movie_crop, cilia_movie_crop_med, cilia_movie_crop_nframes, np):
cilia_movie_crop_mmed = cilia_movie_crop - np.tile(cilia_movie_crop_med, (cilia_movie_crop_nframes, 1, 1))
return (cilia_movie_crop_mmed,)
@app.cell
def _(cilia_movie_crop_nframes, mo):
ii = mo.ui.slider(0, cilia_movie_crop_nframes - 1, 1)
ii
return (ii,)
@app.cell
def _(cilia_movie_crop, cilia_movie_crop_mmed, ii, plt):
figii, axii = plt.subplots()
axii.imshow(cilia_movie_crop[0,:,:], cmap="gray")
axii.imshow(cilia_movie_crop_mmed[ii.value,:,:], cmap="gray")
return
@app.cell
def _(cilia_movie_crop_mmed, plt):
fig1, (ax1a, ax1b) = plt.subplots(2, 1)
ax1a.imshow(cilia_movie_crop_mmed[0,:,:], cmap="gray")
ax1b.hist(cilia_movie_crop_mmed.flatten(), bins=100) #, log=True)
fig1
return
@app.cell
def _(cilia_movie_crop_mmed):
cilia_imin = -15
cilia_imax = 15
cilia_movie_crop_mmed_scaled = 255 * (cilia_movie_crop_mmed - cilia_imin) / (cilia_imax - cilia_imin)
return (cilia_movie_crop_mmed_scaled,)
@app.cell
def _(cilia_movie_crop_nframes, mo):
iii = mo.ui.slider(0, cilia_movie_crop_nframes - 1, 1)
iii
return (iii,)
@app.cell
def _(cilia_movie_crop_mmed_scaled, iii, plt):
fig4, ax4 = plt.subplots()
ax4.imshow(cilia_movie_crop_mmed_scaled[0,:,:], cmap="gray")
ax4.imshow(cilia_movie_crop_mmed_scaled[iii.value,:,:], cmap="gray")
return
@app.cell
def _(cilia_movie_crop_mmed_scaled, np):
cilia_movie_crop_mmed_scaled_std = np.std(cilia_movie_crop_mmed_scaled, 0)
return (cilia_movie_crop_mmed_scaled_std,)
@app.cell
def _(cilia_movie_crop_mmed_scaled_std, plt):
fig5, ax5 = plt.subplots()
ax5.imshow(cilia_movie_crop_mmed_scaled_std, cmap="gray")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## MLE Practice
""")
return
@app.cell
def _(np):
def A(x0, b, x = np.linspace(-3, 4, 100)):
return 3 * np.power(np.abs(x - x0), b) + 4
return
@app.cell
def _(mo):
mo.md(r"""
### Images for \#3-\#4
""")
return
@app.cell
def _(np, si):
def airypsf(xy, l=0.51, NA=0.9, side=0.7, N=210):
center = xy
xs, ys = np.meshgrid(np.linspace(- side * (1 - 1/N) / 2, side * (1 - 1/N)/2, N),
np.linspace(- side * (1 - 1/N) / 2, side * (1 - 1/N)/2, N))
r2s = np.square(xs - center[0]) + np.square(ys - center[1])
v = 2 * np.pi * NA * np.sqrt(r2s) / l
psf = 4 * np.square(si.special.j1(v) / v)
nans = np.isnan(psf)
psf[nans] = 1
scale = side / N
return psf / np.sum(psf), scale
return (airypsf,)
@app.cell
def _(np):
def pixelate(image, inscale, shape=(7, 7)):
outscale = image.shape[0] * inscale / shape[0]
assert image.shape[0] / image.shape[1] == shape[0] / shape[1], "Aspect Ratio must be preserved!"
