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authorAndres Rey <[email protected]>2016-12-22 21:48:49 -0300
committerAndres Rey <[email protected]>2016-12-22 21:48:49 -0300
commitd024c2d80a38d721d6d1d0fd812a706a5fc22562 (patch)
treef19ea7f62cc07f702086182dfac59b9c5397ace3 /test/test-pages/reordering-paragraphs
parente9737116493b2dd2893a9a5ac44d0e768dc363bd (diff)
Corrected all the test cases
Diffstat (limited to 'test/test-pages/reordering-paragraphs')
-rw-r--r--test/test-pages/reordering-paragraphs/expected.html28
1 files changed, 26 insertions, 2 deletions
diff --git a/test/test-pages/reordering-paragraphs/expected.html b/test/test-pages/reordering-paragraphs/expected.html
index 506f291..4a46dd5 100644
--- a/test/test-pages/reordering-paragraphs/expected.html
+++ b/test/test-pages/reordering-paragraphs/expected.html
@@ -1,2 +1,26 @@
- <p id="first">Regarding item# 11111, under sufficiently extreme conditions, quarks may become deconfined and exist as free particles. In the course of asymptotic freedom, the strong interaction becomes weaker at higher temperatures. Eventually, color confinement would be lost and an extremely hot plasma of freely moving quarks and gluons would be formed. This theoretical phase of matter is called quark-gluon plasma.[81] The exact conditions needed to give rise to this state are unknown and have been the subject of a great deal of speculation and experimentation.</p>
- <p id="second">Regarding item# 22222, under sufficiently extreme conditions, quarks may become deconfined and exist as free particles. In the course of asymptotic freedom, the strong interaction becomes weaker at higher temperatures. Eventually, color confinement would be lost and an extremely hot plasma of freely moving quarks and gluons would be formed. This theoretical phase of matter is called quark-gluon plasma.[81] The exact conditions needed to give rise to this state are unknown and have been the subject of a great deal of speculation and experimentation.</p> \ No newline at end of file
+<div>
+ <p id="first">Regarding item# 11111, under sufficiently extreme conditions, quarks may
+ become deconfined and exist as free particles. In the course of asymptotic
+ freedom, the strong interaction becomes weaker at higher temperatures.
+ Eventually, color confinement would be lost and an extremely hot plasma
+ of freely moving quarks and gluons would be formed. This theoretical phase
+ of matter is called quark-gluon plasma.[81] The exact conditions needed
+ to give rise to this state are unknown and have been the subject of a great
+ deal of speculation and experimentation.</p>
+ <p id="second">Regarding item# 22222, under sufficiently extreme conditions, quarks may
+ become deconfined and exist as free particles. In the course of asymptotic
+ freedom, the strong interaction becomes weaker at higher temperatures.
+ Eventually, color confinement would be lost and an extremely hot plasma
+ of freely moving quarks and gluons would be formed. This theoretical phase
+ of matter is called quark-gluon plasma.[81] The exact conditions needed
+ to give rise to this state are unknown and have been the subject of a great
+ deal of speculation and experimentation.</p>
+ <p id="third">Regarding item# 33333, under sufficiently extreme conditions, quarks may
+ become deconfined and exist as free particles. In the course of asymptotic
+ freedom, the strong interaction becomes weaker at higher temperatures.
+ Eventually, color confinement would be lost and an extremely hot plasma
+ of freely moving quarks and gluons would be formed. This theoretical phase
+ of matter is called quark-gluon plasma.[81] The exact conditions needed
+ to give rise to this state are unknown and have been the subject of a great
+ deal of speculation and experimentation.</p>
+ <br id="br2"></br></div> \ No newline at end of file