diff options
| author | dante <dante19031999@gmail.com> | 2020-11-04 18:00:23 +0100 |
|---|---|---|
| committer | Noel Grandin <noel.grandin@collabora.co.uk> | 2020-11-07 07:10:33 +0100 |
| commit | 2b29e16ea0fca627d71b61af98df0f543e6f206b (patch) | |
| tree | 185cb375349afb15cb5eb16cf1fdd8d8faeb9121 /starmath | |
| parent | 5a96093f0ecee53432bdf35f247edd6deb501baf (diff) | |
Starmath examples renovated
Change-Id: Iff286171ddba92373d400763eb78769e37f40f37
Reviewed-on: https://gerrit.libreoffice.org/c/core/+/105302
Tested-by: Jenkins
Reviewed-by: Noel Grandin <noel.grandin@collabora.co.uk>
Diffstat (limited to 'starmath')
| -rw-r--r-- | starmath/inc/strings.hrc | 9 | ||||
| -rw-r--r-- | starmath/source/ElementsDockingWindow.cxx | 11 |
2 files changed, 17 insertions, 3 deletions
diff --git a/starmath/inc/strings.hrc b/starmath/inc/strings.hrc index b9377eff1081..8a303127d245 100644 --- a/starmath/inc/strings.hrc +++ b/starmath/inc/strings.hrc @@ -298,8 +298,15 @@ #define RID_EXAMPLE_CIRCUMFERENCE_HELP NC_("RID_EXAMPLE_CIRCUMFERENCE_HELP", "Circumference" ) #define RID_EXAMPLE_MASS_ENERGY_EQUIV_HELP NC_("RID_EXAMPLE_MASS_ENERGY_EQUIV_HELP", "Mass–energy equivalence" ) #define RID_EXAMPLE_PYTHAGOREAN_THEO_HELP NC_("RID_EXAMPLE_PYTHAGOREAN_THEO_HELP", "Pythagorean theorem" ) -#define RID_EXAMPLE_A_SIMPLE_SERIES_HELP NC_("RID_EXAMPLE_A_SIMPLE_SERIES_HELP", "A simple series" ) +#define RID_EXAMPLE_A_TAYLOR_SERIES_HELP NC_("RID_EXAMPLE_A_TAYLOR_SERIES_HELP", "Taylor series" ) #define RID_EXAMPLE_GAUSS_DISTRIBUTION_HELP NC_("RID_EXAMPLE_GAUSS_DISTRIBUTION_HELP", "Gauss distribution" ) +#define RID_EXAMPLE_EULER_LAGRANGE_HELP NC_("RID_EXAMPLE_EULER_LAGRANGE_HELP", "Euler-Lagrange equation" ) +#define RID_EXAMPLE_FTC_HELP NC_("RID_EXAMPLE_FTC_HELP", "Fundamental theorem of calculus" ) +#define RID_EXAMPLE_CAOS_HELP NC_("RID_EXAMPLE_CAOS_HELP", "Chaos equation" ) +#define RID_EXAMPLE_EULER_IDENTITY_HELP NC_("RID_EXAMPLE_EULER_IDENTITY_HELP", "Euler's identity" ) +#define RID_EXAMPLE_2NEWTON NC_("RID_EXAMPLE_2NEWTON", "Newton's second law" ) +#define RID_EXAMPLE_GENERAL_RELATIVITY_HELP NC_("RID_EXAMPLE_GENERAL_RELATIVITY_HELP", "General relativity") +#define RID_EXAMPLE_SPECIAL_RELATIVITY_HELP NC_("RID_EXAMPLE_SPECIAL_RELATIVITY_HELP", "Special relativity") #define RID_FONTREGULAR NC_("RID_FONTREGULAR", "Standard" ) #define RID_FONTITALIC NC_("RID_FONTITALIC", "Italic" ) diff --git a/starmath/source/ElementsDockingWindow.cxx b/starmath/source/ElementsDockingWindow.cxx index 8850ca49fcbb..aa96a1e0bb7f 100644 --- a/starmath/source/ElementsDockingWindow.cxx +++ b/starmath/source/ElementsDockingWindow.cxx @@ -244,10 +244,17 @@ const SmElementDescr SmElementsControl::m_aOthersList[] = const SmElementDescr SmElementsControl::m_aExamplesList[] = { + {"{func e}^{i %pi} + 1 = 0", RID_EXAMPLE_EULER_IDENTITY_HELP}, {"C=%pi cdot d = 2 cdot %pi cdot r", RID_EXAMPLE_CIRCUMFERENCE_HELP}, - {"E=mc^2", RID_EXAMPLE_MASS_ENERGY_EQUIV_HELP}, {"a^2 + b^2 = c^2", RID_EXAMPLE_PYTHAGOREAN_THEO_HELP}, - {"f ( x ) = sum from { { i = 0 } } to { infinity } { {f^{(i)}(0)} over {i!} x^i}", RID_EXAMPLE_A_SIMPLE_SERIES_HELP}, + {"F = m a", RID_EXAMPLE_2NEWTON}, + {"E = m c^2", RID_EXAMPLE_MASS_ENERGY_EQUIV_HELP}, + {"G_{%mu %nu} + %LAMBDA g_{%mu %nu}= frac{8 %pi G}{c^4} T_{%mu %nu}", RID_EXAMPLE_GENERAL_RELATIVITY_HELP}, + {" %DELTA t' = { %DELTA T } over sqrt{ 1 - v^2 over c^2 } ", RID_EXAMPLE_SPECIAL_RELATIVITY_HELP }, + { "d over dt left( {partial L}over{partial dot q} = {partial L}over{partial q} right)", RID_EXAMPLE_EULER_LAGRANGE_HELP }, + {"int from a to b f'(x) dx = f(a) - f(b)", RID_EXAMPLE_FTC_HELP}, + { "abs{ %delta Z(t) } approx e^{%lambda t} abs{ %delta Z(0) }", RID_EXAMPLE_CAOS_HELP}, + {"f ( x ) = sum from { { n = 0 } } to { infinity } { {f^{(n)}(x_0)} over {n!} (x-x_0)^n}", RID_EXAMPLE_A_TAYLOR_SERIES_HELP}, {"f ( x ) = {1} over {%sigma sqrt{2%pi} }func e^-{{(x-%mu)^2} over {2%sigma^2}}", RID_EXAMPLE_GAUSS_DISTRIBUTION_HELP}, }; |