INK- JET PRINTING METHOD
The present invention relates to a printing ink, and particularly to a method for printing a
hybrid inkjet ink.
Digital inkjet printing is becoming an increasingly popular method for the production of fine
graph ic images for advertising , due to its low implem entation cost and versati lity in
com parison with trad itional techniq ues such as lithog raphic and screen printing . Inkjet
printers comprise one or more printheads that include a series of nozzles through which ink is
ejected onto a substrate. The printheads are typically provided on a printer carriage that
traverses the print width (moves back and forth across the substrate) during the printing
process.
Two main ink chemistries are used : inks that dry by solvent evaporation and inks that dry by
exposure to actinic radiation (typically UV radiation). Wide-format solvent-based inkjet printers
are an economic route into the industry as they are a relatively low-cost option compared to
the more complex machines employed for UV curing. Solvent-based inkjet printing also has
other advantages. As well as the lower cost, the ink films produced are thinner (and therefore
flexible) and yield a good quality natural looking image with a gloss finish. Furthermore, it is
difficult to achieve very high pigment loadings in UV curable inks due to the high viscosity of
the ink: if too much pigment is added , the ink becomes too viscous and cannot be jetted . In
contrast, solvent-based inks include a high proportion of solvent and therefore have a lower
viscosity, which means that higher pigment loadings can be tolerated. In addition, the printed
film produced from solvent-based inkjet inks is formed predominantly of pigment along with
comparatively few other solids that are included in the ink. The pigment is therefore largely
unobscured, resulting in intense, vivid and vibrant colours and a large colour gamut.
However, there are some limitations to solvent-based inkjet technology. In particular, solventbased
inks may not adhere to certain types of substrate, particularly non-porous substrates
such as plastics, and the cured films have poor resistance to solvents. However, the printing
of hig h-quality low-intercolour-bleed inkjet imag es with good mechanical and chem ical
resistance properties onto less receptive substrates is a req uirement in many ind ustrial
printing applications. Such substrates include rigid PVCs, polyester and polycarbonate.
In addition, inkjet inks capable of being printed at small drop sizes and hence producing the
req uired hig h image qual ity have a number of form ulation constrai nts , incl uding the
requirement for low viscosity in order to be printed through these low drop volume printheads.
This is easily achievable with solvent-based ink compositions due the inherent low viscosity of
the organic solvents used. However, these types of ink often have poor chemical and scratch
resistance and can have difficulty in drying on these less receptive materials.
To give adeq uate head stability, solvent-based inkjet inks are typically formu lated with
relatively low evaporation rate solvents and the inks rely on both evaporation and imbibition
into the substrate to give adequate pinning of the ink droplets to fix the image quality (the term
"pinning" is used in the art to mean arresting the flow of the ink by treating the ink droplets
quickly after they have impacted onto the substrate surface). If the solvent is not able to
penetrate into the substrate after deposition of the ink droplet, the rate of viscosity increase is
too slow resulting in excessive bleed . If faster evaporating solvents are used in an attempt to
overcome this problem head stability can be compromised throug h solvent loss leading to
build up of dried ink deposits on the head face plate. In addition the use of faster solvent
blends can also give rise to undesirable Marangoni effects, where faster evaporation at the
edge of the ink deposit gives rise to a surface tension gradient which drives a bulk flow to the
print edges (the so-called "coffee stain effect").
Conventional UV-curable inkjet inks have excellent head stability and typically have better
mechanical and chemical resistance properties than solvent-based inks. Image quality is less
affected by the nature of the substrate as the droplet is cured or partially pinned by exposure
to ultraviolet light immediately after deposition. However, the inherently higher viscosity of the
radiation-curable materials greatly restricts the formulation latitude and in practice inks with
suitably low viscosities have poor mechanical and chemical resistance properties.
Hybrid radiation-curable/solvent-containing inkjet inks (see, for example, international patent
application no. PCT/GB201 0/051 384) can overcome most of the above limitations and allow
UV-curable inks to be formulated to meet the low viscosity requirements (previously met by
purely solvent-based inks) whilst still maintaining the chemical resistance and mechanical
properties (as previously provided mainly by UV-curable inks) required for these industrial
applications. However, in common with purely solvent-based inks, there are limitations to the
substrate types that can be used. This is because, like solvent-based inks, hybrid inks also fix
image quality by solvent loss and imbibition; this means that image quality is reduced on non
solvent receptive substrates and so presents a problem. Accordingly, there remains a need
in the art for approaches which address these problems.
Accordingly, the present invention provides a method of inkjet printing com prising the
following steps, in order:
(i) providing a hybrid inkjet ink comprising an organic solvent, a radiation-curable material, a
photoinitiator and optionally a colorant;
(ii) printing the ink on to a substrate;
(iii) pinning the ink by exposing the ink to actinic radiation at a dose of 1-200 mJ/cm2;
(iv) evaporating at least a portion of the solvent from the ink; and
(v) exposing the ink to additional actinic radiation to cure the ink.
Thus, it has surprisingly been found that it is possible to pin (or partially cure) a hybrid inkjet
ink composition by firstly exposing the wet ink film to a weak UV source immediately after
deposition without first evaporating the organic solvent in the composition. In this manner the
viscosity of the wet ink composition can be increased just sufficiently to arrest the flow of the
ink droplet and prevent degradation of the image quality due to ink bleed , thus avoiding the
problems highlighted hereinabove. At this stage it is critical that the level of UV exposure is
restricted to avoid excessive polymerisation of the film , which will lead to solvent entrapment
and degradation of image quality and resistance properties.
After pinning the solvent is then removed by evaporation, for example by exposure to a
suitable heat source. Finally the film is fully cured, by exposure to a suitable radiation source.
By using this process it is possible to achieve all the key properties required on substrates
typically used in these applications.
The present invention will now be described with reference to the accompanying drawings, in
which:
Fig . 1 shows a perspective view of an exemplary embodiment of an inkjet printing apparatus
according to the present invention;
Fig . 2 shows a section view of an exemplary embodiment of an inkjet printing apparatus (rollto-
roll printer) according to the present invention;
Fig. 3 shows a section view of an exemplary embodiment of an inkjet printing apparatus (flat¬
bed printer) according to the present invention; and
Figs . 4-1 0 show images printed using the method of the present invention (as set out in
Example 3).
The ink
The inks of the present invention comprise a modified ink binder system. The presence of a
radiation-curable material and a photoinitiator in the ink means that crosslinked polymers can
be formed in the dried ink film , leading to improved adhesion to a range of substrates and
improved resistance to solvents. The presence of at least 30% by weight of organic solvent
means that the advantageous properties of solvent-based inkjet inks are expected to be
maintained, however.
By "radiation-curable material" is meant a material that polymerises or crosslinks when
exposed to radiation, commonly ultraviolet light, in the presence of a photoinitiator.
The radiation-curable material can comprise a monomer with a molecular weight of 450 or
less, an oligomer, or mixtu res thereof. The monomers and/or oligomers may possess
different degrees of functionality, and a mixture including combinations of mono, di, tri and
higher functionality monomers and/or oligomers may be used.
Preferably, the radiation-curable material comprises a radiation-curable oligomer.
Radiation-curable oligomers suitable for use in the present invention comprise a backbone,
for example a polyester, urethane, epoxy or polyether backbone, and one or more radiation
polymerisable grou ps . The polymerisable grou p can be any grou p that is capable of
polymerising upon exposure to radiation.
Preferred oligomers have a molecular weight of 500 to 4,000, more preferably 600 to 4,000.
Molecular weights (number average) can be calcu lated if the structu re of the oligomer is
known or molecular weights can be measured using gel permeation chromatography using
polystyrene standards.
In one embodiment the radiation-curable material polymerises by free-radical polymerisation.
Suitable free-rad ical polymerisable monomers are well known in the art and incl ude
(meth)acrylates, ,-unsaturated ethers, vinyl amides and mixtures thereof.
Monofunctional (meth)acrylate monomers are well known in the art and are preferably the
esters of acrylic acid . Preferred examples include phenoxyethyl acrylate (PEA), cyclic TMP
formal acrylate (CTFA), isobornyl acrylate (IBOA), tetrahydrofurfuryl acrylate (THFA), 2-(2-
ethoxyethoxy)ethyl acrylate, octadecyl acrylate (ODA), tridecyl acrylate (TDA), isodecyl
acrylate (IDA) and lauryl acrylate. PEA is particularly preferred.
Suitable multifu nctional (meth)acrylate monomers incl ud e d i-, tri- and tetra-functional
monomers. Examples of the multifunctional acrylate monomers that may be included in the
ink-jet inks include hexaned iol diacrylate, trimethylolpropane triacrylate, pentaerythritol
triacrylate, polyethylene glycol diacrylate (for example tetraethylene glycol diacrylate),
dipropylene glycol diacrylate, tri(propylene glycol) triacrylate, neopentyl glycol diacrylate,
bis(pentaerythritol) hexaacrylate, and the acrylate esters of ethoxylated or propoxylated
glycols and polyols , for example, propoxylated neopentyl glycol diacrylate, ethoxylated
trimethylolpropane triacrylate, and mixtures thereof.
