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Updated CI and Docs deployment.

This commit is contained in:
Nicolas 2025-08-01 14:05:31 +02:00
parent 1e7e7bfead
commit cb563a2df5
15 changed files with 65 additions and 5864 deletions
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58
.github/workflows/ci.yml vendored
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@ -138,3 +138,61 @@ jobs:
with:
name: rendering-results-windows
path: tests/out/test_*_render*.pdf
build-docs:
needs: build-ubuntu
runs-on: ubuntu-latest
steps:
- uses: actions/checkout@v4
- name: Download rendering outputs
uses: actions/download-artifact@v4
with:
name: rendering-results-ubuntu
path: build/html/files/
- name: Set up Python
uses: actions/setup-python@v3
with:
python-version: "3.x"
- name: Install package and dependencies
run: pip install .[doc_build]
- name: Generate Class List
run: python ./docs/source/generate_class_list.py
- name: Build Docs
run: |
mkdir -p docs/source/media
cp media/* docs/source/media/
mkdir -p docs/source/tests
cp tests/test_rendering_example*.py docs/source/tests/
cp LICENSE docs/source/LICENSE.md
cd docs
sphinx-apidoc -o source/ ../src/ -M --no-toc
rm ./source/*.rst
make html
touch ./build/html/.nojekyll
mkdir -p ./build/html/_autogenerated
cp ./build/html/api/* ./build/html/_autogenerated/
- name: Upload artifact
uses: actions/upload-pages-artifact@v3
with:
path: docs/build/html
deploy:
needs: build-docs
runs-on: ubuntu-latest
permissions:
contents: read
pages: write
id-token: write
environment:
name: github-pages
url: ${{ steps.deployment.outputs.page_url }}
steps:
- name: Deploy to GitHub Pages
id: deployment
uses: actions/deploy-pages@v4

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.github/workflows/docs.yml vendored
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@ -1,56 +0,0 @@
name: Build and Deploy Docs
on:
push:
branches:
- main
permissions:
contents: write
jobs:
build:
runs-on: ubuntu-latest
steps:
- uses: actions/checkout@v4
- name: Set up Python
uses: actions/setup-python@v3
with:
python-version: "3.x"
- name: Install package and dependencies
run: pip install .[doc_build]
- name: Generate Class List
run: python ./docs/source/generate_class_list.py
- name: Build Docs
run: |
mkdir -p docs/source/media
cp media/* docs/source/media/
mkdir -p docs/source/tests
cp tests/test_rendering_example*.py docs/source/tests/
cp LICENSE docs/source/LICENSE.md
cd docs
sphinx-apidoc -o source/ ../src/ -M --no-toc
rm ./source/*.rst
make html
touch ./build/html/.nojekyll
mkdir -p ./build/html/_autogenerated
cp ./build/html/api/* ./build/html/_autogenerated/
- name: Upload artifact
uses: actions/upload-pages-artifact@v3
with:
path: docs/build/html
deploy:
needs: build
runs-on: ubuntu-latest
permissions:
contents: read
pages: write
id-token: write
environment:
name: github-pages
url: ${{ steps.deployment.outputs.page_url }}
steps:
- name: Deploy to GitHub Pages
id: deployment
uses: actions/deploy-pages@v4

1
.gitignore vendored
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@ -133,3 +133,4 @@ pyModbusTCP_old/
test.py
test_*.ipynb
settings.json
tests/out/test*

6
README.md
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@ -21,10 +21,10 @@ is a hard problem where LaTeX is superior.
## Example outputs
[![example output](media/output_example.png)](https://raw.githubusercontent.com/Nonannet/pyladoc/refs/heads/main/tests/out/test_latex_render1.pdf)
[![example output](media/output_example.png)](https://nonannet.github.io/pyladoc/files/test_latex_render1.pdf)
- HTML: [test_html_render1.html](https://html-preview.github.io/?url=https://github.com/Nonannet/pyladoc/blob/main/tests/out/test_html_render1.html) ([code](https://github.com/Nonannet/pyladoc/blob/main/tests/out/test_html_render1.html))
- PDF: [test_latex_render1.pdf](https://raw.githubusercontent.com/Nonannet/pyladoc/refs/heads/main/tests/out/test_latex_render1.pdf) ([code](https://github.com/Nonannet/pyladoc/blob/main/tests/out/test_html_render1.tex))
- HTML: [test_html_render1.html](https://nonannet.github.io/pyladoc/files/test_html_render1.html)
- PDF: [test_latex_render1.pdf](https://nonannet.github.io/pyladoc/files/test_latex_render1.pdf) ([LaTeX](https://nonannet.github.io/pyladoc/files/test_html_render1.tex))
The documents are generated by the script [tests/test_rendering_example1_doc.py](tests/test_rendering_example1_doc.py).