out = np.sum(image.reshape(shape[0], int(image.shape[0] / shape[0]),
shape[1], int(image.shape[1] / shape[1])),
axis=(1, 3))
return out, outscale
return (pixelate,)
@app.cell
def _(np):
def fishify(image, N=1, rng=np.random.default_rng()):
return rng.poisson(lam=N * (image / np.sum(image)))
return (fishify,)
@app.cell
def _(airypsf, fishify, np, pixelate):
def simage4(xc, yc, N=7, Np = 1000, B=10):
a, iscale = airypsf(np.array([xc, yc]))
p, scale = pixelate(a, iscale, shape=(N, N))
return fishify(p, Np) + fishify(np.ones((N, N)),N=(B * (N ** 2))), scale
return (simage4,)
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Centroid Localization Timing
""")
return
@app.cell
def _(np):
def centroid(im, scale=None):
ys, xs = np.indices(im.shape)
c = np.hstack([np.sum(xs * im), np.sum(ys * im)]) / np.sum(im)
c = (im * np.mgrid[0:im.shape[0], 0:im.shape[1]]).sum(1).sum(1)/im.sum()
return c if scale is None else scale * (c - np.array(im.shape) // 2)
return (centroid,)
@app.cell
def _(centroid, rng, simage4, timeit):
xys = list(zip(rng.uniform(-0.35, 0.35, 100), rng.uniform(-0.35, 0.35, 100)))
ims = [simage4(x, y)[0] for x, y in xys]
startt = timeit.default_timer()
cs = [centroid(i) for i in ims]
print(timeit.default_timer() - startt, "seconds")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Gaussian MLE for particle localization!
""")
return
@app.cell
def _(plt, simage4):
fig2, ax2 = plt.subplots()
im, sc = simage4(-0.08, 0.03)
ax2.imshow(im)
return (im,)
@app.cell
def _(airypsf, np, pixelate):
def objcam(params, im, l, NA, side):
x, y = params
p, s = airypsf(np.array([x, y]), l=l, NA=NA, side=side)
A, _ = pixelate(p, s, shape=im.shape)
mlogp = np.sum(A - im * np.log(A))
return mlogp
return (objcam,)
@app.cell
def _(np, objcam, sio):
def MLElocalize_knowcam(im, l=0.51, NA=0.9, side=0.7, guess=np.array([-0.05, 0.1])):
bnd = ((-side / 2, side / 2), (-side / 2, side / 2))
res = sio.minimize(objcam, guess, args=(im, l, NA, side), bounds= bnd)
return res
return (MLElocalize_knowcam,)
@app.cell
def _(MLElocalize_knowcam, im):
MLElocalize_knowcam(im)
return
@app.cell
def _(np):
def gausspsf(xc, yc, A0, s, B, N=210, side=0.7):
xs = np.linspace(- side * (1 - 1/N) / 2, side * (1 - 1/N) / 2, N)
ys = np.linspace(- side * (1 - 1/N) / 2, side * (1 - 1/N) / 2, N)
xx, yy = np.meshgrid(xs, ys)
g = A0 * np.exp(-(np.square(xx - xc) + np.square(yy - yc)) / (2.0 * np.square(s))) + B
return g, (side / N)
return (gausspsf,)
@app.cell
def _(gausspsf, pixelate, plt):
fig3, ax3 = plt.subplots()
im3, sc3 = gausspsf(0, 0, 0.02, 0.1, 1) # initial guess
im3p, _ = pixelate(im3, sc3, shape=(7, 7))
ax3.imshow(im3p)
return
@app.cell
def _(gausspsf, np):
def objgauss(params, im, side):
xc, yc, A0, s, B = params
p, sc = gausspsf(xc, yc, A0, s, B, side=side, N=im.shape[0])
#A, _ = pixelate(p, sc, shape=im.shape)
mlogp = np.sum(p - im * np.log(p))
#mlogp = np.sum(A - im * np.log(A))
return mlogp
return (objgauss,)
@app.cell
def _(np, objgauss, sio):
def MLElocalize_gauss(im, side=0.7, guess=None):
if guess is None:
guess = np.array([0, 0, np.max(im), 0.1, np.min(im)])