Suitable multifunctional (meth)acrylate monomers also include esters of methacrylic acid (i.e.
methacrylates), such as hexaned iol dimethacrylate, trimethylolpropane trimethacrylate,
triethyle neg lycol d imethacrylate , diethyl eneglycol dimethacrylate , ethyle neg lycol
dimethacrylate, 1,4-butanediol dimethacrylate. Mixtures of (meth)acrylates may also be used.
(Meth)acrylate is intend ed herein to have its standard mean ing , i.e. acrylate and/or
methacrylate. Mono and multifunctional are also intended to have their standard meanings,
i.e. one and two or more groups, respectively, which take part in the polymerisation reaction
on curing.
,-Unsaturated ether monomers can polymerise by free-radical polymerisation and may be
usefu l for red ucing the viscosity of the ink when used in com bination with one or more
(meth)acrylate monomers. Examples are well known in the art and include vinyl ethers such
as triethylene glycol divinyl ether, diethylene glycol divinyl ether, 1,4-cyclohexanedimethanol
divi nyl ether and ethylene glycol monovi nyl ether. Mixtu res of ,-unsaturated ether
monomers may be used.
N-Vinyl amides and N-(meth)acryloyl amines may also be used in the inks of the invention.
N-vinyl amides are well-known monomers in the art and a detailed description is therefore not
required. N-vinyl amides have a vinyl group attached to the nitrogen atom of an amide which
may be further substituted in an analogous manner to the (meth)acrylate monomers .
Preferred examples are N-vinyl caprolactam (NVC) and N-vinyl pyrrolidone (NVP). Similarly,
N-acryloyl amines are also well-known in the art. N-acryloyl amines also have a vinyl group
attached to an amide but via the carbonyl carbon atom and again may be further substituted
in an analogous manner to the (meth)acrylate monomers . A preferred exam ple is Nacryloylmorpholine
(ACMO).
Particularly preferred radiation-curable materials are oligomers with free-radical polymerisable
groups, preferably (meth)acrylate groups. Acrylate functional oligomers are most preferred.
In one embod iment the oligomer com prises two or more rad ical polymerisable groups,
preferably three or more , more preferably fou r or more . Oligom ers com pris ing s ix
polymerisable groups are particularly preferred.
The oligomer preferably comprises a urethane backbone.
Particularly preferred radiation-curable materials are urethane acrylate oligomers as these
have excellent adhesion and elongation properties. Most preferred are tri-, tetra-, penta-,
hexa- or higher functional urethane acrylates, particularly hexafunctional urethane acrylates
as these yield films with good solvent resistance.
Other suitable examples of radiation-curable oligomers include epoxy based materials such
as bisphenol A epoxy acrylates and epoxy novolac acrylates, which have fast cure speeds
and provide cured films with good solvent resistance.
The radiation-curable oligomer used in the preferred inks of the invention cures upon
exposure to radiation in the presence of a photoinitiator to form a crosslinked , solid film. The
resulting film has good adhesion to substrates and good solvent resistance. Any radiationcurable
oligomer that is compatible with the remaining ink components and that is capable of
curing to form a crosslinked, solid film is suitable for use in the ink of the present invention.
Thus , the ink form ulator is able to select from a wide rang e of suitable oligomers . In
particular, the oligomer can be a low molecular weight material that is in liquid form at 25°C.
This is beneficial when aiming to produce a low viscosity ink. Furthermore, the use of a low
molecular weight, liqu id oligomer is advantageous when formulating the ink because low
molecular weight liquid oligomers are likely to be miscible in a wide range of solvents.
Preferred oligomers for use in the invention have a viscosity of 0.5 to 20 Pa.s at 60°C, more
preferably 5 to 15 Pa.s at 60°C and most preferably 5 to 10 Pa.s at 60°C. Oligomer
viscosities can be measured using an ARG2 rheometer manufactured by T.A. Instruments,
which uses a 40 mm oblique / 2° steel cone at 60°C with a shear rate of 25 seconds ~1 .
In one embodiment the radiation-curable material comprises 50 to 100%, or 75 to 100% by
weight of free-radical curable oligomer and 0 to 50%, or 0 to 25% by weight of free-radical
curable monomer, based on the total weight of radiation-curable material present in the ink.
Preferably the ink comprises less than 20% by weig ht of radiation-curable material (e.g .
(meth)acrylates) having a molecular weight of less than 450 based on the total weight of the
ink, or less than 10% by weight, more preferably less than 5% by weig ht. In a particu larly
preferred embod iment, the ink of the invention is substantially free of radiation-curable
material with a molecular weight of less than 450.
In one embod iment the ink comprises less than 20% by weig ht of (meth)acrylates with a
molecular weight of less than 600 based on the total weight of the ink, or less than 10% by
weight, more preferably less than 5% by weight. In a particularly preferred embodiment, the
ink of the invention is substantially free of (meth)acrylates with a molecular weight of less than
600.
By "substantially free" is meant that no radiation-curable material having a molecular weight of
less than 450 or 600, respectively, is intentionally added to the ink. However, minor amounts
may be present as impurities in commercially available radiation-curable oligomers or in the
pigment dispersion and are tolerated .
In an alternative embodiment of the invention the radiation-curable material is capable of
polymerising by cationic polymerisation. Suitable materials include, oxetanes, cycloaliphatic
epoxides, bisphenol A epoxides, epoxy novolacs and the like. The radiation-curable material
according to this embodiment may comprise a mixture of cationically curable monomer and
oligomer. For example, the radiation-curable material may comprise a mixture of an epoxide
oligomer and an oxetane monomer.
In one embod iment the radiation-curable materia l com prises 0 to 40% by weig ht of
cationically curable oligomer and 60 to 100% by weig ht of cationically curable monomer
based on the total weight of radiation-curable material present in the ink.
The radiation-curable material can also comprise a combination of free-radical polymerisable
and cationically polymerisable materials.
The radiation-curable material is preferably present in the composition in an amount of 2% to
65% by weight, based on the total weight of the ink, more preferably 2 to 45% by weig ht,
more preferably 5 to 35% by weight, more preferably 8 to 25% by weight, and most preferably
10% to 25% by weight.
The ink of the invention includes one or more photoinitiators. When the ink of the invention
includes a free-radical polymerisable material the photoinitiator system includes a free-radical
photoinitiator and when the ink includes a cationic polymerisable material the photoinitiator
system includes a cationic photoinitiator. When the ink comprises a combination of freeradical
polymerisable and cationically polymerisable materials both a free-radical and cationic
initiator are required.
The free-rad ical photoinitiator can be selected from any of those known in the art. For
example, benzophenone, 1-hydroxycyclohexyl phenyl ketone, 1-[4-(2-hydroxyethoxy)-phenyl]-
2-hydroxy-2-methyl-1 -propane-1 -o ne , 2-benzyl-2-dimethylamino-(4-morpholinophenyl)butan-
1-one, isopropyl thioxanthone, benzil dimethylketal, bis(2,6-dimethylbenzoyl)-2,4,4-
trimethylpentylphosphine oxide or mixtures thereof. Such photoinitiators are known and
commercially available such as, for example, under the trade names Irgacure and Darocur
(from Ciba) and Lucerin (from BASF).
In the case of a cationically curable system , any suitable cationic initiator can be used , for
example sulfonium or iodonium based systems. Non limiting examples include: Rhodorsil PI
2074 from Rhodia; MC AA, MC BB, MC CC, MC CC PF, MC SD from Siber Hegner; UV9380c
from Alfa Chemicals; Uvacure 1590 from UCB Chemicals; and Esacure 1064 from Lamberti
spa.
Preferably the photoinitiator is present in an amount of 1 to 20% by weight, preferably 4 to
10% by weight, based on the total weight of the ink.
The ink of the invention contains an organic solvent. The organic solvent is in the form of a
liq uid at ambient tem peratu res and is capable of acti ng as a carrier for the remaini ng
components of the ink. The organic solvent component of the ink of the invention may be a
single solvent or a mixture of two or more solvents. As with known solvent-based inkjet inks,
the organic solvent used in the ink of the present invention is required to evaporate from the
printed ink, typically on heating, in order to allow the ink to dry. The solvent can be selected
from any solvent commonly used in the printing industry, such as glycol ethers, glycol ether
esters, alcohols, ketones, esters and pyrrolidones.
The organic solvent is preferably present in an amou nt of at least 30% by weig ht, more
preferably at least 50% by weight, and most preferably at least 60% by weight based on the
total weight of the ink. The upper limit is typically 85% or 75% by weight based on the total
weight of the ink.
