| The shape of the water is decisive on how the light passes through it. Crinkle patterns and cathedral light. Snell's circle. | |
| The way light diffuses as it interacts with matter, depends on the size of the particles. How to minimise ambient scatter. | |
| How does a strobe cause scatter and how can you minimise it? One of the underwater photographer's worst nightmares. What is the ideal strobe? | |
| Colour changes with depth as water filters out the warm colours. How can you restore colour? Mixed light photography and use of filters. | |
| The intensity of light diminishes rapidly as one goes deeper, depending on circumstances. | |
| Above water your camera angle is not as important as under water. Why? Why do professionals goto coral seas? |
Surface
effects
The
shape of the water is decisive on how the light passes through it. Coming
from an optically less dense medium (air) and entering a denser one (water),
the light is partly reflected back while partly entering the water. Depending
on the shape of the water, the light forms crinkle patterns or becomes
diffused randomly in all directions. |
The amount of light that is reflected upward depends strongly on the height of the sun (place on Earth, time of day and season) and the condition of the sea. A rough sea absorbs more light whereas a mirror-like sea reflects more. In the tropics, the sun stands straight overhead at mid-day, resulting in little loss. In temperate seas during winter, the light diminishes by as much as 3 f-stops immediately under the surface.
As a matter of interest, the reflected light is partly polarised (horizontally)
and so is the part that enters the water (vertically). Polarisation is
maximal in the early morning and late afternoon when the sun stands low
in the sky. The vertically polarised light entering the water makes objects
less shiny, more colourful, and can be used creatively, for instance to
capture the deep colours of shiny fishes in natural light.
The
diagram shows the theoretical loss of light due to reflection. The top
left quarter shows sun rays reaching the water's surface. The top right
quarter shows the amount of light reflected and the bottom right quarter
that of light transmitted. The hours shown are not those of the clock but
of the height of the sun. Only at angles less than 30º with the horizon
('four-o-clock') is the light reflectance significant and does loss of
light become noticeable under water. However, in practice, and perhaps
due to waves and the light diminishing towards sunset/dawn, the light under
water diminishes much more quickly. At 'four-o-clock' one loses a complete
f-stop (50%).
Note how the light enters the sea at a steeper angle (blue lobe), which means that most of the time, the light comes from almost straight above, which limits natural lighting options. The light reluctantly enters a dive mask for instance or poorly lights subjects from their sides. |
| Crinkle patterns
When the water is very calm, its undulations resemble weak positive and negative lenses, the negative ones diffusing the light, resulting in dark patches while the positive ones focussing the light into bright patches. This effect also causes the creative 'cathedral' rays, sometimes visible. |
| A sand flounder enjoying the extra camouflage afforded by the rapidly
moving light patches, known as crinkled light. In an environment where
everything moves, even its movements are no longer noticeable!
This photo was taken with a warming filter and short time exposure, through a 50mm lens. |
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To increase the crinkle effect:
Do as for the crinkle effect but also: Choose a dark background such as a rock wall Choose a dirty water patch with suspended particles Shoot close to the edge of the light Aim the camera towards the light Avoid shooting directly into the sun. Hide the sun behind an object. Shoot during a clear blue sky; avoid clouds Use a wide angle lens Deeply penetrating sun 'rays' are rare, so use your chance well!
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Blue Maomao fish lazing in the mid-day sun in a narrow channel near
Goat Island, in the Goat Island marine reserve, New Zealand.
The example shows how the sun ray effect has been captured by positioning oneself near the edge of the light, close to a vertical wall and shooting towards the sun in a blue sky. A fill flash was used to bring colour to the foreground and to make fish visible in the shade. No colour correction was used in order to accentuate the blue colours of the fish. Note that some clouds are visible in the sky. This picture would have been better without them. Lens: 15mm |
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A snorkeldiver enjoys herself in a shallow alcove of Ngaio Rock,
Poor Knights Islands, New Zealand.
