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@@ -33,7 +33,7 @@
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classes</a>
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</h3></div></div></div>
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<div class="table">
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<a name="id585104"></a><p class="title"><b>Table 1.3. Stepper Algorithms</b></p>
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<a name="id585035"></a><p class="title"><b>Table 1.3. Stepper Algorithms</b></p>
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<div class="table-contents"><table class="table" summary="Stepper Algorithms">
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<colgroup>
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<col>
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@@ -914,10 +914,9 @@
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<p>
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</p>
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<p>
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During the integration approximately 71 steps have been done. Comparing to
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a classical Runge-Kutta solver this is a very good result. For example the
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Dormand-Prince 5 method with step size control and dense output yields ca.
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1531 steps.
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During the integration 71 steps have been done. Comparing to a classical
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Runge-Kutta solver this is a very good result. For example the Dormand-Prince
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5 method with step size control and dense output yields 1531 steps.
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</p>
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<p>
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@@ -93,7 +93,7 @@
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</div>
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</div>
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<table xmlns:rev="http://www.cs.rpi.edu/~gregod/boost/tools/doc/revision" width="100%"><tr>
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<td align="left"><p><small>Last revised: March 31, 2011 at 16:36:47 GMT</small></p></td>
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<td align="left"><p><small>Last revised: March 31, 2011 at 17:46:07 GMT</small></p></td>
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<td align="right"><div class="copyright-footer"></div></td>
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</tr></table>
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<hr>
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@@ -28,7 +28,7 @@ A well know solver for stiff systems is the so called Rosenbrock method. It has
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[integrate_stiff_system]
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During the integration approximately 71 steps have been done. Comparing to a classical Runge-Kutta solver this is a very good result. For example the Dormand-Prince 5 method with step size control and dense output yields ca. 1531 steps.
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During the integration 71 steps have been done. Comparing to a classical Runge-Kutta solver this is a very good result. For example the Dormand-Prince 5 method with step size control and dense output yields 1531 steps.
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[integrate_stiff_system_alternative]
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