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Diving Physics and "Fizzyology"
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Like all animals, human beings
need oxygen in order to survive. When we
breathe, we extract oxygen from the air, and use
that oxygen for metabolism, which is
how we convert the food we eat into useable
energy to do the things that we do. One of the
by-products of metabolism is carbon dioxide;
whenever we exhale, we are getting rid of the
carbon dioxide that our bodies produce.
The main
purpose of breathing, therefore, is to provide
our bodies with oxygen, and rid our bodies of
carbon dioxide. We humans are terrestrial
(land-dwelling) mammals, and as such, our lungs
are designed to breathe gas. Unlike fishes, we
have no gills, so we cannot breathe water.
Therefore, the first problem we must overcome to
explore the underwater realm is a means to
provide breathing gas.
However, if this were the
only barrier humans must overcome to enter the
sea, we would have long-ago discovered most of
the mysteries of the ocean. All we would need to
remain underwater indefinitely would be a long
tube going to the surface -- a huge snorkel --
through which we could breathe. Unfortunately,
there is another problem we must over come when
descending to the depths -- a problem with far
more complex and difficult consequences. .
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Have you ever wondered why nobody makes snorkels
that are ten, or twenty, or a hundred feet long?
The answer becomes obvious as soon as you try to
breathe through a snorkel when your body is more
than two or three feet (~1 meter) beneath the
surface of the water.
If you have ever tried
this, you will know that it becomes extremely
difficult to inhale under those circumstances.
That's because the deeper underwater you go, the
greater the pressure is. Think of
pressure as a force pushing on you from all
directions. At sea-level, we are exposed to
about 14.7 pounds per square inch (psi)
of pressure. This means that each square inch of
our bodies has the equivalent force of about
14.7 pounds pressing on it. The source of this
pressure is actually a result of the weight
of the air in Earth's atmosphere. Like all
gases, the air around us is composed of
molecules of different gases; in this case,
about 21% of these molecules are oxygen, about
78% are nitrogen, and the rest is composed of
assorted trace gases. These gas molecules have
weight, which means that gravity is pulling them
toward Earth. As it turns out, if you took a
column of air, one square inch in cross-section,
extending from sea-level all the way to the edge
of the atmosphere, all the gas molecules in that
column of air would have a combined weight of
about 14.7 pounds -- which leads to 14.7 psi of
pressure at sea level. For convenience,
physicists have defined the "atmosphere"
(abbreviated "ATM") as a unit measurement of
pressure equal to the pressure caused by Earth's
atmosphere at sea level (14.7 psi).
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| Like air, water causes pressure
by its weight. But of course, water is
considerably denser (i.e., heavier for a given
volume) than air. As it turns out, a column of
sea water one inch in cross-section would need
to be only about 33 feet (10 meters) tall to
weigh 14.7 pounds. Therefore, at a depth of 33
feet (10 meters) beneath the sea surface, the
total ambient pressure is about 29.4 psi, or 2
ATM -- 1 ATM caused by the weight of the air in
Earth's atmosphere, plus 1 ATM for the weight of
33 feet (10 meters) of seawater. To avoid
confusion, when people discuss pressures
underwater, the unit "ATA" (referring to
"atmospheres absolute") is often used to
represent the total, "absolute" pressure caused
by both the water and the air above the water
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As is illustrated in the diagram at right, the
ambient pressure increases underwater at an
almost linear rate with increasing depth*.
For every 33 feet (10 meters) of depth in sea
water, the ambient pressure increases by an an
additional 14.7 psi (1 atm).
At a depth of 99
feet (30 meters), the ambient pressure is 4 ATA
-- one ATM caused by the Earth's atmosphere,
plus 3 ATM for every 33 feet (10 meters) of
depth. Similarly, the ambient pressure 297 feet
(90 meters) beneath the surface is 10 ATA.
The
problem with the long-snorkel idea has to do
with the fact that the muscles we use to expand
and contract our lungs during breathing are not
strong enough to overcome much pressure.
Even
just a few feet beneath the surface, the
pressure is great enough that we cannot expand
our lungs against the water pressure to inhale a
breath of air from the surface. Our bodies
simply are not designed to do that.