This photo was taken with a full daylight correction filter before the lens, shooting upward towards the sun but hiding it behind a steep rock face. This cove was carefully selected as an under water 'studio': a steep wall on both sides to make the sun rays stand out against a dark background; and some weeds in the dark lower right corner to frame the picture. The sky is entirely blue. No flash light was used. Lens: 15mm |
The
water's surface has further consequences for how light continues its path.
The diagram shows how light is broken (diffracted) by the surface. A vertically
incident ray passes without breaking but as the incident angle (height)
becomes less, the light ray is bent to descend more steeply. Finally, light
from the horizon passes at an angle of about 45 degrees or more precisely
half of Snell's Angle, named after the Dutch astronomer Snell who discovered
and described this effect (see separate box). To photograph the full circle
from below, one needs a fish-eye lens of focal lens less than 12mm. A 15mm
wide angle lens captures a good part of it. |
| The consequence of Snell's Window or Snell's Circle is that the light
always shines down steeply, even when the sun stands low in the sky. This
makes ambient light difficult for lighting subjects. Top lighting is difficult
to use creatively, making strobes necessary to bring the light in from
the front.
Snell's window is the circle through which the sky is visible. The area around it is a reflection of the seascape and is usually much darker. This light contrast becomes worse in clouded or semi-overcast conditions, causing problems for wide angle lenses. So treat blue sky weather as wide angle weather, particularly when also the water is calm. Look out for steep rock faces to find cathedral light. Try to hide the sun. |
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| In the example, a mangrove tree has been photographed
from below, offering a slightly distorted view of the world above. Snell's
Circle runs through the middle of the frame and the horizon is the edge
between light and dark. The bottom part of the picture reflects the bottom
but about 2 f-stops darker. The photo would have been improved with a graduated
grey filter correcting for one f-stop and by applying a half intensity
fill flash to the branch in the foreground. At the time this photo was
taken, these problems were not apparent.
On the right the same image corrected by techniques explained in the Digital Darkroom chapter. When shooting negative film, one can over expose by one f-stop, which gives one the opportunity of applying a grey filter in the Digital Darkroom. |
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The
Dutch astronomer Willebrord van Roijen Snell (1580-1626) discovered the
important law of light diffraction between two media having differing refractive
indexes or optical densities or light speeds. The Dutch physicist Christiaan
Huyghens later formulated other optical laws in his treatise on light.
Snell formulated that light is refracted (bent) towards the optical axis
perpendicular to the plane between the media when going from a less dense
to a denser media so that
{sin (a2)}/{sin (a1)}=n1 / n2As angle a1 approaches 90 degrees, angle a2 reaches its maximum beyond which total reflection occurs (going from water to air). This critical angle or Snells 'window' is just over 48 degrees to both sides of the vertical: {sin (a2)}/{sin(90º)}=1/1.33Huyghens suggested to look at light beams as travelling fronts of light, like soldiers marching in file can be considered as rows of soldiers. When a light front or row of soldiers meets a denser medium, it is slowed down, causing the front/row to bend and travel/march into a different direction. Note that winds meeting a land mass on an angle, behave similarly. |
Scatter
and diffusion
The way light
diffuses as it interacts with matter, depends on the size of the particles.
For the ultra small water molecules, blue light is bounced off in all directions
equally, while the rest of the light passes through normally. This diffusion
was described by the physicist Rayleigh and explains why both the sky and
the sea look blue. The diffused blue light appears to come from all directions,
particularly deeper down and it has the effect of reducing contrast
while dominating the natural colours.
Particles as large as phyto plankton but not visible to the naked eye (0.1 to 10 micrometre) act like mist particles, reflecting all colour components of the light back to where it came from. This effect makes driving in the mist an undertaking. This form of diffraction was first described by the physicist Tindall. It causes images to blur but it also offers creative opportunities both above and under water. |
Finally, the snow effect that plagues under water photographers and which is called scatter, is light bounced off visible particles like zoo plankton organisms or even their shed moults. Such 'snow' or 'jelly' or 'snot' often collects close to the surface and should be avoided.