Known solvent-based inkjet inks dry solely by solvent evaporation with no crosslinking or
polymerisation occu rring . The film prod uced therefore has limited chem ical resistance
properties. In order to improve resistance of prints to common solvents such as alcohols and
petrol, binder materials that have limited solubility in these solvents are added to the ink. The
binder is typically in solid form at 25°C so that a solid printed film is produced when solvent is
evaporated from the ink. Suitable binders such as vinyl chloride copolymer resins generally
have poor solubility in all but the strongest of solvents such as glycol ether acetates and
cyclohexanone, both of which are classified as "harmful" and have strong odours. In order to
solubilise the binder, these solvents are generally added to the ink.
The ink of the present invention includes radiation-curable material that cures as the ink dries
and it is not therefore necessary to include a binder in the ink in order to provide a printed film
having improved solvent resistance. In one embodiment of the invention the organic solvent
is not therefore required to solubilise a binder such as a vinyl chloride copolymer resin, which
means that the ink formulator has more freedom when selecting a suitable solvent or solvent
mixture.
In a preferred embodiment the organic solvent is a low toxicity and/or a low odour solvent.
Solvents that have been given VOC exem pt status by the United States Environmental
Protection Agency or European Council are also preferred.
The most preferred solvents are selected from glycol ethers and organic carbonates and
mixtures thereof. Cyclic carbonates such as propylene carbonate and mixtures of propylene
carbonate and one or more glycol ethers are particularly preferred.
Alternative preferred solvents include lactones, which have been found to improve adhesion
of the ink to PVC substrates . Mixtu res of lactones and one or more glycol ethers , and
mixtu res of lactones, one or more glycol ethers and one or more organic carbonates are
particularly preferred . Mixtures of gamma butyrolactone and one or more glycol ethers, and
mixtures of gamma butyrolactone, one or more glycol ethers and propylene carbonate are
particularly preferred.
In another embodiment of the invention, dibasic esters and/or bio-solvents may be used.
Dibasic esters are known solvents in the art. They can be described as di(C1-C4 alkyl) esters
of a saturated aliphatic dicarboxylic acid having 3 to 8 carbon atoms having following general
formula:
in which A represents (CH2) -6, and R and R2 may be the same or different and represent -
C4 alkyl which may be a linear or branched alkyl rad ical having 1 to 4 carbon atoms ,
preferably methyl or ethyl, and most preferably methyl . Mixtures of dibasic esters can be
used.
Bio-solvents, or solvent replacements from biological sources, have the potential to reduce
dramatically the amount of environmentally-polluting VOCs released in to the atmosphere and
have the further advantage that they are sustainable. Moreover, new methods of production
of bio-solvents derived from biological feedstocks are being discovered , which allow biosolvent
production at lower cost and higher purity.
Examples of bio-solvents include soy methyl ester, lactate esters, polyhydroxyalkanoates,
terpenes and non-linear alcohols, and D-limonene. Soy methyl ester is prepared from soy.
The fatty acid ester is prod uced by esterification of soy oil with methanol. Lactate esters
preferably use fermentation-derived lactic acid which is reacted with methanol and/or ethanol
to produce the ester. An example is ethyl lactate which is derived from corn (a renewable
source) and is approved by the FDA for use as a food additive. Polyhydroxyalkanoates are
linear polyesters which are derived from fermentation of sugars or lipids. Terpenes and non
linear alcohol may be derived from corn cobs/rice hulls. An example is D-limonene which
may be extracted from citrus rinds.
Other solvents may be included in the organic solvent component. A particularly common
source of other solvents is derived from the way in which the colouring agent is introduced
into the inkjet ink formu lation. The colou ring agent is usually prepared in the form of a
pigment dispersion in a solvent, e.g. 2-ethylhexyl acetate. The solvent tends to be around 40
to 50% by weig ht of the pig ment dis persion based on the total weig ht of the pig ment
dispersion and the pigment dispersion typically makes up around 5 to 15% by weight of the
ink and sometimes more.
The ink is preferably substantial ly free of water, althoug h some water will typically be
absorbed by the ink from the air or be present as impurities in the components of the inks,
and such levels are tolerated. For example, the ink may comprise less than 5% by weight of
water, more preferably less than 2% by weight of water and most preferably less than 1% by
weight of water, based on the total weight of the ink.
The ink of the present invention can be a coloured ink or a colourless ink.
By "colourless" is meant that the ink is substantially free of colorant such that no colour can
be detected by the naked eye. Minor amounts of colorant that do not produce colour that can
be detected by the eye can be tolerated, however. Typically the amount of colorant present
will be less than 0.3% by weig ht based on the total weight of the ink, preferably less than
0 .1%, more preferably less than 0.03%. Colourless inks may also be described as "clear" or
"water white".
Coloured inks of the invention comprise at least one colouring agent. The colouring agent
may be either dissolved or dispersed in the liquid medium of the ink. Preferably the colouring
agent is a dispersible pigment, of the types known in the art and commercially available such
as under the trade-names Paliotol (available from BASF pic), Cinq uasia, Irgalite (both
available from Ciba Speciality Chemicals) and Hostaperm (available from Clariant UK). The
pigment may be of any desired colou r such as, for example, Pigment Yellow 13, Pigment
Yellow 83, Pigment Red 9 , Pigment Red 184, Pigment Blue 15:3, Pigment Green 7 , Pigment
Violet 19, Pig ment Black 7. Especial ly usefu l are black and the colou rs req uired for
trichromatic process printing . Mixtures of pigments may be used.
In one aspect of the invention the following pigments are preferred . Cyan: phthalocyanine
pigments such as Phthalocyanine blue 15.4. Yellow: azo pigments such as Pigment yellow
120, Pigment yellow 15 1 and Pigment yellow 155. Magenta: quinacridone pigments, such as
Pigment violet 19 or mixed crystal quinacridones such as Cromophtal Jet magenta 2BC and
Cinquasia RT-355D. Black: carbon black pigments such as Pigment black 7.
Pig ment particles dispersed in the ink should be sufficiently small to allow the ink to pass
through an inkjet nozzle, typically having a particle size less than 8 , preferably less than 5
, more preferably less than 1 and particularly preferably less than 0.5 .
The colorant is preferably present in an amount of 20 weight% or less, preferably 10 weight%
or less, more preferably 8 weight% or less and most preferably 2 to 5% by weight, based on
the total weight of the ink. A higher concentration of pigment may be required for white inks,
however, for example up to and including 30 weight%, or 25 weig ht% based on the total
weight of the ink.
The ink can optionally contain a thermoplastic resin. The thermoplastic resin does not include
reactive groups that are able to crosslink on exposure to radiation. In other words,
thermoplastic resin is not a radiation-curable material. Suitable materials have molecular
weights ranging from 10,000 to 100,000 as determined by GPC with polystyrene standards.
The thermoplastic resin can be selected from epoxy, polyester, vinyl or (meth)acrylate resins,
for example. Methacrylate copolymers are preferred. When present, the ink can comprise 1
to 5% by weight of thermoplastic resin, based on the total weight of the ink. The
thermoplastic resin increases the viscosity of the ink film prior to curing, leading to improved
print definition. The thermoplastic resin also decreases the glass transition temperature of the
cured ink, giving greater film flexibility for applications such as vehicle side application.
In one embodiment, the ink of the invention comprises at least 50% by weight of organic
solvent based on the total weight of the ink; a radiation-curable material , wherein the
radiation-curable material comprises 50 to 100% by weight of free-radical curable oligomer
having a molecular weight of 600 to 4,000 and 0 to 50% by weight of free-radical curable
monomer having a molecular weight of 450 or less based on the total weight of radiationcurable
material present in the ink; a free-radical photoinitiator; and optionally a colorant.
The inkjet ink exhibits a desirable low viscosity (200 mPa.s or less, preferably 100 mPa.s or
less, more preferably 25 mPa.s or less, more preferably 10 mPa.s or less and most preferably
7 mPa.s or less at 25 °C).
In ord er to prod uce a hig h qual ity pri nted image a s mall jetted drop size is desi rable.
Furthermore, small droplets have a higher surface area to volume ratio when compared to
larger drop sizes, which facilitates evaporation of solvent from the jetted ink. Small drop sizes
therefore offer advantages in drying speed. Preferably the inkjet ink of the invention is jetted
at drop sizes below 50 picolitres, preferably below 30 picolitres and most preferably below 10
picolitres.
To achieve compatibility with print heads that are capable of jetting drop sizes of 50 picolitres
or less, a low viscosity ink is required . A viscosity of 10 mPa.s or less at 25°C is preferred, for
example, 2 to 10 mPas, 4 to 8 mPa.s, or 5 to 7 mPa.s. It is problematic to achieve these low
viscosities with conventional radiation-curable inks due to the relatively high viscosities of
acrylate monomers and oligomers used in the compositions, but the presence of a significant
amou nt of organic solvent in the ink of the invention allows these low viscosities to be
achieved.
Ink viscosity may be measured using a Brookfield viscometer fitted with a thermostatically
controlled cup and spindle arrangement, such as a DV1 low-viscosity viscometer running at
20 rpm at 25 °C with spindle 00.
