ON THE MOLECULAR TACTICS OF A
CRYSTAL
§ 1. My subject this evening is not
the physical properties of crystals, not even their dynamics; it is
merely the geometry of the structure—the arrangement of the
molecules in the constitution of a crystal. Every crystal is a
homogeneous assemblage of small bodies or molecules. The converse
proposition is scarcely true, unless in a very extended sense of
the term crystal (§ 20below). I can best explain a homogeneous assemblage of
molecules by asking you to think of a homogeneous assemblage of
people. To be homogeneous every person of the assemblage must be
equal and similar to every other: they must be seated in rows or
standing in rows in a perfectly similar manner. Each person, except
those on the borders of the assemblage, must have a neighbour on
one side and an equi-distant neighbour on the other: a neighbour on
the left front and an equi-distant neighbour behind on the right, a
neighbour on the right front and an equi-distant neighbour behind
on the left. His two neighbours in front and his two neighbours
behind are members of two rows equal and similar to the rows
consisting of himself and his right-hand and left-hand neighbours,
and their neighbours’ neighbours indefinitely to right and left. In
particular cases the nearest of the front and rear neighbours may
be right in front and right in rear; but we must not confine our
attention to the rectangularly grouped assemblages thus
constituted. Now let there be equal and similar assemblages on
floors above and below that which we have been considering, and let
there be any indefinitely great number of floors at equal distances
from one another above and below. Think of any one person on any
intermediate floor and of his nearest neighbours on the floors
above and below. These three persons must be exactly in one line;
this, in virtue of the homogeneousness of the assemblages on the
three floors, will secure that every person on the intermediate
floor is exactly in line with his nearest neighbours above and
below. The same condition of alignment must be fulfilled by every
three consecutive floors, and we thus have a homogeneous assemblage
of people in three dimensions of space. In particular cases every
person’s nearest neighbour in the floor above may be vertically
over him, but we must not confine our attention to assemblages thus
rectangularly grouped in vertical lines.§ 2. Consider now any particular personC(Fig. 1) on any intermediate
floor,DandD′his nearest neighbours,EandE′his next nearest neighbours all on his own floor. His next
next nearest neighbours on that floor will be in the
positionsFandF′in the diagram. Thus we see that
each personCis surrounded by
six persons,DD′,EE′andFF′, being his nearest, his next
nearest, and his next next nearest neighbours on his own floor.
Excluding for simplicity the special cases of rectangular grouping,
we see that the angles of the six equal and similar
trianglesCDE,CEF, &c., are all acute: and
because the six triangles are equal and similar we see that the
three pairs of mutually remote sides of the hexagonDEFD′E′F′are equal and
parallel.Fig. 1§ 3. Let nowA,A′,A″, &c., denote places of persons of the homogeneous
assemblage on the floor immediately above, andB,B′,B″, &c. on the
floor immediately below, the floor ofC. In the diagram leta,a′,a″be points in which
the floor ofCDEis cut by
perpendiculars to it throughA,A′,A″of the floor above, andb,b′,b″by perpendiculars
fromB,B′,B″of the floor below. Of all the perpendiculars from the floors
immediately above and below, just two, one from each, cut the area
of the parallelogramCDEF: and
they cut it in points similarly situated in respect to the
oppositely oriented triangles into which it is divided by either of
its diagonals. Hence ifalies
in the triangleCDE, the other
five triangles of the hexagon must be cut in the corresponding
points, as shown in the diagram. Thus, if we think only of the
floor ofCand of the floor
immediately above it, we have pointsA,A′,A″vertically abovea,a′,a″. Imagine now a
triangular pyramid, or tetrahedron, standing on the baseCDEand havingAfor vertex: we see that each of its
sidesACD,ADE,AEC, is an acute angled triangle, because, as we have already
seen,CDEis an acute angled
triangle, and because the shortest of the three distances,CA,DA,EA, is (§ 2) greater
thanCE(though it may be either
greater than or less thanDE).
Hence the tetrahedronCDEAhas
all its angles acute; not only the angles of its triangular faces,
but the six angles between the planes of its four faces. This
important theorem regarding homogeneous assemblages was given by
Bravais, to whom we owe the whole doctrine of homogeneous
assemblages in its most perfect simplicity and complete generality.
Similarly we see that we have equal and similar tetrahedrons on the
basesD′CF,E′F′C; and three other tetrahedrons
below the floor ofC, having
the oppositely oriented trianglesCD′E′, &c. for their bases
andB,B′,B″for their vertices. These three tetrahedrons are equal and
heterochirally1similar to the first three. The consideration of these acute
angled tetrahedrons, is of fundamental importance in respect to the
engineering of an elastic solid, or crystal, according to
Boscovich. So also is the consideration of the cluster of thirteen
pointsCand the six
neighboursDEFD′E′F′in the
plane of the diagram, and the three neighboursAA′A″on the floor above, andBB′B″on the floor below.§ 4. The case in which each of the four faces of each of the
tetrahedrons of§ 3is an
equilateral triangle is particularly interesting. An assemblage
fulfilling this condition may conveniently be called an
‘equilateral homogeneous assemblage,’ or, for brevity, an
‘equilateral assemblage.’ In an equilateral assemblageC’s twelve neighbours are all
equi-distant from it. I hold in my hand a cluster of thirteen
little black balls, made up by taking one of them and placing the
twelve others in contact with it (and therefore packed in the
closest possible order), and fixing them all together by fish-glue.
You see it looks, in size, colour, and shape, quite like a
mulberry. The accompanying diagram shows a stereoscopic view of a
similar cluster of balls painted white for the
photograph.Fig. 2.§ 5. By adding ball after ball to such a cluster of thirteen,
and always taking care to place each additional ball in some
position in which it is properly in line with others, so as to make
the whole assemblage homogeneous, we can exercise ourselves in a
very interesting manner in the building up of any possible form of
crystal of the class called ‘cubic’ by some writers and
‘octahedral’ by others. You see before you several examples. I
advise any of you who wish to study crystallo [...]