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tests/out/README.md Normal file
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@ -0,0 +1,3 @@
# Rendering Test Outputs
This is the target directory for the test renderings.

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tests/out/test_html_render1.tex
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@ -1,609 +0,0 @@
\section{Thermal Conductivity of Mixtures}
The determination of the thermal conductivity of gas mixtures is a central aspect of modeling
transport phenomena, particularly in high-temperature and high-pressure processes. Among the
most established approaches is the empirical equation introduced by Wassiljewa, which was
subsequently refined by Mason and Saxena to improve its applicability to multicomponent systems.
This model offers a reliable means of estimating the thermal conductivity of gas mixtures based
on the properties of the pure components and their molar interactions.
The thermal conductivity of a gas mixture, denoted by \(\lambda_{\text{mix}}\), can expressed as
shown in equation \ref{eq:lambda-mixture}.\begin{equation}\label{eq:lambda-mixture}\lambda_{ ext{mix}} = \sum_{i=1}^{n} \frac{x_i \lambda_i}{\sum_{j=1}^{n} x_j \Phi_{ij}}\end{equation}In this equation, \(x_i\) represents the molar fraction of component \(i\) within the mixture,
while \(\lambda_i\) denotes the thermal conductivity of the pure substance \(i\). The denominator
contains the interaction parameter \(\Phi_{ij}\), which describes the influence of component
\(j\) on the transport properties of component \(i\).
The interaction parameter \(\Phi_{ij}\) is given by the relation shown in equation \ref{eq:interaction-parameter}.\begin{equation}\label{eq:interaction-parameter}\Phi_{ij} = \frac{1}{\sqrt{8}} \left(1 + \frac{M_i}{M_j} \right)^{-1/2} \left[ 1 + \left( \frac{\lambda_i}{\lambda_j} \right)^{1/2} \left( \frac{M_j}{M_i} \right)^{1/4} \right]^2\end{equation}Here, \(M_i\) and \(M_j\) are the molar masses of the components \(i\) and \(j\), respectively.
Molar masses and thermal conductivity of the pure substances are listed in table \ref{table:gas-probs}.
The structure of this expression illustrates the nonlinear dependence of the interaction term on
both the molar mass ratio and the square root of the conductivity ratio of the involved species.
\begin{table}
\centering
\caption{Properties of some gases}
\label{table:gas-probs}
\begin{tabular}{lSS}
\toprule
\text{Gas} & \text{Molar mass in g/mol} & \text{Thermal conductivity in W/m/K} \\
\midrule
H2 & 2.016 & 0.1805 \\
O2 & 32.00 & 0.0263 \\
N2 & 28.02 & 0.0258 \\
CO2 & 44.01 & 0.0166 \\
CH4 & 16.04 & 0.0341 \\
Ar & 39.95 & 0.0177 \\
He & 4.0026 & 0.1513 \\
\bottomrule
\end{tabular}
\end{table}This formulation acknowledges that the transport properties of a gas mixture are not a simple
linear combination of the individual conductivities. Rather, they are governed by intermolecular
interactions, which affect the energy exchange and diffusion behavior of each component. These
interactions are particularly significant at elevated pressures or in cases where the gas components
exhibit widely differing molecular masses or transport properties.
The equation proposed by Wassiljewa and refined by Mason and Saxena assumes that binary interactions
dominate the behavior of the mixture, while higher-order (three-body or more) interactions are
neglected. It also presumes that the gases approximate ideal behavior, although in practical
applications, moderate deviations from ideality are tolerated without significant loss of accuracy.
In figure \ref{fig:mixture} the resulting thermal conductivity of an H2/CO2-mixture is shown.
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\caption{Thermal Conductivity of H2/CO2 mixtures}
\label{fig:mixture}
\end{figure}In engineering practice, the accurate determination of \(\lambda_{\text{mix}}\) is essential
for the prediction of heat transfer in systems such as membrane modules, chemical reactors, and
combustion chambers. In the context of membrane-based gas separation, for instance, the thermal
conductivity of the gas mixture influences the local temperature distribution, which in turn affects
both the permeation behavior and the structural stability of the membrane.
It is important to note that the calculated mixture conductivity reflects only the gas phase
behavior. In porous systems such as carbon membranes, additional effects must be considered.
These include the solid-phase thermal conduction through the membrane matrix, radiative transport
in pore channels at high temperatures, and transport in the Knudsen regime for narrow pores.
To account for these complexities, models based on effective medium theory, such as those of
Maxwell-Eucken or Bruggeman, are frequently employed. These models combine the conductivities of
individual phases (gas and solid) with geometrical factors that reflect the morphology of the
porous structure.
\noindent\rule[0.5ex]{\linewidth}{1pt}
Expanded by more or less sensible AI jabbering; based on: \href{https://doi.org/10.14279/depositonce-7390}{doi:10.14279/depositonce-7390}

