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This is a paper published in Convertech & e-Print
White Rose Research Online URL for this paper:
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Paper:
Kapur, N, Hewson, R, Sleigh, PA, Summers, JL, Thompson, HM and Abbott, SJ
(2011) A Review of Gravure Coating Systems. Convertech & e-Print, 1 (4). 56 -
60 (5).
56 CONVERTECH & e-Print July / August 2011
Fundamental Coating Research
A Review of Gravure Coating Systems
N. Kapur1, R. Hewson1, P.A. Sleigh2, J.L Summers1, H.M. Thompson1, S.J. Abbott3
1Institute of Engineering Thermofl uids, Surfaces & Interfaces (iESTI), School of Mechanical Engineering, University of
Leeds, Leeds, UK; 2School of Civil Engineering, University of Leeds, Leeds, UK; 3Consultant to Rheologic Ltd, UK
n.kapur@leeds.ac.uk
Figure 1 (a) the direct gravure process where the gravure roll and web are in intimate contact, (b)
offset gravure coating where transfer is from (i) the gravure roll to the (deformable) applicator roll
and (ii) subsequently from the applicator roll to the web
1. Introduction
Gravure roll coating is a technique used to coat
fluids of a wide range of viscosities (up to 1500mPa s)
onto substrates at speeds of up to 900 m/min (Booth,
1970,1990). Coat thicknesses in the range of less than
1 micron up to 50 microns can be achieved, making this
a versatile process which is finding application across a
growing number of market sectors.
Gravure roll coating differs from many of the
conventional roll coating techniques in that one of the
rolls is patterned with a surface engraving (the ‘gravure’
or ‘anilox’ pattern). Both the shape and the size of the
gravure pattern can be varied which affects the final
properties of the coating.
The term ‘gravure roll coating’ covers a number of
distinct gravure coating arrangements. Two common
variants of these are direct gravure coating and offset
gravure coating, see Figure 1. Direct gravure coating
is where the fluid transfer takes place directly from the
gravure roll to the web, whilst in offset gravure coating,
fl uid is transferred fi rst from the gravure roll to a smooth
deformable roll (often termed the applicator roll), and
then from the deformable roll to the web. Whilst both
are described as gravure coating processes, the fluid
mechanics of these two processes are very different and
will be described separately.
Gravure ‘coating’ is distinct from gravure ‘printing’
(or roto-gravure), in that gravure coating is designed to
give uniform coverage on the substrate whilst gravure
printing is designed to print specifi c patterns. The quality
of gravure coating can be defi ned in terms of the thickness
and variation of the coating, whilst the quality of gravure
printing will include quantifi cation of print characteristics
such as resolution and edge definition. This article will
focus on gravure coating, but many of the emerging
markets, for example in the manufacture of electronic
products such as solar cells, require both large areas of
uniform coating but with good edge defi nition.
This article will fi rst describe the range of gravure cells
available and typical manufacturing techniques, together
with the important parameters that specify the gravure
roller, before describing in more detail the two distinct
gravure roll coating processes.
(a)
(b)
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57July / August 2011 CONVERTECH & e-Print
Fundamental Coating Research
2. Gravure Cell Specifi cation
Correctly specifying the gravure cell is crucial to the success
of the gravure coating process, since the shape and size of
the cell defi ne the operability windows of the coating process.
The cells themselves fall into two distinct categories—trihelical
patterns which are continuous grooves that run at some angle
around the roll surface and discrete patterns that consist of
individual gravure cells cut into the roll surface. Figure 2 shows
a series of images of typical gravure cells.
The process for manufacturing cells can be divided into
two categories—direct engraving of the cylinder or etching
of a cylinder through either chemical or laser means. Direct
engraving is where a master shape is forced into the roll
surface to cause an indentation. This can be done using a
diamond tipped stylus onto a copper plated roll, with each
indentation forming one gravure cell, or taking a hard master
knurling tool and rolling this against the copper plated surface.
In both cases a hard chromium layer is subsequently plated
onto the roll surface to provide longevity of operation. Etching
of a cylinder can either take place via a chemical or laser
ablation process. Of these, the use of lasers for direct ablation
of the surface is by far the most common process. The roll is
prepared by thermal spray coating of a ceramic material onto
the surface of the roll. This is fi nished to give a smooth surface.
