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Advanced Inkjet Technology 2025 FastTrack
Volume: 0 | Article ID: 030408
Abstract
Abstract

The extension of published and projected (IEC/ISO) international standards for inkjet printing that were specifically developed for printed and flexible electronics equipment is considered for their more general application to inkjet printing in industry and in research. A comparison of the inkjet printing equipment requirements between printed electronics (PE) and more general applications is made to provide some guidance to manufacturers, designers, and engineers potentially involved with industrial inkjet printing equipment standards compliance as integrators and/or end users. Reviews for applications and improved techniques of inkjet printing are cited, and an update is provided for international standards for PE inkjet equipment published since earlier reviews.

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Stephen D. Hoath, "International Standards for Inkjet Printingin Journal of Imaging Science and Technology,  2026,  pp 1 - 7,  https://doi.org/10.2352/J.ImagingSci.Technol.2026.70.3.030408

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Copyright © Society for Imaging Science and Technology 2026
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  • received July 2025
  • accepted November 2025
jist
JIMTE6
Journal of Imaging Science and Technology
J. Imaging Sci. Technol.
J. Imaging Sci. Technol.
1062-3701
1943-3522
Society for Imaging Science and Technology
1.
Introduction
International efforts to promote recognized standards for inkjet printing equipment intended for industrial manufacturing applications commenced for printed electronics (PE) a decade ago [1] while several standards for graphics printing equipment were developed before that time.
Several International Electrotechnical Commission (IEC) international standards or reports have been published [29] for PE inkjet printing equipment while further editions of International Organization for Standardization (ISO) standards for graphics printing equipment productivity, metrics, cartridge yield, color, and paper permanence have been released [1015]. However, none are available for any other industrial (non-graphics) manufacturing application. Therefore it appears timely to review whether any of the existing PE standards could be applied elsewhere beyond PE.
2.
Background
The widening range of inkjet (printing) applications includes those for mass production as well as specialized uniquely fabricated products. Useful reviews include “Inkjet printing and 3D printing strategies for biosensing, analytical, and diagnostic applications” [16], “Inkjet printing for pharmaceutics - A review of research and manufacturing” [17], “Inkjet-printed flexible sensors: From function materials, manufacture process, and applications perspective” [18], “Recent developments in inkjet-printed OLEDs for high resolution, large area applications” [19], “Review of digital printing technologies for electronic materials” [20], “A review of inkjet printing technology for personalized-healthcare wearable devices” [21], “Additive manufacture of ceramics components by inkjet printing” [22], “Review—inkjet printing of metal structures for electrochemical sensor applications” [23], “Challenges, prospects, and emerging applications of inkjet-printed electronics: a chemist’s point of view” [24], “Inkjet metrology: high-accuracy mass measurements of microdroplets produced by a drop-on-demand dispenser” [25], “Ultra-high precision inkjet printing technology for display” [26], “Interfaces and pattern resolution of inkjet-printed organic light-emitting diodes with a novel hole transport layer” [27], and “Classifications and applications of inkjet printing technology: a review” [28]. Other papers, such as “Future, opportunities and challenges of inkjet technologies” [29], “Formulation, quality, cleaning and other advances in inkjet printing” [30], and “Inkjet printing quality improvement research progress: A review” [31], outline process improvements in the past decade that support the wider adoption of inkjet printing.
It should be noted that the main international standards for inkjet printing equipment that exist are those developed by the IEC [32] through national experts within its technical committee TC119 on the PE working group WG3. The TC119 committee was formed in 2012, and the status of its standards work projects has been reviewed subsequently in papers by various authors in 2017 (Takahashi [1]), 2018 (Hyodo & Sakai [33], Hoath [34]), and 2022 (Zapka, Chapter 71 [35]). The present paper provides the latest 2025 update.
Key considerations for inkjet-printed functional material within electronics are drop placement accuracy and drop volume reproducibility when roll-to-roll (R2R) printing of flexible electronics, variations in jetted drop speed, and/or arrival times at the moving substrate can additionally limit printing quality. By contrast, for inkjet-printed OLED pixels, drop velocity and volume variations can usefully be averaged out by using multiple droplets spreading into each preformed pixel pit. This application dependency gives clues as to which PE standard might or might not be particularly relevant to more general inkjet printing equipment designs and intended markets.
