In this lecture we shall see how to plot the poles of planes (hkl) onto a stereographic projection when the crystal is not cubic. The Miller indices of planes in the crystal (hkl) are still defined in terms of the inverse of the intercept of the plane on the three crystal axes . However, to plot the normals to the plane (hkl) or the pole of the direction [uvw] onto a stereographic projection we need to recognise that the three crystal unit vectors are not necessarily equal nor need they be mutually perpendicular. Since the analysis developed earlier for cubic crystals relied on the fact that the unit crystal vectors were each identical to the unit vectors of cartesian space, we now need to develop a transfoprmation of co-ordinates matrix that will transform a vector [uvw], expressed in terms of the three crystal unit vectors , into a vector [xyz] expressed in terms of the 3 unit vectors of regular cartesian space. We shall call this matrix M, the mapping matrix. Align the normal to the crystal plane (010) with the y-axis of cartesian space (i.e. the plane defined by the crystal vectors We now draw a line from the end of the vector a perpendicular to the x-axis and parallel to the z-axis. The projected lengths of the vector We now drop a line from the end of the vector b to the x-y plane plane so that the line is perpendicular to the x-y plane and parallel to the z-axis as shown below. The vector b then has projected lengths in the x-y plane and in the z-axis of:- to the x-y plane intersects the x-y plane (q). To do this we recognise that the figure abpq is a simple trapezoid with ap parallel to bq and that d can be calculated from the cosine rule if we know the length e, e is calculated using pythagarus' theorum. Let's see how this works in practice by finding the cartesian vector [xyz] that is equivalent to the crystal vector  in the monoclinic, tetragonal and cubic forms of ZrO In the cubic form  becomes  in cartesian space, in the tetragonal form  becomes [1,1,1.448] while in the monoclinic form  becomes [1.148,1.177,1] in cartesian space. The poles are plotted below on a standard  stereographic projection Source.