diff --git a/libs/numeric/odeint/doc/html/boost_sandbox_numeric_odeint/reference.html b/libs/numeric/odeint/doc/html/boost_sandbox_numeric_odeint/reference.html index af437ee9..22a73eaa 100644 --- a/libs/numeric/odeint/doc/html/boost_sandbox_numeric_odeint/reference.html +++ b/libs/numeric/odeint/doc/html/boost_sandbox_numeric_odeint/reference.html @@ -33,7 +33,7 @@ classes
-

Table 1.3. Stepper Algorithms

+

Table 1.3. Stepper Algorithms

diff --git a/libs/numeric/odeint/doc/html/boost_sandbox_numeric_odeint/tutorial.html b/libs/numeric/odeint/doc/html/boost_sandbox_numeric_odeint/tutorial.html index 2761c0dd..998b336a 100644 --- a/libs/numeric/odeint/doc/html/boost_sandbox_numeric_odeint/tutorial.html +++ b/libs/numeric/odeint/doc/html/boost_sandbox_numeric_odeint/tutorial.html @@ -914,10 +914,9 @@

- 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. + 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.

diff --git a/libs/numeric/odeint/doc/html/index.html b/libs/numeric/odeint/doc/html/index.html index febd208b..bd71b27b 100644 --- a/libs/numeric/odeint/doc/html/index.html +++ b/libs/numeric/odeint/doc/html/index.html @@ -93,7 +93,7 @@

- +

Last revised: March 31, 2011 at 16:36:47 GMT

Last revised: March 31, 2011 at 17:46:07 GMT


diff --git a/libs/numeric/odeint/doc/tutorial_stiff_systems.qbk b/libs/numeric/odeint/doc/tutorial_stiff_systems.qbk index 45583479..29410030 100644 --- a/libs/numeric/odeint/doc/tutorial_stiff_systems.qbk +++ b/libs/numeric/odeint/doc/tutorial_stiff_systems.qbk @@ -28,7 +28,7 @@ A well know solver for stiff systems is the so called Rosenbrock method. It has [integrate_stiff_system] -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. +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. [integrate_stiff_system_alternative]