As inkjet technology development for advanced manufacturing has progressed [35, 36], suppliers of inkjet printheads and printing equipment incorporating them have mainly relied on performance information from the printhead manufacturers before integration into industrial printers. In most cases, this information has included statements of inkjet drop jetting speeds and drop volume (or drop weight), printing frequency ranges, temperature and humidity limits, and ink viscosity. The appropriate choice of printhead is made by the integrator and then tested for the intended application(s) of the printing machine. The end user may specify the printhead manufacturer for commercial reasons, however, but without agreed standards for such equipment, how can the equipment performance or indeed design be judged prior to purchase, design, or acceptance by integrators or end users?
3.
Objectives of this Research
To help establish common criteria for equipment used in printed and flexible electronics manufacture, the IEC [32] dedicated a Technical Committee (TC119) and its Working Group (WG3) to focus on creating and publishing international standards for such printing equipment and the measurement methods used. Other TC119 working groups consider material testing, (e.g., ink properties). Following the last surveys [33, 34] of then published standards and explanation [2, 3] of optical assessments for measuring inkjet droplets, further IEC standards [4, 5, 7, 8] and a technical report [6] have been (or are being [9]) published while the ISO and IEC have become more closely aligned [37]. It seems very timely to revisit the status and explanation of the IEC standards for an advanced inkjet conference audience and to explore their wider applicability for inkjet printing.
4.
Methodology and Experimental Design
This paper examines the measurement basis for each published standard for PE equipment for inkjet printing to help explore whether there could be wider applicability to general or specific equipment for non-PE applications. Discussion of some details within the existing PE standards could assist others to make their own conclusions as to whether to follow any PE standards and/or prompt the creation of alternative inkjet printing standards or measurement methods [38, 39].
Most of the PE standards for inkjet printing equipment have focused on the outcome of the jetting process, the printhead being of the drop-on-demand (DoD) type where each ink drop forms after ink is jetted from a nozzle in response to a drive waveform applied to the channel behind the nozzle. Drops moving from the DoD inkjet printhead towards the deposition location are the initial outcome of the jetting process and, irrespective of the application, are the prime focus. Figure 1 shows a shadowgraph of a transparent UV analogue ink being jetted from a multi-nozzle inkjet printhead at speeds sufficient for generating long ligaments (“tails”) and trailing satellite drops reaching locations typically 1 mm below the nozzle bank (visible at the top of the figure).
Figure 1.
Flash image of 16 “active” DoD nozzles, with characteristic staggered jetting of Xaar shared-wall printhead technology, taken by the author using a 20 ns spark flash and a Nikon D70 with a Navitar macro lens. The image width is approximately 2.3 mm and the drop (and nozzle) diameter is approximately 50 μm. Jetting a transparent analogue UV ink at speeds of approximately 6 m/s shows exaggerated ligament tails and satellite formation. © University of Cambridge Department of Engineering (2006).
The DoD drops of interest in applications are almost invariably (but not exclusively) those reaching the deposition location. It is assumed that they have attained a single spherical shape even if they are formed of more than one fluid body by coalescence during the flight from the DoD nozzle plane. Satellite droplets are often smaller than the main drops, but if still separate at the deposition location are of importance where drop placement is critical (e.g., printed electronics).
Figure 2 shows a schematic (not to scale) of simultaneously jetting nozzles in an array, exaggerating drop speed and size differences in flight towards the deposition location/substrate. These differences are unintended in practice as they can spoil the final deposition outcome, especially if the process involves relative movement between the printhead and the substrate.
Figure 2.
Schematic of inkjet printhead showing jetting from nozzle exits towards the location for deposition, with size and location of arrow heads representing different drop volumes and speeds.
For establishing standards and for other purposes, what is measured must be carefully specified to avoid confusion: individual drops or average drops? The results of individual drop measurements can be averaged after analysis, whereas the measured average of drops does not find variations but may be simpler to measure (e.g., for stable printing) than using individual drop measurements.
Figure 3 shows some image outcomes for different shadowgraph lighting scenarios. These correspond to the following: (a) simple strobe lighting with similar drops nominally arriving at the same location and superposed on the recorded image; (b) single flash lighting for recording an individual drop in the image; and (c) double flash lighting for recording a moving drop at two different times in the same image. Scenarios (b) and (c) are associated with more advanced drop watchers than (a) as they allow analyses of individual drop sizes and speeds rather than of average drop images. The variable drop positions shown in Fig. 3(a) are exaggerated but would be merged in an image with added background for each drop shown, adding to difficulties for the image contrast.
Figure 3.
