Wonders of Nature Weather No background needed About 7 min read

Why Do Zao's "Snow Monsters" Grow Toward the Wind?
― Cloud Droplets Below Freezing Turn to Ice the Moment They Hit

The "snow monsters" standing in rows on winter mountains are not just piled-up snow. They are made of cloud droplets that drifted along unfrozen below freezing, then turned to ice the instant they hit a tree, and slowly grew toward the direction the wind comes from.

Published: 2026.10.31 Difficulty: ★☆☆ (no background needed) The only maths is in the fold-out at the end
First, picture this scene

In winter at Zao or Hakkoda, a herd of white monsters appears outside the ropeway window. Many people have seen them in photos or on TV.

Up close, you see jagged ice like shrimp tails lined up on one side of each branch only. The other side has almost nothing on it.

Snow falls from above, so it should pile up on top. Yet this ice reaches out sideways, and only in one fixed direction. What is going on?

Just two reasons

1
Below freezing, cloud droplets stay liquid

Droplets in the clouds and fog that wrap a mountain can drift unfrozen even below minus 10°C. The moment they hit something, they freeze onto it.

2
Droplets hit only the windward side

Droplets are carried in by the wind, so they strike only the side facing it. Thin, pointed spots catch them best, so the ice keeps growing upwind.

So a snow monster is not something that "piled up". It is made of water droplets the wind carries in, which the tree catches head-on and "glues" in place. Let's go through it step by step.

Why don't cloud droplets freeze below zero?

We learn that water freezes at 0°C. But that holds only when the water contains something that can "start" the ice. Cloud droplets are tiny, about 0.01 to 0.02 mm across.

The smaller a droplet is, the less likely it is to hold a speck of dust that can start ice. So many droplets stay liquid even at minus 10°C or minus 20°C. This is called supercooling.

A supercooled droplet freezes all at once at the slightest jolt. Slamming into a leaf or twig is exactly that kind of jolt. The droplet freezes on the spot, and the next one freezes on top of it.

Tiny gaps are left between the droplets. That is why the ice is not clear but white, full of trapped air. The northwest winter monsoon from the Sea of Japan carries plenty of water vapour from the sea, so these droplets keep blowing against the mountaintops.

Left = upwind: supercooled droplets blow in Wind (arrows) Droplets (dots) Branch Downwind side: no droplets curl round, so no ice Ice grows upwind (shrimp tail) Growth per hour (rough) about 1.4 cm In 12 h about 16 cm *Rough estimate with cloud water, catch rate and ice density fixed (same formula as the fold-out)
Move the slider to change how far the ice grows upwind
Figure 1: A branch seen from the side. The arrows on the left are the wind, and the dots are cloud droplets blowing in. Droplets hit the left (upwind) side of the branch and freeze, and pointed white ice grows to the left. Almost none forms on the right (downwind) side. Raise the wind speed with the slider and more droplets arrive, so the ice grows longer in half a day.

Look at Figure 1. Ice forms only on the upwind side of the branch and grows toward the wind. The stronger the wind, the more droplets arrive each hour, so the ice grows faster.

Why does the ice keep growing upwind?

Droplets riding the wind try to slip past an object by turning with the air just before it. But droplets have weight, so they can't turn sharply. Only the ones that fail to turn hit the surface.

What matters here is how thick the object is. In front of a thick trunk, the air starts curving gently from far away. Small droplets can follow that flow, so most of them swerve around the trunk.

In front of a thin leaf or twig, the air bends sharply right at the surface. Droplets can't keep up and fly straight in. So the thinner the object, the better it catches droplets (Figure 2).

Left: thick trunk Flow bends early; droplets swerve too Trunk Dotted = droplet path (most miss) Right: thin leaf or twig Flow bends late; droplets can't turn Hit and freeze Dotted = droplet path (straight hit)
Figure 2: The effect of thickness. In front of the thick trunk on the left, the grey flow lines bend widely from far ahead, and the dotted droplet paths follow them around the trunk. In front of the thin leaf on the right, the flow bends only at the last moment, so the dotted droplets go straight in and hit, forming white ice.

This shows how snow monsters keep growing upwind. The tip of the ice is itself a "thin, pointed bump". So the next droplets hit the tip first, and the ice juts out further into the wind.

Falling snow then catches on the shrimp tails that form on each branch. Ice and snow pile up in turn, until the tree becomes a white mass several metres tall. That is what a "snow monster" is.

💡 Few mountains can grow snow monsters

Big snow monsters need three things together: strong monsoon winds carrying supercooled droplets, a moderate amount of snow, and conifers with fine needles that hold snow well (such as Maries' fir). In Japan they are said to be limited to a few mountains in the Tohoku region, such as Zao, Hakkoda and Hachimantai.

💡 Snow monsters are natural weathervanes

The direction the shrimp tails point is the direction the wind blew from most that winter. Winter hikers are said to use it as a clue to direction when fog hides the view.

Summary

Snow monsters form when cloud droplets that drift unfrozen below freezing turn to ice the moment they hit a tree. Droplets arrive on the wind, so they strike only the windward side. Thin, pointed spots catch them best, so the tip of the ice gathers still more droplets, and the ice keeps growing into the wind.

A snow monster is not piled-up snow.
It is the mark left where a tree met the wind's "water that wants to freeze" head-on.

For how water can stay liquid below 0°C, see "We learn that water freezes at 0°C, so why is there water that won't freeze even at minus 20°C?" For another winter case of ice growing from the ground, see "Why do frost columns sprout up out of the soil?"

