Table of Contents (click to expand)
- What Is A Diamond, Atom For Atom?
- Why Does Carbon "Prefer" To Be Graphite, Not Diamond?
- What Pressure And Heat Does It Actually Take To Make Diamond?
- How Do You Squeeze A Diamond Into Existence?
- How Do You Grow A Diamond One Atom At A Time?
- So How Much Energy Does Each Method Really Use?
- Why Would The "High-Tech" Method Cost More Energy?
- So, Could You Ever Really "Grow" A Diamond?
A modern press grows one carat of gem-quality diamond on about 36 kilowatt-hours of electricity, roughly a quarter to a third of what mining one carat costs. That figure assumes cheap open-circuit cooling, though, and roughly doubles on a press that runs chillers. Growing the same carat by depositing it atom by atom out of a hot gas is the route that refuses to give one answer: commercial reactors land between 28 and 77 kilowatt-hours, undercutting every mine on the list, while one research rig on closed-loop cooling ran past 200, nearly half of it spent on refrigeration rather than on making diamond. No bacterium, enzyme, or living cell can supply the crushing pressure either lab method depends on, so no diamond has ever been grown by biology, and none can be today.
Somewhere on Reddit's r/AskChemistry, someone asked a strange, ambitious question. Could you engineer bacteria to bond carbon atoms together? Could you grow a diamond, the way an oyster grows a pearl?
It is a good question. It is also wrong, in an interesting way. A diamond does not form like a pearl does. A pearl just needs time and a mild chemical nudge. A diamond needs a squeeze so violent that biology has no tool for it. Not in 3.7 billion years of evolution has one shown up.
To see why, start with what a diamond actually is. Not what it looks like. What it is, atom by atom.
What Is A Diamond, Atom For Atom?
A diamond and the graphite inside a pencil are made of one thing: carbon. Nothing else. The only difference is how the atoms connect. That single difference is why one scratches glass and the other rubs off on paper.
In diamond, every carbon atom bonds to four neighbors. Each of those neighbors bonds to four more. The pattern repeats in every direction, forming one unbroken 3D framework. Picture a milk crate welded solid, every strut locked to the next, no give anywhere. That rigidity makes diamond the hardest known natural material. ScienceABC has covered this before.
Graphite uses the same atoms on a different plan. Each carbon bonds to only three neighbors. The bonds form flat hexagonal sheets, like chicken wire. The sheets themselves are strong. Sheet to sheet, though, weak forces hold them together, the way loose pages sit stacked in a book. Push sideways and the pages slide. That is the entire reason pencil "lead" rubs off. You are not breaking carbon bonds. You are peeling sheets off each other. ScienceABC has explained this bonding contrast in full. Hold onto this one idea for everything that follows: diamond is a welded 3D cage. Graphite is a loose stack of flat sheets.

Why Does Carbon "Prefer" To Be Graphite, Not Diamond?
Here is the part that trips people up. At room temperature, graphite is more stable than diamond. Not the other way around. If a diamond ever settled into its lowest-energy state, it would turn into a heap of graphite.
The reason lives in a number chemists call Gibbs free energy. It tells you which of two arrangements a system prefers. ScienceABC has an explainer on how it works. The short version is one equation:
G = H − TS
G is the free energy. H is the heat locked into the bonds. T is temperature. S is entropy, a measure of disorder. Lower G wins.
At room temperature, real numbers for carbon tell the story. Graphite sits about 2.9 kilojoules per mole below diamond (Chemistry LibreTexts). Graphite wins, by a small but real margin.
So why doesn't your ring dissolve into pencil shavings? Because winning on paper is not the same as winning in practice. Getting from diamond to graphite means breaking carbon-carbon bonds, and each one costs about 356 kilojoules per mole (Chemistry LibreTexts). Every route between the two runs through breaking a great many of them at once, which puts an enormous hump in the way. At room temperature, nothing has the energy to climb it. So the diamond just sits there. It holds a shape it "shouldn't" want, for what amounts to forever. Chemists have a word for this: metastable. Diamonds, in the strictest sense, are not forever. They are just patient.

