Diamond is a solid form of pure carbon with its atoms arranged in a crystal. Solid carbon comes in different forms known as
allotropes depending on the type of chemical bond. The two most common
allotropes of pure carbon are diamond and
graphite. In graphite, the bonds are sp2
orbital hybrids and the atoms form in planes, with each bound to three nearest neighbors, 120 degrees apart. In diamond, they are sp3 and the atoms form tetrahedral, with each bound to four nearest neighbors. Tetrahedra are rigid, the bonds are strong, and, of all known substances, diamond has the greatest number of atoms per unit volume, which is why it is both the hardest and the least
compressible. It also has a high density, ranging from 3150 to 3530 kilograms per cubic metre (over three times the density of water) in natural diamonds and 3520 kg/m in pure diamond. In graphite, the bonds between nearest neighbors are even stronger, but the bonds between parallel adjacent planes are weak, so the planes easily slip past each other. Thus, graphite is much softer than diamond. However, the stronger bonds make graphite less flammable. Diamonds have been adopted for many uses because of the material's exceptional physical characteristics. It has the highest
thermal conductivity and the highest sound velocity. It has low adhesion and friction, and its coefficient of
thermal expansion is extremely low. Its optical transparency extends from the
far infrared to the deep
ultraviolet, and it has high
optical dispersion. It also has high electrical resistance. It is chemically inert, not reacting with most corrosive substances, and has excellent biological compatibility.
Thermodynamics The equilibrium pressure and temperature conditions for a transition between graphite and diamond are well established theoretically and experimentally. The equilibrium pressure varies linearly with temperature, between at and at (the diamond/graphite/liquid
triple point). However, the phases have a wide region about this line where they can coexist. At
standard temperature and pressure, and , the stable phase of carbon is graphite, but diamond is
metastable, with a significant kinetic energy barrier that the atoms must overcome to reach the lower energy state, and its rate of conversion to graphite is negligible, with a timescale of millions to billions of years. Rapid conversion of graphite to diamond requires pressures well above the equilibrium line: at , a pressure of (about 350,000 standard atmospheres) is needed. At high pressures,
silicon and
germanium have a BC8
body-centered cubic crystal structure, and a similar structure is predicted for carbon at high pressures. At , the transition is predicted to occur at . Results published in
Nature Physics in 2010 suggest that, at ultra-high pressures and temperatures (about 10 million atmospheres or 1 TPa and 50,000 °C), diamond melts into a metallic fluid. The extreme conditions required for this to occur are present in the
ice giant planets
Neptune and
Uranus, both of which are made up of approximately 10 percent carbon and could hypothetically contain oceans of liquid carbon. Since large quantities of metallic fluid can affect the magnetic field, this could serve to explain why the geographic and magnetic poles of the two planets are not aligned.
Crystal structure The most common crystal structure of diamond is called
diamond cubic. It is formed of
unit cells stacked together. Although there are 18 atoms in the figure, each corner atom is shared by eight unit cells and each atom in the center of a face is shared by two, so there are a total of eight atoms per unit cell. The length of each side of the unit cell is denoted by
a and is 3.567
angstroms. The nearest neighbor distance in the diamond lattice is 1.732
a/4 where
a is the lattice constant, usually given in Angstrøms as
a = 3.567 Å, which is 0.3567 nm. A diamond cubic lattice can be thought of as two interpenetrating
face-centered cubic lattices with one displaced by of the diagonal along a cubic cell, or as one lattice with two atoms associated with each lattice point.
Crystal habit Diamonds occur most often as
euhedral or rounded
octahedra and
twinned octahedra known as
macles. As diamond's crystal structure has a cubic arrangement of the atoms, they have many
facets that belong to a
cube, octahedron,
rhombicosidodecahedron,
tetrakis hexahedron, or
disdyakis dodecahedron. The crystals can have rounded-off and unexpressive edges and can be elongated. Diamonds (especially those with rounded crystal faces) are commonly found coated in
nyf, an opaque gum-like skin. Some diamonds contain opaque fibers. They are referred to as
opaque if the fibers grow from a clear substrate or
fibrous if they occupy the entire crystal. Their colors range from yellow to green or gray, sometimes with cloud-like white to gray impurities. Their most common shape is cuboidal, but they can also form octahedra, dodecahedra, macles, or combined shapes. The structure is the result of numerous impurities with sizes between 1 and 5 microns. These diamonds probably formed in kimberlite magma and sampled the volatiles. Diamonds can also form polycrystalline aggregates. There have been attempts to classify them into groups with names such as
boart,
ballas, stewartite, and framesite, but there is no widely accepted set of criteria. It has never been observed in a volcanic rock. There are many theories for its origin, including formation in a star, but no consensus.
