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Diffstat (limited to 'test/test-pages/reordering-paragraphs/expected.html')
| -rw-r--r-- | test/test-pages/reordering-paragraphs/expected.html | 31 |
1 files changed, 5 insertions, 26 deletions
diff --git a/test/test-pages/reordering-paragraphs/expected.html b/test/test-pages/reordering-paragraphs/expected.html index 4a46dd5..7d15fcc 100644 --- a/test/test-pages/reordering-paragraphs/expected.html +++ b/test/test-pages/reordering-paragraphs/expected.html @@ -1,26 +1,5 @@ -<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 +<div id="readability-page-1" class="page"> + <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"/> </div>
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