Schematic images of drops in flight recorded using various lighting methods: (a) strobe shows multiple drops; (b) single flash shows a single drop; (c) double flash shows a single drop.
The DoD drop formation process takes a small but finite time after the drive waveform start trigger. This arises from the motion of the ink meniscus that spans the DoD nozzle in response to the drive waveform and the later ejection of a jetted drop separated from the residual ink meniscus [40]. In academic studies of jetting inkjet printheads [41], jetted drop separation or first emergence of the meniscus has been adopted as the time zero for jetted drop speed measurements. In industrial systems, the drive start trigger is often taken as the time zero to exploit synchronism with substrate (or printhead) motion control timing for reliable drop location with stable inkjet printing.
Figure 4 shows the schematic representations of two unreliable jetting scenarios: (a) depicts a “failed” inkjet nozzle having no jetted ink owing to an excess of fluid across the exit (a “flooded” nozzle), resulting in a missed deposition (not shown); (b) depicts one of the “first drop effects” immediately following a “latency” period without jetting, showing the successive jetted drop locations below a single “active” nozzle after the travel time designed to reach the substrate location (shown by the dashed line) for continuous jetting through the nozzle. “Failed” nozzles can arise from (ink) particle residues, stray satellite drops, and/or nozzle plane wetting from other nozzles if the driving waveform is not optimum. “First drop” effects could occur after the evaporation of ink components.
Figure 4.
(a) Schematic example of a missed jet due to excessive ink obstructing the nozzle exit; (b) schematic of first drop effects of drop speed causing delayed arrival at the deposition location.
Can DoD inkjet printing ever be considered stable? First drop effects on drop speed and/or drop volume from a DoD nozzle are often found after a (latency) period of non-jetting [25, 42], which disappear once the jetting frequency increases beyond a certain level. Such effects are inherent [43] in piezo-DoD printheads, but the use of non-jetting channel drive waveforms, jetting waveform compensation methods, and nozzle cleaning may alleviate such unwanted changes in drop speed and volume. Avoidance of first drop effects in printing applications without heavy duty cycles on the DoD channels requires special measures, which might include nozzle cleaning, using “spitting” areas prior to production printing, and ink reformulation to avoid evaporation at nozzles.
The DoD jetting and drops are observed in flight by using optical means such as drop watchers [44] that record images that are synchronized (but fixed-time-delayed) with the applied drive waveform. Two-dimensional (2D) images are typically shadowgraphs of the drops, using short light flashes to reduce any drop motion blur. The images are recorded at high digital resolution to permit image processing software to extract drop locations and contours [45] for the analysis of speed and volume. The jetted liquid drops rapidly assume near-spherical shape in flight, which aids image analysis.
Recorded 2D images may correspond to single or double light flashes: the former is used for stable printing (assuming reproducible drops) and the latter is used for finding the speed of a single drop.
For the highest accuracy (especially for drop contour/size determination), the drop watcher image plane should remain properly focused on the drop motion throughout the region of interest. As jetted drops generally move in three-dimensional (3D) space and not just in 2D space, 3D directional information may be obtained using two orthogonal drop watchers simultaneously viewing in the nominal jetting (z-) direction and a sideways (x- or y-) direction. The 3D imaging is needed for single-nozzle printheads; as one sideways x-direction of a single 2D drop watcher image may well contain the major deviation from the nominal jetting direction; this 2D x-direction is often conveniently parallel to an array (row) of multiple nozzle outlets, ignoring any residual deviation.
Figure 5 schematically represents shape measurements on images of inkjet drops in flight or of jetted deposits on a planar substrate, using software to determine some key parameters of interest in applications: the diameter D and/or the area A, and the circularity C of the shape.
Figure 5.
Schematic representations of the common standards measurements on imaged shapes (shown by the solid curves) on a planar substrate for (a) the diameter D; (b) the area A; and (c) the ratio C of the fitted circular circumference (shown dashed) to the periphery of the shape. These measurements on images can be of drops in flight or of the deposits on a planar substrate.
Typical drop travel (throw) distances for DoD inkjet printing equipment designs are 1 mm [35, 44], so a common industrial guideline used to quote the drop impact speed adopts the time taken to travel from a somewhat shorter distance to a slightly longer distance in the formula for this speed:
(1)
Drop speed at impact=Difference in travel distance Difference in travel time .
Travel time differences are usually far more precisely known than the drop location differences [41]. The location of the drop is determined from either the center or the leading edge of the 2D image [42], with the center usually having higher precision. The image plane magnification and pixel calibration factors need to be established before reporting the jetted drop impact speeds in meter/second.
