4
I D T A th b a b w p a th s I im a fr d in p f e m ( p c m in h a f u A in f s ta fu c s r p I in k Influenc Dynami Tri Tuladhar, Jo Abstract This paper he timescale rel between good an Ink fluid mapaccount of the p bulk and key dyn whereby the “ink printhead geome and temperature hat meets both b satellite formatio ntroduction Recent adva mposed stricte applications wit requency, (iii) directionality an ncreased mistin permanent line d luctuation, etc) effect can be m mechanism (wav DoD) devices properties) withi cases and for modification of d Ink’s conv nsufficient guid high frequency actuation, high s light. Small va upstream flow dy A fundamental u ndividual compo low behaviour substrate during ailor specialized uture printheads It is import components (i) substrate and pr educed satellite/ print reliability. nk formulat One of the nks that are con key parameters ce of Pri ic Prope hn Tatum and P investigates key levant to the ink nd bad inks whi is created fo printhead geom namic properties k fluid map” is u etry and print co e) for a given i bulk and dynam on and improved n ances in inkjet te er requirements th (i) increased controlled d nd (v) be able ng/satellites and drop out, floodin work against ac mitigated to som veform and driv and fluid m n the window o novel applic drive electronics ventional phys de to ink perform pressure fluct shear at the noz ariations in ink ynamics and jet understanding of onents, as well a in-channel, thro printing is vita d inkjet fluids fo s. tant to look at th printhead, (ii) rocess condition /mist formation tion and jet key challenges nsistent. Ink for within specifica inthead erties on Paul Drury; Xaar y dynamic prope kjet printing, tha ich otherwise lo or specific prin metry, jetting con s. This paper pr utilised to (i) iden onditions (veloci ink; (ii) formula mic properties fo d reliability. echnology and in s on both ex d drop velocity drop size, and to jet exotic d reliability issu ng, drop directio chieving these r me extent by op ve amplitude) in modifications ( of printhead oper ations, printhe may be required sical properties mance. The flu tuations in the zzle wall and l dynamic prope break-up mecha ink chemistry a as the ink as-a-w ough the nozzle al. This under or new applicatio he combined in drive profile, n to achieve ta , high print spe tting behavi in ink formula rmulations are m ations, yet it is Geomet n the Jet r plc, Cambridg erties of the ink, at can differenti ooked identical. nthead which ta nditions and in resents case stud ntify optim ity, print frequen ate/recommend or reduced misti nk chemistry, ha xisting and n y, (ii) high pr d (iv) improv fluids. Howev ues (temporary onality and veloc requirements. T ptimising the dr n drop on dema (composition a ration. In extre ad redesign a d. s alone are uid is subjected e channel duri arge extension erties influence anism downstrea and the influence whole, on dynam , in-flight and o standing will h ons in existing a fluence of all fo (iii) ink and ( argeted drop si eed, frequency a iour ation is to devel maintained to ke often noticed t try, Prin tting Beh ge, UK at iate An ake nk’s dies um ncy ink ng, ave new rint ved ver, or city The rive and and me and an d to ing in- the am. e of mic on- help and our (iv) ize, and lop eep that there ar batches Th of the in carrier f behavio and/or concentr Dispersa resins a contribu gloss, r variation the fluid could re formula Figure1. identical i Cyan Figure2. UV ink se Fig characte the ink same je m/s dr nt Cond haviour re marked differ or between colo ough ink carrier nk are mainly N fluid produces c our. This is due physical inter ration of the pig ants are added t are often present ute to the prope resistance to he ns in any of the d and also it’s el esult in marked ators will find it v Batch 1 High speed in-fl inks. Images obtai n Mag Differences in the ets: Top row (In-flig gures 1 and 2 eristic varied be was jetted using etting condition op velocity. A ditions a rences in the je ours of apparentl r components (s Newtonian, intro onsiderable dev to particle asso raction) during gment particles a o stabilise the p t to bind other rties of the ink eat, chemicals ese additives can asticity due to th d differences in very difficult to light jetting photog ined from Xaar 100 genta Y e jetting behavior be ght) and bottom row show such ex etween batches a g the same print (drive profile an As a conseque and Fluid etting performan ly identical inks. solvent, oil, varn oduction of pigm viations from the ociation (by chem flow. The affect ink’s bulk igments. Additi components of once on the su and water). n influence the heir polymeric n the jetting beh adjust these pro Batch 2 graphs between tw 01 PH using Spark Yellow B etween colours of w (on-paper) Image xamples where and colours. In thead (Xaar 100 nd drive volt) t ence extensive d nce between . nish, water) ments to the e Newtonian mical bonds size and k properties. ives such as the ink and bstrate (e.g. Any subtle viscosity of nature which havior. Ink perties. wo batches of Flash Rig Black a commercial es. the jetting both cases, 01) with the o achieve 6 and time 70 ©2011 Society for Imaging Science and Technology

