Of the simple, undecomposable substances, which chemists call elements, and of which somewhat more than seventy have been identified on the earth, only about twenty enter at all largely into the composition of the earth’s crust,’ so far as this is accessible to examination. It is estimated that 97 per cent of the crust is made up of ten elements.
| Non-Metallic |
Metallic |
| Oxygen |
O |
Aluminium |
Al |
| Hydrogen |
H |
Potassium |
K |
| Silicon |
Si |
Sodium |
Na |
| Carbon |
C |
Calcium |
Ca |
| Â |
 |
Magnesium |
Mg |
| Â |
 |
Iron |
Fe |
The remaining ten are far less abundant, but yet of considerable importance.
| Chlorine |
Cl |
Lithium |
Li |
| Fluorine |
F |
Barium |
Ba |
| Sulphur |
S |
Manganese |
Mn |
| Phosphorus |
P |
Titanium |
Ti |
| Boron |
B |
Zirconium |
Zr |
Only two of these elements, carbon and sulphur, are found in a more or less impure state as minerals or rock masses; the others occur as compounds, formed by the union of two or more of them.
A mineral is a natural, inorganic substance, which has a homogeneous structure, definite chemical composition and physical properties, and usually a definite crystalline form.
Crystals are solids of more or less regular and symmetrical shape, bounded, usually, by plane surfaces. The number of known crystalline forms is already very great, and yet they may be all reduced to thirteen fundamental shapes, which are prisms, octahedrons (eight-sided), or dodecahedrons (twelve-sided).
The thirteen fundamental forms and their innumerable secondary derivatives fall into six systems, which are characterized by the relations of their axes. The axes of a crystal are imaginary lines, which connect the centres of opposite faces, or opposite edges, or opposite solid angles, and which intersect one another at a point in the interior of the crystal.
The Systems of Crystalline Forms have received many names, the following being those which are most generally used in this country: -
Isometric System (monometric, cubical, regular)
In this system the three axes are of equal length and intersect one another at right angles; it includes the cube, regular octahedron, and rhombic dodecahedron, forms which are symmetrical in all positions.
Tetragonal System (dimetric, pyramidal)
The axes intersect at right angles, but are not all of equal length; the two lateral axes are of equal length, but the vertical axis is longer or shorter than the laterals. Includes the right square prism and the square octahedron, the faces of which are isosceles triangles.
Hexagonal System
Here four axes are employed, three equal lateral axes intersecting at angles of 60 degrees, and a vertical axis, which is perpendicular to and longer or shorter than the laterals. Includes the rhombohedron, hexagonal prism, and scalenohedron.
Orthorhombic System (rhombic, trimetric)
The three axes intersect at right angles and are all of different lengths; rectangular and rhombic prisms, and rhombic octahedron.
Monoclinic System (mono-symmetric, oblique)
All three axes are of different lengths; two of the axes, usually the laterals, are at right angles to each other, while the third is oblique: right rhomboidal and oblique rhombic prisms.
Tric1inic System (anorthic, asymmetric)
Three axes of unequal lengths and oblique to one another: oblique rhomboidal prism, doubly oblique octahedron.
It is important to bear in mind the relations which the fundamental forms sustain toward one another. For example, a regular octahedron may be derived from a cube by evenly paring off the eight solid angles, until the planes thus produced intersect one another, the centres of the faces of the cube becoming the apices of the solid angles of the octahedron. Conversely, a cube may be formed from an octahedron by symmetrically truncating the angles, until the planes thus formed intersect. By slicing away the twelve edges of a cube or an octahedron a dodecahedron will result. These crystalline forms are, therefore, so related as to be all derivable one from another, and the relations of their axes remain unchanged; all three forms may be assumed by the same mineral, and they thus properly belong in the same system. Similar relations may be observed between the crystalline forms of the other systems.
It might be supposed that the crystalline systems and the relations of their imaginary axes were merely mathematical devices to reach a convenient classification of forms. Such a conclusion would, however, be a very erroneous one. Crystalline form is the expression of molecular structure, and many of the physical properties of minerals are determined by their mathematical figure. It is clear that the physical properties which depend upon form are not inherent in the molecules of the mineral, but are conditioned by the way in which the molecules are built up into the crystal. Amorphous substances refract light equally in all directions, and are thus called isotropic, but when an amorphous substance crystallizes, it assumes the qualities proper to its crystalline form. Thus water is isotropic, while the hexagonal crystals of ice are singly refractive in only one direction, doubly refractive in two. The same substance may, under different circumstances, crystallize in different systems, and will then display the properties appropriate to each system.
Not only the refractive powers of a crystal, but also its mode of expansion when heated, and its conductivity of electricity and heat depend upon its form.
