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PeriodicDeck

Element 6 · reactive nonmetal

Carbon (C)


Every diamond in every ring is thermodynamically doomed. At room temperature and ordinary pressure, graphite is the stable form of carbon and diamond is not; the conversion releases energy and is entirely spontaneous in the thermodynamic sense. It simply never happens, because turning diamond into graphite requires breaking every carbon-carbon bond in the crystal at once and rebuilding them in a different geometry. The barrier is so high that the expected waiting time comfortably exceeds the age of the universe. Diamonds are metastable, which is a much more interesting status than permanent.

Two arrangements of one atom, and nothing in common

The difference between the two familiar forms is a matter of how many neighbours each atom commits to. In diamond every carbon bonds tetrahedrally to four others in a rigid three-dimensional lattice. In graphite each atom bonds to three, forming flat hexagonal sheets held to one another only by weak dispersion forces.

The consequences are almost comically divergent. Graphite is soft enough to leave a mark on paper, because the sheets slide; diamond is the hardest natural material known. Graphite conducts electricity along the plane of its sheets, because the fourth electron on each atom is delocalised across the layer; diamond is an excellent electrical insulator with a band gap of about 5.5 electronvolts.

The property that most surprises people is thermal. Diamond conducts heat better than any other bulk material at room temperature — around five times better than copper — not by moving electrons, which it cannot do, but by carrying phonons through an exceptionally stiff and light lattice with very little to scatter them. This is why a jeweller's "diamond tester" is not an optical instrument at all. It is a thermal probe, and it works because no imitation stone can dump heat that fast.

Natural diamonds form at depths of 150 kilometres and more and reach the surface only in kimberlite pipes, whose magma ascends fast enough that the carbon has no time to relax into graphite on the way up. A slower eruption would deliver soot.

Why nothing else can build a molecule this large

Carbon's real distinction is catenation: its willingness to bond to itself indefinitely, in chains, branches and rings, without the structure becoming unstable. Tens of millions of carbon compounds are catalogued. No other element approaches this.

Silicon sits directly below and is often floated as an alternative basis for chemistry, but the numbers do not support it. The silicon-silicon single bond is markedly weaker than the carbon-carbon one, and long silicon chains hydrolyse readily. The decisive difference is in the oxides. Carbon forms strong double bonds to oxygen and produces carbon dioxide, a small molecule that is a gas at ordinary temperatures and dissolves in water. Silicon does not double-bond comfortably at all; its oxide polymerises into a network solid, which is sand. An organism running on silicon would exhale rock.

That distinction is exactly why carbon can cycle. A carbon atom can be part of a tree, then part of the atmosphere, then dissolved in the ocean, then locked in limestone, and back again, because every one of those forms is chemically accessible from the others.

The isotope that dates the dead, and the two accidents in its record

Carbon-14 is produced continuously in the upper atmosphere when cosmic-ray neutrons strike nitrogen-14. It mixes into the carbon dioxide reservoir, enters living tissue through photosynthesis and the food chain, and then, from the moment an organism dies and stops exchanging carbon with its surroundings, decays with a half-life of about 5,730 years. Willard Libby worked this out at Chicago in the late 1940s and took the 1960 chemistry Nobel for it.

Two human interventions have written themselves into the atmospheric record. Burning coal and oil releases carbon so old that it contains no carbon-14 at all, diluting the atmospheric fraction — the Suess effect, which makes anything grown in the industrial era read as slightly older than it is. Then atmospheric nuclear testing between the mid-1950s and the 1963 test ban did the opposite, roughly doubling atmospheric carbon-14 before the level began falling back as the excess mixed into the oceans.

That falling curve is steep, well measured and unambiguous, which makes it a clock accurate to about a year for anything that grew between 1955 and the present. Jonas Frisén's group in Stockholm used it on human tissue, dating the carbon in the DNA of individual cell types to establish when those cells were born. The finding that neurons in the cerebral cortex carry the same carbon-14 signature as the year of the person's birth is direct physical evidence that they are never replaced.

The atom the mole was built on

From 1961 until 2019, the atomic mass unit was defined as exactly one twelfth of the mass of an unbound carbon-12 atom at rest in its ground state.

