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High altitude, low pressure: why your mechanical watch loses its bearings

Haute altitude, basse pression : pourquoi votre montre mécanique y perd ses repères

The balance wheel of a mechanical watch beats four times per second. Nearly seven hundred thousand oscillations a day, each one snatched from a fluid we forget because it is transparent. The balance wheel pushes the air away, drags some of it along, lets it fall back, and starts over. At the seaside, nobody cares. At the summit of Everest, where the atmosphere weighs only a third of what it does in Brest, the question becomes legitimate: what does a mechanical watch really do at high altitude?

The answer circulating on forums and on a few online calculators has the merit of being simple. It predicts a gain of so many seconds per thousand meters, as if the timepiece obeyed a rule of three. What laboratories have to say is more interesting, and significantly less comfortable.


EPFL, Asulab, and the air carried by the balance wheel

At the EPFL Laboratory of Fluid Mechanics and Instabilities, Professor François Gallaire, together with Thierry Hessler of Asulab, the Swatch Group's research division, conducted a project with an unusually modest title: "Effect of the entrained air on the natural frequency of a balance-spring." The title is enough to shift the problem: the air surrounding the balance wheel is not neutral. It has long been known, the two men write, that a watch’s rate varies with atmospheric pressure. One second a day seems trivial. For a mechanical movement, however, it is a tiny margin: with each oscillation, the balance wheel must reproduce almost exactly the same movement. At this scale, even air counts. The balance wheel pushes it away, drags a small amount along with it, and encounters resistance that varies with its density. It is this phenomenon, invisible on the wrist, that the EPFL and Asulab researchers sought to measure and model, while also observing the influence of the elements surrounding the balance wheel inside the movement. A balance wheel does not beat in an abstract atmosphere: it beats in the small amount of air trapped under a crystal.

That leaves the question everyone asks. At altitude, the air thins. The balance wheel therefore encounters less resistance and can oscillate with a slightly different amplitude. Less air means less damping, hence more amplitude: so far, the physics is compliant. But that does not mean the watch will systematically run fast. Everything depends on how its movement reacts to this variation in amplitude. Watchmakers speak of isochronism: ideally, a large oscillation should last exactly as long as a smaller one. In reality, no movement is perfectly indifferent to these variations. Each caliber therefore has its own behavior.

Depending on its regulation, its hairspring, and its escapement, the same ascent could cause one watch to run slightly fast and another to run slow. Added to this are the cold, the position on the wrist, the state of lubrication, or even magnetism. In other words, no one can seriously predict what your watch will do at 4,000 meters based solely on altitude. It is less spectacular than a ready-made formula, but much closer to reality.


Riefler and Shortt: precision through a vacuum

Watchmakers didn't wait for EPFL to be wary of the atmosphere. They simply handled the problem the hard way, by removing the air.

In Munich, starting in the late 1880s, Siegmund Riefler enclosed his astronomical regulators in airtight cases maintained at reduced pressure, with built-in barometric compensation. In 1921, the British engineer William Hamilton Shortt went even further. His free-pendulum clock, the Shortt-Synchronome, suspended its master pendulum in a vacuum chamber and stopped touching it almost entirely: an electromagnetic pulse of three-tenths of a second every thirty seconds, and the pendulum remained free the rest of the time, that is, ninety-nine percent of its existence. The device served as a reference for observatories for over twenty years, from Edinburgh to Greenwich. In 1984, the US Naval Observatory brought out a Shortt and compared it to an atomic clock: one second of error in ten years.

Part of the 20th-century quest for mechanical precision therefore consisted of removing the oscillator from the atmosphere rather than learning to better cope with it. You don't compensate for the air; you evacuate it. The wristwatch never had that luxury. Its balance wheel beats in the ambient air, and that air changes with the weather as much as with altitude: a watch sitting on a table undergoes pressure variations without having moved an inch. Between the vacuum-sealed observatory and the Himalayan summit, the scale changes, but the problem remains the same: the environment in which the regulator oscillates is not a constant.


How NASA pushed the Omega Speedmaster out of the air

Only one mechanical chronograph was pushed to the logical extreme of this concept, and it was not a mountaineering watch.

On March 1, 1965, NASA qualified the Omega Speedmaster for manned spaceflight. To achieve this, the chronograph had to undergo a series of particularly severe tests: humidity, oxygen-rich atmosphere, shocks, vibrations, noise, extreme temperatures, and very low pressure. A millionth of an atmosphere; the summit of Everest, by comparison, is a well-heated living room. Yet the Speedmaster emerged from this campaign in working order, which contributed to its qualification by NASA. The competing chronographs from Rolex and Longines-Wittnauer submitted to the same tests did not all pass every one of them. How can one not notice the irony: the only mechanical timepiece of which we know exactly how it behaves when the air disappears is a chronograph designed not for mountaineering, but for timing automobile races.