The printhead is always held stationary and upright during measurements for standards purposes although it might be moved sideways across the optical field of view of the drop watcher for channel selection purposes. Drop watchers are often used to monitor jetted drops simultaneously from several inkjet printhead nozzles, for straightforward visual drop (speed) comparison purposes, but this compromises the available image resolution for drop volume determination. Alternatively, average drop volume could be estimated by using drop weighing rather than shadowgraph methods applied to single drops. Inkjet ink properties such as liquid density, surface tension, and viscosity under jetting conditions are beyond the scope of this paper.
Drop placement accuracy relies on optical scanning after drop deposition on suitable media. Usually, the media are moved under a fixed printhead with multiple inkjet nozzles jetting, with rigid media on flatbeds and flexible media on R2R stations. In contrast to jetting conditions used for in-flight measurements for standards purposes, most inkjet deposition arrangements necessarily include realistic airflows between the printhead and the substrate [46].
5.
Description and Analysis of Results
5.1
Drop Speed
Fundamental effects on round inkjet drops flying through still air are viscous drag, electrical forces, and gravity; however, for flights of 1 mm or less, gravity and electrical forces have little detectable effect on DoD inkjet drops. Those drops that are still changing shape are usually newly formed following DoD jetting from a nozzle or are low (aqueous) viscosity or elastic inks. Viscous drag on the inkjet drop slows it down in flight so that all measured inkjet drop speeds depend on the travel distance. Furthermore, travel speed depends on the time interval as well as the travel distance, whereas instantaneous speed [47] depends on the gradient (slope) of the travel distance–time curve. Both are important: drop arrival times at a moving substrate determine the location of the deposition on the substrate and drop impact speed determines the spreading on the substrate (whether moving or not). To measure the travel speed, find the travel distance divided by the elapsed time between the drop arrival and the start time (trigger) of the printhead drive waveform; the drop impact speed does not rely on knowing the start time trigger.
5.2
Drop Volume
In some applications, a knowledge of the ink volume per drop deposited on a substrate is very important, for example, loading each color pixel of a display with a precise quantity of material; several ink drops are jetted onto the display pixel area to achieve a specific material thickness. This material thickness σ (lower case sigma) may be specified in terms of drop weight W rather than drop volume V , using known ink density ρ (lower case rho) to convert between drop weight and drop volume, finding the deposited ink thickness σ after also dividing by the color pixel surface area S:
(2)
σ=VA=W(ρS).
The drop volume (V ) can be deduced from the measured digital image of an inkjet droplet from the fitted drop diameter (D) in pixels and the linear calibration of the image plane (k) in micrometers per pixel (μm/pixel): adapting the well-known expression for the volume V = (4∕3)πr3 (lower case pi) of a sphere of radius r=12D gives
(3)
V=16π(kD)3.
Alternatively, if the area (A) in pixels squared is fitted to the digital image of an inkjet droplet, then
(4)
V=134πk3(Aπ)32.
The common practice with traditional drop watcher images is the use of a straightforward analysis with pixel resolution, but this choice has consequences, especially for absolute droplet volume. To achieve a precision result (p) in percentage for the deduced drop volume V , Eq. (3) shows that the number of pixels across the image diameter D should be known to (p∕3) in percentage; so for example to obtain a 1% volume precision, the diameter needs to be measured to 13%, requiring that for D = 30 pixels, the fitted drop diameter must be obtained to 0.1 pixel precision, that is, using sub-pixel resolution. Such a high level was achieved (Snyder et al. [48]) for picoliter drop volumes down to 1.1 pL of rheologically challenging materials following guidelines in the published PE standard [3]. Drop watcher system setups monitoring several nozzles across the image plane do not usually have this level of precision and using merely pixel level resolution could limit drop volume measurements to >10%. Such an uncertainty in absolute volume might be insufficient for many applications (e.g., tablet dosing, thin film coatings).
An analysis of Eq. (3) reveals that the linear calibration k of the image plane is also required at high precision for absolute drop volume determination. This might be achieved using sub-pixel resolution fitting to the nozzle spacing in an image of a multi-nozzle inkjet printhead. Without the knowledge of k, a common practice is to compare inkjet drop sizes measured in pixels rather than micrometers, but the drop image fitting used should be sub-pixel rather than manual.
The average drop weight can be found by weighing a stream of drops over a known period, using a microbalance [25]. This is usually found by checking the accumulated mass at several intermediate time points within this period and then during a succeeding (latency) period without printing any inkjet drops.