Other components of types known in the art may be present in the ink to improve the
properties or performance. These components may be, for example, surfactants, defoamers,
dispersants, synergists for the photoinitiator, stabilisers against deterioration by heat or light,
reodorants, flow or slip aids, biocides and identifying tracers.
In one aspect of the invention the surface tension of the ink is controlled by the addition of
one or more surface active materials such as commercially available surfactants. Adjustment
of the surface tension of the ink allows control of the surface wetting of the ink on various
substrates, for example, plastic substrates. Too high a surface tension can lead to ink pooling
and/or a mottled appearance in high coverage areas of the print. Too low a surface tension
can lead to excessive ink bleed between different coloured inks. The surface tension is
preferably in the range of 20-32 mNnr and more preferably 2 1-27 mNnri .
The present invention also provides an ink set comprising a cyan ink, a magenta ink, a yellow
ink and a black ink (a so-called trichromatic set), wherein at least one of the inks is an ink
according to the present invention. Preferably all of the inks in the ink set are inks according
to the present invention. The inks in a trichromatic set can be used to produce a wide range
of secondary colours and tones by overlaying the printed dots on white substrate.
The ink set of the present invention can optionally include one or more light colour inks. Light
colou r versions of any colou r ink can be used but preferred colours are light cyan , light
magenta and light black. Particularly preferred are light cyan inks and light magenta inks.
Light colour inks serve to extend the colour gamut and smooth the gradation from highlight to
shadow areas of the printed image.
The ink set of the present invention can optionally include one or more of a green ink, an
orange ink and a violet ink. These colours further extend the gamut of colours that can be
produced. Violet and orange inks are preferred, most preferred is orange ink.
The ink set of the present invention can optionally include a white ink. White ink can be used
in two ways. When printing onto a transparent substrate, white ink can be printed over the
image such that the image can be viewed from the reverse. Alternatively, white ink can be
used to print a base coat onto a coloured substrate before the image is printed.
Even with the range of inks detailed above, some colou rs can be particularly difficult to
produce. Where it is essential that a printed colour is an exact match to a standard, such as a
corporate colour, the ink set of the invention can optionally contain one or more inks having
matched spot colours, which are designed to be printed in pure form with no overlaying.
The ink of the present invention can produce an image having a hig h gloss finish. This
means that when the ink is printed on a substrate having low gloss, areas of the image that
have high deposits of ink (for example where the image has deep colou r or dark shading )
have a significantly higher gloss level than areas of the image that have low deposits of ink
(for example, where there is only light shading in the image). In other words, highlight areas
of the print will have a lower gloss level than the shadow areas. Sharp lines can appear in the
image where the transitions from heavy to light shading (e.g . from heavy gloss to low gloss)
occur, which can lead to unattractive prints.
In order to provide an even finish and therefore improve the image quality, the entire print can
optionally be coated with a colourless ink or varnish . Preferably, however, the ink of the
invention is printed together with a colou rless ink. The ink set of the present invention
therefore preferably includes a colourless ink.
The colou rless ink is jetted at the same time as the colou red ink of the invention but the
colourless ink is deposited in blank or hig hlig ht areas of the image that do not have hig h
deposits of coloured ink. This means that the ink film covers the entire printed surface of the
substrate, which results in prints with a more even finish across the print. The prints can also
tend to have a more even ink film weight across the film, which improves the appearance of
the prints because the surface topog raphy is more even and the transitions between the
areas of heavy coloured ink deposits to highlights are smoother.
Print heads accou nt for a significant portion of the cost of an entry level printer and it is
therefore desirable to keep the number of print heads (and therefore the number of inks in the
ink set) low. Reducing the number of print heads can reduce print quality and productivity,
however. It is therefore desirable to balance the number of print heads in order to minimise
cost without compromising print quality and productivity. One preferred ink set of the present
invention comprises a cyan ink, a yellow ink, a magenta ink and a black ink. This limited
combination of colours can achieve prints with a very high gloss that is even across the print,
very good graduations of tone and a high colour gamut. Further variations of the above ink
set can include the above ink set plus either one or more of a clear varnish, a metallic and a
white ink. Another example of ink set is a cyan ink, a yellow ink, a magenta ink and a black
ink, a colourless ink, a light cyan ink, a light magenta ink and an orange ink.
When the ink of the present invention is provided in an ink set, the surface tensions of the
different inks in the ink set preferably differ by no more than 2 mNm 1 , more preferably no
more than 1 mNm 1 and most preferably no more than 0.5 mNm 1 . Carefully balancing the
surface tension of the different inks in this manner can lead to improvements in the quality
and appearance of the printed image.
The ink set of the invention can optionally include one or more metallic effect inks. The use of
metallic colours such as silver is becoming increasing popular in advertising images, for
example.
Conventional solvent-based metal lic inks can prod uce very brig ht metallic effects. The
metallic pigments are in the form of flakes or platelets and these are randomly orientated in
the undried liquid ink. In the case of solvent-containing inks, the flakes can align parallel to
the print surface as the ink film thickness reduces as a result of solvent loss in the drying
process. The alig nment of metallic pigment flakes parallel with the print surface results in
good reflectivity and metallic lustre. However, the films produced can often have very poor
rub properties, which means that the pigment can be easily removed from the print surface.
UV cured metallic inks generally have better rub properties but are often dull in appearance
because the metallic pigment flakes do not have time to align during the rapid UV curing
process.
Metallic inks of the present invention overcome these problems because the inks dry in two
stages, as discussed below. During the solvent evaporation step the metallic flakes have
time to align, allowing a bright metallic effect to be produced in the final image. However, the
UV curing stage yields a rub-resistant film.
Colou rless inks accord ing to the present invention may be used as a varnish . In one
embodiment of the invention the colourless ink may be used as a varnish for a conventional
solvent-based metallic effect ink. Metallic effect prints can be protected with known UV
curable varnishes but the high film weight produced when these materials are jetted dulls the
metallic lustre of the prints and is deleterious to their appearance. The presence of a
relatively large proportion of volatile solvent in the colou rless inks of the present invention
allows a low film weight to be deposited , however. Typically a UV varnish would produce a
12 film over the surface of the print. By using a colourless ink according to the present
invention, the film weig ht can be red uced to 2 to 3 . The low film weig ht of the hybrid
varnish has a far less deleterious affect on the appearance of the metallic print.
The inks of the present invention are primarily designed for printing onto flexible substrates
but the natu re of the substrate is not limited and includes any substrate which may be
subjected to inkjet printing such as glass, metals, plastics and paper. Most preferred are
flexible substrates, especially flexible substrates used for the graphic printing industry. Non
limiting examples include, polyesters, fabric meshes, vinyl substrates, paper and the like. The
inks of the present invention are particularly suited for printing onto self adhesive vinyl and
banner grade PVC substrates.
The ink may be prepared by known methods such as stirring with a high-speed water-cooled
stirrer, or milling on a horizontal bead-mill.
The printing method
The printing method of the present invention requires the initial pinning of the inkjet ink by
exposing the ink to a low dose of actinic radiation. This provides a partial cure of the ink and
thereby maximises image quality by controlling bleed and feathering between image areas.
The ink is then dried by the evaporation of the solvent in order to provide a high-viscosity
coating which is capable of undergoing further curing. The coating is then exposed to further
actinic radiation to cure the ink fully.
It should be noted that the terms "dry" and "cure" are often used interchangeably in the art
when referring to radiation-curable inkjet inks to mean the conversion of the inkjet ink from a
liquid to solid by polymerisation and/or crosslinking of the radiation-curable material. Herein,
however, by "drying" is meant the removal of the solvent by evaporation and by "curing" is
meant the polymerisation and/or crosslinking of the rad iation-cu rable material. With the
hybrid inks and method of the present invention , pinning and drying leads to a marked
increase in viscosity, whereas the final cure converts the inkjet ink from a liquid ink to a solid
film.
Fig. 1 shows a perspective view of an exemplary embodiment of an inkjet printing apparatus
for use in the method according to the present invention. The apparatus includes a printer
head ( 1) , a heating unit (2) and a UV curing unit (3).
Fig . 2 shows a section view of an exemplary embodiment of an inkjet printing apparatus for
use in the method according to the present invention. The printer is a roll-to-roll printer. The
apparatus includes a print carriage including a print head ( 1) , heating unit(s) (2), a UV curing
unit (3) comprising a reflector (4) and a bulb (5).
Fig. 3 shows a photograph of a flat-bed printer which also falls within the scope of the present
invention.
With conventional solvent-based inks, the printer productivity is governed by the system's
ability to expel the bulk solvent. If too much wet ink is laid down on the medium , the ink flows
to blur the printed image. For this reason, solvents with a high vapour pressure are preferred
in the ink. However, if the solvent vapour pressure is too high, ink drying on the printhead
nozzle plate may lead to blocked nozzles. This compromise in solvent selection leads to a
limitation in productivity.