A high-powered laser is then used to ablate the surface to give
the desired pattern. The ceramic is hard and gives excellent
wear resistance. The choice of the manufacturing process
directly dictates the shape of the gravure cell. Direct engraving
is often associated with quadrangular, pyramidal and trihelical
cells, whilst those cells produced by laser engraving tend to be
hexagonal in shape.
Quantitatively, the cells are described by the average cell
volume and the line count. In addition, the pattern of cells will
lie at some angle to the axis of the gravure roll, this is known as
the mesh or engraving angle and typically lies between 30 and
60 degrees (Fig. 2).
The average cell volume is used to express the volume
of the gravure cells contained on a unit area of roll surface.
One typical industry unit includes BCM (Billion Cubic Microns
per square inch), or to convert to the SI unit, 1 BCM is equal
to 1.55cm3/m2 or 1.55 microns. The average cell volume
expressed in SI units is the same as average incoming film
thickness if the fluid within the cells were evenly distributed
over the roll surface, giving an intuitive link between average
cell volume and equivalent inlet thickness. The line count of the
cell is a linear count of the cells along the angle of engraving
with typical units being lpi (lines per inch) or lpcm (lines per
cm). Typical screen counts can lie anywhere between 20 and
1500lpi, with average cell volumes of 1.5 to 75 microns (1 to
50 BCM), depending on the manufacturing method and cell
shape.
Whilst these parameters are commonly used for the
specifi cation of gravure rolls, there are other parameters which
are of importance in understanding the behavior of gravure
coating processes. Figure 2(d, i-ii) shows a schematic of
the cross-section through two gravure cells of the same cell
volume and the same line count. Clearly the shape of the two
cells is different, and as discussed later the characteristics
of fluid transfer out of these cells will differ. This highlights
a third parameter that is of importance—that of the area of
cell opening per unit area of roll surface. This parameter is
not explicitly controlled during manufacture, and is one point
of inconsistency between two rolls specified only by the cell
volume and line count.
3. Direct Gravure Coating
Direct gravure coating, Figure 1(a), is one of the most simple
of the coating processes from a mechanical perspective,
but (for single layer coatings at any rate) the fluid mechanic
processes are perhaps one of the most complex. It consists
of a gravure roller rotating in a bath of fluid (or alternatively
through an enclosed feed chamber), the action of which fills
the gravure cells with fl uid. Excess fl uid is removed from the
surface of the roll, so that the cells alone meter fl uid into the
(a) (b)
(c) (d)
Mesh
angle
i
ii
Figure 2 Schematic showing typical gravure
cells. (a) pyramidal, (b) quadrangular,
(c) continuous trihelical, (d) laser engraved
ceramic cells. A cross-section through each
of the cells along the line of engraving is also
shown
gravureleeds.indd 57gravureleeds.indd 57 11/09/14 8:3111/09/14 8:31
58 CONVERTECH & e-Print July / August 2011
Fundamental Coating Research
coating transfer region, using a doctor blade. Kapur (1999)
demonstrated that as the loading of the reverse angle doctor
blade against the roll is increased, the coated film thickness
falls to some minimum, associated with the point where excess
fl uid above the roll surface has been removed. Wear models
have been postulated to account for the wear of the doctor
blade as a function of time (Hanumanthu, 1999). The gravure
cells enter the coating transfer region, where fl uid is transferred
out of the cells onto the web, held against the roller with some
tension, T, and a wrap angle, β. The web generally moves in
the opposite direction to that of the roll to give a wider coating
window (Benkreira and Cohu, 1998). This coating transfer
region is illustrated in Figure 3. At the upstream meniscus, the
pressure gradient generated across the bead causes a fraction
of the fl uid to be evacuated from the cell.
For a Newtonian fl uid, the key parameters that determine
the behavior of the system are the fluid properties (viscosity
and surface tension), the web speed and the roll speed, and
to a lesser extent the web tension and wrap angle. Both the
shape and the size of the gravure cell also play a key role in
determining the fi nal coating properties. For a given gravure
pattern, there is only a small window over which the coating
thickness can be varied through changing process parameters.
Therefore the correct specifi cation of the gravure pattern at the
outset is important.