bnd = ((-side / 2, side / 2), (-side / 2, side / 2), (0, np.max(im)), (1e-2, None), (0, None))
res = sio.minimize(objgauss, guess, args = (im, side), bounds= bnd)
return res
return (MLElocalize_gauss,)
@app.cell
def _(MLElocalize_gauss, im):
res = MLElocalize_gauss(im)
res
return (res,)
@app.cell
def _(gausspsf, plt, res):
fig8, ax8 = plt.subplots()
im8, _ = gausspsf(*res.x, side=0.7, N=7)
ax8.imshow(im8)
return
@app.cell
def _(MLElocalize_gauss, simage4):
resx = []
for _ in range(100):
im9, sc9 = simage4(0.03, 0.03)
res9 = MLElocalize_gauss(im9)
resx.append(res9.x[0] - 0.03)
return (resx,)
@app.cell
def _(plt, resx):
figh, axh = plt.subplots()
axh.hist(resx, bins="auto")
figh
return
@app.cell
def _(MLElocalize_gauss, np, plt, simage4):
figs, axs = plt.subplots()
xs = np.linspace(-0.05, 0.05, 10)
ys = np.zeros(10)
imss = [simage4(xs[i], ys[i])[0] for i in range(10)]
es = [MLElocalize_gauss(image).x[0] for image in imss]
axs.scatter(xs, es - xs)
#axs.set_ylim([-0.5, 0.5])
return
@app.cell
def _(MLElocalize_gauss, np, plt, rng, simage4):
figr, axr = plt.subplots()
xss = rng.uniform(-0.5 * 0.1, 0.5 * 0.1, 100)
yss = rng.uniform(-0.5 * 0.1, 0.5 * 0.1, 100)
imsss = [simage4(xss[i], yss[i])[0] for i in range(100)]
ess = np.array([MLElocalize_gauss(image).x[0] for image in imsss])
axr.scatter(xss, ess - xss)
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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# -*- coding: utf-8 -*-
# radialcenter_ImAnClass.py
"""
Author: Raghuveer Parthasarathy
Created on Mon Oct 31 13:33:05 2022
Last modified on Mon Oct 31 13:33:05 2022
Description
-----------
Particle localization by radial symmetry
Python translation of MATLAB radialcenter.m
** Version for Image Analysis Class**
Same as radialcenter.py , but with sigma and meand2 outputs removed,
and output positions returned relative to image center.
Uses 0 indexing of positions (unlike MATLAB)
NOTE: *Does not* optimize for image stacks (like radialcenter_stk.m);
just single image
Copyright 2011-2022, Raghuveer Parthasarathy, The University of Oregon
Calculates the center of a 2D intensity distribution.
Method: Considers lines passing through each half-pixel point with slope
parallel to the gradient of the intensity at that point. Considers the
distance of closest approach between these lines and the coordinate
origin, and determines (analytically) the origin that minimizes the
weighted sum of these distances-squared.
Applies simple smoothing if size > 3x3
Inputs
I : 2D intensity distribution (i.e. a grayscale image)
Size need not be an odd number of pixels along each dimension
Outputs
xc, yc : the center of radial symmetry, px, relative to image center
Note that y increases with increasing row number (i.e. "downward")
To do:
- Test more (like MATLAB version)
- Faster grid creation than meshgrid? (like in MATLAB code)
see notes August 19-25, Sept. 9, Sept. 19-20 2011
Raghuveer Parthasarathy
The University of Oregon
August 21, 2011 (begun)
"""
import numpy as np # Will assume numpy is already imported as np !
