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Scarica gli atti - Gruppo del Colore

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2. Printer Mo<strong>del</strong><br />

The mo<strong>del</strong> of the printer we refer to is based on the well-known Yule-Nielsen<br />

Spectral Neugebauer equation. According to the YNSN mo<strong>del</strong>, the spectrum of a<br />

N-inks halftone print is the weighted sum of 2 N different colors, called Neugebauer<br />

primaries, given by all the possible overprints of inks. The weight of each<br />

Neugebauer primary is the area it covers in the halftone cell. The YNSN mo<strong>del</strong> for<br />

a 4-ink halftone print is:<br />

R<br />

54<br />

15 1<br />

⎢ n<br />

pr int, = ∑ a p R p,<br />

λ<br />

⎢ p=<br />

0<br />

n<br />

⎡ ⎤<br />

⎥<br />

λ λ = 1..<br />

8<br />

(1)<br />

⎥<br />

⎣ ⎦<br />

where Rprint,λ is the reflectance of the printed color, n is the Yule-Nielsen factor,<br />

Rp,λ is the reflectance of the p-th Neugebauer primary, and ap is the primary area<br />

coverage. The area coverage is the percentage of the halftone cell covered by the<br />

Neugebauer primary.<br />

A mo<strong>del</strong> by Demichel can be used to compute the percentage of the area covered<br />

by each primary. The dot overlap is the product of the relative area covered by<br />

single inks, computed in a stochastic fashion that assumes the ink dots are<br />

randomly arranged. The mo<strong>del</strong> is considered valid for random or rotated halftone<br />

screen [8]; it fails in all cases in which there is a singular screen superposition,<br />

although the color deviation observed is not excessively large [9]. For dot-on-dot<br />

printing a different formulation must be considered [10]. We have used the mo<strong>del</strong><br />

for a random screen, and computed area coverage according to the equations in<br />

Table 1, where c = [ c , m,<br />

y,<br />

k]<br />

represents the concentration of inks for printing a<br />

given color.<br />

We consider each printer an RGB device and mo<strong>del</strong> the driver according to<br />

Equation 2, where the gray component is composed of equal amounts of cyan,<br />

magenta and yellow.<br />

c = c'−U<br />

⋅ k,<br />

m = m'−U<br />

⋅ k,<br />

y = y'−U<br />

⋅ k,<br />

k = min( c',<br />

m',<br />

y'<br />

),<br />

0 ≤ U ≤ 1;<br />

where c' = 1−<br />

r,<br />

m'=<br />

1−<br />

g,<br />

y'=<br />

1−<br />

b .<br />

In our mo<strong>del</strong>, the complex interaction of inks and substrate determining optical and<br />

mechanical dot gains depends upon the wavelength, but also upon the quantity and<br />

number, and types of inks in the halftone. The function used to compute the<br />

effective ink concentration, tuned with only one parameter, is:<br />

(2)

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