Experimental work of Kapur (2003) demonstrates the
interplay between cell shape and size. A smooth shallow
cell was found to give better pickout (defined as the fraction
of the fl uid evacuated from the cell) than a more angular and
deeper cell. The effect of increasing the web speed whilst
keeping the roll speed constant has also been explored. Here
the pickout asymptotically increases to some maximum value
below the theoretical maximum value of 1. This suggests that
a proportion of fluid within the cell remains trapped. If this
fl uid remains in the base of the cell it may have a signifi cantly
increased residence time within the process. Once this upper
limit has been reached, then further increases in the web
speed result in a decrease in the coated fi lm thickness since
the flux of coating solution onto the web remains constant,
but the average film thickness reduces as the web speed
increases. At high web-to-roll speed ratios, the upper limit of
the operating window is dictated by the point the coating bead
between the web and roller breaks, causing streaking along
the web. Typical behavior is illustrated in Figure 3.
Efforts are ongoing to develop appropriate models to
capture the behavior of the direct gravure coating process.
Early work considered the complex evacuation process at the
upstream meniscus, where a pressure gradient causes fl uid to
be swept out of the cell. Rees (1995) studied the behavior of
a single (2-dimensional) cell as it moved beneath a meniscus,
Schwartz et al. (1998) studied a more realistic cell pattern
but used lubrication theory to examine the effect of the cell
geometry on pickout. However, without knowledge of the
conditions within the entire coating bead, it is not possible
to relate the emptying behavior of the cell to the process
parameters. A more recent method (Hewson et al. 2011)
has used a multi-scale approach to link the large scale fluid
mechanics within the coating bead to that of the small scale
fl uid mechanics within a single gravure cell. Computational fl uid
dynamic simulations model the fl ow between a single cell and
moving web (an example of which is shown in Fig. 4), and a
modifi ed lubrication approach based on these fi ndings is used
Fi
lm
th
ic
kn
es
s
μm
Speed ratio
15
10
5
0
0 0.5 1.51 2
60lpi laser engraved
100lpi laser engraved
200lpi laser engraved
300lpi laser engraved
60lpi quadrangular
200lpi quadrangular
0.8
0.6
0.4
0
0 0.5 1.51 2
0.2
60lpi laser engraved
100lpi laser engraved
200lpi laser engraved
300lpi laser engraved
60lpi quadrangular
200lpi quadrangular
Speed ratio
Fr
ac
tio
na
l p
ic
ko
ut
(a)
(b)
Figure 3 Typical variation in (a) coated fi lm
thickness and (b) fractional pickout for a range
of gravure rolls as the web-to-roll speed ratio
is varied.
Conditions: roll speed 0.66m/s, fl uid viscosity
1mPa s, surface tension 33mN/m. (taken from
Kapur (1999))
gravureleeds.indd 58gravureleeds.indd 58 11/09/14 8:3111/09/14 8:31
59July / August 2011 CONVERTECH & e-Print
Fundamental Coating Research
to approximate the dynamics of the whole bead. Early results
from this approach look promising and offer the potential
for a fully predictive framework in which the influence of the
parameters that defi ne the direct gravure coating process can
be fully explored.
4. Offset Gravure Coating
In offset gravure roll coating, illustrated in Figure 1(b), there
is an intermediate transfer from the gravure roll to a deformable
roll. The smooth liquid film on the deformable roll is then
metered onto the web, most commonly via a forward or reverse
kiss coating nip. The addition of this extra transfer region gives
additional fl exibility in adjusting the fi nal fi lm thickness on the
web. The kiss coating processes are illustrated in Figure 5.
Whilst the direct gravure process described in section 3 is
generally run in reverse mode, the transfer between the gravure
roll and the deformable roll is generally run in forward mode,
with both roll surfaces passing through the coating transfer
region in the same direction. This is to minimize wear on the
deformable roll. The pickout process from the gravure cell
is significantly different than that of direct gravure coating as
illustrated in Figure 1(b).
There is little published work describing the transfer
between the gravure roll and deformable roll. Kapur (1999)
showed that as the nip force between the gravure roller and
the deformable roll increases, then the fi lm thickness decreases
to some lower limit. Similarly, as the speed of the two rolls are
increased (noting that the ratio of speeds between the gravure
roll and the deformable roll is fi xed at 1 to prevent excessive
wear) then the film thickness leaving the gravure-deformable
transfer region asymptotes to some limiting value. For the
range of gravure cells presented by Kapur et al. (2001) covering
a range of quadrangular and laser engraved rolls with volumes
between 10 and 60 microns and line counts of 60 and 200lpi),
this occurred at relatively low speeds (<60m/min), which
suggests that in most practical situations the fi lm thickness that
is transferred into the kiss coating nip is not strongly affected
by speed. The pickout from these cells at this asymptotic limit
lies between 10 and 25%, and in common with direct gravure
coating, shallow smooth cells give a greater fractional pickout.
