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Effect of Flexo Dot Geometry on Print Performance and Gain
1. The Effect of Flexo Dot Geometry
on Print Performance:
Theoretical and Empirical Models of Dot Gain
Mechanisms
Timothy Gotsick
May 28, 2013
MacDermid Printing Solutions
2. A little bit about myself…
2
In my natural
habitat, waiting for
a delayed flight.
Timothy Gotsick, VP Technology
• R&D
• Application Development
• Based in Atlanta, GA
• 10 years with MacDermid
• Background in organic chemistry
• Still being tutored in print technology
• Management of new product development
in chemical industries
• Strong interest in understanding print fundamentals
3. Outline
• What is Print Gain?
• Why and where is it a problem?
• What causes Print Gain?
• The effect of shoulder angle on print gain
• Case Study: Corrugated Postprint “Fluting”
• Case Study: Highlight dot gain
• Further work: Effects of dot shape on ink distribution
9. What are the root causes of dot gain?
Mechanism
Factors
Type of Effect
Print Result Dot Gain
Mechanical
Ink
Spreading
Ink Rheology
Substrate-Ink
Interaction
Dot
Deformation
Inking
(Anilox)
Printing
(Substrate)
Optical
Density
Uniformity Smoothness
10. Truly Big Dots
• Molded from 32 Shore A photopolymer
• 7 cm tall
• 1 cm tip
• Θ = 53 , 62 , 71 , 79
Θ
20. Board vs Dot
• Board structure changes the impression level experienced by dots
across the surface of the board
– Dots printing on flute „tip‟ are harshly compressed
– Dots printing on flute „valley‟ are minimally compressed
21. Print Pressure Variations
“Striping on Flexo Post-printed Corrugated Board”
Martin Holmvall, Thesis
Fibre Science and Communication Network, Department of Natural Sciences, Mid Sweden University, SE-851
70 Sundsvall, Sweden, 2007
29. Conclusions (pt. 1)
• Fluting is caused by differences in the impression
environment the dots are subjected to at the flute tips
and valleys
• Dot shoulder angle influences dot gain because:
– Contact patch size (gain) increases with impression, but it
increases less for dots with shallower shoulder angles
– Impression force increases with impression, but it increases
less for dots with shallower shoulder angles
• The dot shoulder angle model of gain prediction
seems to explain empirical results well
31. The Quest for the Smallest Dot
1% <1%
Dot size vs stability: How low can you go?
32. Gain throughout the tone range
0.00
1.00
2.00
3.00
4.00
5.00
0 10 20 30 40
DotDiameer,mils
174 lpi File Dot Size, %
Theoretical
Measured
33. Gain is a bigger problem for smaller dots
y = 3.672x-0.53
R² = 0.977
0%
50%
100%
150%
200%
250%
300%
350%
400%
0 10 20 30 40
IncreaseinDotSizefromFiletoPrint
174 lpi File Dot Size, %
Gain vs Dot Size
39. What are the root causes of dot gain?
Mechanism
Factors
Type of Effect
Print Result Dot Gain
Mechanical
Ink
Spreading
Ink Rheology
Substrate-Ink
Interaction
Dot
Deformation
Inking
(Anilox)
Printing
(Substrate)
Optical
Density
Uniformity Smoothness
44. 44
LUX: It is that simple
Existing process LUX process
Ablate
Plate
Digital
Plate
Expose
Process
Plate
Standard
Digital
Plate
Mem
brane
Remove
Membrane
LUX
Lamination
46. Optimizing Dot Profile
• Lots of dots work. Some dots work better.
– These factors seem to matter most
46
Dot Surface
Morphology Shoulder AngleValley DepthEdge definition Dot Surface
47. Thank You
47
Timothy Gotsick
VP Technology, MacDermid Printing Solutions
tgotsick@macdermid.com
http://www.macdermid.com/printing
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Notes de l'éditeur
Although I previously showed pictures of dots actually undergoing impression, it is actually quite hard to visually observe dot deformation under real-world conditions. You can imagine how nervous printers get when we start asking them to remove all the safety shielding so we can try and poke microscopes inside their press! As an alternative to this perilous and messy situation, we went the other direction and made a collection of macroscopic dots. Ironically, we are much better at making millions of 70 μm x 500 μm dots (which we produce every day) than we are at making 1 cm by 7 cm dots, which required some creativity on the part of our researchers. But we did succeed in creating these macro dots from the same photopolymer used in our commercial plates, and with a variety of dot shoulder angles, as shown above.