Because of their lower productivity, the capital cost for solvent printers has to be relatively low
to remain commercially viable. The internal mechanisms are therefore kept simple, with as
few printheads as possible to produce a reasonable quality image. The low complexity makes
these machines easy to operate and maintain.
Over recent years, UV curable ink systems have largely replaced solvent ink printers in the
higher productivity range, wide format graphics market. Unlike solvent printers, the ink
deposited on the surface does not appreciably evaporate upon heating. Instead, the material
is transformed into a solid through exposure to an energy source. In most cases, the energy
source is an intense UV light, which causes photo-crosslinking of curable molecules in the
presence of a photoinitiator to form a solid.
The greatest perceived benefit of UV curable printers is their ability to deliver high production
rates. In most UV printers, the cure source is mounted on the shuttling printhead carriage, on
one or both sides of the printhead cluster. In some cases, cure systems are also placed
between printheads. With a typical separation distance of less than 100 mm between the
print heads and cure unit, the maximum time between print and cure would be 0 .1 s for a
printhead carriage moving at 1 m/s. UV ink solidification times of less than one second
compare favourably with solvent inks that can take several minutes to dry. Inkjet printers for
UV curable inks are necessarily more complex and consequently more expensive than inkjet
inks printers for solvent-based inks, however.
The ink of the present invention can be printed using inkjet printers that are suitable for use
with solvent-based inkjet inks, in combination with a source of actinic radiation.
The features of printers that are suitable for printing solvent-based inkjet inks are well known
to the person skilled in the art and include the features described below.
As discussed above, printers suitable for printing solvent-based inkjet inks typically have a
low capital cost, which means that the printers tend to have simple internal mechanisms. In
practice, this means that inkjet printers suitable for printing solvent-based inks typically
comprise gravity feed systems for delivering ink from the ink supply to the printhead. In
contrast, UV printers use a pressu rised header tank for delivering the ink to the printhead ,
which allows control of the meniscus position in the nozzle.
Since printheads accou nt for a large proportion of the overall printer cost, inkjet printers
suitable for printing solvent-based inkjet inks include the minimum number of printheads that
is required to provide a high quality image. In any event, because solvent-based inkjet inks
typically require longer to dry than UV inks, there is less advantage in using many printheads
to apply large quantities of ink to the substrate because this causes the ink to pool and the
image to blur.
Furthermore, printheads that are for printing solvent-based inkjet inks are not provided with a
means for heating the ink because solvent-based inks have a low viscosity and do not
therefore require heating at the printhead to produce a jettable viscosity (in contrast with UV
curable inks). Thus, known solvent-based inks are jetted at ambient temperatures.
Solvent-based inkjet inks are susceptible to drying on the nozzle plate due to evaporation of
the solvent. Printers for solvent-based inkjet inks therefore typically include suction cups
which can be used to cap the printheads when not in use, allowing a solvent vapour saturated
environ ment to be established , which lim its evaporation . Shou ld a printhead become
blocked , the suction cup can be used to pull a small volume of ink throug h the blockage,
using a peristaltic pump, to recover performance after excess ink is removed using a wiper
blade.
The ink of the present invention comprises both a solvent and a radiation-curable component
and therefore dries by a combination of evaporation of the organic solvent and curing of the
radiation-curable component upon exposure to actinic radiation.
The ink of the present invention can surprising ly be used in printers that are suitable for
printing conventional solvent-based inkjet inks, provided that a source of actinic radiation is
also provided . Typically the printheads of inkjet printers for solvent-based inks are not
externally heated . The inks of the present invention can be jetted at ambient temperature,
preferably below 35°C, or below 30°C or about 25°C, and are therefore compatible with the
printheads and nozzles that are used to print solvent-based inkjet inks. The use of a printer
that is for printing conventional solvent-based inkjet inks, particularly printheads, nozzles and
ink delivery systems that are for use with conventional solvent-based inkjet inks, as the basis
of the printing apparatus of the invention means that printing apparatus of the invention has a
low capital cost.
A printer that is suitable for printing a conventional solvent-based inkjet ink may be adapted
before use in printing the inks of the present invention. Depending on the exact nature of the
ink and the location of the cure sou rce, opaque ink feed components that are chemically
compatible with the ink may be used and/or a UV screen filter film may be applied to the print
window on the front of the apparatus. These are minor adaptations that wou ld not have a
significant effect on printer cost or performance.
In one embodiment, the printing apparatus of the present invention comprises one or more
piezo drop on demand printheads. Preferably the printheads are capable of jetting ink in drop
sizes of 50 picolitres or less, more preferably 30 picolitres or less, particularly preferably 10
picolitres or less.
The printing apparatus of the present invention comprises means for evaporating solvent from
the ink at the appropriate time after the ink has been applied to the substrate. Any means
that is suitable for evaporating solvent from known solvent-based inkjet inks can be used in
the apparatus of the invention. Examples are well known to the person skilled in the art and
include dryers, heaters, air knives and combinations thereof.
In one embodiment, the solvent is removed by heating . Heat may be applied through the
substrate and/or from above the substrate, for example by the use of heated plates (resistive
heaters, inductive heaters) provided under the substrate or radiant heaters (heater bars, IR
lamps, solid state IR) provided above the substrate. In a preferred embodiment, the ink can
be jetted onto a preheated substrate that then moves over a heated platen. The apparatus of
the invention may comprise one or more heaters.
When printing the ink of the present invention, a significant portion of the solvent is preferably
allowed to evaporate before the ink is cured . Preferably substantially all of the solvent is
evaporated before the ink is finally cured . This is achieved by subjecting the printed ink to
conditions that would typically dry conventional solvent-based inkjet inks. In the case of the
ink of the present invention, such conditions will remove most of the solvent but it is expected
that trace amou nts of solvent will remain in the film given the presence of the radiationcurable
component in the ink.
The solvent evaporation step is thought to be important because it is believed to provide
further definition to the image quality. Thus, it is thought that the solvent evaporation step
results in a printed image with high gloss, as would be expected for conventional solventbased
inks. Furthermore, the loss of a significant portion of the ink through the evaporation of
the solvent leads to the formation of a printed film that is thinner than the film that would be
prod uced by jetti ng an equiva lent vol ume of known radiation-curable ink . T his is
advantageous because thinner films have improved flexibility.
Unlike standard solvent-based inks, once the solvent has evaporated, the ink is not expected
to be completely solid. Rather, what remains on the surface is a high viscosity version of a
radiation-curable ink. The viscosity is sufficiently high to inhibit or significantly hinder ink flow
and prevent image degradation in the timescale that is needed to post-cure the ink. Upon
exposure to a radiation source, the ink cures to form a relatively thin polymerised film . The
ink of the present invention typically produces a printed film having a thickness of 1 to 20 ,
preferably 1 to 10 , for example 2 to 5 . Film thicknesses can be measured using a
confocal laser scanning microscope.
The source of actinic radiation can be any source of actinic radiation that is suitable for curing
radiation-curable inks but is preferably a UV sou rce. Suitable UV sources include mercury
discharg e lam ps , f luorescent tubes , lig ht emitti ng d iod es (LEDs) , flas h lam ps and
combinations thereof. One or more mercury discharge lamps, fluorescent tubes, or flash
lam ps may be used as the rad iation source. When LEDs are used , these are preferably
provided as an array of multiple LEDs.
Preferably the source of actinic radiation is a source that does not generate ozone when in
use.
The source of actinic radiation for the initial pinning of the ink may be the same or different to
the source of actinic radiation for performing the final cure of the ink.
The source of UV radiation could be situated off-line in a dedicated conveyor UV curing unit,
such as the SUVD Svecia UV Dryer. Preferably, however, the source of radiation is situated
in-line, which means that the substrate does not have to be removed from the printing
apparatus between the heating and curing steps.
The radiation source can be mobile, which means that the source is capable of moving back
and forth across the print width, parallel with the movement of the printhead.
In one embodiment, one or more sources of actinic radiation are placed on a carriage that
allows the source of actinic radiation to traverse the print width. The carriage may be placed
up and downstream of the printer carriage in allow irradiation before and after evaporation of
the solvent. In this embodiment the source of actinic radiation moves independently of the
printer carriage and movement of the printhead does not therefore have to be slowed in order
to provide adequate time for solvent evaporation. Thus, overall productivity can be improved.
When the source of radiation is provided on separate carriage, it is necessary to provide an
add itional carriage rail , motor and control systems. This adaptation can lead to large
increases in equipment costs.
Preferably the sou rce of rad iation is static. This means that the sou rce does not move
backwards and forwards across the print width of the substrate when in use. Instead the
source of actinic radiation is fixed and the substrate moves relative to the source in the print
direction.
When the sou rce of actin ic rad iation is provided in the pri nt zone of the pri nter, lig ht
contamination at the printhead , which could lead to premature curing in the nozzle, must be
avoided. Adaptations to prevent lig ht contamination , such as lamp shutters, give rise to
additional costs. The source of radiation is therefore preferably located outside the print zone
of the printing apparatus. By print zone is meant the region of the printing apparatus in which
the printhead can move and therefore the region in which ink is applied to the substrate.