def radialcenter(I):
# The main function -- see header comments for details
(Ny, Nx) = I.shape
# grid coordinates are -n:n, where Nx (or Ny) = 2*n+1
# grid midpoint coordinates are -n+0.5:n-0.5
xm, ym = np.meshgrid(np.arange(-(Nx-1)/2.0 + 0.5, (Nx-1)/2.0+0.5),
np.arange(-(Ny-1)/2.0 + 0.5, (Ny-1)/2.0+0.5))
# Calculate derivatives along 45-degree shifted coordinates (u and v)
# Note that y increases "downward" (increasing row number) -- we'll deal
# with this when calculating "m" below.
dIdu = I[0:Ny-1,1:]-I[1:,0:Nx-1]
dIdv = I[0:Ny-1,0:Nx-1]-I[1:,1:]
# Smoothing -- perhaps should be optional
fdu = dIdu # will overwrite if smoothing
fdv = dIdv
if np.min((Nx, Ny))>3:
# Only smooth if image is >3px in the smallest dimension
# Smooth by simple 3x3 boxcar, which I'll code directly rather than
# calling a convolution.
# Zero-pad (expand by 1 on each side)
dIdu_pad = np.zeros((Ny+1,Nx+1)) # dIdu array is size Ny-1, Nx-1
dIdv_pad = np.zeros((Ny+1,Nx+1)) # dIdv array is size Ny-1, Nx-1
dIdu_pad[1:Ny, 1:Nx] = dIdu
dIdv_pad[1:Ny, 1:Nx] = dIdv
fdu = np.zeros_like(dIdu)
fdv = np.zeros_like(dIdv)
for j in range(Ny-1):
for k in range(Nx-1):
fdu[j,k] = np.mean(dIdu_pad[j:j+3,k:k+3])
fdv[j,k] = np.mean(dIdv_pad[j:j+3,k:k+3])
dImag2 = fdu*fdu + fdv*fdv # gradient magnitude, squared
# Slope of the gradient . Note that we need a 45 degree rotation of
# the u,v components to express the slope in the x-y coordinate system.
# The negative sign "flips" the array to account for y increasing
# "downward"
m = -(fdv + fdu) / (fdu-fdv)
# Not smoothed version: m = -(dIdv + dIdu) ./ (dIdu-dIdv)
infslope = 9e9 #replace infinite slope values with this extremely large number
m[np.isinf(m)] = infslope
# Shorthand "b", which also happens to be the
# y intercept of the line of slope m that goes through each grid midpoint
b = ym - m*xm
# Weighting: weight by square of gradient magnitude and inverse
# distance to gradient intensity centroid.
sdI2 = np.sum(dImag2)
xcentroid = np.sum(dImag2*xm)/sdI2
ycentroid = np.sum(dImag2*ym)/sdI2
w = dImag2/np.sqrt((xm-xcentroid)*(xm-xcentroid) +
(ym-ycentroid)*(ym-ycentroid))
# if the intensity is completely flat, m will be NaN (0/0)
# give these points zero weight (and set m, b = 0 to avoid 0*NaN=NaN)
w[np.isnan(m)]=0
b[np.isnan(m)]=0
m[np.isnan(m)]=0
# least-squares minimization to determine the translated coordinate
# system origin (xc, yc) such that lines y = mx+b have
# the minimal total distance^2 to the origin:
# Unilke the MATLAB version, where I have a separate function
# for this (lsradialcenterfit), I'll just write the calculation here:
# Note m, b, w are defined on a grid; w are the weights for each point
wm2p1 = w/(m*m+1)
sw = np.sum(wm2p1)
smmw = np.sum(m*m*wm2p1)
smw = np.sum(m*wm2p1)
smbw = np.sum(m*b*wm2p1)
sbw = np.sum(b*wm2p1)
det = smw*smw - smmw*sw
xc = (smbw*sw - smw*sbw)/det # relative to image center
yc = (smbw*smw - smmw*sbw)/det # relative to image center
return xc, yc

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@ -0,0 +1,362 @@
