Intracranial saccular aneurysms are balloon-like distensions of the ar
terial wall: they increase in size gradually, a few to the point of bl
eeding or catastrophic rupture, Collagen is the primary structural com
ponent of the aneurysmal wall, and because only a small fraction of an
eurysms fail, the collagen fabric must effectively reorganize in order
to maintain mechanical integrity as an aneurysm changes size. Data we
re obtained from four human aneurysms, fixed at 100 mmHg of distending
pressure with 10% buffered formalin, and sectioned completely through
at 4 mu m thickness. Each set of measurements included groups of data
taken layer by layer from a radial corridor across the aneurysm wall.
Each three-dimensional orientation measurement, for which we used a Z
eiss polarizing microscope with a universal stage attachment, is defin
ed by an azimuth and elevation angle relative to the section plane. We
compared the interdependence of these measured angles with a mathemat
ical model based on fibres following great circle trajectories, and re
lated the measured azimuth and elevation angles to the relative depth
of the section into the aneurysm. Data were plotted on Lambert equal-a
rea projections, along with the theoretical relation between azimuth a
nd elevation, that included wall thickness and depth of sectioning. Th
e graphical relationship between measured azimuth and elevation for co
llagen fibres across the layered fabric of the aneurysmal wall is cons
istent with the theoretical great circle trajectories for collagen fib
re alignment, Analysis was based on statistics for spherical data to g
ive values for the mean orientation and the circular standard deviatio
ns (CSD) about that mean, The results indicate that any given region o
n the aneurysm wall is made up of many, very thin sublayers, most of w
hich have a relatively coherent organization (mean CSD 8 degrees). The
se measurements agree well with the mathematical model and. when consi
dered collectively, the layers provide a balanced distribution for bea
ring the biaxial tensile stress of the wall.