Changeset 4513 for trunk/doc/pslib/psLibADD.tex
- Timestamp:
- Jul 7, 2005, 5:58:24 PM (21 years ago)
- File:
-
- 1 edited
-
trunk/doc/pslib/psLibADD.tex (modified) (5 diffs)
Legend:
- Unmodified
- Added
- Removed
-
trunk/doc/pslib/psLibADD.tex
r4512 r4513 1 %%% $Id: psLibADD.tex,v 1.7 7 2005-07-08 03:55:45price Exp $1 %%% $Id: psLibADD.tex,v 1.78 2005-07-08 03:58:24 price Exp $ 2 2 \documentclass[panstarrs]{panstarrs} 3 3 … … 1523 1523 inverse of the above equations: 1524 1524 \begin{eqnarray} 1525 \phi & = & \atan(p_1, p_0) \\ 1526 \theta & = & \asin(p_2) \\ 1527 \end{eqnarray} 1528 Note that in this case, we neglect the scalar component of the 1529 quaternion --- it should be zero. 1525 \phi & = & \arctan(p_1, p_0) \\ 1526 \theta & = & \arcsin(p_2) \\ 1527 \end{eqnarray} 1528 where $\phi$ is the longitude and $\theta$ is the latitude. Note that 1529 in this case, we neglect the scalar component of the quaternion --- it 1530 should be zero. 1530 1531 1531 1532 \subsubsection{Quaternion for a rotation} … … 1541 1542 Note that the sine and cosine are taken of the half-angle of the 1542 1543 rotation. Note also that this implies that the quaternion components 1543 are normalized such that $| q| \equiv q_0^2 + q_1^2 + q_2^2 + q_3^21544 are normalized such that $|r| \equiv r_0^2 + r_1^2 + r_2^2 + r_3^2 1544 1545 = 1$. 1545 1546 … … 1595 1596 \end{eqnarray} 1596 1597 \item Second, about the Y axis: 1598 \begin{eqnarray} 1597 1599 s_0 & = & 0 \\ 1598 1600 s_1 & = & \sin(\delta_p/2) \\ … … 1607 1609 t_3 & = & \cos(\phi_p/2) \\ 1608 1610 \end{eqnarray} 1611 \end{itemize} 1609 1612 1610 1613 These three quaternions may be multiplied together to yield the
Note:
See TracChangeset
for help on using the changeset viewer.