Influence of Printhead Geometry, Print Conditions, …...change fluid physical properties (such as density, surface tension, viscoelasticity, speed of sound) beyond the existing printhead

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Page 1: Influence of Printhead Geometry, Print Conditions, …...change fluid physical properties (such as density, surface tension, viscoelasticity, speed of sound) beyond the existing printhead

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InfluencDynamiTri Tuladhar, Jo

Abstract This paper

he timescale relbetween good an“Ink fluid map”account of the pbulk and key dynwhereby the “inkprinthead geomeand temperaturehat meets both b

satellite formatio

ntroductionRecent adva

mposed stricteapplications witfrequency, (iii)directionality anncreased mistin

permanent line dfluctuation, etc) effect can be mmechanism (wavDoD) devices

properties) withicases and for modification of d

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high frequency actuation, high sflight. Small vaupstream flow dyA fundamental undividual compo

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and time

70 ©2011 Society for Imaging Science and Technology

Page 2: Influence of Printhead Geometry, Print Conditions, …...change fluid physical properties (such as density, surface tension, viscoelasticity, speed of sound) beyond the existing printhead

consuming ink reformulation and validation (optimization and/or separate waveform development) are carried out for each batch or between colours to achieve satisfactory jetting. This issue is further complicated when developing inks for niche applications which could contain special (i) pigments/particles with high loading concentration and density, (ii) polymers/binders of high molecular weight, (iii) carrier fluid with different physical and chemical properties. Any variations in the composition could change fluid physical properties (such as density, surface tension, viscoelasticity, speed of sound) beyond the existing printhead operating windows.

Bulk and dynamic properties In any inkjet system, the ink goes through various physical

and geometrical constraints which influence the flow dynamics and finally the jetting characteristics. Most print heads have a narrow operating range in terms drop of velocity, print frequency and fluid properties.

Inkjet ink is carefully formulated to achieve ink stability and bulk properties that meet jetting, substrate and process/environment requirements while also ensuring it is chemically compatible with printhead material.

Bulk properties such as surface tension and viscosity play a key role in the jetting of the inkjet ink. Their roles are varied depending whether they are in the upstream or downstream. As the jet emerges from the nozzle, the viscosity and elastic stresses resist the necking motion of the liquid filament, whereas surface tension and inertia influence the resulting shape and form of the emerging drop. The optimum values of the surface tension and viscoelasticity becomes a compromise of what is required upstream (in the channel) and downstream (in-flight). Ink’s combined bulk properties have to be matched to operate efficiently at jetting temperature.

Controlling droplet formation and in particular, the break up and corresponding tail or ligament is highly dependent on the combined influence of these bulk properties and the rheology of ink as it flows through the nozzle.

In the case of DoD, apart from physical properties of the ink, the dynamic properties (viscoelasticity, intermittent pigment stability, dynamic surface tension) also play an important role in the ejection of the ink and subsequent drop formation as the ink is a cocktail of many components and is subjected to different flow regimes during jetting.

For piezo-electric inkjet devices, high frequency voltage pulses (waveform) are applied to a piezo-electric element. This causes an ink-filled channel to deform, thereby creating a fluctuating pressure profile. Through fluid acoustics two or more consecutive waves are super-positioned which guide the pressure pulses towards the nozzle [1]. The required super-position is achieved via adjustments to the electrical signals driving the piezoelectric actuator i.e. waveform frequency, voltage amplitude and pulse duration [1]. As a result, a strong acceleration of fluid occurs inside the nozzle which overcomes the viscous dissipation and the energy associated with forming a new surface so that fluid is jetted at high speed. The propagation and reflection of acoustic pressure waves are function of fluid properties, printhead design and constituent materials. The amplitude of the applied voltage

pulse modifies the fluid acceleration in the channel and hence velocity of the jet ejected from the printhead.

Ink fluid map The inkjet printhead operates in microsecond timescale and

small differences in printhead geometry, print conditions and dynamic fluid properties in microsecond timescale also influence the jetting characteristics. It is therefore very important to characterise ink properties in the timescale relevant to the jetting conditions.

