The invention relates to a method of ink jet printing, wherein liquid ink is supplied to a plurality of nozzles via a common ink supply passage, and actuators associated with the nozzles are controlled to cause ink droplets to be expelled from the nozzles in accordance with image information to be printed.
It is known that pressure fluctuations in the liquid ink at the nozzles may degrade the quality of a printed image because such fluctuations affect the process of droplet formation and the stability of the jetting angle under which the ink droplets are expelled. The pressure fluctuations may also cause an increased tendency of the nozzle face of the print head to become wetted with ink, so that the droplet ejection is affected by residues of liquid ink at the periphery of the nozzle orifices.
In known ink jet printers it has therefore been attempted to design the ink supply system such that the pressure of liquid ink at the nozzles is kept as constant as possible, regardless of any fluctuations in the consumption of ink by the nozzles.
It is an object of the invention to provide an ink jet printing method by which the print quality can be improved for a given design of the ink supply system of the printer.
In order to achieve this object, the method according to the invention is characterized by the steps of:
It has been found that, surprisingly, such agitation pulses can suppress the negative effect of the pressure fluctuations which occur in a transient state in which a certain number of nozzles stop printing almost simultaneously.
In such a situation, the inertia of the liquid ink in the ink supply passage (inside or outside the print head) will generally give rise to an increased pressure at the nozzles which are connected to the common ink supply passage.
The agitation pulses applied to the actuators change the shape of the meniscus at the nozzle and thereby have the effect to mitigate the negative effects of the pressure fluctuations. A possible explanation for this effect may be that the agitation of the meniscus causes part of the liquid ink that forms the meniscus to be replaced by fresh ink from the interior of the liquid body. Since surfactants that are normally present in the liquid ink tend to accumulate at the meniscus, replacing some of the ink that forms this meniscus will at least temporarily reduce the concentration of surfactants and will thereby stabilize the meniscus against the pressure fluctuations.
More specific optional features of the invention are indicated in the dependent claims.
The agitation pulses may be applied over a certain time period which should be at least as large as the internal pressure relaxation time in the print head and may also depend upon the number of nozzles that stop printing and/or upon the times at which the nozzles will stop printing.
In piezoelectric ink jet printers it has been known to utilize the piezoelectric actuators also as pressure sensors which are capable of detecting residual pressure waves that decay in a liquid volume adjacent to the nozzle after a droplet has been expelled from the nozzle. The decay pattern of these pressure waves may provide information on the condition of the nozzle and its meniscus, e.g. a condition where a nozzle has become clogged with contaminants, and may also provide information on the shape of the meniscus. Therefore, in a further development of the invention, the detection signal from the actuator is used for judging the condition of the meniscus, which permits to fine-tune the agitation pulses in order to optimize the stability of the meniscus.
The invention is also related to an ink jet printer in which the method according to the invention is implemented.
Embodiment examples will now be described in conjunction with the drawings, wherein:
The present invention will now be described with reference to the accompanying drawings, wherein the same or similar elements are identified with the same reference numeral.
In
A recess that forms a pressure chamber 20 is formed in the face of the wafer 14 that engages the membrane 18, i.e. the bottom face in
An opposite end of the pressure chamber 20, on the right side in
Adjacent to the membrane 18 and separated from the pressure chamber 20, the support member 16 forms another cavity 30 accommodating a piezoelectric actuator 32 that is bonded to the membrane 18.
An ink supply system which has not been shown here keeps the pressure of the liquid ink in the pressure chamber slightly below the atmospheric pressure, e.g. at a relative pressure of −1000 Pa, so as to prevent the ink from leaking out through the nozzle 26. In the nozzle orifice, the liquid ink forms a meniscus 34.
The piezoelectric actuator 32 has electrodes that are connected to an electronic circuit 36 which controls a voltage to be applied to the actuator. The circuit 36 further includes a detection system 38 for detecting pressure fluctuations in the pressure chamber 20, using the piezoelectric actuator as a pressure sensing element.
When an ink droplet is to be expelled from the nozzle 26, the circuit 36 outputs a voltage pulse to the actuator 32. This voltage pulse causes the actuator to deform in a bending mode. More specifically, the actuator 32 is caused to flex downward, so that the membrane 18 which is bonded to the actuator 32 will also flex downward, thereby to increase the volume of the pressure chamber 20. As a consequence, additional ink will be sucked-in via the supply passage 22. Then, when the voltage pulse falls off again, the membrane 18 will flex back into the original state, so that a positive acoustic pressure wave is generated in the liquid ink in the pressure chamber 20. This pressure wave propagates to the nozzle 26 and causes an ink droplet to be expelled.