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tests/out/test_html_render2.html
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tests/out/test_html_render2.tex
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@ -1,589 +0,0 @@
\section{Special characters}
{\"o} {\"a} {\"u} {\"O} {\"A} {\"U} {\ss} @ $\Delta$
$\pi$ $\approx$ $\pm$ $\Delta$ $\Sigma$
{\pounds} {\yen} \$ €
{\OE}
\section{Link}
This is a hyperlink: \href{https://www.nonan.net}{nonan.net}
\section{Table}
\begin{tabular}{rll}\toprule
Anz. & Typ & Beschreibung \\
\midrule
12 & BK9050 & Buskoppler \\
2 & KL1104 & 4 Digitaleing{\"a}nge \\
2 & KL2404 & 4 Digitalausg{\"a}nge (0,5 A) \\
3 & KL2424 & 4 Digitalausg{\"a}nge (2 A) \\
2 & KL4004 & 4 Analogausg{\"a}nge \\
1 & KL4002 & 2 Analogausg{\"a}nge \\
22 & KL9188 & Potenzialverteilungsklemme \\
1 & KL9100 & Potenzialeinspeiseklemme \\
3 & KL3054 & 4 Analogeing{\"a}nge \\
5 & KL3214 & PT100 4 Temperatureing{\"a}nge (3-Leiter) \\
3 & KL3202 & PT100 2 Temperatureing{\"a}nge (3-Leiter) \\
1 & KL2404 & 4 Digitalausg{\"a}nge \\
2 & KL9010 & Endklemme \\
\bottomrule
\end{tabular}
\noindent\rule[0.5ex]{\linewidth}{1pt}
\section{Equations}
This line represents a reference to the equation \ref{eq:test1}.
\begin{equation}\label{eq:test1}y = a + b * \sum_{i=0}^{\infty} a_i x^i\end{equation}\begin{figure}
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\makeatother%
\endgroup%
\caption{Bar chart with individual bar colors}
\end{figure}\begin{table}
\centering
\caption{This is a example table}
\label{table:example1}
\begin{tabular}{lSSSSSS}
\toprule
\text{Row1} & \text{Row2} & \text{Row3} & \text{Row4} & \text{Row5} & \text{Row6} & \text{Row7} \\
\midrule
Line1 & 120 & 12 g/km & 5 stars & 3.500000 & 1850 kg & 600 Nm \\
Line2 & 95 km/h & {\textgreater} 150 g/km & 4 stars & 7.800000 & 150 kg & 250 Nm \\
Line3 & 110 & -110 g/km & 5 stars & 8.500000 & 140 kg & 280,8 Nm \\
Line4 & 105 km/h & 1140 g/km & 4.5 stars & 6.900000 & 1600 kg & 320 Nm \\
Line5 & 130 & -13.05 g/km & 5 stars & 4.200000 & 17.55 kg & 450 Nm \\
\bottomrule
\end{tabular}
\end{table}

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tests/out/test_markdown_characters.html
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<h1>Special caracters</h1>
<p>Umlaute: ÖÄÜ öäü</p>
<p>Other: ß, €, @, $, %, ~, µ</p>
<p>Units: m³, cm²</p>
<p>Controll characters: <, >, ", ', &, |, /, \</p>

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tests/out/test_markdown_equations.html
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<h1>Source Equations</h1>
<ol>
<li>$4(3x + 2) - 5(x - 1) = 3x + 14$</li>
<li>$
rac{2y + 5}{4} +
rac{3y - 1}{2} = 5$</li>
<li>$
rac{5}{x + 2} +
rac{2}{x - 2} = 3$</li>
<li>$8(3b - 5) + 4(b + 2) = 60$</li>
<li>$2c^2 - 3c - 5 = 0$</li>
<li>$4(2d - 1) + 5(3d + 2) = 7d + 28$</li>
<li>$q^2 + 6q + 9 = 16$</li>
</ol>
<h1>Result Equations</h1>
<ol>
<li>$x =
rac{1}{4}$</li>
<li>$y =
rac{17}{8}$</li>
<li>$z =
rac{7}{3}$</li>
<li>$x = 1$ or $x = -6$</li>
<li>$a =
rac{1}{3}$ or $a = 2$</li>
<li>$x = -
rac{2}{3}$ or $x = 3$</li>
<li>$b =
rac{23}{7}$</li>
</ol>
<h1>Step by Step</h1>
<ol>
<li>Distribute: $12x + 8 - 5x + 5 = 3x + 14$</li>
<li>Combine like terms: $7x + 13 = 3x + 14$</li>
<li>Subtract $3x$: $4x + 13 = 14$</li>
<li>Subtract $13$: $4x = 1$</li>
<li>Divide by $4$: $x =
rac{1}{4}$</li>
</ol>

