Mechanical energy mostly affects divers in the form of sound. Sound is a periodic
motion or pressure change transmitted through a gas, a liquid, or a solid. Because
liquid is denser than gas, more energy is required to disturb its equilibrium. Once
this disturbance takes place, sound travels farther and faster in the denser medium.
Several aspects of sound underwater are of interest to the working diver.
In any body of water, there may be two or more
distinct contiguous layers of water at different temperatures; these layers are
known as thermoclines. The colder a layer of water, the greater its density. As the
difference in density between layers increases, the sound energy transmitted
between them decreases. This means that a sound heard 50 meters from its source
within one layer may be inaudible a few meters from its source if the diver is in
another layer.
In shallow water or in enclosed spaces, reflections and
reverberations from the air/water and object/water interfaces produce anomalies in
the sound field, such as echoes, dead spots, and sound nodes. When swimming in
shallow water, among coral heads, or in enclosed spaces, a diver can expect periodic
losses in acoustic communication signals and disruption of acoustic
navigation beacons. The problem becomes more pronounced as the frequency of
the signal increases.
Because sound travels so quickly underwater (4,921 feet per second), human ears
cannot detect the difference in time of arrival of a sound between each ear. Consequently,
a diver cannot always locate the direction of a sound source. This
disadvantage can have serious consequences for a diver or swimmer trying to
locate an object or a source of danger, such as a powerboat.
Open-circuit scuba affects sound reception by producing
high noise levels at the diver’s head and by creating a screen of bubbles that
reduces the effective sound pressure level (SPL). When several divers are working
in the same area, the noise and bubbles affect communication signals more for
some divers than for others, depending on the position of the divers in relation to
the communicator and to each other.
A neoprene wet suit is an effective barrier to sound above 1,000 Hz and it becomes
more of a barrier as frequency increases. This problem can be overcome by
exposing a small area of the head either by cutting holes at the ears of the suit or
by folding a small flap away from the surface.
Sound is transmitted through water as a series of pressure
waves. High-intensity sound is transmitted by correspondingly high-intensity
pressure waves. A high-pressure wave transmitted from the water surrounding a
diver to the open spaces within the body (ears, sinuses, lungs) may increase the
pressure within these open spaces, causing injury. Underwater explosions and
sonar can create high-intensity sound or pressure waves. Low intensity sonar, such
as depth finders and fish finders, do not produce pressure waves intense enough to
endanger divers. However, anti-submarine sonar-equipped ships do pulse
dangerous, high-intensity pressure waves.
It is prudent to suspend diving operations if a high-powered sonar transponder is
being operated in the area. When using a diver-held pinger system, divers are
advised to wear the standard ¼-inch neoprene hood for ear protection. Experiments
have shown that such a hood offers adequate protection when the ultrasonic
pulses are of 4-millisecond duration, repeated once per second for acoustic source levels up to 100 watts, at head-to-source distances as short as 0.5 feet (Pence and
Sparks, 1978).
An underwater explosion creates a series of waves that
are transmitted as hydraulic shock waves in the water, and as seismic waves in the
seabed. The hydraulic shock wave of an underwater explosion consists of an initial
wave followed by further pressure waves of diminishing intensity. The initial
high-intensity shock wave is the result of the violent creation and liberation of a
large volume of gas, in the form of a gas pocket, at high pressure and temperature.
Subsequent pressure waves are caused by rapid gas expansion in a non-compressible
environment, causing a sequence of contractions and expansions as the gas
pocket rises to the surface.
The initial high-intensity shock wave is the most dangerous; as it travels outward
from the source of the explosion, it loses its intensity. Less severe pressure waves
closely follow the initial shock wave. Considerable turbulence and movement of
the water in the area of the explosion are evident for an extended time after the
detonation.
Some explosives have characteristics
of high brisance (shattering power in the immediate vicinity of the explosion)
with less power at long range, while the brisance of others is reduced to increase
their power over a greater area. Those with high brisance generally are used for
cutting or shattering purposes, while high-power, low-brisance explosives are
used in depth charges and sea mines where the target may not be in immediate
contact and the ability to inflict damage over a greater area is an advantage. The
high-brisance explosives create a high-level shock and pressure waves of short
duration over a limited area. Low brisance explosives create a less intense shock
and pressure waves of long duration over a greater area.
Aside from the fact that rock or other bottom
debris may be propelled through the water or into the air with shallow-placed
charges, bottom conditions can affect an explosion’s pressure waves. A soft
bottom tends to dampen reflected shock and pressure waves, while a hard, rock
bottom may amplify the effect. Rock strata, ridges and other topographical
features of the seabed may affect the direction of the shock and pressure waves,
and may also produce secondary reflecting waves.
Research has indicated that the magnitude of
shock and pressure waves generated from charges freely suspended in water is
considerably greater than that from charges placed in drill holes in rock or coral.
At great depth, the shock and pressure waves are drawn out by the
greater water volume and are thus reduced in intensity. An explosion near the
surface is not weakened to the same degree.
In general, the farther away from the explosion,
the greater the attenuation of the shock and pressure waves and the less the intensity.
This factor must be considered in the context of bottom conditions, depth of water, and reflection of shock and pressure waves from underwater structures and
topographical features.
A fully submerged diver receives the total
effect of the shock and pressure waves passing over the body. A partially
submerged diver whose head and upper body are out of the water, may experience
a reduced effect of the shock and pressure waves on the lungs, ears, and sinuses.
However, air will transmit some portion of the explosive shock and pressure
waves. The head, lungs, and intestines are the parts of the body most vulnerable to
the pressure effects of an explosion. A pressure wave of 500 pounds per square
inch is sufficient to cause serious injury to the lungs and intestinal tract, and one
greater than 2,000 pounds per square inch will cause certain death. Even a pressure
wave of 500 pounds per square inch could cause fatal injury under certain
circumstances.
There are various formulas for estimating
the pressure wave resulting from an explosion of TNT. The equations vary
in format and the results illustrate that the technique for estimation is only an
approximation. Moreover, these formulas relate to TNT and are not applicable to
other types of explosives.
The formula below (Greenbaum and Hoff, 1966) is one method of estimating the
pressure on a diver resulting from an explosion of tetryl or TNT.
|   |
  |
13,000   3 √ W |
| p |
= |
_____________________ |
|   |
  |
r |
where:
| P |
= |
pressure on the diver in pounds per square inch |
| W |
= |
weight of the explosive (TNT) in pounds |
| r |
= |
range of the diver from the explosion in feet |
Sample Problem Determine the pressure exerted by a 45-pound charge at a
distance of 80 feet.
| 1. |
|
Substitute the known values. |
|   |
  |
13,000   3 √ 45 |
| p |
= |
_____________________ |
|   |
  |
80 |
| 2. |
|
Solve for the pressure exerted. |
|   |
  |
13,000   3 √ 45 |
| p |
= |
_____________________ |
|   |
  |
80 |
|   |
  |
13,000 X 3.56 |
| |
= |
_____________________ |
|   |
  |
80 |
Round up to 579 psi
A 45-pound charge exerts a pressure of 579 pounds per square inch at a distance of
80 feet.
When expecting an underwater blast, the
diver shall get out of the water and out of range of the blast whenever possible. If
the diver must be in the water, it is prudent to limit the pressure he experiences
from the explosion to less than 50 pounds per square inch. To minimize the
effects, the diver can position himself with feet pointing toward and head directly
away from the explosion. The head and upper section of the body should be out of
the water or the diver should float on his back with his head out of the water.