🧪 On a winter morning, look for the upwind mark
  1. On a cold, foggy morning, look at wire fences, thin twigs and grass near power lines. See whether any white ice grains have formed on them.
  2. If you find ice, check which side has more. Use a compass app on your phone to note which direction that side faces.
  3. In the same place, compare a thin wire with a thick post. See whether the thinner one carries more ice.

Even on low ground, small amounts of rime can appear on a bitterly cold, foggy morning. Watch your step so you don't slip on frozen paths.

For those who want more ― terms, formulas and links to textbooksEach part is labelled by level, from middle school science to university courses
How to read the labels below
  • Middle schoolCovered in middle school science
  • High schoolCovered in high school Earth science or physics
  • High school+Advanced high school material, or textbook sidebars
  • UniversityNot taught in high school; university courses (cloud physics, fluid dynamics)
  • ResearchNot yet settled even at university; researchers are still investigating

Middle schoolTerms: this phenomenon has names

Middle schoolHigh schoolCheck it with a formula: how much does rime grow in an hour?

We work out how much water the wind carries onto a branch each second, and how thick it would be as ice. All values are rough; real growth varies a lot with the weather.

⓪ The basic formula
In symbols(growth rate) = E × w × v ÷ ρ
In wordsThickness grown per second = catch rate × water per cubic metre of air × wind speed ÷ density of rime
Where it comes fromConservation of mass: of the water the wind carries to a surface (water amount × wind speed), the caught part all turns to ice. Dividing mass by density gives volume, that is, thickness
① Starting values
SymbolMeaning and unit
w (cloud water)0.3 g per cubic metre of air (roughly 0.1 to 0.5 g in mountain fog)
v (wind speed)10 m per second
E (catch rate)0.5 (a guide for thin leaves and twigs; much smaller for thick trunks)
ρ (rime density)400000 g per cubic metre (less than half that of ordinary ice because it holds air)
② Work it out
Water carried to 1 square metre per second (g)0.3 × 10 = 3
Part that is caught (g)3 × 0.5 = 1.5
Built up in 1 hour (3600 s) (g)1.5 × 3600 = 5400
As ice thickness (m)5400 ÷ 400000 = 0.0135
In centimetres (cm)0.0135 × 100 = 1.35
Growth in 1 day (24 hours) (cm)1.35 × 24 = 32.4

That is about 1.4 cm in an hour and over 30 cm in a day. In a single night, ice longer than the width of your palm grows upwind. As the formula shows, the growth rate is proportional to wind speed. The slider in Figure 1 uses this formula as it is.

High schoolHigh school+Why don't droplets freeze, and why is the ice white?

High schoolFor water to freeze, a tiny seed of ice must form. The smaller the droplet, the less likely it holds the dust (ice nuclei) that seeds it, so it stays supercooled. The heat released on freezing (latent heat of fusion) escapes quickly into the cold air, so a droplet that hits freezes in an instant.

High school+When droplets freeze one by one at once, they stack up keeping their shapes, and air is trapped in the gaps. This is white, light rime. When the air is near 0°C and the droplets are large, they spread out before they freeze, giving clear, heavy ice. This kind can cause damage by its weight when it builds up on power lines and the like.

UniversityCatch efficiency and the Stokes number

Whether a droplet can bend with the flow is expressed by the Stokes number in fluid dynamics. It is the ratio of "the time a droplet needs to change direction" to "the time the flow takes to bend in front of an obstacle". If the Stokes number is well above 1, the droplet goes straight and hits; if it is small, the droplet rides the flow and swerves.

The obstacle's width is in the denominator, so the thinner it is, the larger the Stokes number. Estimating with a 0.02 mm droplet and a 10 m/s wind, it is far above 1 for a 1 mm needle and about 0.05 for a 30 cm trunk. In cloud physics this catch rate is called the collection efficiency (collision efficiency), and the same idea is used to predict icing on aircraft and power lines.

📖 Derivations and further reading: Wikipedia, "Stokes number" (Japanese) / Wikipedia, "Supercooling" (Japanese)

ResearchWhat is still not clear

So this article, too, is "an explanation of what is known so far". How droplets freeze is well established, but how the snow-monster scenery will change is still being watched.

Links to textbooks (by level)

LevelSubject / unitWhere in this article
Middle schoolScience: "Changes of state", "Weather (monsoons)"Water turning to ice; the northwest winter monsoon
High schoolEarth science: "Structure of the atmosphere, how clouds form"Supercooled cloud droplets, ice nuclei
High school+Physics: "Heat (latent heat of fusion)"White rime versus clear ice
UniversityFluid dynamics, cloud physicsStokes number, collection efficiency, icing
ResearchClimate change and mountain ecosystemsShifts in snow monster range, forest restoration
―Links to daily lifeWinter mountain scenery, wind direction clues, icing on power lines
References and sources
  1. Wikipedia (Japanese), "Muhyō (霧氷)" (rime, including snow monsters)
  2. Yoshimitsu Ogura (小倉義光), Ippan Kishōgaku (一般気象学, "General Meteorology"), University of Tokyo Press (東京大学出版会)
  3. H. R. Pruppacher, J. D. Klett, Microphysics of Clouds and Precipitation, Springer
  4. Japan Meteorological Agency (気象庁), "Yohō Yōgo" (予報用語, "Forecast Terminology"), entries on rime and icing
  5. Wikipedia (Japanese), "Stokes number (ストークス数)"

*This article is a general-audience science explainer. The figures given are rough estimates to help you understand the mechanism. When heading into the winter mountains, follow local weather information and facility guidance.