Turbulent orange gas streams in three primordial dark matter halos spiral into dense clumps forming the first stars.

Were the First Stars Shaped by Turbulence?

How Turbulence Shaped the Universe’s First Stars

What if the very first stars were never the lonely giants we pictured for thirty years? Welcome, fellow stargazers. We’re glad you’re here. Today we walk you through a 2026 study that rewrites the opening scene of cosmic history. Stay with us to the end, and you’ll see how a single force—turbulence—may have quietly reshaped the family tree of every star you’ve ever seen.

Short answer: New high-resolution simulations show that supersonic turbulence, stirred up as gas fell into dark matter halos, broke the first star-forming clouds into many clumps of roughly 2.6 to 66.5 solar masses. That means the Universe’s first stars (Population III) were likely smaller and far more varied than the 40–500 solar-mass giants once assumed.

What were the Universe’s first stars?

Rewind to roughly 300 million years after the Big Bang. Space was cold and dark. Hydrogen and a little helium drifted with no place to go. Then gravity pulled this gas into pockets of dark matter, and the first stars switched on.

We call these stars Population III, or Pop III for short. They formed from pristine gas with no heavy elements at all. Astronomers think they lived inside dark matter halos weighing 100,000 to a million Suns. Those halos were the cradles where everything began.

One detail matters more than any other. In today’s clouds, carbon and oxygen radiate heat away fast, letting gas cool and shrink into modest stars. The early Universe had none of that. The only working coolant was molecular hydrogen, and it works poorly, cooling gas only to about 200 kelvin.

Why did we think the first stars were giants?

Here’s the logic that ruled for decades. Cooling sets a threshold called the Jeans mass. A gas cloud has to gather more than that mass before gravity wins and collapse begins. Weak cooling pushes the Jeans mass up. A higher threshold means bigger building blocks.

Early theory ran with this. It predicted Pop III stars of 40 to 500 solar masses—monsters far beyond anything common in the Milky Way today. The picture was tidy: one calm cloud, one smooth collapse, one enormous star.

Newer work started to crack that tidiness. Simulations began producing a wide spread of masses, anywhere from a thousandth of a Sun to a hundred Suns, once turbulence and stellar feedback entered the math. The giants weren’t wrong, just incomplete.

What did the new simulations actually do?

A team led by Meng-Yuan Ho at Academia Sinica in Taipei pushed the question further. Their 2026 paper in The Astrophysical Journal simulated 15 separate minihalos, each weighing between 100,000 and 7.7 million Suns, at redshifts of about 17 to 20.

They started from IllustrisTNG, a large cosmological simulation, then zoomed in hard. Using a particle-splitting trick, they boosted the resolution by a factor of 100,000. That let them track gas on scales smaller than a single light-year—down to 0.05 parsecs for gas particles weighing just 0.2 Suns.

Why does resolution matter so much? Older studies sharpened only the tiny core of each cloud and left the wider halo blurry. The blur hid the very thing that drives the action: gas streaming in from far out and crashing together. This study kept the whole region sharp.

What is supersonic turbulence, and why does it matter?

Picture a calm pond versus a river plunging over rocks. The pond is smooth. The river is chaotic, full of eddies and shocks. That chaos is turbulence. When the flow moves faster than its own sound speed, we call it supersonic.

The ratio of gas speed to sound speed has a name: the Mach number. A jet breaking the sound barrier sits at Mach 1. The early gas in these halos ran well past that.

v / cs

= Mach number v = gas speed relative to the halo cs = local sound speed

The sound speed itself depends on how hot the gas is and what it’s made of. Colder gas carries sound slowly, so even gentle motions can turn supersonic. Here’s the relation the team used:

cs= γRTμmH

γ = adiabatic index (5/3 for ideal monatomic gas) R = ideal gas constant T = gas temperature μ = mean molecular weight mH = hydrogen mass

Where does the energy come from? Gravity. As gas falls into a dark matter well, it picks up speed. Streams arrive from many directions at once, collide near the center, and stir the cloud into a froth. No stars needed—the halo itself does the mixing.