What is much better understood is the kiss coating region
that exists between the deformable roll and the moving web.
Here there are two possible arrangements, reverse kiss coating
(Figure 5(a)), where the web and roll motion through the fl uid
transfer region are in opposite directions and forward kiss
coating (Figure 5(b)) where the web and roll motions through
the transfer region are in the same direction.
Since the roll is smooth, the use of lubrication theory to
establish an analytic model is valid. For the reverse kiss coat,
Gaskell et al. (1998a) developed a model that to predict the fi lm
thickness (Hweb) incorporated the effects of applicator speed
(Uapp) web-to-roll speed ratio (S), roll radius (R), the web tension
(T) and wrap angle (β) and the fl uid properties of viscosity (µ)
and surface tension (σ). This resulting expression,
Figure 5 (a) reverse mode kiss coating nip (b) forward mode kiss coating nip
Uapp
Uweb
Hweb
T
Hin
Uapp
Uweb
Hweb
T
Hin
(a) (b)
ȕ ȕ
Figure 4 Flow between the moving web and
the gravure cell within the web-to-roll transfer
region. The black lines show the streamlines
and highlight a closed eddy within the cell, the
colors indicate the magnitude of the velocity
(blue = low, red = high)
gravureleeds.indd 59gravureleeds.indd 59 11/09/14 8:3111/09/14 8:31
60 CONVERTECH & e-Print July / August 2011
Fundamental Coating Research
Hweb =
R
S
Hin
R
− 6
5
μUapp
σ
⎛
⎝ ⎜
⎞
⎠ ⎟
1− S( )2 σ
Tβ
⎛
⎝ ⎜
⎞
⎠ ⎟
⎡
⎣
⎢
⎤
⎦
⎥
(1)
is valid for S<1 and non-zero wrap angles.
At speeds ratios greater than 1 in the reverse mode of
operation, all fl uid is observed to transfer from the applicator
roll to the web and the resulting thickness is given by
Hweb =
Hin
S (2)
For the forward mode of operation, the fluid pressure
within the kiss bead has to overcome the tension holding the
web onto the substrate. If the inlet has an excess of fl uid, the
action of the web will cause some metering of the fl uid so only
a limiting amount passes the gap between the web and roll.
Eshel and Elrod (1965) derived an expression for a foil bearing
which can be used to estimate this limiting thickness
Hmin = 0.65R
6μ Uweb +Uapp( )
T
⎡
⎣
⎢
⎢
⎤
⎦
⎥
⎥
2
3
(3)
As is often the case, the inlet film thickness produced
from the gravure-deformable nip will be less than this limiting
thickness, and in this case all the inlet fi lm will transfer between
the web and roll. The effective fi lm thickness is given by
Heff =min Hmin,Hin( ) (4)
At the outlet, the fluid carried through the coating bead
must split between the upper moving web and the deformable
roll surface. Assuming the fi lm-split follows that of a forward
roll coating arrangement (Gaskell et al. 1998b), where the fl uid
is split depending on the web-to-roll speed ratio, then the fi nal
coated fi lm thickness is given by
Hweb =
Heff S S + 3( )
3S +1 (5)
where S is the ratio of the web speed to applicator speed.
5. Conclusions
Gravure coating is a versatile process which is finding
application across a growing number of sectors. To fully
understand the process, it is important to recognize the
differences between different arrangements of coat heads
and to understand the interaction of each fl uid transfer region.
Models are extremely useful in understanding this behavior
and can be used as a guide in both specifying equipment
at the design stage and in troubleshooting during operation.
For gravure coating these models are under continuous
development and offer the exciting prospect of being able to
establish a formal link between the process parameters and
the fi nal fi lm thickness.
6. References
[1] Benkreira, H.; Cohu, O., Direct forward gravure coating
on unsupported web, Chemical Engineering Science, 53 (6)
1223–1231, 1998.
[2] Booth, G.L., Coating Equipment and Processes Lockwood,
Publishing Company, New York, 1970.
[3] Booth, G.L., Coating converting processes: Traditional
methods
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