This book starts with pressure. Under water, the weight of the water above you presses on you and on everything you carry. 3 laws of physics describe what that pressure does to the gas you breathe. This chapter covers the first one, Boyle’s law. Chapter 2 covers Dalton’s law and chapter 3 covers Henry’s law.
Boyle’s law in one sentence
When you squeeze a gas, it gets smaller: double the pressure on it and it takes up half the space.
You can feel this with a bicycle pump. Put a finger over the end and push the handle. The air inside gets smaller and pushes back harder. Let go and it springs back.
Pressure under water
Divers measure pressure in ATA (atmospheres absolute, about the same as bar). 1 ATA is about the pressure of the air around you at sea level.
Water is much heavier than air. Every 10 m of sea water adds about 1 more ATA. The total pressure on you, air plus water, is the ambient pressure, also called the absolute pressure. A cylinder or depth gauge that reads 0 at the surface shows gauge pressure, which leaves out that first 1 ATA of air. The gas laws always use absolute pressure.
Every other number in this book starts from the pressure at your depth, so it is worth knowing how to work it out.
DiveLogic’s planner uses the real density of sea water and the air pressure at the dive site’s altitude, so its figures differ slightly from this rule.
Your body is mostly water, and water barely squeezes. The gas you carry does squeeze: the air in your lungs, your ears, your mask, your equipment and your cylinder.
Boyle’s law tells you how much that gas squeezes. Multiply the pressure by the volume before a change, and you get the same answer after it.
Planned with DiveLogicWork out the gas for a dive
A balloon at the surface
Tie off a balloon of air at the surface. It stays the same size because the air inside pushes out as hard as the air outside pushes in: 1 bar.
Now take it down. The deeper it goes, the more water is above it and the harder it is squeezed.
10 m: twice the pressure, half the volume
At 10 m the pressure is 2 bar, and the same air takes up half the space. No air has left the balloon. The gas molecules are just closer together.
This is Boyle’s law: for a fixed amount of gas at a steady temperature, pressure multiplied by volume stays the same. Going from 1 bar to 2 bar, the volume becomes half of what it was. Double the pressure and the volume halves.
30 m: a quarter of the volume
At 30 m the pressure is 4 bar, and the balloon is a quarter of its surface size.
The first 10 m halved the volume. The next 20 m took away only another quarter. What matters is the ratio of the pressures, not the number of metres. So each metre changes the volume most near the surface.
The last 10 m of an ascent
On the way up, the pressure halves between 10 m and the surface, from 2 bar to 1 bar. The volume doubles. This is the biggest change of the whole ascent, and it happens in the last 10 m.
Your lungs follow the same law. If you hold your breath on the way up, the air in them grows and can tear the lung. This is why the first rule of diving is never to hold your breath while ascending.
Gas used per breath
Now fill the balloon back up to its surface size at 30 m. It holds 4 times as many gas molecules as it did at the surface.
Your lungs work the same way. They do not shrink at depth, because your regulator (the valve you breathe from) gives you gas at the pressure around you. So a full breath at 30 m is the same size as at the surface, but it takes 4 times as much gas from your cylinder.
Gas spaces in your body and equipment
Boyle’s law applies to every space that holds gas. A diver carries several.
- Lungs. Your regulator keeps your lungs at the pressure around you. If you hold your breath on the way up, the trapped air expands. A rise of only a few metres can overexpand the lungs, most easily near the surface where the change is biggest. This injury is called pulmonary barotrauma. It can push air into the chest or into the blood, where a bubble can block an artery (an arterial gas embolism). Chapter 5 covers it along with decompression sickness.
- Ears and sinuses. Your middle ear is a small air space joined to your throat by a narrow tube. On the way down it gets squeezed unless you push air in through that tube. That is what equalising means. Equalise early and often in the first 10 m, where the change is fastest.
- Mask. Your mask is pressed onto your face as you go down. Breathe out gently through your nose into it to keep it the same size.
- BCD and drysuit. A BCD (buoyancy control device) is a jacket or wing you add air to so you float at the depth you want. A drysuit also holds a layer of air. On the way down this air is squeezed, so you sink more and must add air. On the way up it expands, so you float up more and must let air out. The biggest changes are in the last 10 m.
Gas use at depth
Your SAC rate (surface air consumption) is how much gas you breathe per minute, measured as if you were at the surface. Divers also call it RMV (respiratory minute volume) when it is given in litres per minute. It stays about the same at any depth for the same effort. But at depth each breath holds more gas, in step with the ambient pressure.
So to find your gas use at depth, multiply your SAC rate by the pressure in ATA. If you breathe 15 L/min at the surface, at 30 m (4 ATA) you use 15 × 4 = 60 L/min. A cylinder lasts about a quarter as long at 30 m as at the surface, and about a fifth as long at 40 m (5 ATA). Multiply by the minutes you spend there to get the gas for that part of the dive.
Think of it like packing a suitcase: at 30 m each breath is the same size case, packed 4 times as tight.
With normal scuba, called open circuit, every breath goes out into the water as bubbles. A rebreather recycles your breath, so its gas use depends far less on depth. Chapter 20 compares the two. Chapter 24 covers planning your gas, including the reserve you need to get back to the surface. You can work out the gas for a depth and time with the gas needed tool.
Where the law comes from
Robert Boyle (1627-1691) worked in Oxford. His assistant, Robert Hooke, built him an air pump, and Boyle used it to study the “spring” of the air: how it pushes back when squeezed. He published these experiments in 1660.
In 1662 he trapped air in the sealed end of a J-shaped glass tube, poured in mercury to squeeze it, and measured how much it shrank. Boyle credited the idea to Richard Towneley, who had done similar tests with Henry Power in 1661. In France the same rule is called Mariotte’s law, after Edme Mariotte, who published it on his own in 1676.
What to remember
- The absolute (ambient) pressure is about 1 ATA at the surface and rises by about 1 ATA for every 10 m of sea water.
- Boyle’s law: for a fixed amount of gas at a steady temperature, pressure multiplied by volume stays the same. Double the pressure and the volume halves.
- The change depends on the ratio of pressures, so it is biggest near the surface: gas doubles in volume between 10 m and the surface.
- Never hold your breath on the way up. Expanding air can overexpand the lungs, even over a few metres.
- Each breath at depth holds more gas, in step with the ambient pressure. Multiply your SAC rate by the pressure in ATA to get your gas use at depth.
Gas needed for a dive
DiveLogic’s gas needed tool uses Boyle’s law on a planned dive. Give it a depth, a time and your breathing rate. It tells you how much gas you will use, in litres and in bar from your cylinder.
Sources
- Boyle R. (1660). New Experiments Physico-Mechanicall, Touching the Spring of the Air, and its Effects. Oxford: H. Hall for T. Robinson.
- Boyle R. (1662). New Experiments Physico-Mechanical, Touching the Air: Whereunto is Added A Defence of the Authors Explication of the Experiments, Against the Obiections of Franciscus Linus, and, Thomas Hobbes, 2nd edition. Oxford: H. Hall for T. Robinson. (Contains A Defence of the Doctrine touching the Spring and Weight of the Air and the J-tube table.)
- West J. B. (1999). The original presentation of Boyle’s law. Journal of Applied Physiology 87(4): 1543-1545.
- West J. B. (2005). Robert Boyle’s landmark book of 1660 with the first experiments on rarified air. Journal of Applied Physiology 98(1): 31-39.
- Webster C. (1963). Richard Towneley and Boyle’s law. Nature 197: 226-228.