How a bubble is born, rises and bursts
Cellulose fibres · engraved glasses · about a million bubbles
Most champagne bubbles are born inside tiny hollow cellulose fibres stuck to the glass, not on flaws in the glass itself.1,2 Each bubble grows as it rises and bursts at the surface, and a flute that is left alone releases, by one estimate, about a million of them.3
Birth: gas pockets in fibres
A bubble cannot appear on its own in champagne. At the supersaturation found after uncorking, a new bubble would need a radius of about 0.25 µm to survive, and such bubbles do not form spontaneously; a pre-existing pocket of gas is needed.4 These pockets sit inside hollow, roughly cylindrical cellulose fibres, about 100 µm long, that fall from the air or are left by the cloth used to wipe the glass.1,4
CO2 diffuses into the trapped gas, a bubble swells at the mouth of the fibre and detaches at a radius close to that of the fibre, about 10 µm.4 In a study described in a physics society magazine, the rhythm three minutes after pouring ranged from less than 1 to almost 30 bubbles per second per site.1 One fibre can release several tens of thousands of bubbles before the dissolved CO2 drops too low.5
Engraved glasses
Some glasses have laser-etched spots at the bottom of the bowl. They act as permanent nucleation sites, and a review calls this artificial effervescence.4 In a symposium paper from Reims, a single impact in a tasting glass produced one bubble train that did not mix the wine, while a ring of 50 impacts mixed the whole glass, with liquid speeds up to about 9 cm/s.6
Rise and growth
A bubble of about 10 µm starts slowly, at about 50 µm/s.5 Dissolved CO2 keeps entering it, so it grows as it rises: the review gives growth rates around 400 µm/s in champagne against about 150 µm/s in beer.4 Champagne holds about twice as much dissolved CO2 as beer, so its bubbles end up larger.4 Champagne also has only about 5 mg/L of surface-active compounds, against several hundred mg/L in beer, so its bubbles behave more like fluid spheres.2
How many bubbles
A 2017 review estimates that about a million bubbles form and rise in a flute under standard tasting conditions if it is not drunk.3 A separate model links this number to the wine and the glass.7
Bursting
The film of a bubble at the surface breaks in 10 to 100 µs, and hundreds of bubbles burst every second in the first minutes.1 Each burst throws up a small jet that breaks into droplets, suggested to carry more surface-active and possibly aromatic material than the wine below.2 According to a review (a preprint), the droplets evaporate above the glass and release their own aroma fingerprint.4
See also
Sources
- European Physical Society / EDP Sciences. Liger-Belair G., Jeandet P. Effervescence in a glass of champagne: a bubble story. Europhysics News 33(1): 10-14. DOI 10.1051/epn:2002103 (2002-01)
- EDP Sciences. Liger-Belair G. La physique des bulles de champagne. Annales de Physique 27(4): 1-106. DOI 10.1051/anphys:2002004 (abstract page) (2002)
- EDP Sciences / Springer (EPJ ST). Effervescence in champagne and sparkling wines: From grape harvest to bubble rise. Eur. Phys. J. Special Topics (2017). DOI 10.1140/epjst/e2017-02678-7 (abstract page; group: Equipe Effervescence Champagne et Applications, GSMA UMR CNRS 7331, Reims) (2017-01-06)
- Mathijssen A.J.T.M., Lisicki M., Prakash V.N., Mossige E.J.L. Culinary fluid mechanics and other currents in food science. arXiv:2201.12128v2 (review) (2022-10-14)
- Société Française de Physique / EDP Sciences. Liger-Belair G., Tufaile A., Jeandet P., Sartorelli J.-C. La nucléation des bulles de champagne: une sorte de goutte-à-goutte inversé ? Reflets de la Physique 9. DOI 10.1051/refdp:2008009 (2008)
- PSFVIP-10 proceedings (Università di Napoli Federico II). Beaumont F., Liger-Belair G., Polidori G. Flow visualization in engraved champagne tasting glasses. 10th Pacific Symposium on Flow Visualization and Image Processing, Naples, paper 60 (2015-06)
- FAO AGRIS record. Liger-Belair G. How many bubbles in your glass of bubbly? J. Phys. Chem. B 118(11): 3156-3163. DOI 10.1021/jp500295e (bibliographic record + abstract) (2014)
Facts checked on 2026-10-19