What Pressure And Heat Does It Actually Take To Make Diamond?
If graphite wins at everyday conditions, when does diamond take over? Only once you leave everyday conditions behind.
Squeeze carbon hard enough, and the free-energy math flips. High pressure punishes graphite's loose sheets. It punishes diamond's dense, welded cage far less. Past a certain point, diamond becomes the shape carbon prefers.
That crossover point is not fixed. It climbs as things get hotter (Oganov et al., Reviews in Mineralogy & Geochemistry, 2013). At the 1,300 to 1,600 °C where industrial presses and the deep mantle both operate, the line sits at roughly 5 to 6 gigapascals. One gigapascal is about 10,000 times ordinary air pressure. This is not a gentle nudge.
Being the stable form and being the form that actually turns up are two different things, though, and a 2025 study makes the point beautifully. It simulated carbon crystallizing straight out of a melt at 3,650 to 4,100 kelvin, and found graphite still winning that race at pressures up to 15 gigapascals, deep inside territory where diamond is the more stable phase. Only at 17 did diamond take over (Donadio et al., Nature Communications, 2025). Those are nucleation rates, not stability: a question of which phase gets organized first, not which one wins on paper. The same simulations place the triple point, where graphite, diamond, and molten carbon all meet at once, near 10.5 gigapascals and 4,650 kelvin, though the authors' second model puts it considerably higher. Carbon, it turns out, is stubborn about doing the thermodynamically obvious thing.
Nature runs this experiment for real. It happens about 150 to 190 kilometers under your feet, in the roots of ancient continents, where pressures run 5 to 6 gigapascals (GIA). That is just the local weather down there. Most mined diamonds formed in that layer, and many sat through an immense stretch of geologic time before anything disturbed them. A rarer class, called sublithospheric or superdeep, formed much further down still, from 300 kilometers to more than 700 (Timmerman et al., Nature, 2023).
Getting out is the hard part. At those depths diamond is the stable form, so sitting still costs it nothing. The danger is the ride up, where the pressure falls away and diamond goes back to being the merely metastable one. A volcanic pipe called a kimberlite solves that by moving fast, spending so little time in the danger zone that there is no opportunity to turn into graphite. Take the scenic route and you arrive with a pipe full of pencil lead.
Lab methods have to reproduce that same pressure-and-heat neighborhood on a factory floor. There are two different ways to do it.

How Do You Squeeze A Diamond Into Existence?
The first lab method is called high-pressure high-temperature growth, or HPHT. It is brute force, industrialized.
A press clamps a small chamber of graphite between anvils. Three designs are common: the belt press, the cubic press, and the split-sphere, or BARS, press. Each squeezes the chamber to roughly 5 to 6 gigapascals. Each also heats it to about 1,300 to 1,600 °C (GIA, "HPHT and CVD Diamond Growth Processes"). That reproduces the mantle's own conditions. It happens in a machine roughly the size of a delivery truck, not 150 kilometers of solid rock.
A molten metal catalyst, usually iron, nickel, or cobalt, sits inside the chamber too. This is the quiet trick that makes the whole process work. Molten metal dissolves graphite far faster than solid graphite converts on its own. Carbon atoms migrate through the melt and settle onto a tiny diamond seed. Left running for days, the seed grows, layer by layer, into a finished stone. ScienceABC has covered this same mechanism before, in a piece on whether diamonds last forever. HPHT is a kimberlite pipe's trick, compressed from geologic time down into a single work week.

How Do You Grow A Diamond One Atom At A Time?
The second method drops nearly all of the crushing pressure. That should be impossible, given everything above. It works anyway, because it cheats. Not on the physics. On the chemistry.
Chemical vapor deposition, or CVD, fills a chamber with methane and hydrogen gas. The pressure sits close to a single atmosphere. That is nowhere near the gigapascal range HPHT and nature both need. A microwave source, tuned to 2.45 gigahertz, turns that gas into a glowing plasma. The plasma rips methane apart and frees individual carbon atoms. Those atoms drift down and stick to a heated seed wafer, sitting at roughly 900 to 1,200 °C (GIA). ScienceABC mentioned this same technique, in an article on how to tell if a diamond is real. A CVD stone can carry its own faint tells under a gemologist's loupe.
Here is the chemistry doing pressure's job. The hydrogen in that plasma is not a bystander. Atomic hydrogen attacks any graphite-like bonds that try to form on the growing surface. It leaves diamond's tighter bonds alone. Graphite keeps forming and keeps getting stripped off, atom by atom. Only the diamond-style bonds survive and pile up. It is less like squeezing a diamond into shape. It is more like printing one, one atomic layer at a time, at roughly one to ten micrometers an hour. Growing a usable crystal this way takes days to weeks, longer than HPHT needs.

