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authorKristian Evers <kristianevers@gmail.com>2017-09-18 22:21:20 +0200
committerKristian Evers <kristianevers@gmail.com>2017-09-18 22:21:20 +0200
commit6d1a1ff4e470bb4d26be46bdf01de3d94e6ab8e9 (patch)
tree7bec3d77463fba3ff68ebabcc127ad504da0836d /docs/source/projections/fouc_s.rst
parent1f60b8c407ac202916cf4570683935fcca451531 (diff)
downloadPROJ-6d1a1ff4e470bb4d26be46bdf01de3d94e6ab8e9.tar.gz
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Moved projection list to using chapter and created a list of transformations. Both are grouped in a section called operations.
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-.. _fouc_s:
-
-********************************************************************************
-Foucaut Sinusoidal
-********************************************************************************
-
-.. image:: ./images/fouc_s.png
- :scale: 50%
- :alt: Foucaut Sinusoidal
-
-
-The `y`-axis is based upon a weighted mean of the cylindrical equal-area and
-the sinusoidal projections. Parameter :math:`n=n` is the weighting factor where
-:math:`0 <= n <= 1`.
-
-.. math::
-
- x &= \lambda \cos \phi / (n + (1 - n) \ cos \phi)
-
- y &= n \phi + (1 - n) \sin \phi
-
-For the inverse, the Newton-Raphson method can be used to determine
-:math:`\phi` from the equation for :math:`y` above. As :math:`n \rightarrow 0` and
-:math:`\phi \rightarrow \pi/2`, convergence is slow but for :math:`n = 0`, :math:`\phi =
-\sin^1y`