Update pl translations

ricktu288 · Nov 30, 2023 · 6642896 · 6642896
1 parent dc299f3
commit 6642896
Show file tree

Hide file tree

Showing 31 changed files with 636 additions and 6,576 deletions.
diff --git a/cn/gallery/index.html b/cn/gallery/index.html
@@ -563,7 +563,7 @@ <h2>其他</h2>
       <span id="language">语言：简体中文</span>
       <span class="caret"></span></button>
       <ul class="dropdown-menu">
-        <li><a href="https://phydemo.app/ray-optics/gallery/">English</a></li><li><a href="https://phydemo.app/ray-optics/pl/gallery/">polski <span style="color:gray">(98% 已翻译)</span></a></li><li><a href="https://phydemo.app/ray-optics/cn/gallery/">简体中文 <span style="color:gray">(100% 已翻译)</span></a></li><li><a href="https://phydemo.app/ray-optics/tw/gallery/">正體中文 <span style="color:gray">(100% 已翻译)</span></a></li>
+        <li><a href="https://phydemo.app/ray-optics/gallery/">English</a></li><li><a href="https://phydemo.app/ray-optics/pl/gallery/">polski <span style="color:gray">(100% 已翻译)</span></a></li><li><a href="https://phydemo.app/ray-optics/cn/gallery/">简体中文 <span style="color:gray">(100% 已翻译)</span></a></li><li><a href="https://phydemo.app/ray-optics/tw/gallery/">正體中文 <span style="color:gray">(100% 已翻译)</span></a></li>
       </ul>
     </div>
   </div>

diff --git a/cn/gallery/logarithmic-spiral-lens.html b/cn/gallery/logarithmic-spiral-lens.html
@@ -13,6 +13,7 @@
 <meta property="og:locale" content="zh-CN">
 <link rel="canonical" href="https://phydemo.app/ray-optics/cn/gallery/logarithmic-spiral-lens">
 <link rel="alternate" href="https://phydemo.app/ray-optics/gallery/logarithmic-spiral-lens" hreflang="en">
+<link rel="alternate" href="https://phydemo.app/ray-optics/pl/gallery/logarithmic-spiral-lens" hreflang="pl">
 <link rel="alternate" href="https://phydemo.app/ray-optics/cn/gallery/logarithmic-spiral-lens" hreflang="zh-CN">
 <link rel="alternate" href="https://phydemo.app/ray-optics/tw/gallery/logarithmic-spiral-lens" hreflang="zh-TW">
 
@@ -59,7 +60,7 @@ <h1><b><span>等角螺线形的光线路径</span></b></h1>
       <span id="language">语言：简体中文</span>
       <span class="caret"></span></button>
       <ul class="dropdown-menu">
-        <li><a href="https://phydemo.app/ray-optics/gallery/logarithmic-spiral-lens">English</a></li><li><a href="https://phydemo.app/ray-optics/cn/gallery/logarithmic-spiral-lens">简体中文</a></li><li><a href="https://phydemo.app/ray-optics/tw/gallery/logarithmic-spiral-lens">正體中文</a></li>
+        <li><a href="https://phydemo.app/ray-optics/gallery/logarithmic-spiral-lens">English</a></li><li><a href="https://phydemo.app/ray-optics/pl/gallery/logarithmic-spiral-lens">polski</a></li><li><a href="https://phydemo.app/ray-optics/cn/gallery/logarithmic-spiral-lens">简体中文</a></li><li><a href="https://phydemo.app/ray-optics/tw/gallery/logarithmic-spiral-lens">正體中文</a></li>
       </ul>
     </div>
   </div>