import marimo
__generated_with = "0.19.11"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
return (mo,)
@app.cell
def _():
import numpy as np
rng = np.random.default_rng()
return np, rng
@app.cell
def _():
import matplotlib
import matplotlib.pyplot as plt
plt.ion();
return (plt,)
@app.cell
def _():
from skimage import io, restoration
import scipy.ndimage as nd
return io, nd, restoration
@app.cell
def _():
import scipy as si
import scipy.optimize as sio
return si, sio
@app.cell
def _():
import timeit
return
@app.cell
def _(mo):
from pathlib import Path
mo.pdf(src=Path("Homework7.pdf"), width="100%", height="50vh")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Gaussian MLE and number of photons
""")
return
@app.cell
def _(np, si):
def airypsf(xy, l=0.51, NA=0.9, side=0.7, N=210):
center = xy
xs, ys = np.meshgrid(np.linspace(- side * (1 - 1/N) / 2, side * (1 - 1/N)/2, N),
np.linspace(- side * (1 - 1/N) / 2, side * (1 - 1/N)/2, N))
r2s = np.square(xs - center[0]) + np.square(ys - center[1])
v = 2 * np.pi * NA * np.sqrt(r2s) / l
psf = 4 * np.square(si.special.j1(v) / v)
nans = np.isnan(psf)
psf[nans] = 1
scale = side / N
return psf / np.sum(psf), scale
return (airypsf,)
@app.cell
def _(np):
def pixelate(image, inscale, shape=(7, 7)):
outscale = image.shape[0] * inscale / shape[0]
assert image.shape[0] / image.shape[1] == shape[0] / shape[1], "Aspect Ratio must be preserved!"
out = np.sum(image.reshape(shape[0], int(image.shape[0] / shape[0]),
shape[1], int(image.shape[1] / shape[1])),
axis=(1, 3))
return out, outscale
return (pixelate,)
@app.cell
def _(np):
def fishify(image, N=1, rng=np.random.default_rng()):
return rng.poisson(lam=N * (image / np.sum(image)))
return (fishify,)
@app.cell
def _(airypsf, fishify, np, pixelate):
def simage4(xc, yc, N=7, Np = 1000, B=10):
a, iscale = airypsf(np.array([xc, yc]))
p, scale = pixelate(a, iscale, shape=(N, N))
return fishify(p, Np) + fishify(np.ones((N, N)),N=(B * (N ** 2))), scale
return (simage4,)
@app.cell
def _(np):
def gausspsf(xc, yc, A0, s, B, N=210, side=0.7):
xs = np.linspace(- side * (1 - 1/N) / 2, side * (1 - 1/N) / 2, N)
ys = np.linspace(- side * (1 - 1/N) / 2, side * (1 - 1/N) / 2, N)
xx, yy = np.meshgrid(xs, ys)
g = A0 * np.exp(-(np.square(xx - xc) + np.square(yy - yc)) / (2.0 * np.square(s))) + B
return g, (side / N)
return (gausspsf,)
@app.cell
def _(gausspsf, np):
def objgauss(params, im, side):
xc, yc, A0, s, B = params
p, sc = gausspsf(xc, yc, A0, s, B, side=side, N=im.shape[0])
#A, _ = pixelate(p, sc, shape=im.shape)
mlogp = np.sum(p - im * np.log(p))
#mlogp = np.sum(A - im * np.log(A))
return mlogp
return (objgauss,)
@app.cell
def _(np, objgauss, sio):
def MLElocalize_gauss(im, side=0.7, guess=None):
if guess is None:
guess = np.array([0, 0, np.max(im), 0.1, np.min(im)])
bnd = ((-side / 2, side / 2), (-side / 2, side / 2), (0, np.max(im)), (1e-2, None), (0, None))
res = sio.minimize(objgauss, guess, args = (im, side), bounds= bnd)
return res
return (MLElocalize_gauss,)
@app.cell
def _():
