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New trends in physics teaching, v.4; The ... - unesdoc - Unesco

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Colour<br />

illum<strong>in</strong>ation appears colourless. This power of adapt<strong>in</strong>g to the colour quality of the prevail<strong>in</strong>g<br />

illum<strong>in</strong>ation is known as general colour adaptation. By means of it, we become less aware of the<br />

physical conditions exist<strong>in</strong>g at the time. Thus we are not ‘misled’, for example, to the conclusion<br />

that objects seen at sunset are actually ruddy <strong>in</strong> hue, or that our companions’ complexion under<br />

candlelight is yellow. Colourfilm, hav<strong>in</strong>g no such built <strong>in</strong> adaptation, gives good results only when<br />

exposed under illum<strong>in</strong>ation of the quality for which the film was balanced, as mentioned below.<br />

Ret<strong>in</strong>ex theory of colour vision<br />

<strong>The</strong> crux of the problem of colour vision lies less <strong>in</strong> the primary process (there can be no doubt<br />

that, under normal illum<strong>in</strong>ation, the cones, with their three ranges of spectral sensitivity <strong>in</strong> the red,<br />

green and blue, provide the <strong>in</strong>itial response) but with what happens <strong>in</strong> the ret<strong>in</strong>a, the pathway to<br />

the bra<strong>in</strong> and the visual cortex afterward. <strong>The</strong> eye is not a spectrophotometer, record<strong>in</strong>g light<br />

levels and send<strong>in</strong>g them to the bra<strong>in</strong> - it is much more like a m<strong>in</strong>icomputer back<strong>in</strong>g the process<br />

of detection of light - and it does this by a complex system compar<strong>in</strong>g the impulses from various<br />

parts of the ret<strong>in</strong>a. A model of such a system is the ‘ret<strong>in</strong>ex’ theory of colour vision discussed<br />

by Edw<strong>in</strong> Land. We have already seen how the ganglion signals emerg<strong>in</strong>g from the ret<strong>in</strong>a are<br />

coded differently from the anticipated response of the <strong>in</strong>dividual detector cells. Furthermore, our<br />

psychological perception of colour is, aga<strong>in</strong>, quite different from what the ‘photometer’ picture<br />

of the eye might give us. As an example of the necessity for a theory of this nature, let us return<br />

to colour photography. It is well known that two types of film are normally available, one for<br />

outdoors and the other for <strong>in</strong>candescent light illum<strong>in</strong>ation. We say the latter is for a lower colour<br />

temperature. Yet, why should this be necessary? If we enter a room under <strong>in</strong>candescent light, we<br />

do not obta<strong>in</strong> the impression that everyth<strong>in</strong>g is t<strong>in</strong>ged with red or yellow, as is the case for a<br />

colour slide made of that room us<strong>in</strong>g daylight film.Obviously, our eyes compensate <strong>in</strong> some way<br />

for the different illum<strong>in</strong>ation, and Land po<strong>in</strong>ts out that the ability for this compensation is<br />

surpris<strong>in</strong>gly large. One may see this compensation <strong>in</strong> an achromatic experiment where we hang<br />

a piece of black velvet nearby, and a sheet of white paper further away. We can now illum<strong>in</strong>ate<br />

the velvet and its surround<strong>in</strong>gs so that a photometer tells us that the velvet is giv<strong>in</strong>g out more<br />

light than the white paper - yet the paper still looks white, and the velvet black. It appears the<br />

eye makes a series of comparisons between the velvet and the paper, and takes account of the<br />

illum<strong>in</strong>ation becom<strong>in</strong>g dimmer as we approach the paper, Land refers to this property of an<br />

object as ‘lightness’ - thus, the paper is lighter than the velvet, even though the latter may give<br />

out more light. This is a perceptual, not a physical quantity - it is based on the assessment of<br />

several experimenters. It is detected even under extremely low levels of illum<strong>in</strong>ation, when only<br />

one set of sensors, the rods, is excited. Return<strong>in</strong>g to coloured objects, we wish to relate the<br />

perceptual quantity of ‘lightness’ with its physical equivalent. Over a long series of experiments,<br />

Land’s subjects matched irregular rectangular blocks of colour of various k<strong>in</strong>ds called ‘Mondrians’,<br />

after their resemblance to pa<strong>in</strong>t<strong>in</strong>gs by that artist, with chips from the Munsell Book of Color [2l ,<br />

a colour-order system. By illum<strong>in</strong>at<strong>in</strong>g these colours with three narrow bands of the spectrum<br />

at 630, 530 and 450 nm <strong>in</strong> different proportions, it was possible to show that the physical<br />

property of reflectance appeared to be associated with lightness - both the Munsell chips, and<br />

the blocks of the Mondrians reflected the same proportions of 630, 530 and 450 nm wavelengths,<br />

irrespective of the nature of the <strong>in</strong>cident illum<strong>in</strong>ation, which was different for both. A mechanical<br />

picture of the way <strong>in</strong> which the ret<strong>in</strong>ex system might analyze the ret<strong>in</strong>al output to perform such<br />

a trick has been proposed. It is suggested that the eye is very sensitive to changes <strong>in</strong> light yields<br />

over the edges of objects <strong>in</strong> the field of view. Thus, the eye takes the three highest outputs<br />

relevant to the three types of cone and compares everyth<strong>in</strong>g else to them, tak<strong>in</strong>g the ratio of<br />

reflectances over each edge, but ignor<strong>in</strong>g the change <strong>in</strong> <strong>in</strong>tensity which occurs over the body of<br />

the object. Effectively, it traces a path from the object with the highest reflectance, to the object<br />

225

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