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template<typename T> octonion<T> spherical(T const & rho, T const & theta, T const & phi1, T const & phi2, T const & phi3, T const & phi4, T const & phi5, T const & phi6); template<typename T> octonion<T> multipolar(T const & rho1, T const & theta1, T const & rho2, T const & theta2, T const & rho3, T const & theta3, T const & rho4, T const & theta4); template<typename T> octonion<T> cylindrical(T const & r, T const & angle, T const & h1, T const & h2, T const & h3, T const & h4, T const & h5, T const & h6);

These build octonions in a way similar to the way polar builds complex numbers, as there is no strict equivalent to polar coordinates for octonions.

`spherical`

is a simple transposition
of `polar`

, it takes as inputs
a (positive) magnitude and a point on the hypersphere, given by three angles.
The first of these, *theta* has a natural range of -pi
to +pi, and the other two have natural ranges of -pi/2 to +pi/2 (as is the
case with the usual spherical coordinates in * R^{3}*).
Due to the many symmetries and periodicities, nothing untoward happens if
the magnitude is negative or the angles are outside their natural ranges.
The expected degeneracies (a magnitude of zero ignores the angles settings...)
do happen however.

`cylindrical`

is likewise a
simple transposition of the usual cylindrical coordinates in * R^{3}*, which in turn is another derivative of
planar polar coordinates. The first two inputs are the polar coordinates
of the first

`multipolar`

is yet another
simple generalization of polar coordinates. This time, both * C* components of the octonion are given
in polar coordinates.

In this version of our implementation of octonions, there is no analogue of the complex value operation arg as the situation is somewhat more complicated.