A bit more creativity gave us a test environment where we could ‘print’ these dots in a controlled fashion using an instrument that can precisely control the distance and rate of compression while measuring the force generated during the dot’s compression.
This is a video of the instrument in action, in this case compressing the 7 cm tall dot by 2 cm. Watch closely, there is a lot going on.
One of the effects you probably noticed in the video was that as the dot was compressed, the top of the dot was pressed into the ‘substrate’ and thus the ‘contact patch’ grew in size. This is not surprising, and you would be correct in thinking that this is likely a major cause of gain. However, we wanted to be able to understand how this contact patch expansion proceeded with compression.
To do so, we located some pressure sensitive material that allowed us to visualize the contact patch at varying levels of impression. As shown in this slide, the material changes color as pressure is applied to it, revealing the actual size of the contact patch. Furthermore, this visualization technology can actually detect differences in pressure across the contact interface, as shown in the top row of samples. We are currently studying the distribution of force across the contact patch, although this work does not include such detail.
Here is the result. This graph shows the growth in the contact patch of four different dots at multiple impression levels. The four dots differed only in the angle of their shoulders, with the 53° dot having the broadest profile and the 79° dot having the narrowest profile. The most important things we learned were the following:1. All dots showed two ‘regions’ in their response to compression. At relatively low compression levels, contact patch increased relatively slowly, but at higher compression levels (between 8 and 10 mm in this graph), the contact patch growth accelerated. The onset and magnitude of this acceleration was dependent on dot shoulder angle. Broader dots (e.g. 53°) hit their inflection point at lower compression levels and the contact patch growth was faster once it did. In contrast, dots with steeper shoulders (e.g. 79°) showed less change in contact patch at all compression levels and their transition to the ‘accelerated growth’ portion of the curve occurred later in the compression cycle.
In addition to the contact patch, we also studied the change in force of the same dots during compression. Again, there were major differences in the behavior of dots with different shoulders angles. The broader the dot, the faster the growth in force during compression. What was also interesting to note was the non-linear growth in force, which actually follows a second order polynomial growth curve. This is in contrast to the expected behavior of a mechanical spring system, where force rises in direct proportion to the compression distance.
The reason for this non-linearity can be understood by considering the simultaneous expansion in contact patch that occurs during dot compression. The force rises exponentially because the contact patch increases; not only is the material being compressed more, but more material is being compressed. This is an especially relevant finding for the study of fluting. As you may recall from my description of Holmvall’s work, the print density on corrugated board rose non-linearly with pressure/force. This means that at certain portions of the print process, both print density (through force) and dot gain (through contact patch growth) are increasing exponentially at the same time.
Here is a close-up view of what is at the heart of fluting – two very different print environments experienced on the same print surface, with predictably different effects on the plate’s dots.
However, even with the use of thick, soft plates, the pressure experienced by the plates in the micro-environments of the flute peaks and valleys can be quite different, and this difference becomes even more pronounced with increasing print squeeze or impression, as shown here.
Now let’s tie all this together and explain fluting once and for all. In the ‘valleys’ of the corrugated board, the contact patch growth (and the force growth) is operating in this region of the curve, where gain is minimized and relatively stable.
But at the flute tips, the dots are operating in this region of the graph, where contact patch and force growth are both higher and on a much steeper slope. More gain and more print density. Also, note that the problems in this region are very different for dots with different shoulder angles – the broadest dot studied (53°) had a contact patch twice as large as the narrower dots (71° and 79°) at many compression levels.
The results can be seen in print and in actual observation of dots on board. Steeper shoulder angles give a dot that tolerates compression better, giving print density that is similar at the flute tips and valleys and reducing the unwanted visual effects that density variations bring.
In conclusion, I hope that I have provided a strong case for three statements.First, fluting is caused by differences in the impression that dots printing on the tips of the flutes receive compared to those printing in the valleys of the flutes.Second, that the dot shoulder angle is an important determinant of print gain behavior, becauseThe contact patch of broader dots increases faster with impression compared to narrower dots.The impression force generated by broader dots increases faster with impression compared to narrower dots.And third, the exposure technology used to make dots can have a large and beneficial effect on the shoulder angle, with new flat-topped dot technologies creating not only flat tops, but steep shoulder angles throughout the tone range, not just at the highlights, which allows corrugated plates made with this technique to print with an unprecedentedly low level of fluting AND more consistently so.