The acoustic wave that has caused a droplet to be expelled from the nozzle 26 will be reflected (with phase reversal) at the open nozzle and will propagate back into the pressure chamber 20. Consequently, even after the droplet has been expelled, a gradually decaying acoustic pressure wave is still present in the pressure chamber 20, and the corresponding pressure fluctuations exert a bending strain on the membrane 18 and the actuator 30. This mechanical strain on the piezoelectric transducer leads to a change in the impedance of the actuator, and this change can be measured with the detection system 38. The measured impedance changes represent the pressure fluctuations of the acoustic wave and can therefore be used to derive a time-dependent function P(t) that describes these pressure fluctuations.
The single printing element that has been shown in cross-section in
In operation, the print head assembly 42 scans a recording sheet 44 by performing a reciprocating movement in a main scanning direction y normal to the direction x of the nozzle rows.
Similarly, the rightmost nozzle row of the print head 10B has just passed over the right edge of the dark image area 46 which includes a step 50. A part of nozzles of the nozzle row (below the step 50) have already left the image area 46, whereas another part of the nozzles of the row is still printing but will soon stop printing as well. Consequently, in the ink supply passage 20 for this nozzle row, there will also be a certain rise in pressure, although the rise will be smoother and less pronounced than in case of the print head 10D.
It will be understood that the nozzles of the right nozzle row of the print head 10B will have to resume their print operation as soon as they reach the left edge of the image area 48.
According to the invention, when an increase in the pressure at the nozzle 26 has occurred or is expected, the meniscus 34 is agitated, as has been symbolically shown in
Due to the agitation of the meniscus 34, fresh ink from the interior of the chamber 24 will be pumped into the meniscus, whereas some of the ink that had so far formed the meniscus will be withdrawn into the interior of the chamber 24. This changes the concentration of surfactants at the meniscus 34 and, consequently, the surface tension of the ink at the meniscus. More precisely, the concentration of surfactants will be reduced and the surface tension will increase, which reduces the amount of bulging of the meniscus 34 (as had been illustrated in
Optionally, the stabilizing effect that the agitation pulses have on the meniscus 34 may be monitored by means of the detection system 38 (
Up to a time t0, print pulses 58 have been applied to the actuator 32 in order to expel droplets from the nozzle. At the time t0 the print operation stops because the print head has reached the edge of the dark area 46 or 48 to be printed. Then, a program which may be implemented in the controller 40 checks on the basis of the image information how many of the nozzles 26 that are connected to the same ink supply passage 22 as the present nozzle have stopped printing or will stop printing within a certain time interval T around the time t0. If the number of nozzles that stop printing exceeds a certain value, agitation pulses 60 are applied to the present nozzle and similarly to all the other nozzles that have stopped printing. In the example shown, the amplitude of the agitation pulses 60 is gradually decreased. After a certain time, the pressure surges caused by the abrupt decrease in the demand for ink will have relaxed, i.e. the pressure of the ink at the nozzle has returned to normal, and the agitation pulses 60 may be suspended. Then, the print pulses 58 may be resumed as required by the image to be printed.
The steps of a method according to the invention have been summarized in flow diagram in
A step S1 comprises counting the number N of nozzles 26 that have stopped printing or will stop printing the time interval T shown in
In step S2, it is checked whether the counted number N is larger than a certain maximum value N_max. If that is not the case (N), the print operation may be continued in the usual way (step S3).
Otherwise (result Y in step S2) the number of agitation pulses 60 to be applied to each of the nozzles that have stopped printing is calculated in step S4 as a function of the number N counted in step S1. Thus, the number of agitation pulses will be adapted to the intensity of the pressure surge. Similarly, the amplitude of the agitation pulses 60 may also be determined as a function of the number N. Then, in step S5, the number of agitation pulses as calculated in step S4 will be applied to the actuators of all non-printing nozzles and, optionally, the amplitudes of the agitation pulses will be modulated as calculated in step S4. After step S3 or step S5, another cycle of the process is started with step S1. Preferably, the process is repeated with a frequency which is at least 1/T, so that a decision whether or not agitation pulses are to be generated is taken at least once for every time interval T.
Number | Date | Country | Kind |
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17175506 | Jun 2017 | EP | regional |
Number | Name | Date | Kind |
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6508528 | Fujii | Jan 2003 | B2 |
20090244139 | Takahashi | Oct 2009 | A1 |
20100245437 | Nakamura | Sep 2010 | A1 |
20120268511 | Sasagawa et al. | Oct 2012 | A1 |
20130257944 | Yasutani | Oct 2013 | A1 |
Number | Date | Country |
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0788882 | Aug 1997 | EP |
Entry |
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Search Report issued in European priority application 17175506.9, dated Dec. 5, 2017. |
Number | Date | Country | |
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20180354258 A1 | Dec 2018 | US |