Figure 6 is a schematic representation of this technique. Determining the slopes of the mass graphs during (I) and after (II) printing can compensate for the effects of evaporation during accumulation.
Figure 6.
Schematic representation of the total accumulated jetted drop weight during (I) and after (II) continuous jetting from an inkjet printhead. The slopes fitted to the measured weight changes with time are used to estimate the average inkjet drop weight and hence the drop diameter.
In practice, the mass resolution of the microbalance needs to be typically 0.01 mg or smaller for achieving drop mass values smaller than 10% for the typical drop mass of 4 ng for a 20 μm diameter (4.2 pl volume) drop.
5.3
Drop Direction
Without prior knowledge of the directionality of the jetted drops from a single-nozzle printhead, the 2D image plane of a drop watcher, or more commonly the horizontal orientation of the printhead, should be set up to keep the motion of the jetted drops in focus during their vertical travel distance in the field of view. Modern multi-nozzle (array) DoD printheads have many rows so that good control of the jetting rows and nozzles is necessary to aid the image plane setup for measurements and simplify the image analysis. Modern printheads produce well-directed jets and drops, so the highest sub-pixel resolution and analysis is required to measure off-axis directions, 3D trajectories, and drop volume. Inkjet drop watchers purpose-designed for R&D are available (for example, [49]).
Figure 7 shows two drop locations measured simultaneously by two orthogonal drop watchers (a) and (b), with these 2D image planes referred to the 3D space and polar coordinates in (c). The distance r shown between the drops in (c) is a measure of the absolute (3D) speed of the drop. Using a single drop watcher such as (a) would determine a (lower) projected drop speed if θ (lower case Greek theta) > 0.
Figure 7.
Two orthogonal 2D geometric images of a representative inkjet drop in flight for the vertical z-axis in the nominal jetting direction for (a) xz image plane; (b) yz image plane; and (c) their 3D combination in polar coordinates (r, θ, ψ). Angle θ (lower case Greek theta) is the off-axis (zenith) direction while the plane zψ (lower case Greek psi) is a rotation about z-axis (equivalent to θ = 0) by an (azimuth) angle ψ from a fixed direction (e.g., the x-axis) such as the printhead nozzle row.
5.4
Drop Placement
The measurement of drop placement accuracy requires specification of the medium used to register drops on impact. For PE equipment purposes, the medium is either a liquid absorbing layer on a planar substrate or a hydrophilic or a hydrophobic layer on a planar substrate because the medium specified depends on the functional ink that is jetted by the printhead. Sometimes a different medium from that of the final application must be used, for example to make visible the drops of a transparent ink. Therefore mechanical thickness and physical properties (e.g., temperature and humidity dependencies) of the test and application media must be known.
Figure 8 schematically represents an intermediate stage of image analysis of drops deposited on a planar substrate. The distribution of shapes and locations would be compared with the design for substrate printing. They might also indicate jetting failures or ink spreading deficiencies.
Figure 8.
An intermediate stage of image analysis of drop deposits on a planar substrate. The individual shapes in the images have each been fitted with circles (dashed lines) and centroids (crosses) located with reference to a 2D grid.
Accurate alignment and registration of the medium relative to the printhead may be arranged by mounting this medium on a carrier with suitable fiducial marks during the ink drop placement and then optically scanning drops on the medium afterwards using suitable auto-analysis software. The circularity C of the deposited drops on the medium may be used to judge the inkjet print quality:
(5)
C=Circumference of fitted circular drop Actual circumference of deposited drop .
Further discussion of the drop placement standard [8] for PE awaits its final publication in 2025.
6.
Conclusion
Work has already progressed on standardizing alternative means to assess inkjet drop speed [39], weight and volume [9], and potentially jetted drop direction, with plenty of opportunities for further technology experts to join the IEC TC119 working groups. Applying one or more of the existing PE equipment standards to applications beyond PE seems timely. Perhaps another international group working under ISO should consider developing general inkjet standards based on the existing published work.
Acknowledgment
The author thanks his many past and present international colleagues in IEC TC119 WG3 who have contributed to inkjet equipment standards meetings, development, and publications and his colleagues at the University of Cambridge (UK) Inkjet Research Centre for their collaboration. He also thanks the Society for Imaging Science and Technology for the 2024 Johann Gutenberg Prize.
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49JetXpert 3D, ImageXpert Inc., Nashua, New Hampshire, USA