Unlike bulk properties, it is not easy to quantify the dynamic properties of the inkjet ink at the print conditions (very high frequencies, shear rates and velocity) using conventional measuring tools. Recently some prototypes have been developed [2-5], which have a capability to measure some of the dynamic parameters at conditions similar to those encountered during jetting. The quantitative measurements from this have given deeper insight into the link between the fluid dynamic properties and jetting characteristics. [2-6] have used such tools to look at the influence of ink dynamic properties on the on the jetting behavior.

Over the last few years, fundamental background studies have been carried out to establish a link between fluid bulk and dynamic properties and jetting. Key dynamic properties have been identified at the timescale relevant to the inkjet printing to identify key features within good and bad inks which otherwise looked identical. These features can be utilised to distinguish subtle differences between batches or colour, thus generating “ink physical fingerprint”. One of the many feature incorporated in ink physical finger print is elasticity as reported earlier [3-6]. The optimum elasticity value is printhead and jetting condition specific. High elasticity influences jetting velocity and could forms a thin ligature which breaks up at multiple points resulting in many satellites (or mist). In extreme cases, the jet does not detach from the nozzle and is either pulled back into the nozzle or floods the nozzle. Low or no elasticity results in satellite formation at high jetting speed. The presence of some optimum elasticity is required whereby the liquid filament connecting the main drop is instantly pulled into the main droplet after breaking from the nozzle giving a satellite free drop.

Xaar exploits complex rheological techniques to analyse ink and generate a fluid map to determine the suitability of the ink. The fluid map also takes into account the combined influence of bulk properties, jetting conditions (print frequency, drop speed and size) and ink physical finger print. The fluid map is tailored to specific printhead and gives us a good indication of the degree of misting, satellite and reliability.

Figure 3 shows examples of the Xaar fluid map. The Xaar’s fluid map uses 5 criteria (labelled as A-E) to establish the ink’s suitability for the given jetting condition and predict its jetting characteristic. For commercial reason, the detailed of the Xaar criteria are not disclosed in this paper. These 5 criteria include printhead geometry, jetting conditions, bulk static properties and dynamic properties of the fluid at conditions similar to that experienced in the printhead. Each criterion can be associated with misting, satellite and reliability. Some criteria represent more than one failures mode depending on where it is on the scale. Ideally, an ink should satisfy all the criteria and fall within the preferred recommended zone (“80-100”) to give optimum jetting

NIP 27 and Digital Fabrication 2011 Technical Program and Proceedings 71

Page 3: Influence of Printhead Geometry, Print Conditions, …...change fluid physical properties (such as density, surface tension, viscoelasticity, speed of sound) beyond the existing printhead

characteristics. The severity of failure depends on (i) number of failed criteria and (ii) how far-off (below or above) the recommended range. We have encountered very few commercial inks that meet all the criteria.

Case studies The “ink fluid map” is a powerful tool to differentiate

between inks and can be used to prescreen inks, recommend jetting conditions and aid ink reformulation.

I. Differentiate between inks Figure 1a shows the fluid map comparisons between colours

(Brown, yellow and pink) of a commercial ceramic inks. Though all three inks had similar bulk properties and speed of sound, the fluid map indicates that the jetting behaviour will be marked different. The pink meets criteria A-C and close to the recommended range for criterion D where as brown colour met only one criterion. This would indicate that pink is a better ink and should give better jetting characteristic than brown it met only one criteria. Jetting tests showed pink to be most reliable and gave fewer satellites and misting in agreement with the fluid map.

II. Influence of temperature Jetting characteristic of the ink is sensitive to temperature due

to changes in the bulk properties. The effect is noticeable for 10-20°C variation in temperatures. In some cases, the ink shows drastic jetting behaviour changes for small differences (±1-5°C). This drastic behaviour can not be linked to bulk properties alone. In such fluid, we found some of the dynamic properties change significantly over few degrees centigrade. Figure 3b shows an example of such ink whose criteria D and E deteriorated when the temperature dropped from 45 to 40°C. Jetting observations also showed that this ink performance improved significantly when jetted at 45°C as opposed to 40°C. It is for this reason, the ink usually come with recommended jetting temperature and have to be strictly adhered to such sensitive inks. If possible, it is usually recommended to avoid such sensitive inks.

III. Print conditions Jetting conditions play an important role. It influences many

of the fluid map criteria and thus the jetting characteristic. Figure 3c shows an example of the ink whose fluid map criteria varied as a function of final drop velocity. In this instance, the ink should give the best results at 4-5 m/s.