Favre-Leuba Bivouac, 1962: the mechanical watch that measured altitude

Yet there exists a family of timepieces that does not suffer from pressure, but reads it.

In 1962, Favre-Leuba introduced the Bivouac, the first mechanical wristwatch to combine a barometer and an altimeter. The principle lies in an aneroid capsule, a small, sealed metallic accordion that expands when the air thins and contracts when it densifies. Its movement is transmitted to a hand. The first Bivouac thus made it possible to measure up to 3,000 meters without a battery or electronics. Everything rests on the mechanical reaction of this thin metallic capsule to variations in the air.

The Bivouac cut its teeth where it mattered. Walter Bonatti wore it in 1964 on the north face of the Pointe Whymper, in the Grandes Jorasses. Junko Tabei took it to Everest in 1975, the year she became the first woman to reach its summit. When the brand revisited the concept in 2017 with the Raider Bivouac 9000, it extended the scale to 9,000 meters, enough to cover the 8,848 meters of Everest, in a 48-millimeter titanium case. One detail summarizes the specialization of this piece quite well: capable of measuring very high altitude, it is, however, only water-resistant to 30 meters. It was designed to read pressure in only one direction.

Vintage Favre-Leuba Bivouac advertisement
1964 Favre-Leuba Bivouac advertisement

Everest, May 29, 1953: an unresolved horological question

Everest holds another uncertainty for horology enthusiasts. On May 29, 1953, at half-past eleven, Tenzing Norgay and Edmund Hillary reached the summit. We know that Norgay wore a Rolex Oyster Perpetual, as he confirmed it himself. For Hillary, the question remains open. An Oyster Perpetual manufactured in 1950 had been given to him before the expedition, and it is currently on display in Zurich. But the mountaineer also acknowledged having brought along a British Smiths De Luxe, now preserved at the Clockmakers' Company museum in London. Both pieces exist, both accounts persist, and the archives do not allow us to say with certainty which one was on his wrist at the summit.

You can read our article on the mountaineering watches that truly conquered the Himalayas.

What altitude refuses to measure

We readily expect horology to respond with a precise figure. Altitude is precisely a domain where this precision becomes deceptive. What can be affirmed is ultimately quite simple: when the pressure decreases, the balance wheel encounters less resistance in the air, and its oscillation can change slightly. This change can alter the watch's rate, but its direction and significance depend on the movement itself, its regulation, and the conditions in which it operates.

This is probably what makes the question more interesting than a simple number of seconds lost or gained per thousand meters. Two watches can go up to the same summit together and not react in exactly the same way. The work of EPFL shows how deep into fluid mechanics one must go to understand only a part of what is happening between a balance wheel and the few cubic centimeters of air that surround it.

As for knowing whether your watch will run fast or slow at the next mountain pass, you will have to take it there. Regulation cannot be guessed from the valley.

FAQ

How much can a mechanical watch drift at altitude?

No reliable value is published, and that is a point to remember before trusting online estimators that promise so many seconds per thousand meters. These calculators ignore temperature, the position of the watch, the movement in question, and its state of maintenance—four factors whose effect often exceeds that of pressure alone. The available academic work describes the mechanism, not a universal constant. The correct method remains to record the rate of your watch on your wrist before and after the trip, which will give you its own specific behavior rather than a theoretical average.

Can my watch be affected by pressure without me leaving sea level?

Yes. Atmospheric pressure does not depend only on altitude; it also varies with the weather. The passage of a low-pressure system and a high-pressure system changes the density of the air around the balance wheel even while the watch has not moved from the bedside table. The effect remains weak, but it serves as a reminder that a mechanical watch is an instrument open to its environment, not a closed system.

Why were observatory clocks in a vacuum, while wristwatches never are?

Because a precision clock is a piece of furniture, and a watch is a wearable object. Isolating a pendulum in a vacuum chamber, as Riefler and later Shortt did, requires a volume, immobility, and maintenance incompatible with a forty-millimeter case that you wind, jostle, and open for service. The Shortt-Synchronome equipped observatories, not wrists. The compromise chosen for the wristwatch has always been to live with the air rather than get rid of it.

Is a watch water-resistant to 200 meters better equipped for high mountains?

Not necessarily, as it is not the same constraint. A diver's case is designed to withstand external pressure higher than internal pressure, whereas altitude produces exactly the opposite: the air trapped in the watch becomes denser than the air outside. The Favre-Leuba Raider Bivouac 9000, capable of measuring 9,000 meters of altitude, is only water-resistant to 30 meters, which illustrates the independence of the two performance metrics. For the mountains, the state of the seals, the movement's resistance to cold, and protection against shocks matter more than a depth rating.


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