Mechanical Hardness er. Diamond is the hardest material on the
qualitative Mohs scale. To conduct the
quantitative Vickers hardness test, samples of materials are struck with a pyramid of standardized dimensions using a known force – a diamond crystal is used for the pyramid to permit a wide range of materials to be tested. From the size of the resulting indentation, a Vickers hardness value for the material can be determined. Diamond's great hardness relative to other materials has been known since antiquity, and is the source of its name. This does not mean that it is infinitely hard, indestructible, or unscratchable. Indeed, diamonds can be scratched by other diamonds and worn down over time even by softer materials, such as vinyl
phonograph records. Diamond hardness depends on its purity, crystalline perfection, and orientation: hardness is higher for flawless, pure crystals oriented to the Miller index#Case of cubic structures| direction (along the longest diagonal of the cubic diamond lattice). Therefore, whereas it might be possible to scratch some diamonds with other materials, such as
boron nitride, the hardest diamonds can only be scratched by other diamonds and
nanocrystalline diamond aggregates. The hardness of diamond contributes to its suitability as a gemstone. Because it can only be scratched by other diamonds, it maintains its polish extremely well. Unlike many other gems, it is well-suited to daily wear because of its resistance to scratching—perhaps contributing to its popularity as the preferred gem in
engagement or
wedding rings, which are often worn every day. The hardest natural diamonds mostly originate from the
Copeton and
Bingara fields located in the
New England area in
New South Wales, Australia. These diamonds are generally small, perfect to semiperfect octahedra, and are used to polish other diamonds. Their hardness is associated with the
crystal growth form, which is single-stage crystal growth. Most other diamonds show more evidence of multiple growth stages, which produce inclusions, flaws, and defect planes in the crystal lattice, all of which affect their hardness. It is possible to treat regular diamonds under a combination of high pressure and high temperature to produce diamonds that are harder than the diamonds used in hardness gauges. Diamonds cut glass, but this does not positively identify a diamond because other materials, such as quartz, also lie above glass on the
Mohs scale and can also cut it. Diamonds can scratch other diamonds, but this can result in damage to one or both stones. Hardness tests are infrequently used in practical gemology because of their potentially destructive nature. these tend to result in extremely flat, highly polished facets with exceptionally sharp facet edges. Diamonds also possess an extremely high refractive index and fairly high dispersion. Taken together, these factors affect the overall appearance of a polished diamond and most
diamantaires still rely upon skilled use of a
loupe (magnifying glass) to identify diamonds "by eye".
Toughness Somewhat related to hardness is another mechanical property
toughness, which is a material's ability to resist breakage from forceful impact. The
toughness of natural diamond has been measured as 50–65
MPa·m1/2.{{contradictory inline|reason=Unit of toughness as given at the article on toughness is newton-metres per cubic metre, dimensionally equivalent to newtons per square metre i.e. pascals. What is this factor of m^{1/2} doing here? Should we actually be talking about and linking to
Fracture toughness (which unfortunately doesn't have a discussion of units)?|date=October 2023}} This value is good compared to other ceramic materials, but poor compared to most engineering materials such as engineering alloys, which typically exhibit toughness over 80MPa·m1/2. As with any material, the macroscopic geometry of a diamond contributes to its resistance to breakage. Diamond has a
cleavage plane and is therefore more fragile in some orientations than others.
Diamond cutters use this attribute to cleave some stones before faceting them. This exceptionally high value, along with the hardness and transparency of diamond, are the reasons that
diamond anvil cells are the main tool for high pressure experiments. These anvils have reached pressures of . Much higher pressures may be possible with
nanocrystalline diamonds. with a maximum local tensile stress of about , very close to the theoretical limit for this material.
Electrical conductivity Other specialized applications also exist or are being developed, including use as
semiconductors: some
blue diamonds are natural semiconductors, in contrast to most diamonds, which are excellent
electrical insulators. The conductivity and blue color originate from boron impurity. Boron substitutes for carbon atoms in the diamond lattice, donating a hole into the
valence band. Substantial conductivity is commonly observed in nominally
undoped diamond grown by
chemical vapor deposition. This conductivity is associated with
hydrogen-related species adsorbed at the surface, and it can be removed by
annealing or other surface treatments. Thin needles of diamond can be made to vary their electronic
band gap from the normal 5.6 eV to near zero by selective mechanical deformation. High-purity diamond wafers 5 cm in diameter exhibit perfect resistance in one direction and perfect conductance in the other, creating the possibility of using them for quantum data storage. The material contains only 3 parts per million of nitrogen. The diamond was grown on a stepped substrate, which eliminated cracking.