How fast and chaotic was the gas?

The numbers tell a clear story. Across the sample, the characteristic Mach number ran from about 1.8 to 4.2. Heavier halos churned harder, with deeper gravity and faster infall. The link was steady: the mean Mach number climbed by 1 for every 2.8 million solar masses of extra halo mass.

The team picked three halos to compare across the low, middle, and high end.

Three representative minihalos at the end of each simulation. Data: Ho, Chen & Tung (2026).
HaloVirial mass (M☉)Virial radius (pc)Mass class
A4.9 × 105121.8Low
H2.54 × 106213.3Intermediate
O7.71 × 106311.7High

Most halos weren’t uniform. A small slice of gas raced much faster than the rest. In the heaviest halo, peak Mach numbers touched roughly 24, and the conclusion notes velocities reaching near Mach 30. Only about 0.01 to 0.1 percent of the gas hit Mach 10 or more—but in a million-solar-mass halo, that still adds up to around 1,000 Suns’ worth of fast-moving gas.

When the team measured how the turbulent energy spread across scales, it matched the classic Kolmogorov pattern seen in everyday flows on Earth. The same math that describes smoke curling off a candle described gas swirling in a halo 13 billion years ago. Turbulence, it turns out, plays by familiar rules.

How did turbulence break the cloud into clumps?

This is the heart of the matter. A calm cloud collapses into one dense knot. A turbulent cloud can’t. Shocks compress some patches and rarefy others. Spherical symmetry shatters. The gas tears into filaments and clumps.

Each halo ended the simulation with at least one dense, gravitationally bound clump already collapsing. Several halos held more. The clump masses ranged from a slim 2.6 Suns to a hefty 66.5 Suns—and every one of them topped its local Jeans mass, the sign that collapse is locked in.

Selected dense clumps and their properties. A clump’s mass caps the mass of any star it can build. Data: Ho, Chen & Tung (2026), Table 2.
HaloClump mass (M☉)Jeans mass (M☉)Peak density (cm−3)Temp (K)
H2.622.372.90 × 106130
A13.792.991.14 × 106111
N61.960.811.47 × 108236
G66.500.528.98 × 108322

A clump can’t grow a star heavier than the gas it holds. So these masses set ceilings. Instead of one 500-Sun colossus per cloud, we get a scattered family—some chunky, some slight. Here’s the old picture set beside the new one.

The shift in how we picture the first stars.
FeatureOlder viewWhat the new work shows
Typical Pop III mass40–500 M☉ giants2.6–66.5 M☉ clumps, wide spread
Cloud environmentCalm, smooth collapseTurbulent, supersonic, fragmented
Role of turbulenceSubsonic, minorSupersonic (Mach 2–5), central
Stars per cloudOne massive starMultiple clumps, several possible stars

Does this solve the metal-poor star puzzle?

There’s a stubborn riddle in astronomy. If the first stars were all giants, most would have died young in violent supernovae, flooding space with heavy elements. The next generation should then carry a strong chemical signature.

The trouble is, many ancient stars in the Milky Way carry the faint fingerprint of Pop III parents—yet they’re strikingly poor in metals. That low metallicity hints their ancestors weren’t the giants we assumed.

Turbulence offers a way out. If the first clouds fragmented into smaller, less explosive stars, they spread fewer metals. Their descendants would then look as metal-poor as we actually observe. The chaos in the cradle leaves a mark we can still read today.

What can JWST and ancient stars tell us?

We can’t photograph a Pop III star. They lived briefly, sat at enormous distances, and faded fast. Even the James Webb Space Telescope can’t catch one directly.

We can read their echoes, though. The mass of the first stars shaped the heat, light, and chemistry of the earliest galaxies—the very objects JWST hunts at the edge of time. Bigger first stars push harder on their surroundings, choking off later star birth. Their size sculpted the young galaxies and their bright cores.