The crystals of the isometric system, which have their three axes of equal length, are singly refractive in all directions, expand equally when heated, and conduct heat and electricity equally in all directions. Those of the tetragonal and hexagonal systems, which have one axis longer or shorter than the others, are doubly refractive along the lateral axes, expand equally when heated, and show equal conductivity along these axes. Along the principal axis they are singly refractive, expand to a different degree when heated, and display a different conductivity along this axis than along the others. In the orthorhombic, monoclinic, and triclinic systems, which have all the axes of unequal lengths, the crystals are singly refractive in two directions; they expand unequally and conduct differently along all their axes.
The optical properties of minerals are of great value in the study of rocks, and by the aid of the polarizing microscope very minute crystals may be identified.
Most substances which are solid under any circumstances are capable of assuming a crystalline form, so that solidification and crystallization are usually identical. For the formation of large and regular crystals, it is necessary that the process be gradual and that space be given for the individual crystals to grow. Usually crystallization begins at many points simultaneously, and the crystals crowd upon one another, resulting in a mass of more or less irregular crystalline grains. The same substance which, when very rapidly solidified, forms an amorphous glass, will give rise to distinct crystals, if slowly solidified.
Crystallization requires that the molecules be free to move upon each other, and thus to arrange themselves in a definite fashion. It may take place either by the deposition of a solid from solution, by cooling from a state of fusion, or by solidification from the condition of vapour. In all cases the size and regularity of the crystals depend upon the time and space allowed for their growth. In a manner not yet understood, amorphous solids may be converted into crystalline aggregates. This has been observed in the case of certain glassy volcanic rocks, which, though amorphous when first solidified, have gradually become crystalline, without losing their solidity. This process is called devitrification.
The actual steps of crystallization may be observed by slowly evaporating a solution of some crystalline salt under the microscope. The first visible step in the process is the appearance of innumerable dark points in the fluid, which rapidly grow, until their spherical shape is made apparent. The globules then begin to move about rapidly and arrange themselves in straight lines, like strings of beads, and next suddenly coalesce into straight rods. The rods arrange themselves into layers, and thus build up the crystals so rapidly, that it is hardly possible to follow the steps of change. In certain glassy rocks, which solidified too quickly to allow crystallization to take place, the incipient stages of crystals, in the form of globules and hair-like rods, may be detected with the microscope.
Secondary Forms of Crystals
A great variety of crystalline forms is produced by the occurrence of secondary planes or faces on the angles or edges of the primary forms. All the similar parts of the crystal may be modified in the same way, or alternating similar parts may be so modified.
Certain faces may be obliterated by the enlargement of others; but however great the variation, the angle at which corresponding faces meet almost invariably remains constant for each mineral.
Massive and imperfectly crystallized minerals may consist of grains, fibres, or thin layers (lamina;).
Hardness
The hardness of minerals is a useful means of identifying them. For this purpose they are referred to a scale of hardness, ranging from such soft substances as may be readily scratched with the finger-nail, to the hardest known substance, diamond. The degree of hardness is expressed by the numerical place of the mineral in the scale, and intermediate grades are indicated by fractions. Thus a mineral which is scratched by quartz and scratches orthoclase with equal ease, has a hardness of 6.5. The scale is as follows:
| 1. |
Talc |
6. |
Orthoclase |
| 2. |
Selemite |
7. |
Quartz |
| 3. |
Calcite |
8. |
Topaz |
| 4. |
Fluor-spar |
9. |
Sapphire |
| 5. |
Apatite |
10. |
Diamond |
Cleavage
Many minerals split readily along certain planes, still retaining a crystalline form, while in other directions they break irregularly. This property is called cleavage. Cleavage is uniform in the different varieties of the same mineral, and takes place either in planes parallel to one or more faces of the fundamental form of the crystal, or along the diagonals of that form.
Pseudomorphs occur when one mineral assumes the crystalline form proper to another. This may take place either by the addition or the removal of certain constituents, or some constituents may be removed and others substituted for them. The entire substance of a mineral may be removed and its place taken, molecule by molecule, by another, retaining the form, sometimes even the cleavage, of the first. The study of pseudomorphs is often of the greatest service, as throwing light upon the history of the rock in which they occur.
Compound crystals are formed by the joining of simple crystals.
When two half-crystals are united along a plane in such a way that their faces and axes do not correspond, they are said to be twinned. When the twinning is repeated along numerous parallel planes, the crystal is a polysynthetic twin. Two crystals united at the ends to form a right angle, are called geniculate, while two geniculate crystals may be so combined as to form a cross, and then are said to be cruciform.
Crystals of the same form may vary in length and in the size of their corresponding faces, which gives rise to numerous irregularities of shape.
Rock-forming Minerals
The number of known minerals is exceedingly great, and is constantly increasing, but only a few enter in any important way into the constitution of the earth’s crust. We now proceed to a consideration of these constituent minerals, which are called rock-forming minerals, because the rocks are aggregations of them. It must be emphasized that the student can gain no real knowledge of minerals or rocks by merely reading about them; it is necessary that he should familiarize himself with actual specimens.