Surface property Diamonds are naturally
lipophilic and
hydrophobic, which means the diamonds' surface cannot be wet by water, but can be easily wet and stuck by oil. This property can be utilized to extract diamonds using oil when making synthetic diamonds. However, when diamond surfaces are chemically modified with certain ions, they are expected to become so
hydrophilic that they can stabilize multiple layers of
water ice at
human body temperature. The surface of diamonds is partially oxidized. The oxidized surface can be reduced by heat treatment under hydrogen flow. That is to say, this heat treatment partially removes oxygen-containing functional groups. But diamonds (sp3C) are unstable against high temperature (above about ) under atmospheric pressure. The structure gradually changes into sp2C above this temperature. Thus, diamonds should be reduced below this temperature.
Chemical stability At room temperature, diamonds do not react with any chemical reagents including strong acids and bases. In an atmosphere of pure oxygen, diamond has an
ignition point that ranges from to ; smaller crystals tend to burn more easily. It increases in temperature from red to white heat and burns with a pale blue flame, and continues to burn after the source of heat is removed. By contrast, in air the combustion will cease as soon as the heat is removed because the oxygen is diluted with nitrogen. A clear, flawless, transparent diamond is completely converted to carbon dioxide; any impurities will be left as ash. Heat generated from cutting a diamond will not ignite the diamond, and neither will a cigarette lighter, but house fires and blow torches are hot enough. Jewelers must be careful when molding the metal in a diamond ring. Diamond powder of an appropriate grain size (around 50microns) burns with a shower of sparks after ignition from a flame. Consequently,
pyrotechnic compositions based on
synthetic diamond powder can be prepared. The resulting sparks are of the usual red-orange color, comparable to charcoal, but show a very linear trajectory which is explained by their high density. Diamond also reacts with fluorine gas above about .
Color in
Washington, D.C. Diamond has a wide
band gap of corresponding to the deep
ultraviolet wavelength of 225nanometers. This means that pure diamond should transmit visible light and appear as a clear colorless crystal. Colors in diamond originate from lattice defects and impurities. The diamond crystal lattice is exceptionally strong, and only atoms of
nitrogen,
boron, and
hydrogen can be introduced into diamond during the growth at significant concentrations (up to atomic percents). Transition metals
nickel and
cobalt, which are commonly used for growth of synthetic diamond by high-pressure high-temperature techniques, have been detected in diamond as individual atoms; the maximum concentration is 0.01% for nickel and even less for cobalt. Virtually any element can be introduced to diamond by ion implantation. Nitrogen is by far the most common impurity found in gem diamonds and is responsible for the yellow and brown color in diamonds. Boron is responsible for the blue color. Color in diamond has two additional sources: irradiation (usually by alpha particles), that causes the color in green diamonds, and
plastic deformation of the diamond crystal lattice. Plastic deformation is the cause of color in some brown and perhaps pink and red diamonds. In order of increasing rarity, yellow diamond is followed by brown, colorless, then by blue, green, black, pink, orange, purple, and red. In May 2009, a
blue diamond fetched the highest price per carat ever paid for a diamond when it was sold at auction for 10.5 million Swiss francs (6.97 million euros, or US$9.5 million at the time). That record was, however, beaten the same year: a vivid pink diamond was sold for US$10.8 million in Hong Kong on December 1, 2009.
Clarity Clarity is one of the 4C's (color, clarity, cut and carat weight) that helps in identifying the quality of diamonds. The
Gemological Institute of America (GIA) developed 11 clarity scales to decide the quality of a diamond for its sale value. The GIA clarity scale spans from Flawless (FL) to included (I) having internally flawless (IF), very, very slightly included (VVS), very slightly included (VS) and slightly included (SI) in between. Impurities in natural diamonds are due to the presence of natural minerals and oxides. The clarity scale grades the diamond based on the color, size, location of impurity and quantity of clarity visible under 10x magnification. Inclusions in diamond can be extracted by optical methods. The process is to take pre-enhancement images, identifying the inclusion removal part and finally removing the diamond facets and noises.
Fluorescence (top) and normal light (bottom) Between 25% and 35% of natural diamonds exhibit some degree of fluorescence when examined under invisible long-wave ultraviolet light or higher energy radiation sources such as X-rays and lasers. Incandescent lighting will not cause a diamond to fluoresce. Diamonds can fluoresce in a variety of colors including blue (most common), orange, yellow, white, green and very rarely red and purple. Although the causes are not well understood, variations in the atomic structure, such as the number of nitrogen atoms present are thought to contribute to the phenomenon.
Thermal conductivity Diamonds can be identified by their high thermal conductivity (900–). Their high
refractive index is also indicative, but other materials have similar refractivity. == Geology ==