A preferred printing apparatus according to the present invention that com prises a static
source of radiation located outside the print zone is expected to be economically attractive
and therefore suitable for entry level wide format digital graphics use. This embodiment is
therefore particularly preferred . By entry level is meant the simplest and cheapest printers
that are suitable for wide format digital graphics use.
By locating the source of actinic radiation outside the print zone, and by avoiding the use of
mobile radiation sources, potentially expensive adaptations to the printing apparatus can be
avoided .
Static curing units preferably span the full print width, which is typically at least 1.6 m for the
smaller wide format graphics printers. Fluorescent tubes, mercury discharge lamps, and light
emitting diodes can be used as static curing units.
Any of the sources of actinic radiation discussed herein may be used for the initial pinning of
the inkjet ink. The dose of actinic rad iation is lower than the dose req uired to cure the
radiation-curable material fully, namely 1-200 mJ/cm2, preferably 1- 100 mJ/cm2, more
preferably 1-50 mJ/cm2 and most preferably about 35 mJ/cm2.
The wavelength of the pinning source is typically 200-700 nm, preferably 300-500 nm and
most preferably 350-450 nm.
It is preferable to arrest the flow of the ink by pinning the ink droplets quickly after they have
impacted on the substrate surface. To achieve a good quality image it is preferable that the
inks are pinned within 5 seconds of impact, preferably within 1 second and most preferably
within 0.5 seconds. As a resu lt of the pinn ing , the viscosity of the ink is increased by
polymerisation and/or crosslinking of the radiation-curable material thereby arresting the flow
of the ink and improving the final image quality.
Following evaporation of the solvent, the com position is exposed to add itional actinic
radiation. That is , an additional dose of radiation to that req uired for pinning . The dose
required to achieve the final cure will be higher than the pinning dose. The dose provided
results in the formation of a solid film. A suitable dose would be greater than 200 mJ/cm2,
more preferably at least 300 mJ/cm2 and most preferably at least 500 mJ/cm2. The upper
limit is less relevant and will be limited only by the commercial factor that more powerful
radiation sources increase cost. A typical upper limit would be 5 J/cm2. The delay between
evaporating the solvent and providing a final cure of the ink is less critical than the initial
pinning of the ink, but is typically at least 1 minute after jetting.
High and medium pressure mercury discharge lamps can be relatively expensive to operate.
The lamp units themselves can be heavy and expensive and often additional shielding is
required to prevent unintentional UV exposure to the operator. Extraction is also required to
remove ozone that is produced by the lamps. Furthermore, where high discharge currents are
involved for high output lamps, electronic ballast is required because the resistance of the gas
used in the lamp changes during use. High and medium pressure mercury discharge lamps
are not therefore preferred UV sources according to the present invention.
LED sources that are currently available are relatively expensive and a printing apparatus
comprising a LED source of UV radiation is unlikely to be suitable for use an entry level
printer. Thus, a source of actinic radiation comprising currently available LEDs is not
preferred. However, development of UV LED sources for curing inks is ongoing and it is
envisaged that the cost of LED sources will decrease significantly in the future. In this case, a
printing apparatus according to the present invention that includes a source of actinic
radiation comprising LEDs would be suitable for entry level printing systems.
In one embodiment of the invention, the source of radiation comprises a UV fluorescent lamp.
In another embodiment of the invention the source of radiation comprises one or more flash
lamps. Flash lamps operate by discharge breakdown of an inert gas, such as xenon or
krypton, between two tungsten electrodes. Unlike mercury discharge lamps, flash lamps do
not need to operate at high temperature. Flash lamps also have the advantage of switching
on instantaneously, with no thermal stabilisation time. The envelope material can also be
doped, to prevent the transmission of wavelengths that would generate harmful ozone. Flash
lamps are therefore economical to operate and therefore suitable for use in entry level
printers.
Flas h lam ps can be operated in a number of mod es , includ ing cold pulse mod e and
modulation mode. Cold pulse mode is when the lamp output is switched on for a very brief
period from fully off every time a flash of UV radiation is required . Normally, the intermittent
natu re of cold pulsing a flash lamp would exclude its applicability to conventional curing
applications, where it is usual to require a constant lamp output. However, when a flash lamp
is used to cure the inkjet ink of the present invention downstream from the print zone, the
intermittent nature of the cure source does not have a detrimental affect. For example, while
the average production speed of a printer for solvent-based inkjet inks is typically 0.5 m/min,
the motion of the substrate through the printer actually occurs in steps of 3-6 mm, at the end
of each printhead carriage pass. This means that the substrate is static for between 1-3
seconds at a time, which is more than sufficient time for the lamp to flash at hig h power
several times over the same image region in order to cure the ink. Provided that the lamp is
triggered in synchronicity with the substrate advancement steps, the pulsed nature of the
lamp output is capable of providing sufficient dose and peak irradiance to cure the ink, while
not leading to thermal damage of the substrate.
When operating in this mode flash lamps do not emit constant radiation when in use and are
therefore "off" for a significant proportion of the time in which the lamp is over the substrate,
which reduces the risk of thermally damaging temperature-sensitive substrates.
The circuit elements required to create the voltage pulse to drive the flash lamp are relatively
cheap, consisting of an AC-DC converter, high voltage capacitor and inductor. The simplicity
and considerably lower average power consumption than the mercury discharge lamp make
the capital and running costs for this lam p economical for use in the entry level hybrid
solvent/UV printer.
The flash lamp is preferably operated in modulation mode, however. In modulation mode
large instantaneous UV power output is achieved during pulses, but the lamp lifetime is
extended because repeat triggering of the gas discharge is not required. Modulation also has
the benefit that, between pulses, there is relatively low current flowing in the lamp which
enhances the infra red (IR) output of the lamp. Since the absolute power between pulses is
low, the lamp will act as a low power IR heater that assists with solvent removal from the
printed ink.
Flash lamps typically require cooling during use and the maximum average power output of
the flash lamp depends on the cooling method used. For higher power outputs, more
sophisticated cooling methods are required. If convective air cooling is used the maximum
average power output is around 0-1 5 W/cm2, if forced air cooling is used the maximum
average power output is around 15-30 W/cm2 and if water cooling is used the maximum
average power output is around 30-60 W/cm2. While it is preferable to maximise the lamp's
power output in order to achieve rapid ink curing , when providing an economical source of UV
radiation this requirement has to be balanced with the cost of providing an appropriate cooling
means. The provision of a recirculating water cooler adds significantly to the cost and is
therefore unlikely to be suitable for use in entry level printers. The maximum average power
output of the flash lamp is therefore preferably about 30 W/cm2 and the lamp is preferably
cooled using a forced air cooling system.
The UV output of the flash lamp can be enhanced compared to the IR output by providing a
high current density. This can be achieved by increasing the power output of the lamp. The
power output of the lamp is proportional to the lamp's internal diameter and enhancement of
the UV output compared to the IR output can therefore be achieved by using a large internal
diameter lamp with a large power supply. For example, a lamp internal diameter of around
10 mm would be capable of producing 94 W/cm , compared to 38 W/cm for a 4 mm internal
diameter lamp
Using a single 1.6 m long flash lamp with an internal diameter of 10 mm would req uire a
power supply capable of providing over 15 kW. Despite the simplicity of construction, a power
supply of this mag nitude cou ld still be expensive and may need a three phase power
connection. The source of radiation is therefore preferably formed from a series of shorter
lamps that extend along the print width with a smaller power supply that switches between
them. The passage of the printed substrate through printing apparatus is preferably relatively
slow and the lamps can therefore be rapidly pulsed in sequence across the full print width
befo re t he s ubst rate adva nces . Since t he imag e q ua lity prov id ed by a hyb r id
solvent/radiation-curable inkjet ink is thought to be defined by solvent removal stage, the
slightly different exposure times experienced by the print across its width are not expected to
have an impact on image quality.
Medium pressure mercury lamps are used widely in the printing industry to achieve UV cure
of inks designed for a range of applications. Medium pressure mercury lamps are relatively
inefficient with typically only 15% of the energy input converted to the desired UV radiation;
the remainder of the input energy is converted to infrared radiation / heat and visible light. The
high heat output of medium pressure mercury lamps can lead to problems with degradation or
distortion of heat sensitive substrates used for some printing applications. One solution is to
use dichroic reflectors that channel heat away from the substrate, focussing only the UV
radiation onto the material. These however limit the efficacy of the lamp and add considerably
to the cost.
Low pressure mercury lamps are much more efficient than medium pressure mercury lamps.
Approximately 35% of the energy input is converted to UV radiation , 85% of which has a
wavelength of 254 nm (UVC). These lamps therefore generate less heat in use than medium
pressure mercury lamps, which means that they are more economical to run and less likely to
damag e sens itive substrates . Furthermo re , low press ure mercury lam ps ca n be
manufactured in such a way as not to generate ozone in use and are therefore safer to use
than medium pressure mercury lamps.