That definition settled a genuinely awkward split. Chemists had been using oxygen as the reference and assigning 16 to the natural isotopic mixture; physicists had been assigning 16 to oxygen-16 specifically. The two scales differed by roughly 275 parts per million, which is nothing in a teaching laboratory and a serious problem in precision work. Carbon-12 was chosen as the compromise because it was close enough to the old chemical scale to avoid rewriting every published table, and because carbon-12 is a clean, abundant, easily handled reference for mass spectrometry.

The 2019 revision of the SI cut the link, fixing the Avogadro constant to an exact number instead. Carbon-12's mass is now something to be measured rather than something defined, though the value remains within experimental reach of exactly 12 by design.

Fred Hoyle predicted a nuclear energy level because he existed

Stars fuse hydrogen into helium easily. Getting from helium to carbon is much harder, because two helium nuclei make beryllium-8, which falls apart again in about 10⁻¹⁶ seconds. A third helium nucleus has to arrive within that window.

In 1953 Fred Hoyle argued that the reaction could only be fast enough if carbon-12 happened to have an excited state at almost exactly the combined energy of beryllium-8 plus a helium nucleus — a resonance that would let the reaction proceed far more readily than chance allowed. His entire evidence was that carbon exists in quantity and that he was made of it. He pressed William Fowler's group at Caltech to look, they looked reluctantly, and the state was there, at 7.65 MeV. It has been called the Hoyle state ever since and remains the most-cited example of a successful anthropic prediction.

What the world does with it

Overwhelmingly, burns it. Coal consumption alone runs to billions of tonnes a year, and that is before oil and gas. Every other application is small by comparison.

Among the non-fuel uses, the largest by tonnage is carbon black — fine soot made by incomplete combustion of heavy petroleum fractions — and roughly nine tenths of it goes into rubber, mostly tyres, where it is not a pigment but a reinforcing filler that multiplies the wear life of the tread. Graphite is the second: natural and synthetic graphite together supply the anodes of essentially every lithium-ion cell in production, a demand that has grown fast enough to make graphite a strategic commodity, and China's introduction of export licensing on graphite products in 2023 was felt immediately by battery manufacturers elsewhere.

And in steel, carbon is a trace ingredient that changes everything. Iron with almost no carbon is soft; iron with a few tenths of a per cent, quenched, is hard enough to hold a cutting edge. The carbon atoms sit in the interstices of the iron lattice and jam the planes that would otherwise slip past one another.

Two Nobel prizes for shapes nobody expected

Harold Kroto, Robert Curl and Richard Smalley found C₆₀ in 1985 while trying to simulate the chemistry of carbon-rich stars, and named the closed cage buckminsterfullerene for the architect whose geodesic domes it resembles. They shared the 1996 chemistry prize.

Graphene — a single sheet of graphite, one atom thick — was long assumed to be impossible, on the theoretical grounds that two-dimensional crystals should be thermodynamically unstable. Andre Geim and Konstantin Novoselov isolated it in Manchester in 2004 using adhesive tape to peel layers off a graphite block, and had the physics Nobel six years later. Geim remains the only person to hold both a Nobel and an Ig Nobel, the latter for magnetically levitating a live frog.

Isotopes of Carbon

2 isotopes of Carbon occur naturally, in the proportions below.

Isotopes of Carbon with relative atomic mass and natural abundance
IsotopeRelative atomic massNatural abundance
12C1298.93%
13C13.00335483507(23)1.07%
14C14.0032419884(40)none

6

C

Carbon

reactive nonmetal

Standard atomic weight
[12.0096, 12.0116]an interval, not a single value — the conventional value 12.011 is used in calculations
Group / period / block
14 · 2 · p
Electron configuration
[He] 2s2 2p2
Electrons per shell
2, 4
State at 20 °C
solid
Melting point
3823 K · 3550 °C
Boiling point
4098 K · 3825 °C
Density
2.267 g/cm³
Electronegativity
2.55 (Pauling)
First ionisation energy
11.26 eV
Common oxidation states
+4, +2, -4
Discovery
known since antiquity

Hazard facts

No flag in this site’s hazard vocabulary applies to Carbon. That is not the same as harmless: it means none of the eleven categories used here — reactive with water, pyrophoric, flammable, oxidising, corrosive, irritant, acutely toxic, accumulating in the body, carcinogenic, asphyxiant or radioactive — is on record for the element itself.

These are properties of the element, stated as facts. Nothing on this site describes how to handle or work with any substance.

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