Ink trappings were studied using polyethylene terephthalate (PET) film with black inks for offset proofing and synthetic paper. By observing printed matter from reverse side through the PET film, we detected many air bubbles between the ink layer and the PET film. They are classified roughly to two groups, small number of large ones (φ=2-5μm) and many small ones (φ=0.5-1.0μm). Number of small air bubbles(N
air bubble, measured immediately after the trapping)decreased with increasing the amount of ink trapped (y) and increased with increasing the ink distribution time. Therefore, the small air bubbles have been yielded by the ink distribution. We also measured many ink peaks (immediately after the trapping) and pinholes (at 24h) on the printed surface. Numbers of ink peaks and pinholes (N
ink peak and N
pinhole, respectively) increased with increasing the ink distribution time. Next, we studied effects of nip width on these values (distribution time=2min.; nip width=2, 3 and 4mm). The N
air bubble value decreased with increasing nip width contrary to increase the N
ink peak and N
pinhole values. The latter effect can be represented by differences in the values of 2 and 4mm nip widths. At y=2gm
-2, the difference in the N
air bubble values is about one third (synthetic paper ink) or a half (offset proofing ink) of the difference in the N
ink peak values.
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