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
### a.
See solution from last week! Looks unbiased:
""")
return
@app.cell
def _(MLElocalize_gauss, np, plt, rng, simage4):
figr, axr = plt.subplots()
xs = rng.uniform(-0.5 * 0.1, 0.5 * 0.1, 100)
ys = rng.uniform(-0.5 * 0.1, 0.5 * 0.1, 100)
ims = [simage4(xs[i], ys[i])[0] for i in range(100)]
es = np.array([MLElocalize_gauss(image).x[0] for image in ims])
axr.scatter(xs, es - xs)
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
### b.
""")
return
@app.cell
def _(np):
def RMSE(xs, ts=None):
if ts is None:
ts = np.zeros_like(xs)
return np.sqrt(np.mean(np.square(xs - ts), axis=1))
return (RMSE,)
@app.cell
def _(MLElocalize_gauss, np, simage4):
Nps = np.logspace(1, 5, 30)
imss = [simage4(0, 0, Np=i)[0] for i in Nps]
ess = np.array([MLElocalize_gauss(image).x for image in imss])[:,0:2]
return Nps, ess
@app.cell
def _(Nps, RMSE, ess, np, plt):
fig2, ax2 = plt.subplots()
ax2.loglog(Nps, RMSE(ess))
ax2.loglog(Nps, 0.51 / 2 / 0.9 / np.sqrt(Nps)) # theoretical baseline
return
@app.cell
def _(mo):
mo.md(r"""
TODO: Need to RMSE over multiple samples for each Np, not just one like this, but trend is already looking on-point.
""")
return
@app.cell
def _(mo):
mo.md(r"""
## Radial-symmetry-based particle localization
TODO: Mostly running Prof. code.
""")
return
@app.cell
def _(mo):
mo.md(r"""
## Assessing Deconvolution
""")
return
@app.cell
def _(np):
def gausspsff(xc, yc, A0, s, B, N=210, side=0.7):
xs = np.linspace(- side * (1 - 1/N) / 2, side * (1 - 1/N) / 2, N)
ys = np.linspace(- side * (1 - 1/N) / 2, side * (1 - 1/N) / 2, N)
xx, yy = np.meshgrid(xs, ys)
g = A0 * np.exp(-(np.square(xx - xc) + np.square(yy - yc)) / (2.0 * np.square(s))) + B
return g / np.sum(g), (side / N)
return (gausspsff,)
@app.cell
def _(np):
def fishifyf(image, N=1, rng=np.random.default_rng()):
return rng.poisson(lam=N * (image / np.sum(image)))
return
@app.cell
def _(gausspsff, plt):
fig, ax = plt.subplots()
gpsf = gausspsff(0, 0, 1, 7, 0, 35, 35)[0]
gpsf2 = gausspsff(0, 0, 1, 5, 0, 35, 35)[0]
ax.imshow(gpsf)
return (gpsf,)
@app.cell
def _(io):
mouse_glial_cells_crop_png = io.imread("mouse_glial_cells_RBurdan_crop.png", as_gray=True)
return (mouse_glial_cells_crop_png,)
@app.cell
def _(mouse_glial_cells_crop_png, plt):
fig3, ax3 = plt.subplots()
ax3.imshow(mouse_glial_cells_crop_png, cmap="gray")
return
@app.cell
def _(gpsf, mouse_glial_cells_crop_png, nd):
mouse_glial_cells_crop_conv = nd.convolve(mouse_glial_cells_crop_png, gpsf, mode="constant")
return (mouse_glial_cells_crop_conv,)
@app.cell
def _(mouse_glial_cells_crop_conv, plt):
fig4, ax4 = plt.subplots()
ax4.imshow(mouse_glial_cells_crop_conv, cmap="gray")
return
@app.cell
def _(mouse_glial_cells_crop_conv, rng):
mouse_glial_cells_crop_fish = rng.poisson(mouse_glial_cells_crop_conv)
return (mouse_glial_cells_crop_fish,)
@app.cell
def _(mouse_glial_cells_crop_fish, plt):
fig5, ax5 = plt.subplots()
ax5.imshow(mouse_glial_cells_crop_fish, cmap="gray")
return
@app.cell
def _(gpsf, mouse_glial_cells_crop_fish, restoration):