IV. Printhead type Physical geometry, size and shapes of printhead channels,

nozzles and the drive profile are different for each printhead type. It is for this reason, inks are usually tailored to operate for specific printhead which has narrow operating windows and can handle ink of set properties. Figure 4d shows a suitability of a commercial ink in four Xaar printhead. The fluid map incorporates printhead geometry to determine the suitability of the ink. Based on the fluid map, this particular ink is ideally suitable for Proton 35 (P35) and to some extent in 1001. It is very likely that this ink will perform badly in Proton 60 (P60) and Electron heads.

(a)

(b)

(c)

(d) Figure 3. Xaar fluid map showing differences between (a) colours; (b) temperature; (c) jetting conditions and (d) printhead type.

V. Ink reformulation The detailed understanding of the inks dynamic properties,

printhead operating windows and drive profile can be exploited to expand the ink envelope that gives good jetting characteristic (lower satellite/misting and good reliability) and also show insensitivity to temperature fluctuation and drive profile.

72 ©2011 Society for Imaging Science and Technology

Page 4: Influence of Printhead Geometry, Print Conditions, …...change fluid physical properties (such as density, surface tension, viscoelasticity, speed of sound) beyond the existing printhead

(a) (b) In-flight high speed jetting photographs Ink A (original) Ink B (reformulated 1) Ink C (reformulated 2)

Std

wav

efor

m

Tune

d w

avef

orm

(c) on-substrate image Ink A (original) Ink C (reformulated)

Std

wav

efor

m

Tune

d w

avef

orm

Figure 4. Fluid characterization of commercial and reformulated inks for 1001at 6 m/s drop velocity: (a) Xaar fluid map; (b) in-flight images (c) substrate images after printing continuously for 300 metres.

Figure 4 provide such example where the performance of a commercial UV ink (Ink A) is significantly improved. The fluid map (Figure 4a) shows that the ink A meets most criteria but lacked criterion E. The ink was then reformulated with special additives to improve criterion E while still maintaining the bulk properties and other dynamic criteria similar to original ink. The

fluid map shows that both reformulated ink B and C should jet better than the original ink A. The ink C would be the best candidate as it was closer to the recommended range in criterion E.

Ink B and C gave fewer satellites as compared to original ink A for the same jetting condition as shown in-flight photographs (Fig 4b). Further tuning of the drive profile further reduced the satellite. The overall reliability of the ink was also found to be significantly improved with the reformulated ink. The figure 4c shows the images on substrate after continuously printing 300 metres from a commercial label printer utilising 1001 printheads. The modified ink C had much fewer print defects than original ink A. The performance of the ink C varied little with different drive profile indicating it to be less sensitivity to drive profile. Furthermore, the print performance of ink C did not change over 10°C (±5°C of the recommended value) where as the print defect increased outside the recommended temperature for original ink A.

This example demonstrate that complex rheological knowledge can be used to formulate/recommend ink that meets both bulk and dynamic properties for reduced misting, satellite formation and improved reliability for the given printhead and jetting condition.

Conclusions The subtle changes in the ink properties during printing are important as far as the jetting of the fluids are concerned. Novel rheological techniques to quantify fluid properties close to printing conditions can provide quantitative correlations between jetting and rheological properties. These techniques have proved useful as a prescreening tool to rank inks by detecting subtle changes in ink properties between batches and colours. They can also be exploited during formulations by being able to quantify, control and match dynamic properties (higher frequency viscoelasticity and extensional properties) of the ink. Further techniques capable of quantifying fluid rheology at printhead system resonance frequency, dynamic surface tension in microsecond time domain, meniscus and pressure profile during jetting, and mists at the print condition have to be explored to obtain more detailed insight into fluid properties and jetting.

Acknowledgements We would like to thank all our industrial and academic

partners with whom we have worked closely over the years.

References [1] Drury et al. NIP25, 95-8 (2009) [2] TR Tuladhar, MR Mackley, J. Non-Newtonian Fluid Mech., 148, 97-

108 (2008). [3] TR Tuladhar et al. NIP25, 423-426 (2009) [4] D C Vadillo et al. NIP25, 736-739 (2009) [5] D C Vadillo, et al., J. Rheol, (2010). [6] S Hoath et al., J. Image Sci. Tech, 53(4), 041208(2009).

Author Biography Tri Tuladhar received his PhD in Chemical Engineering from the

University of Cambridge (2001). He has over 10 years experience in R&D in academia and industry. Recently, he has focused on rheology of inkjet printing ink and developed measurement techniques to link fluid rheology to jetting behaviour. Currently, he heads Xaar’s development in the rheological characterisation of inks in the inkjet environment.

NIP 27 and Digital Fabrication 2011 Technical Program and Proceedings 73