Used html instead of haml

friedrich · Apr 10, 2013 · 34e295e · 34e295e
1 parent add0c04
commit 34e295e
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Showing 5 changed files with 111 additions and 39 deletions.
diff --git a/Gruntfile.coffee b/Gruntfile.coffee
@@ -16,6 +16,7 @@ module.exports = (grunt) ->
 	grunt.loadNpmTasks("grunt-contrib-connect")
 	grunt.loadNpmTasks("grunt-contrib-livereload")
 	grunt.loadNpmTasks("grunt-regarde")
+	grunt.loadNpmTasks("grunt-contrib-copy")
 	# grunt.loadNpmTasks("grunt-contrib-uglify")
 
 	grunt.initConfig
@@ -42,6 +43,12 @@ module.exports = (grunt) ->
 						path.replace(/^src\//, "build/").replace(/\.haml$/, ".html")
 				})
 
+		copy:
+			all:
+				files: [
+					{ expand: true, cwd: "src", src: ["**/*.html"], dest: "build" }
+				]
+
 		concat:
 			js:
 				files:
@@ -82,10 +89,14 @@ module.exports = (grunt) ->
 				files: ["src/**/*.haml"]
 				tasks: ["haml"]
 				spawn: true
+			copy:
+				files: ["src/**/*.html"]
+				tasks: ["copy"]
+				spawn: true
 			livereload:
 				files: ["assets/**", "build/**"]
 				tasks: ["livereload"]
 
-	grunt.registerTask("build", ["haml", "compass", "coffee", "concat", "symlink"])
+	grunt.registerTask("build", ["copy", "haml", "compass", "coffee", "concat", "symlink"])
 	grunt.registerTask("default", ["clean", "build"])
 	grunt.registerTask("server", ["clean", "build", "livereload-start", "connect", "regarde"])
diff --git a/build/index.html b/build/index.html
@@ -1,2 +1,49 @@
 <!DOCTYPE html>
-<html><head><meta charset="utf-8" /><link href="/styles/screen.css" rel="stylesheet" type="text/css" /><title>The Interactive String</title></head><body><div class="container"><header><h1>The Interactive String</h1><p>Friedrich Schöller</p></header><div data-string="main" class="string"><div data-string-display="data-string-display" class="display"><noscript><p>Javascript is required.</p></noscript></div><div data-string-controls="data-string-controls" class="controls"><!--%button.string-type open / closed--><textarea data-string-modes="data-string-modes"></textarea></div></div><div class="description"><h2 class="numbered">Calculations</h2><p>The length of the string is set equal to one. Center of mass variables are chosen to make the string oscillate around the point of origin. This leaves us with the transverse oscillators as degrees of freedom. In the classical description the string is massive, except when all modes have zero amplitude which makes it massless (and boring).</p><!--%h3.numbered Open String--><!--\[X^i = 2 sqrt{2alpha'} sum_{n=1}^infty rac{1}{n} left( a_n^i sin(pi cn	au) - b_n^i cos(pi cn	au) ight) cos(pi nsigma) ]--><!--%h3.numbered Closed String--><h2>References</h2><ol><li>Polchinski, Joseph (1998). <i>String Theory</i>, Cambridge University Press</li></ol></div></div><script src="/js/index.js"></script></body></html>
+<html>
+  <head>
+    <meta charset="utf-8">
+    <link href="/styles/screen.css" rel="stylesheet" type="text/css">
+    <title>The Interactive String</title>
+  </head>
+  <body>
+    <div class="container">
+      <header>
+        <h1>
+          The Interactive String
+        </h1>
+        <p>Friedrich Schöller</p>
+      </header>
+      <div class="string" data-string="main">
+        <div class="display" data-string-display>
+          <noscript>
+            <p>Javascript is required.</p>
+          </noscript>
+        </div>
+        <div class="controls" data-string-controls>
+          <!-- %button.string-type open / closed -->
+          <textarea data-string-modes></textarea>
+        </div>
+      </div>
+      <div class="description">
+        <h2 class="numbered">Calculations</h2>
+        <p>
+          The length of the string is set equal to one. Center of mass variables are chosen to make the string oscillate around the point of origin. This leaves us with the transverse oscillators as degrees of freedom. In the classical description the string is massive, except when all modes have zero amplitude which makes it massless (and boring).
+        </p>
+        <!-- %h3.numbered Open String -->
+        <!-- \\[X^i = 2 \sqrt{2\alpha'} \sum_{n=1}^\infty \frac{1}{n} \left( a_n^i \sin(\pi cn\tau) - b_n^i \cos(\pi cn\tau) \right) \cos(\pi n\sigma) \] -->
+        <!-- %h3.numbered Closed String -->
+        <h2>References</h2>
+        <ol>
+          <li>
+            Polchinski, Joseph (1998).
+
+            <i>String Theory</i>
+            , Cambridge University Press
+          </li>
+        </ol>
+      </div>
+    </div>
+    <script src="/js/index.js"></script>
+    <!-- <script src="http://cdn.mathjax.org/mathjax/latest/MathJax.js?config=TeX-AMS-MML_HTMLorMML"></script> -->
+  </body>
+</html>
diff --git a/package.json b/package.json
@@ -9,6 +9,7 @@
     "grunt-contrib-connect": "~0.2.0",
     "grunt-haml": "~0.4.0",
     "grunt": "~0.4.1",
-    "grunt-symbolic-link": "~0.3.1"
+    "grunt-symbolic-link": "~0.3.1",
+    "grunt-contrib-copy": "~0.4.1"
   }
 }
diff --git a/src/index.haml b/src/index.haml
diff --git a/src/index.html b/src/index.html
@@ -0,0 +1,49 @@
+<!DOCTYPE html>
+<html>
+  <head>
+    <meta charset="utf-8">
+    <link href="/styles/screen.css" rel="stylesheet" type="text/css">
+    <title>The Interactive String</title>
+  </head>
+  <body>
+    <div class="container">
+      <header>
+        <h1>
+          The Interactive String
+        </h1>
+        <p>Friedrich Schöller</p>
+      </header>
+      <div class="string" data-string="main">
+        <div class="display" data-string-display>
+          <noscript>
+            <p>Javascript is required.</p>
+          </noscript>
+        </div>
+        <div class="controls" data-string-controls>
+          <!-- %button.string-type open / closed -->
+          <textarea data-string-modes></textarea>
+        </div>
+      </div>
+      <div class="description">
+        <h2 class="numbered">Calculations</h2>
+        <p>
+          The length of the string is set equal to one. Center of mass variables are chosen to make the string oscillate around the point of origin. This leaves us with the transverse oscillators as degrees of freedom. In the classical description the string is massive, except when all modes have zero amplitude which makes it massless (and boring).
+        </p>
+        <!-- %h3.numbered Open String -->
+        <!-- \\[X^i = 2 \sqrt{2\alpha'} \sum_{n=1}^\infty \frac{1}{n} \left( a_n^i \sin(\pi cn\tau) - b_n^i \cos(\pi cn\tau) \right) \cos(\pi n\sigma) \] -->
+        <!-- %h3.numbered Closed String -->
+        <h2>References</h2>
+        <ol>
+          <li>
+            Polchinski, Joseph (1998).
+
+            <i>String Theory</i>
+            , Cambridge University Press
+          </li>
+        </ol>
+      </div>
+    </div>
+    <script src="/js/index.js"></script>
+    <!-- <script src="http://cdn.mathjax.org/mathjax/latest/MathJax.js?config=TeX-AMS-MML_HTMLorMML"></script> -->
+  </body>
+</html>