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Scatter
from strobe light
Strobelight
scatter is caused by brightly lit small objects close to both the strobe
light and the lens. As the particle is usually out of focus, it projects
the scape of the aperture onto the film. It is a photographer's nightmare
because it spoils the photo but more annoyingly because it is never visible
when taking the photo.
In the drawing the red numbers illustrate that at half the distance from strobe to subject, the light is four time stronger. At half that distance again, 16 times! It decreases quadratically with distance, thus increasing dramatically towards to the strobe. |
Fortunately a number of approaches can
be followed to reduce its devastating effect:
|
Move
the strobe away from the corners of the image, towards the centre of the
long side. This effect is dramatic, but it also produces unnatural looking
light. Also when turning the camera for a vertical shot, the side lighting
becomes unnatural. But a compromise position can be chosen. Many photographers
use the centre position for macro photography, as the light needs to be
brought close in for subjects close to the lens.| What is the ideal strobe?
The strobe is an inseparable part of underwater photography and you will buy one as soon as you have decided on what camera to buy. So what are the ideal strobe's characteristics? |
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Loss of
colour
Water
particles interact with light by absorbing certain wave lengths (see diagram).
First the reds and oranges disappear, later the yellows, greens and purples
and last the blue. Loss of the colour red is dramatic and is already noticeable
at 50cm! At 5 metres depth some 90% has disappeared. Since the loss
of colour varies critically with distance, it is necessary to make corrections
by applying colour correction filters. Their use is described later on
and their effect is quite substantial. Note that colour filters applied
under water, do not taint the blue background, but when they are applied
in the computer or in the laboratory, they do.
The picture shows that it is the total light path that matters. In the
case of the strobe, this amounts to about twice the subject distance whereas
for ambient light it amounts to depth plus subject distance.
|
The diagram on right gives accurate light extinction figures for one metre water. Where clear oceanic water (probably with visibility 50m) gives 40% loss in red light per metre (blue curve), the light remaining (transmission) is thus 60%. For two metres it would be 60% of 60% remaining, = 36%. Clear oceanic water has its least loss in the blue colour, which means that distanct objects would look blue. As a rule of thumb remember that you lose one f-stop (50%) in the reds for one metre light path. So a subject at 50cm distance from the strobe already loses that one f-stop. Average coastal water extinction in the reds (green curve) is about 70%, thus transmission is 30%. Over 2 metres the remaining red light is 30% x 30% = 9%. The dip of this curve rests in the green wavelengths, which makes distant objects look green. |
Loss
of intensity
This
graph shows actual measurements of light intensity (in f-stops) as it decreases
with depth (in metres). The measurements were done in northern New Zealand
towards the end of February, our summer in the southern hemisphere. Although
well on its return to winter, the sun still stands high in the sky, causing
minimal loss of light directly under the surface: just under two f-stops.
In the tropics only one f-stop is lost, which can be traded off for finer
grained film. In temperate seas it is common sense to use faster film like
400ASA. In mid-winter when the sun stands low in the sky, or in early morning
or evening, the loss of light can be dramatic, amounting to 4 f-stops!
The two measurements demonstrate the dramatic loss of light due to poor visibility (red squares), compared to good visibility (blue triangles). At 30m depth in poor visibility, almost no natural light photography can be done on moving objects. Yet, using a tripod combined with fill flash, remarkable results can be obtained, even at -9 f-stops with shutter speeds of 1 second or longer! |
camera
angles
How
to aim your camera is of critical importance underwater. The diagram serves
to give you a feel of what the consequences are of your position in the
water and the way you aim your camera. Read it with care.
|
| Why do professionals prefer coral seas?
Professionals have a job to do, photos to sell and for them time is money and quality is a must. So they all do their work in warm tropical seas. Why? |