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pigmented colorants: dependence on media and time - Cornell ...

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equal amounts at all visible wavelengths, as seen in Figure 3.8. C<strong>on</strong>trast this with<br />

the distributi<strong>on</strong> of energy from a fluorescent light bulb, where there are relatively<br />

large peaks in the lower <strong>and</strong> central wavelengths (blue <strong>and</strong> green, respectively).<br />

This is why photographs taken inside under fluorescent light often have the charac-<br />

teristic of being slightly more greenish-blue than pictures taken in natural lighting.<br />

Figure 3.8: Intensity of the D65 illuminate (typical average daylight) <strong>and</strong><br />

fluorescent light over the visible spectrum. Adapted from [G95b].<br />

In order to quantify the physical energy of the spectral distributi<strong>on</strong>s of emissive<br />

light sources, <strong>on</strong>e must integrate the illuminant’s energy over all wavelengths. In<br />

discrete math, the energy reaching the eye at all wavelengths from emitted light,<br />

P = <br />

λ E(λ), where E(λ) is the emitted light energy at each wavelength.<br />

Light does not <strong>on</strong>ly reach the eye via emitted light, but also from reflecti<strong>on</strong>s.<br />

The percepti<strong>on</strong> of light reflected from the surface is dependent <strong>on</strong> both the re-<br />

flectance properties of the material <strong>and</strong> the given light source. Therefore, changes<br />

in lighting will affect the perceived appearance of an object. Artists attempt to<br />

work under similar lighting c<strong>on</strong>diti<strong>on</strong>s to that of the envir<strong>on</strong>ment where the art<br />

will be exhibited, save encountering problems in hue shifting.<br />

Physically, the energy reaching the eye at all wavelengths from reflected light,<br />

P = <br />

λ E(λ)R(λ), where R(λ) is the reflected light energy at each wavelength.<br />

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