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| One way to overcome this
problem is to protect the diver's body from the
ambient pressure. "Atmospheric Pressure Diving"
technology, the most familiar of which are deep
sea submersibles, do exactly that. The pressure
on the inside of a submersible is maintained at
1 ATA - the same pressure that we experience at
the sea surface. Underwater, the increased
ambient pressure acts on the hull of the
submersible, not the diver inside. Thus, the
person inside the submersible is protected from
the ambient pressure at all times and has no
difficulty breathing.
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Another way to overcome the
problem of breathing under pressure is to
provide a pressurized breathing gas mixture to
the diver. If the breathing gas supply is
delivered at the same pressure as the
surrounding ambient pressure, the diver's lungs
do not have to work against the water pressure
(i.e., the pressure in the surrounding water and
the pressure in the inhaled gas supply are
balanced). However, when using this sort of
"Ambient Pressure Diving" technology, the
diver's body is directly exposed to the ambient
pressure. More importantly, the gas inhaled into
the diver's lungs is pressurized. To understand
the physiological ramifications of this, it's
important to understand the effects of increased
pressure on gases.
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As mentioned above, gas is
composed of molecules. As the pressure of the
gas increases, these molecules (which are in
constant motion) get packed more closely
together. At a higher pressure, a given number
of gas molecules will occupy a smaller volume
(or a given volume will be occupied by a larger
number of gas molecules). For example, if you
had a balloon filled with gas at the surface,
and then pulled that balloon underwater, the
balloon would shrink in size. In fact, if you
brought the balloon down to a depth of 33 feet
(10 meters), it would be half the size it was at
the surface. At 66 feet (20 meters) it would be
one-third the size it was at the surface; at 99
feet (30 meters) it would be one fourth the
size, and so on. If, at a depth of 99 feet (30
meters), you wanted to expand the balloon to its
original size, you would have to fill it with
four times as many gas molecules as were
required at the surface. Returning the
re-inflated balloon back to the surface would
cause it to grow to four times its original
size. It doesn't require much imagination to
understand what would happen to a diver's lungs
if he or she took a full breath at depth, and
held it while ascending to the surface. This is
why the golden rule of diving is "never hold
your breath". People who forget this rule (for
example, in a state of panic), run the risk of
suffering from ruptured lungs, allowing gas
bubbles to directly enter the blood. It's called
embolism, and it can lead to serious
symptoms including paralysis and death.
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A key point here for
understanding other aspects of diving physics
and physiology, is to realize that the greater
the pressure, the more tightly packed (i.e.,
more highly concentrated) gas molecules are.
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*Note:
Because water is very slightly compressible, the
relationship between depth and pressure is not
exactly linear all the way to the
bottom of the sea; however, for the purposes of
diving technology, the deviation from a linear
relationship is trivial.
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To understand the physiological
ramifications of breathing various gas mixtures
under pressure, it is useful to understand the
concept of partial pressure. The
partial pressure of a particular gas constituent
in a gas mixture is a representation of the
portion of the total pressure of the gas mixture
exerted by the particular constituent.
If you
add up all the partial pressures of all the
different components of a gas mixture, their
total would be equal to the total pressure of
the mixture. As confusing as this may sound,
partial pressures are actually quite easy to
calculate: all you need to know is the fraction
of each gas constituent in the mixture, and the
total pressure of the gas mixture.