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<p>Below is an in-depth explanation of the AArch64 (ARM64)
unconditional branch instruction—often simply called the
“B” instruction—and how its 26‐bit immediate field (imm26)
is laid out and later relocated during linking.</p>
<hr>
<h2>Instruction Layout</h2>
<p>The unconditional branch in AArch64 is encoded in a 32‑bit
instruction. Its layout is as follows:</p>
<pre><code>Bits: 31 26 25 0
+-------------+------------------------------+
| Opcode | imm26 |
+-------------+------------------------------+
</code></pre>
<ul>
<li><strong>Opcode (bits 31:26):</strong></li>
<li>For a plain branch (<code>B</code>), the opcode is <code>000101</code>.</li>
<li>
<p>For a branch with link (<code>BL</code>), which saves the return
address (i.e., a call), the opcode is <code>100101</code>.
These 6 bits determine the instruction type.</p>
</li>
<li>
<p><strong>Immediate Field (imm26, bits 25:0):</strong></p>
</li>
<li>This 26‑bit field holds a signed immediate value.</li>
<li>
<p><strong>Offset Calculation:</strong> At runtime, the processor:</p>
<ol>
<li><strong>Shifts</strong> the 26‑bit immediate left by 2 bits.
(Because instructions are 4-byte aligned,
the two least-significant bits are always zero.)</li>
<li><strong>Sign-extends</strong> the resulting 28‑bit value to
the full register width (typically 64 bits).</li>
<li><strong>Adds</strong> this value to the program counter
(PC) to obtain the branch target.</li>
</ol>
</li>
<li>
<p><strong>Reach:</strong></p>
</li>
<li>With a 26‑bit signed field that’s effectively 28 bits
after the shift, the branch can cover a range
of approximately ±128 MB from the current instruction.</li>
</ul>

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<h2>Klemmen</h2>
<table>
<thead>
<tr>
<th style="text-align: right;">Anz.</th>
<th>Typ</th>
<th>Beschreibung</th>
</tr>
</thead>
<tbody>
<tr>
<td style="text-align: right;">12</td>
<td>BK9050</td>
<td>Buskoppler</td>
</tr>
<tr>
<td style="text-align: right;">2</td>
<td>KL1104</td>
<td>4 Digitaleingänge</td>
</tr>
<tr>
<td style="text-align: right;">2</td>
<td>KL2404</td>
<td>4 Digitalausgänge (0,5 A)</td>
</tr>
<tr>
<td style="text-align: right;">3</td>
<td>KL2424</td>
<td>4 Digitalausgänge (2 A)</td>
</tr>
<tr>
<td style="text-align: right;">2</td>
<td>KL4004</td>
<td>4 Analogausgänge</td>
</tr>
<tr>
<td style="text-align: right;">1</td>
<td>KL4002</td>
<td>2 Analogausgänge</td>
</tr>
<tr>
<td style="text-align: right;">22</td>
<td>KL9188</td>
<td>Potenzialverteilungsklemme</td>
</tr>
<tr>
<td style="text-align: right;">1</td>
<td>KL9100</td>
<td>Potenzialeinspeiseklemme</td>
</tr>
<tr>
<td style="text-align: right;">3</td>
<td>KL3054</td>
<td>4 Analogeingänge</td>
</tr>
<tr>
<td style="text-align: right;">5</td>
<td>KL3214</td>
<td>PT100 4 Temperatureingänge (3-Leiter)</td>
</tr>
<tr>
<td style="text-align: right;">3</td>
<td>KL3202</td>
<td>PT100 2 Temperatureingänge (3-Leiter)</td>
</tr>
<tr>
<td style="text-align: right;">1</td>
<td>KL2404</td>
<td>4 Digitalausgänge</td>
</tr>
<tr>
<td style="text-align: right;">2</td>
<td>KL9010</td>
<td>Endklemme</td>
</tr>
</tbody>
</table>