Although low pressure mercury lamps are used extensively in the water purification industry,
they have not yet found widespread application in the printing industry. Typical medium
pressure mercu ry lamps have an output in the range of 80 to 240 W/cm . In contrast, the
maximum output for low pressure mercury lamps is around 30 to 440 mW/cm, which means
that the peak irradiance of low pressure mercury lamps is also low. The low power output
and low peak irradiance of these lamps suggests that they would not provide effective curing
of radiation-curable inkjet inks.
A single low pressure mercury lamp or two or more low pressure mercury lamps can be used.
The lUPAC Compendium of Chemical Terminology (PAC, 2007, 79, 293 "Glossary of terms
us e d i n p ho t o c h emis t ry " , 3 rd e d i t io n ( l UPA C Re co mme nd a t io ns 2 0 0 6 ) ,
doi: 10 .1351/pac200779030293) describes a low pressure mercury lamp as a : "resonance
lamp that contains mercury vapour at pressures of about 0 .1 Pa (0.75 * 10 Torr; 1 Torr =
133.3 Pa). At 25°C, such a lamp emits mainly at 253.7 and 184.9 nm. They are also called
germicidal lamps. There are cold- and hot-cathode as well as cooled electrodeless (excited by
microwaves) low-pressure mercury lamps. The Wood lamp is a low-pressure mercury arc with
an added fluorescent layer that emits in the UV-A spectral region (31 5-400 nm)."
Low pressure mercury lamps predominantly emit UV rad iation with a peak wavelength of
around 254 nm but the wavelength of the radiation can be varied by coating the internal
surface of the lamp with a phosphor. In a preferred embodiment of the lamp, there is no such
phosphor coating. In the method of the present invention the lamp preferably emits radiation
with a peak wavelength of around 254 nm, or put another way, the natural or unaltered
wavelength of radiation emitted by mercury vapour in a low pressure lamp environment.
The use of a phosphor coating can lead to a reduction in lamp luminous efficiency. The
preferred phosphor-free lamps used according to the invention have an efficiency exceeding
45% for UVC generation , however. This high efficiency helps to minimise the cure unit
running costs.
In low pressure mercury lamps the UV output varies with temperature. When the lamp is first
switched on the liquid mercury starts to vaporise and as the temperature increases, the
vapour pressure of the mercury reaches an optimum level and the output of UVC radiation
reaches a maximum. As the temperature of the lamp increases further the vapour pressure
continues to rise, red ucing the UVC output. Low pressu re mercury lam ps are therefore
operated at an optimum temperature at which maximum UVC output can be achieved and
this temperature is typically around 25-40°C for standard low pressure lamps. This limit on
the operating temperature limits the energy input, however, because the lamp temperature
can be raised above the optimum temperature if the energy input is too hig h . Limiting the
energy input limits the maximum UV output achievable. The maximum UV output achievable
from a low pressure mercury lamp is therefore limited by the operating temperature and the
energy input. Standard low pressure mercury lamps have linear power densities of less than
380 mW/cm in their normal configuration. However, U shaped lamps can have effective total
power densities of up to twice this, for example 650 mW/cm.
Although the UVC output of standard low pressure mercury lamps is sufficient to cure the inks
of the current invention within an acceptable time frame, the UVC cure dose is preferably
delivered over a shorter time period, allowing faster cure speeds.
The low pressure mercury lamp may be an amalgam lamp. In amalgam lamps an amalgam
of mercury, typically with bismuth and/or indium, is used instead of liquid mercury. Other
suitable materials that are compatible with, or are capable of forming an amalgam with
mercury could be used instead of bismuth or indium, however. Amalgam lamps have the
same spectral output as conventional low pressu re mercu ry lamps. In operation , the
amalgam gradually releases mercury vapour as the temperature increases, but vapour is
reabsorbed if the pressure becomes too high. This self-regulation means that the optimum
mercury vapour pressure is achieved at a higher temperature, approximately 80-1 60°C, for
example 83°C, depending on the type of lamp and manufacturer. Amalgam lamps therefore
operate at a higher optimum temperature than standard low pressure mercury lamps, which
means that hig her energy inputs can be tolerated . A hig her energy input leads to an
accompanying increase in UVC output, which remains stable during extended operation of
the lamp.
Typically, amalgam lamps can run at temperatures up to 140°C with linear power densities
exceeding 380 mW/cm and such lamps can achieve outputs that equate to approximately five
times the output of a conventional low pressu re mercu ry lamp. The combination of the
increased radiation and heat generated by the amalgam lamp offers a useful advantage in
drying and curing the inks used in the present invention when com pared to reg ular low
pressure mercury lamps.
In an embodiment of the invention the cure lamp linear power density is below 2,000 mW/cm,
preferably 200 mW/cm to 1500 mW/cm , more preferably 380 mW/cm to 1,500 mW/cm. In a
more preferred embodiment the linear power density is 380 mW/cm to 1,200 mW/cm and in a
most preferred embodiments either 380 to 1,000 mW/cm or 500 to 1,000 mW/cm.
Standard low pressure mercury lamps have current densities not exceeding 0.45 Amps/cm
whereas amalgam lamps have current densities above this level.
The temperature of the amalgam lamp may be controlled in order to allow the optimal UV light
output to be maintained . Temperature control can be achieved by immersing the lamp in
water within a quartz sleeve. As well as providing electrical insulation against the water, the
air gap around the lamp prevents overcooling by the water. By controlling the water flow past
the lamps, the optimal lamp temperature can be maintained for maximum UV output. While
convenient, this method is not preferred as it incurs the additional cost of a chiller.
In a preferred embodiment air is blown across the low pressure mercury lamp(s) to control the
lamp temperature. In a further preferred embodiment, forced air that has been warmed by the
lamp(s) is directed over the surface of the printed image to aid removal of the solvent prior to
curing . For example, one or more fans can be positioned at the rear of the lamp reflector in
order to extract and transport excess warm air upstream in the print process to assist in
drying and pinning the printed image, thus increasing efficiency of the printer.
The low pressure mercury lamp is preferably used together with auxiliary ballast electronics in
order to regulate the current through the lamp. Many types of ballast are available. Preferred
for use in this invention are electron ic ballasts that convert input mains freq uency to
frequencies greater than the relaxation time of the ionised plasma in the lam p, thereby
maintaining optimal light output.
In a more preferred embodiment, an electronic ballast operating in rapid or instant start mode
is provided wherein electrodes of the low pressure mercury lamp may be pre-warmed before
ig nition in order to reduce electrode damage caused by frequent switching . Though more
expensive to implement than cold-start methods, pre-heating is preferred because the
preferred amalgam lamp of the present invention is high power, operates at high temperature
and in use is likely to be frequently switched.
Low pressure mercury lamps emit light in all directions. For efficient UV curing of printed
images, the lamp is therefore preferably used in conjunction with at least one reflector to
ensure that the majority of emitted UV light is efficiently directed to the printed surface. The
reflector is preferably made of a material that efficiently reflects the UV light with minimal loss,
for example aluminium , which has a reflective efficiency of greater than 80%. To prevent
hazi ng of the mirror f inish dur ing long term UV expos ure, pre-anod ised alu minium is
preferred, such as 320G available from Alanod . This material is easily formed into curved or
faceted shapes by rolling or bending to provide efficient reflectors.
In one embodiment the reflector preferably has an elliptical shape such that the radiation
directed at the printed substrate is focussed to a narrow line, thereby increasing the peak
irradiance at the printed substrate. "Elliptical reflector" is a term known in the art and refers to
a reflector having a general shape as shown in Figure 4 .
The finite diameter of the low pressure mercury lamp prevents all of the emitted light from
originating at the focus of the ellipse. In a preferred embodiment low pressure mercury lamps
with diameter below 30 mm, preferably below 20 mm and more preferably below 10 mm are
therefore used in combination with an elliptical reflector, in order to increase the peak
irradiance at the substrate even further.
In one embodiment, the bulb of the low pressure mercury lamp is partially coated with a
reflective coating such that the radiation produced by the bulb is directed towards the print
surface. The reflective material can be any material that reflects UVC radiation, and the
coating can be can be applied by painting or vacuum deposition, for example.
The total UV dose received by the ink printed on the substrate is inversely proportional to the
speed that the substrate moves past the lamp. Although the low pressure mercury lamps
used according to the preferred embod iment of the present invention have a relatively low
power output when compared to medium pressure mercury lamps, the use of a static lamp
allows the printed ink to be exposed to the radiation from the lamp for longer periods than are
achieved with traditional scanning type large format printers. Hence, the total dose provided
by the low pressure lamps can exceed that provided by scanning type cure units using higher
output lamps.