For example, consider a person
breathing air (a gas mixture containing
approximately 80% nitrogen and 20% oxygen) at
sea level. As discussed earlier, the ambient
pressure at the sea surface is 1 ATA. Therefore,
the pressure of the air which the person
inspires is also 1 ATA. To get the partial
pressure of nitrogen in the inspired air, simply
multiply the fraction of nitrogen in the
breathing mixture (80%) by the total pressure (1
ATA), and you calculate a nitrogen partial
pressure of 0.8 ATA. Similarly, multiplying 20%
oxygen times 1 ATA results in an oxygen partial
pressure of 0.2 ATA. Now consider what happens
when that same person descends to a depth of 99
feet (30 meters), where the ambient pressure is
4 ATA. In order for that person to be able to
breathe at all, the inspired air pressure must
be the same as the ambient pressure. Therefore,
the inspired partial pressure of nitrogen is 80%
times 4 ATA, or 3.2 ATA. The oxygen partial
pressure is 20% times 4 ATA, or 0.8 ATA. At 99
feet (30 meters), the ambient pressure is four
times greater than it is at the surface, and the
partial pressures of each of the gases is also
four times greater (although the percentages of
each gas are the same in both cases). As
discussed earlier, the gas molecules are more
closely packed when under pressure; at a depth
of 99 feet (30 meters), there are four times
as many gas molecules (both nitrogen and
oxygen) in a lung-full of air as there are at
the surface. An easy way to think of partial
pressures of gases is that the partial pressure
represents an absolute concentration of
that gas, regardless of depth or pressure. If a
person breathed a gas mixture containing 80%
oxygen at the surface, the oxygen partial
pressure would be 0.8 ATA, which is exactly the
same partial pressure of oxygen when breathing
air at a depth of 99 feet (30 meters). In both
cases (80% oxygen at the surface and air at 99
feet/30 meters), the concentration of oxygen
molecules in the lungs (i.e., the total number
of oxygen molecules in the lungs on each inhaled
breath) is the same.
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Just a word on notation: in
their gaseous forms, both oxygen and nitrogen
are binary molecules; that is, they are
bound in pairs of atoms. An oxygen gas molecule
consists of two oxygen atoms bound together, and
a nitrogen gas molecule consists of two nitrogen
atoms bound together. The notation for oxygen is
the letter "O", so oxygen gas is referred to as
"O2"; the subscript "2" indicating
two atoms of oxygen. Similarly, nitrogen gas is
referred to as "N2", and carbon
dioxide as "CO2". When discussing
partial pressures of gases, the gas notation is
usually prefaced by a capital "P". Thus, "oxygen
partial pressure" is written as "PO2",
and "nitrogen partial pressure" is written as
"PN2".
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Henry's Law states that "The amount of any
given gas that will dissolve in a liquid at a
given temperature is a function of the partial
pressure of that gas in contact with the
liquid..." What this means for divers is that
gas molecules will dissolve into the blood in
proportion to the partial pressure of that gas
in the lungs (as "warm-blooded" creatures, our
core body temperature remains relatively
constant).
In the diagram at right, the top figure (1)
represents a close-up of the interface between
the lungs and the blood and tissues of a diver.
At sea level, the dissolved gases in the blood
and tissues are in proportion to the partial
pressures of the gases in the person's lungs at
the surface.
As the diver descends underwater,
the ambient pressure increases, and therefore
the pressure of the gas inside the lungs
increases correspondingly. Because the partial
pressures of the gases in the lungs are now
greater than the dissolved partial pressures of
these gases in the blood in tissues, gas
molecules begin to move from the lungs into the
blood and tissues (represented by the blue and
red arrows in the middle figure, 2).
Eventually,
the concentration of the dissolved gases in the
blood and tissues will be proportional to the
the partial pressures in the breathing gas
(i.e., a state of equilibrium).
The physiological complexities of "Ambient
Pressure Diving" are a direct result of the
effects of these increased dissolved
concentrations of gases in the blood and
tissues, and how those increased concentrations
affect the way our bodies work.
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Oxygen
is the only gas we really need to breathe in
order to stay alive. If we don't breathe oxygen
(or if we don't breathe enough oxygen), we soon
die. Interestingly enough, too much
oxygen can be a bad thing also. At right is a
diagram illustrating the range of oxygen
concentrations that we can breathe safely.
The
green and red bar represents a scale of inspired
oxygen partial pressures (PO2),
ranging from zero oxygen on the left, to a PO2
of 2.0 ATA on the right. Through evolution, our
bodies have become optimized to breathe oxygen
at a partial pressure (PO2) of 0.21
ATA.
If the inspired PO2 is much less
than this, our bodies begin to shut down --
leading to unconsciousness when the PO2
drops below about 0.1 ATA (i.e., 10% oxygen at
sea level). This is called hypoxia.
Breathing more than 0.21 ATA oxygen is generally
fine ... up to a point. If the inspired PO2
is maintained above about 0.5 ATA for prolonged
periods of time (many hours to days), people
begin to suffer what is usually referred to as
"pulmonary" or "chronic" oxygen toxicity.