diff --git a/gallery/GRIN-slab.html b/gallery/GRIN-slab.html
@@ -45,7 +45,7 @@ <h1><b><span>GRIN slab</span></b></h1>
 Contributor: Stas Fainer
 </p>
 <div class="description">
-<p>This is a simulation of a rectangular dielectric material with a refractive index \(n(\rho) = n_0 \sqrt{1-(\alpha \rho)^2}\), where \(n_0=2\) is the refractive index on its central axis and \(\rho \) is the radial distance from its central axis, such that \(\alpha=\frac{\sqrt{3}}{2R} \) where \(R=100 \) is its radius.<br>The top dielectric in this simulation is made of thin dielectric rectangles of constant refractive index, according to \(n(\rho)\) (the script for creating this dialectric is available <a href="https://phydemo.app/ray-optics/gallery/GRIN-slab.py" target="_blank">here</a>), while the bottom dielectric is a gradient-index material with the refractive index \(n(\rho)\).</p>
+<p>This is a simulation of a rectangular dielectric material with a refractive index \(n(\rho) = n_0 \sqrt{1-(\alpha \rho)^2}\), where \(n_0=2\) is the refractive index on its central axis and \(\rho \) is the radial distance from its central axis, such that \(\alpha=\frac{\sqrt{3}}{2R} \) where \(R=100 \) is its radius.<br>The top dielectric in this simulation is made of thin dielectric rectangles of constant refractive index, according to \(n(\rho)\) (the script for creating this dielectric is available <a href="https://phydemo.app/ray-optics/gallery/GRIN-slab.py" target="_blank">here</a>), while the bottom dielectric is a gradient-index material with the refractive index \(n(\rho)\).</p>
 </div>
 <p>
 <a href="https://phydemo.app/ray-optics/simulator/#GRIN-slab" target="_blank" class="btn btn-success btn-lg">Open in Simulator</a>

diff --git a/gallery/data.json b/gallery/data.json
@@ -342,7 +342,7 @@
           "Stas Fainer"
         ],
         "title": "GRIN slab",
-        "description": "<p>This is a simulation of a rectangular dielectric material with a refractive index \\(n(\\rho) = n_0 \\sqrt{1-(\\alpha \\rho)^2}\\), where \\(n_0=2\\) is the refractive index on its central axis and \\(\\rho \\) is the radial distance from its central axis, such that \\(\\alpha=\\frac{\\sqrt{3}}{2R} \\) where \\(R=100 \\) is its radius.<br>The top dielectric in this simulation is made of thin dielectric rectangles of constant refractive index, according to \\(n(\\rho)\\) (the script for creating this dialectric is available <a href=\"https://phydemo.app/ray-optics/gallery/GRIN-slab.py\" target=\"_blank\">here</a>), while the bottom dielectric is a gradient-index material with the refractive index \\(n(\\rho)\\).</p>"
+        "description": "<p>This is a simulation of a rectangular dielectric material with a refractive index \\(n(\\rho) = n_0 \\sqrt{1-(\\alpha \\rho)^2}\\), where \\(n_0=2\\) is the refractive index on its central axis and \\(\\rho \\) is the radial distance from its central axis, such that \\(\\alpha=\\frac{\\sqrt{3}}{2R} \\) where \\(R=100 \\) is its radius.<br>The top dielectric in this simulation is made of thin dielectric rectangles of constant refractive index, according to \\(n(\\rho)\\) (the script for creating this dielectric is available <a href=\"https://phydemo.app/ray-optics/gallery/GRIN-slab.py\" target=\"_blank\">here</a>), while the bottom dielectric is a gradient-index material with the refractive index \\(n(\\rho)\\).</p>"
       },
       {
         "id": "inferior-mirage",

diff --git a/gallery/index.html b/gallery/index.html
@@ -564,7 +564,7 @@ <h2>Miscellaneous</h2>
       <span id="language">Language: English</span>
       <span class="caret"></span></button>
       <ul class="dropdown-menu">
-        <li><a href="https://phydemo.app/ray-optics/gallery/">English</a></li><li><a href="https://phydemo.app/ray-optics/pl/gallery/">polski <span style="color:gray">(98% translated)</span></a></li><li><a href="https://phydemo.app/ray-optics/cn/gallery/">简体中文 <span style="color:gray">(100% translated)</span></a></li><li><a href="https://phydemo.app/ray-optics/tw/gallery/">正體中文 <span style="color:gray">(100% translated)</span></a></li>
+        <li><a href="https://phydemo.app/ray-optics/gallery/">English</a></li><li><a href="https://phydemo.app/ray-optics/pl/gallery/">polski <span style="color:gray">(100% translated)</span></a></li><li><a href="https://phydemo.app/ray-optics/cn/gallery/">简体中文 <span style="color:gray">(100% translated)</span></a></li><li><a href="https://phydemo.app/ray-optics/tw/gallery/">正體中文 <span style="color:gray">(100% translated)</span></a></li>
       </ul>
     </div>
   </div>

