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Add What's new entry for 1.10 and remove previous NEW IN/UPDATED IN
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HISTORY.txt

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@@ -17,7 +17,7 @@ v1.9.2 (2024-03-04)
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treated as a spherical potential). Kuzmin-like potentials are obtained by
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replacing the spherical radius r with \sqrt(R^2 + (a + |z|^2)), while
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Miyamoto-Nagai-like potentials are obtained by replacing the spherical
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radius with \sqrt(R^2 + (a + \\sqrt(z^2 + b^2))^2). The standard KuzminDiskPotential
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radius with \sqrt(R^2 + (a + \sqrt(z^2 + b^2))^2). The standard KuzminDiskPotential
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and MiyamotoNagaiPotential are obtained by applying this procedure to a point-mass
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potential and the Kuzmin/Miyamoto-Nagai-like potentials generalize this to any
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spherical potential.

doc/source/actionAngle.rst

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We start by discussing the forward and reverse transformations for the two
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specific potentials: the isochrone and the harmonic potentals.
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**UPDATED IN v1.8.2** Action-angle coordinates for the isochrone/harmonic potentials
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+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
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Action-angle coordinates for the isochrone/harmonic potentials
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++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
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The harmonic and isochrone potentials are the only potentials for which all of
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the actions, frequencies, and angles can be calculated analytically and for
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.. _aafwd:
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**UPDATED IN v1.8.2** Forward action-angle transformations (**x**, **v**) --> (**J**, **O**, **a**)
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+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
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Forward action-angle transformations (**x**, **v**) --> (**J**, **O**, **a**)
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+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
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Action-angle coordinates for spherical potentials
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--------------------------------------------------
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.. _aareverse:
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**UPDATED IN v1.8.2** Reverse action-angle transformations (**J**, **a**) --> (**x**, **v**, **O**)
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++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
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Reverse action-angle transformations (**J**, **a**) --> (**x**, **v**, **O**)
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+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
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Reverse action-angle transformations for one-dimensional potentials
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------------------------------------------------------------------

doc/source/orbit.rst

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.. _orbitsos:
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**NEW in v1.9** Surfaces of section
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-----------------------------------
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Surfaces of section
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-------------------
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``galpy`` can compute surfaces of section for two- and three-dimensional
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orbits using a special integration method that exactly determines the

doc/source/whatsnew.rst

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@@ -5,6 +5,32 @@ This page gives some of the key improvements in each galpy
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version. See the ``HISTORY.txt`` file in the galpy source for full
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details on what is new and different in each version.
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v1.10
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+++++
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Version 1.10 is a largely incremental update to version 1.9, with a few new features,
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bug fixes, and small improvememts to the documentation. The major new additions are:
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* Added ``KuzminLikeWrapperPotential``, a potential wrapper that allows
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one to make a Kuzmin-like or Miyamoto-Nagai-like potential out of any
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spherical or axisymmetric potential (evaluated in the plane, i.e.,
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treated as a spherical potential). Kuzmin-like potentials are obtained by
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replacing the spherical radius r with :math:`\sqrt{R^2 + (a + |z|^2)}`, while
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Miyamoto-Nagai-like potentials are obtained by replacing the spherical
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radius with :math:`\sqrt{R^2 + (a + \sqrt{z^2 + b^2})^2}`. The standard KuzminDiskPotential
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and MiyamotoNagaiPotential are obtained by applying this procedure to a point-mass
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potential and the Kuzmin/Miyamoto-Nagai-like potentials generalize this to any
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spherical potential.
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* Allow vector inputs of solar parameters to Orbit initialization: ``ro``, ``zo``, ``vo``,
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and ``solarmotion``. Useful when sampling over the uncertainty in the solar
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parameters.
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* Increased support for using OpenMP with clang and, in particular, added OpenMP support
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in the released Mac wheels.
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* Converted all docstrings to numpy-style format with the help of GitHub Copilot.
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v1.9
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