The metal-poor stars near us act as a second archive. Their chemical mix preserves the recipe of the first supernovae. Read carefully, those abundances point back to the masses of stars that vanished long ago.

What did the researchers leave out?

Good science names its limits, and this team is honest about theirs. They left out stellar feedback, since the chosen halos held no earlier stars. They also set aside baryon–dark matter streaming velocities, leftover ripples from the early Universe.

Both choices were deliberate. They wanted to isolate one effect: turbulence born purely from gas falling into gravity wells. Add streaming motions or radiation back in, and the team expects the turbulence would grow stronger, not weaker. The clumpy picture would likely hold, perhaps sharpen.

Science rarely flips a story overnight. It revises, the way our model of the cosmos has been revised many times—as far back as the move to a Sun-centered system. This study is one careful revision, not the final word. The clumps still need to be followed all the way down to glowing stars, which takes even sharper simulations.

So what changes?

Let’s gather the threads. The first stars formed inside dark matter halos from clean hydrogen and helium. Gas poured in, collided, and turned supersonic, with Mach numbers near 2 to 5 and spikes toward 30. That turbulence broke each cloud into clumps of 2.6 to 66.5 Suns rather than one giant. The result is a richer, messier, more believable origin story—one that finally fits the metal-poor stars we still see overhead.

It’s worth sitting with the bigger idea. The calm beginning we imagined was mostly an artifact of blurry models. Sharpen the picture, and chaos appears—the same chaos that stirs rivers, clouds, and coffee. Even the dawn of starlight, it seems, was turbulent. The next time you look up, remember that the gentle points of light above were born in a storm. We invite you back to FreeAstroScience.com to keep questioning, keep looking, and keep your mind switched on.

Frequently asked questions

What are Population III stars?

Population III (Pop III) stars are the Universe’s first generation of stars. They formed from pristine gas of hydrogen and a little helium, with no heavier elements, inside dark matter halos roughly 100,000 to a million times the Sun’s mass, about 300 million years after the Big Bang.

Why did scientists once think the first stars were so massive?

The early Universe lacked the elements that cool gas efficiently today. Weak cooling raised the Jeans mass—the amount of gas needed before gravity can win—so collapse favored very large stars. Early theory predicted Pop III masses of 40 to 500 Suns.

How does turbulence change the first stars’ masses?

Supersonic turbulence breaks the gas cloud’s smooth, spherical collapse. Instead of one giant knot, the gas fragments into many clumps. In the 2026 simulations these clumps spanned 2.6 to 66.5 solar masses, suggesting first stars were smaller and more varied than the giants once assumed.

What is the Mach number, and how high did it get?

The Mach number is the ratio of gas speed to the local sound speed; above Mach 1 the flow is supersonic. In these minihalos the characteristic Mach number ran from 1.8 to 4.2, rising with halo mass, while a small fraction of gas reached values near 24 to 30.

Can the James Webb Space Telescope see Population III stars directly?

No. Pop III stars were short-lived, extremely distant, and faint, so even JWST cannot image one directly. Astronomers instead study them indirectly through the first galaxies JWST observes and through the chemical fingerprints of ancient, metal-poor stars near us.

This article was written for you by FreeAstroScience.com, where we make hard science simple without making it shallow. We believe you should never switch off your mind, since the sleep of reason breeds monsters. Keep questioning. Keep looking up.

Gerd Dani, President, FreeAstroScience

Sources

  1. Ho, M.-Y., Chen, K.-J., & Tung, P.-C. (2026). Turbulence in Primordial Dark Matter Halos and Its Impact on the First Star Formation. The Astrophysical Journal, 1004, 246. https://doi.org/10.3847/1538-4357/ae731d
  2. Gough, E. (2026, June 25). The Universe’s First Stars Were Shaped By Turbulence and Were Not As Massive as Thought. Universe Today. universetoday.com
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