diff --git a/gallery/logarithmic-spiral-lens.html b/gallery/logarithmic-spiral-lens.html
@@ -13,6 +13,7 @@
 <meta property="og:locale" content="en">
 <link rel="canonical" href="https://phydemo.app/ray-optics/gallery/logarithmic-spiral-lens">
 <link rel="alternate" href="https://phydemo.app/ray-optics/gallery/logarithmic-spiral-lens" hreflang="en">
+<link rel="alternate" href="https://phydemo.app/ray-optics/pl/gallery/logarithmic-spiral-lens" hreflang="pl">
 <link rel="alternate" href="https://phydemo.app/ray-optics/cn/gallery/logarithmic-spiral-lens" hreflang="zh-CN">
 <link rel="alternate" href="https://phydemo.app/ray-optics/tw/gallery/logarithmic-spiral-lens" hreflang="zh-TW">
 
@@ -58,7 +59,7 @@ <h1><b><span>Logarithmic spiral ray path</span></b></h1>
       <span id="language">Language: English</span>
       <span class="caret"></span></button>
       <ul class="dropdown-menu">
-        <li><a href="https://phydemo.app/ray-optics/gallery/logarithmic-spiral-lens">English</a></li><li><a href="https://phydemo.app/ray-optics/cn/gallery/logarithmic-spiral-lens">简体中文</a></li><li><a href="https://phydemo.app/ray-optics/tw/gallery/logarithmic-spiral-lens">正體中文</a></li>
+        <li><a href="https://phydemo.app/ray-optics/gallery/logarithmic-spiral-lens">English</a></li><li><a href="https://phydemo.app/ray-optics/pl/gallery/logarithmic-spiral-lens">polski</a></li><li><a href="https://phydemo.app/ray-optics/cn/gallery/logarithmic-spiral-lens">简体中文</a></li><li><a href="https://phydemo.app/ray-optics/tw/gallery/logarithmic-spiral-lens">正體中文</a></li>
       </ul>
     </div>
   </div>

diff --git a/pl/gallery/GRIN-slab-thumbnail.png b/pl/gallery/GRIN-slab-thumbnail.png
diff --git a/pl/gallery/GRIN-slab.html b/pl/gallery/GRIN-slab.html
@@ -45,7 +45,7 @@ <h1><b><span>Płyta GRIN (gradientowa)</span></b></h1>
 Osoba wnosząca wkład: Stas Fainer
 </p>
 <div class="description">
-<p>Jest to symulacja materiału dielektrycznego o współczynniku załamania światła \(n(\rho) = n_0 \sqrt{1-(\alpha \rho)^2}\), gdzie \(n_0\) jest współczynnikiem załamania światła na jego osi centralnej, a \(\rho \) jest odległością radialną od jego osi centralnej, taką, że \(\alpha=\frac{\sqrt{3}}{2R} \), gdzie \(R=100 \) jest jego promieniem. Zauważ, że dielektryk w tej symulacji składa się z cienkich prostokątów dielektryka o stałym współczynniku załamania światła, zgodnie z poprzednim równaniem dla \(n(\rho)\).</p>
+<p>Jest to symulacja prostokątnego materiału dielektrycznego o współczynniku załamania \(n(ho) = n_0 \sqrt{1-(\alpha \rho)^2}\), gdzie \(n_0=2\) jest współczynnikiem załamania światła na jego osi centralnej, a \(\rho \)  jest odległością radialną od jego osi centralnej, taką, że \(\alpha=\frac{\sqrt{3}}{2R} \), gdzie \(R=100 \) jest jego promieniem.<br>Górny dielektryk w tej symulacji składa się z cienkich prostokątów dielektrycznych o stałym współczynniku załamania światła, zgodnie z \(n(\rho)\) (skrypt do tworzenia tego dielektryka jest dostępny <a href="https://phydemo.app/ray-optics/gallery/GRIN-slab.py" target="_blank">tutaj</a>), podczas gdy dolny dielektryk jest materiałem gradientowym o współczynniku załamania \(n(ho)\).</p>
 </div>
 <p>
 <a href="https://phydemo.app/ray-optics/simulator/?pl#../pl/gallery/GRIN-slab" target="_blank" class="btn btn-success btn-lg">Otwórz w symulatorze</a>