The effects of this include a burning sensation
or irritation in the lungs, and can affect
breathing. Except for people who spend days
under pressure at a time (e.g., commercial
divers on oil rigs), this form of oxygen
toxicity is not much of a problem for divers.
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| However, as the inspired PO2
starts to climb above about 1.2 to 1.4 ATA,
another kind of oxygen toxicity, called "CNS"
(for "Central Nervous System") or "acute" oxygen
toxicity, becomes a significant problem.
Although a variety of subtle symptoms such as
muscular twitching in the face and tunnel vision
have been attributed to this kind of oxygen
toxicity, the really important symptom is
severe, uncontrolled convulsions. Although these
convulsions do not appear to cause any sort of
permanent damage by themselves, the problem of a
diver experiencing such convulsions being able
continue to hold a regulator in his or her mouth
is obvious. More than a few divers have drowned
underwater, apparently a result of
oxygen-induced convulsions. This is perhaps the
most serious and insidious of diving maladies,
because it comes on unpredictably and without
warning, and usually results in the death of the
afflicted diver.
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There is no clear understanding
on the exact biochemical processes involved with
CNS oxygen toxicity, nor is there a clear
consensus on what the "safe" upper PO2
limit should be. Convulsions have occurred in
divers breathing an inspired PO2 as
low as 1.2 ATA, but such cases usually involve
extenuating circumstances (such as medical
conditions in the divers which pre-dispose them
to convulsions).
Conversely, commercial divers
in Europe have routinely breathed oxygen partial
pressures as high as 1.9 ATA in the water, and
hyperbaric chamber facilities regularly expose
patients to 2.8 ATA of oxygen (or more) without
difficulty. Amid the ambiguities, two trends
seem very consistent. The first is that high
levels of exercise (perhaps more specifically,
high levels of CO2 in the blood)
appear to increase the probability of suffering
from a convulsion.
Secondly, divers immersed in
water have a lower tolerance to elevated
concentrations of inspired oxygen than do divers
kept dry in a hyperbaric chamber or undersea
habitat. (this over and above the fact that
divers in a dry habitat are much more likely to
survive a convulsion than are divers immersed in
water). Another unavoidable reality regarding
oxygen toxicity is the extreme range of
variation both between individuals, and within a
single individual.
When immersed underwater, most
divers regard a PO2 of 1.4 ATA as a safe upper
limit during periods of physical exertion, and
1.6 ATA during periods of rest.
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Eighty percent of the gas molecules in air
are nitrogen (N2). Our bodies do not need or use
nitrogen for metabolism, so it serves little
function in a breathing gas mixture, other than
to dilute the concentration of oxygen. When high
concentrations of nitrogen become dissolved in
our bodies, however, nitrogen can affect our
central nervous system.
Familiar to all divers
is the effect known as "nitrogen narcosis".
Cousteau called it "rapture of the deep", and
its effects have been likened to alcohol
inebriation. When breathed at high
concentrations, nitrogen can impair our
neurological abilities. The exact biochemistry
is not known, but the symptoms include impaired
judgement, loss of short-term memory, slowed
response time, and sometimes euphoria.
Obviously, just as one should not drive while
intoxicated, diving with impaired mental
abilities is at the very least unwise.
As with
oxygen toxicity, there is a wide range of
variation in susceptibility to nitrogen narcosis
both between, and within individuals. There is
some evidence that repeated exposure can lead to
an "adaptation" effect, but this is a topic
subject to continued debate. Some divers begin
to notice the symptoms while breathing air as
shallow as 90 feet (27 meters) or so, while
other claim to suffer no incapacitation at
depths in excess of 200 feet (61 meters).
Impairment likely occurs at lower PN2 levels
than those at which divers begin to detect overt
symptoms. In any case, the greater the inspired
PN2, the more severe the narcosis. There is some
evidence that oxygen also contributes to
narcosis, but probably only at concentrations
above which CNS oxygen toxicity would be of
primary concern.
Nitrogen plays another important role in
limiting conventional scuba diving: it's
involvement with decompression sickness. This
will be discussed in greater detail in the
following section on decompression.
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Go to Diving
Physics and Fizzyology Page 2
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| By
Richard Pyle Copyright © 1997, by
Bishop
Museum |
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