The envelope of a low pressure mercury lamp is typically made from fused quartz, which
allows production of lamps with lengths exceeding one meter. To ensure even curing across
the full print width using a static in-line cure unit, it is preferable to provide a lamp with an arc
length exceeding the print width by several centimetres to counter the emission variance near
the electrodes. Together with the electrode encapsulation, the final lamp length could
approach 3 m in some cases. This length of lamp is achievable for envelopes with a wide
diameter. However, narrower lamps would be more fragile and require additional support
along their length, which could interfere with the irradiance profile. In this case, it may be
preferable to use several smaller lamps in a castellated or staggered arrangement to achieve
full width curing.
The invention will now be described with reference to the following examples, which are not
intended to be limiting.
Examples
Example 1
Inkjet inks were prepared according to the formu lations set out in Table 1. The inkjet ink
formulations were prepared by mixing the components in the given amounts. Amounts are
given as weight percentages based on the total weight of the ink.
Table 1.
Gamma butyrolactone and diethylene glycol diethyl ether are organic solvents . Nippon
Gohsei 7630B is a hexafunctional urethane acrylate oligomer with a viscosity of 6.9 Pa.s at
60°C.
The cyan pigment dispersion is com posed of Disperbyk 168 (20.0 wt%) as a dispersing
agent, Rapicure DVE3 (50.0 wt%) which is triethylene glycol divinyl ether and Irgalite blue
GLVO (30.0 wt%) which is the pigment. The magenta, yellow and black pigment dispersions
are analogous although the pigments are clearly different colours.
Irgacure 8 19 and Irgacure 2959 are free-radical photoinitiators. UV 12 is a stabiliser and BYK
331 is a polyether modified polydimethylsiloxane and reduces surface tension.
Example 2
A 220 micron gloss PVC and a coated clear gloss polyester film were selected as test
substrates since both of these materials had been found to be non-receptive to solvents in the
above inkjet ink compositions and thus had slow pinning responses.
Then, 12 micron (wet) films of the inks from Example 1 were cast onto the test substrates
using a No. 2 K-bar applicator. The wet films were exposed to a 395 nm UV LED source
suspended over a conveyor running at a speed of 20 m/min at a distance of 3 mm. The 395
nm LED was supplied by Nordson and had a nominal power of 10W (at the array surface).
After exposu re the prints were assessed for signs of physical changes typically associated
with a curing process, principally the surface skinning viscosity increase. The changes are
assessed by dragging a spatula through the ink film and recording any changes to the nature
of the film and thereby determining whether or not partial cure has been achieved. The power
of the LED was reduced in stages until no change to the film was evident after exposure. The
results are set out in Tables 2-5.
Table 2 . Cyan ink (ink 1)
Table 3 . Magenta ink (ink 2)
Table 5 . Black ink (ink 4)
These results show that partial film cure is still evident in the cast films even at low LED
power. The cyan and magenta inks showed evidence of physical changes after exposure
even at 2.5% of the full LED power. The yellow and black inks, whilst less reactive, still,
showed evidence of physical changes after exposu re to the LED running at 1/ 10th of full
power.
The intensity and dose of UV light was measured at a range of LED power settings using a
Power puck 2 supplied by EIT. A summary of the findings is set out in Tables 6 and 7 .
Table 6 .
Table 7 . The wavelengths of the UV radiation.
Designation Minimum Maximum
wavelength (nm) wavelength
(nm)
UVA2 375 4 15
UVB 280 320
UVC 250 260
UVV 395 445
These data show that the inks respond to very low doses of UV light at 395 nm without the
need for solvent removal, still showing evidence of physical change at low dose and light
intensity. When running at full power the LED used req uires water cooling which adds
considerably to the complexity and cost of printer. A low power LED system will not require
this expensive cooling and that the physical changes prod uced by the low UV doses are
sufficient to pin the ink droplets of the ink on the substrate surface preventing bleed and
excessive dot spread on non receptive substrates.
Example 3
Ink 1 as set out in Table 1 hereinabove was used to evaluate the effect on image quality when
the ink was exposed to various levels of UV light from a 395 nm UV LED prior to removal of
the solvent.
This exam ple used : a test pri nter rig fitted with a Xaar 1001 printhead and ink supply
(theoretical drop range, 42 to 6 nanograms in 6 nanogram units); a Phoseon 395 nm 4W UV
LED source; a XY translation table; a monochrome digital camera fitted with an extension
tube; and a power puck 2 supplied by EIT (see Table 7 for the output from the channels).
The ink was printed onto a 220 micron Genotherm (gloss rigid PVC) substrate supplied by
Klockner-Pentaplast GmbH (a non-receptive material ) . Seven rows of droplets were
deposited, two of each size, prod ucing 14 rows of drops with the theoretical drop size
decreasing from left to right. The ink was jetted in the array of drops described hereinabove
to form a 180 x 180 dpi test pattern on to the substrate. After deposition of this first array of
drops the test print was exposed to a range of UV doses from the LED source. The data from
the UVA2 channel were used as this is the closest match to the 395 nm output of the
Phoseon 395 nm LED.
The UV exposure was as follows.
LED distance from substrate surface: 10 mm
Effective LED linear speed over image: 200 mm/s
LED array distance from head: 10 cm
Drop residence time on substrate before pinning: 0.5 seconds
The results are set out in Table 8 .
Table 8 .
UV dose (mJ/cm2) Intensity (mW/cm2) Image number (see Figs. 4-
10)
226.8 1577.25
17 1.73 12 19.3 2
109.75 779 3
54.45 385.3 4 (and 7)
29.57 203.68 5 (and 8)
0 0 6 (and 9)
After the deposition and pinning of the first array of droplets a second array was deposited
that was offset by half a nozzle pitch (70 microns) in the Y direction. This effectively produced
a final array of drops 180 x 360 dpi where drops were deposited between the previously
pinned drops.
It is possible to assess the effectiveness of the UV pinning process by visual inspection of the
images captured , the first areas of the array to show droplet spreading and merging as the
UV pinning does is reduced are the pair of rows employing the largest drop mass.
Looking more closely at these areas, images 8 and 9 , which correspond to the top left hand
sections of images 5 and 6 , respectively, it is clear that the exposure to a pinning dose of
29.57 mJ/cm2 has reduced the merging of adjacent droplets and would hence produce a
higher-quality printed image with reduced ink pooling and inter-colour bleed.
Image 7 similarly shows the effect of increasing the pinning dose where the flow of the
droplets has been further restricted, but care is needed to avoid over pinning the droplets as
this can lead to an a deterioration of the image quality, for example in solid colour areas of a
print, where a degree of drop spread is required to give full coverage of the ink on the
substrate.
Image 1 corresponds to the full power setting of the LED. This dose results in an over pinning
the image which traps solvent in the film before the thermal drying stage leading to bloom or a
hazy appearance. A further problem with image quality also results because an insufficient
degree of drop spread may prevent full coverage of the substrate leading to the substrate
showing behind the image.
Claims
1. A method of inkjet printing comprising the following steps, in order:
(i) providing a hybrid inkjet ink comprising an organic solvent, a radiation-curable material, a
photoinitiator and optionally a colorant;
(ii) printing the ink on to a substrate;
(iii) pinning the ink by exposing the ink to actinic radiation at a dose of 1-200 mJ/cm2;
(iv) evaporating at least a portion of the solvent from the ink; and
(v) exposing the ink to additional actinic radiation to cure the ink.
2 . A method as claimed in claim 1, wherein ink comprises at least 30% by weig ht of
organic solvent based on the total weight of the ink.
3 . A method as claimed in claim 1 or 2 , wherein the ink comprises less than 5% by weight
of water based on the total weight of the ink.
4 . A method as claimed in any preceding claim , wherein the radiation-curable material is
present in an amount of 2 to 65% by weight based on the total weight of the ink.
5 . A method as claimed in any preceding claim , wherein the radiation-curable material
comprises a radiation-curable oligomer.
6 . A method as claimed in any preceding claim, wherein the ink contains less than 20% by
weight of radiation-curable material having a molecular weight of less than 450, based on the
total weight of the ink.
7 . A method as claimed in any preceding claim, wherein the photoinitiator is a radical
photoinitiator.
8 . A method as claimed in any preceding claim , wherein the inkjet ink is a component of
an inkjet ink set.
9 . A method as claimed in any preceding claim , wherein the inkjet ink is printed using a
piezo drop-on-demand printhead.
10 . A method as claimed in any preceding claim, wherein the source of actinic radiation is a
UV source selected from a mercury discharge lamp, an LED, a flash lamp, a UV fluorescent
lamps and combinations thereof.
11. A method as claimed in any preceding claim , wherein the ink is jetted at less than 35°C.
12 . A method as claimed in any preceding claim, wherein, in step (iii), the dose is 1- 100
mJ/cm2.
13 . A method as claimed in any preced ing claim , wherein step (iii) is initiated within 5
seconds of impact of the ink onto the substrate.
14 . A method as claimed in any preceding claim , wherein the solvent is evaporated by
heating the printed ink.
15 . A method as claimed in any preceding claim, wherein the printing is performed on a rollto-
roll printer or flat-bed printer.