So How Much Energy Does Each Method Really Use?
Now for the number behind the Reddit question. What does any of this cost, in electricity, per carat?
A 2021 study in the journal Energies lined up all three routes side by side (Zhdanov et al., 2021). It is worth knowing what kind of study it is before leaning on it. The authors metered their own two machines, took the mining numbers from company sustainability reports, and picked up the rest secondhand. It is a careful estimate, not a full life-cycle assessment, and it remains the most detailed public comparison of its kind.
A modern HPHT press, cooled by an open water circuit, uses about 36 kilowatt-hours per carat. Mining runs higher: ALROSA about 96 kilowatt-hours per carat, De Beers about 150.
CVD is the one that refuses to give a single answer. The paper's own laboratory reactor, a small research rig on a closed water-cooling loop, needed roughly 215 kilowatt-hours per carat, and the authors call it their least energy-efficient case. About half of that went to the chiller alone. Commercial reactors do dramatically better. IIa Technology comes in at 77, undercutting every mining operation on the list, and the lowest figure anywhere in the table, 28, belongs to Apollo Diamond, a Boston company that grew its crystals by CVD.
Two rows in that table are filed under the wrong heading, and since almost everyone who quotes it repeats the mistake, it is worth flagging. The paper lists Apollo under HPHT, though Apollo was a CVD outfit from the day it opened. It also lists "Ekati Mine" at 143 kilowatt-hours as a CVD grower. Ekati is a diamond mine in Canada's Northwest Territories that has never run a reactor in its life, and 143 lands exactly where you would expect a third mining operation to land. Both figures reached the paper secondhand, from a single web page. Read the table as three miners and four growers, not the other way round.
One more thing keeps this from being a clean race. That 36 kilowatt-hour HPHT figure assumes an open cooling circuit, the arrangement most Chinese growers use, where a shared reservoir cools an entire hall of presses. The authors note that a closed circuit needs chillers and would roughly double the energy use. A chilled press therefore lands near 72 kilowatt-hours per carat, which is a tie with IIa's 77, not a rout. HPHT still looks like the cheaper route on this evidence. The size of its lead just depends on a plumbing decision.
Sit with that spread for a second, because it is more interesting than a straight inversion. HPHT sounds like a medieval torture device, and it comes out cheap. CVD sounds delicate and futuristic, and what it actually costs turns almost entirely on which machine you use and how that machine is cooled. The authors' own conclusion is that CVD can reach "energy efficiency similar to or even higher than mining" given the right conditions. "Lab-grown" and "energy-efficient" are not the same claim, in either direction.

Why Would The "High-Tech" Method Cost More Energy?
The paradox stops looking strange once you check two things: how much power each machine actually draws, and how much diamond it hands back.
Start with the press. Its hydraulic pumps are the dramatic part, 29.5 kilowatts of them, but they only run flat out for ten or fifteen minutes at the beginning, and after that they wake up for half a minute at a time to top the pressure back up. Averaged across a whole cycle, the entire installation sits at about 5 kilowatts, most of it just keeping the chamber hot. Twelve days later it hands over roughly 40 carats.
Now the reactor. A 2.45 gigahertz CVD rig pulls about 8.8 kilowatts and holds it there, continuously: 3.6 for the magnetron, 1 for the hydrogen station, 3.7 for the chiller, and a little for the lights. A month later it hands over roughly 30 carats.
So the press is not the brute and the reactor is not the gentle one. The press draws less power and returns about three times as much diamond per day. That is the whole gap, and it has nothing to do with one method being violent and the other patient. Notice, too, which line item is biggest on the reactor: the chiller, drawing more than the magnetron doing the actual work. A good share of what a CVD diamond costs in electricity never goes into making diamond at all. It goes into refrigeration.

So, Could You Ever Really "Grow" A Diamond?
Which brings us back to the Reddit thread that started this. Could bacteria, or some engineered cell, take over from the press and the plasma reactor?
No. Not "not yet." Not "unlikely." Just no. Every route to diamond here needs one thing. Either gigapascal-scale pressure, or a chemical shortcut around it. HPHT's anvils. CVD's plasma. The mantle's own slow patience. All three. No known enzyme, motor protein, or cell membrane can do it. None can generate anything close to that pressure at the scale of a single molecule. This is not a live research question waiting on more funding. It is a wall. Biology has no tool for it, now or on any visible horizon.
What the Reddit poster stumbled onto instead was an underappreciated fact. Roughly 97% of the industrial diamond the United States uses today is already synthetic, and domestic manufacturers turn out around 160 million carats of it a year (USGS Mineral Commodity Summaries, Diamond). Almost none of that is the kind of stone this article has been describing. It is bort, grit, dust and powder, the abrasive bonded onto saw blades and drill bits, and American producers made no industrial diamond stone whatsoever in 2025. Grit is press territory: crush what an HPHT run gives you and sieve it by size, which is exactly the industrial job those presses were built for in the 1950s. The bacteria were never going to be the interesting part of this story. The machines quietly out-producing a hundred and fifty kilometers of mantle rock always were.
References (click to expand)
- A Comparative Analysis of Energy and Water Consumption of Mined versus Synthetic Diamonds. Zhdanov et al., Energies, 2021
- Metastability and Ostwald Step Rule in the Crystallisation of Diamond and Graphite from Molten Carbon. Donadio et al., Nature Communications, 2025 (PMC)
- HPHT and CVD Diamond Growth Processes. Gemological Institute of America (GIA)
- Mineral Commodity Summaries 2026, Diamond (Industrial). U.S. Geological Survey
- Day 32: Gibbs Free Energy and Work, Kinetic Metastability. Chemistry LibreTexts
- Update on Laboratory-Grown Diamonds — Gems & Gemology, Summer 2024 (GIA)
- Structure, Bonding, and Mineralogy of Carbon at Extreme Conditions. Oganov et al., Reviews in Mineralogy & Geochemistry, 2013
- Sublithospheric Diamond Ages and the Supercontinent Cycle. Timmerman et al., Nature, 2023 (PMC)