mouse_glial_cells_crop_restored = restoration.richardson_lucy(mouse_glial_cells_crop_fish, gpsf, num_iter=20, clip=False)
return (mouse_glial_cells_crop_restored,)
@app.cell
def _(mouse_glial_cells_crop_restored, plt):
fig6, ax6 = plt.subplots()
ax6.imshow(mouse_glial_cells_crop_restored, cmap="gray")
return
@app.cell
def _(
gpsf,
mouse_glial_cells_crop_fish,
mouse_glial_cells_crop_png,
np,
restoration,
):
rmss = []
imsi = []
for i in range(1, 250, 10):
mouse_glial_cells_crop_restorei = restoration.richardson_lucy(mouse_glial_cells_crop_fish, gpsf, num_iter=i, clip=False)
mouse_glial_cells_crop_restorei = mouse_glial_cells_crop_restorei[35:-35, 35:-35]
mouse_glial_cells_crop_restorei -= np.min(mouse_glial_cells_crop_restorei)
mouse_glial_cells_crop_restorei *= (np.max(mouse_glial_cells_crop_png[35:-35, 35:-35]) - np.min(mouse_glial_cells_crop_png[35:-35, 35:-35])) / np.max(mouse_glial_cells_crop_restorei)
mouse_glial_cells_crop_restorei += np.min(mouse_glial_cells_crop_png[35:-35, 35:-35])
imsi.append(mouse_glial_cells_crop_restorei)
rms = np.sqrt(np.mean(np.square(mouse_glial_cells_crop_restorei - mouse_glial_cells_crop_png[35:-35, 35:-35])))
rmss.append(rms)
return imsi, rmss
@app.cell
def _(plt, rmss):
fig7, ax7 = plt.subplots()
ax7.scatter(range(1, 250, 10), rmss)
return
@app.cell
def _(imsi, np, plt, rmss):
fig8, ax8 = plt.subplots()
ax8.imshow(imsi[np.argmin(rmss)], cmap="gray")
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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@ -0,0 +1,88 @@
import marimo
__generated_with = "0.19.11"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
return (mo,)
@app.cell
def _():
import numpy as np
rng = np.random.default_rng()
return
@app.cell
def _():
import scipy as si
return
@app.cell
def _():
from skimage import io, morphology as mf
return io, mf
@app.cell
def _():
import matplotlib
import matplotlib.pyplot as plt
plt.ion();
return (plt,)
@app.cell
def _(mo):
from pathlib import Path
mo.pdf(src=Path("Homework8.pdf"), width="100%", height="50vh")
return
@app.cell(hide_code=True)
def _(mo):
mo.md(r"""
## Spot Removal
""")
return
@app.cell
def _(io, plt):
lichtenstein_imageduplicator_1963_png = io.imread("Lichtenstein_imageDuplicator_1963.png")
lichtenstein_imageduplicator_1963_gray = io.imread("Lichtenstein_imageDuplicator_1963_gray.png")
fig0, (ax0a, ax0b) = plt.subplots(1, 2)
ax0a.imshow(lichtenstein_imageduplicator_1963_png)
ax0b.imshow(lichtenstein_imageduplicator_1963_gray, cmap="gray")
return (lichtenstein_imageduplicator_1963_gray,)
@app.cell
def _(lichtenstein_imageduplicator_1963_gray, mf):
lichtenstein_imageduplicator_1963_close = mf.closing(lichtenstein_imageduplicator_1963_gray, mf.disk(4))
lichtenstein_imageduplicator_1963_close = mf.closing(lichtenstein_imageduplicator_1963_gray, mf.disk(2))
return (lichtenstein_imageduplicator_1963_close,)
@app.cell
def _(lichtenstein_imageduplicator_1963_close, plt):
fig1, ax1 = plt.subplots()
ax1.imshow(lichtenstein_imageduplicator_1963_close, cmap="gray")
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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