COMPENSATION FOR CROSSTALK BETWEEN CHANNELS OF AN INK JET PRINTER

Abstract: The invention relates to a method of compensating for crosstalk between adjacent charging electrodes (14) in an ink jet printer having multiple printing jets (12) or channels, each with one charging electrode (14). In order to provide a desired drop charge in a specific channel X, there is applied, to the corresponding charging electrode (14X), a charge potential VX which is compensated for in response to (i) any charge potentials VX-1 and VX+1 applied to charging electrodes (14X-1, 14X+1) of the nearest channel X-1 and X+1, respectively, on each side of the specific channel X, and (ii) in response also to at least charge potentials VX-2 and VX+2 applied to charging electrodes (14X-2, 14X+2) of the next nearest channel X-2 and X+2, respectively, on each side of the specific channel X. The compensation is achieved by selecting VX as equalling a value V(I) associated with a charge situation I at issue and included in a matrix of compensated predetermined potential values compiled by an iterative, or equivalent, technique.

Description: Compensation for crosstalk between channels of an in jet printer The present invention relates generally to ink jet printers with multiple ink jets or channels. More parti¬ cularly, the invention relates to a method of compensating for crosstalk between charging electrodes in such an ink jet printer. In an ink jet printer, ink drops are applied to a printing surface to jointly form a picture, a text, etc. To provide such a print, ink jet printers with multiple continuous ink jets have a printing head comprising a nozzle with a number of orifices distributed in one or more rows and communicating with a liquid container acccm- modating an electrically conductive liquid. The liquid is forced by pressure through each nozzle orifice in the form of separate continuous printing jets which are decomposed into drops, i.e. each printing jet is transformed into a drop train. A multiple jet ink printer further comprises, imme¬ diately adjacent the drop formation point of each printing jet, a separate charging electrode associated with the printing jet and adapted to generate a charge field for selectively charging the drops of the corresponding drop train. Drop charge-controlling electrode potentials are applied selectively to each charging electrode to charge the drops when these are being formed at the drop forma¬ tion points. In other words, each continuous printing jet is transformed into a drop train consisting of drops with selectively controlled charges. The drop trains with their selectively charged drops pass from the drop formation points through a deflection field which is associated with the printer and in which charged drops are deflected and uncharged drops pass in undeflected paths. The printing surface, for example a paper on a rotating roller may be adapted, depending upon the printer construction, to receive either the unde- flected or the deflected drops. During start-up of an ink jet printer of this type, the pressure in the liquid container is increased for a short but by no means negligible time during which the paths of the printing jets and the drop trains are unpre¬ dictable and the drop formation process is not fully deve¬ loped. This unstable function lasts until the correct ope¬ rating pressure has been attained in the liquid container. Conditions are essentially the same upon shut-down of the printer. When the pressure in the liquid container decreases and the liquid flow through the nozzle orifices is reduced, the printing jets and the drop trains become unstable and difficult to control. During start-up and shut-down of an ink jet printer there is, therefore, a considerable risk that liquid will be deposited on the charging electrodes, causing physical obstacles to the printing jets and/or the drops, and this again may result in an erroneous text or no text at all. Also during normal operation, there may occur, for various reasons, an undesired deposition of drops on the charging electrodes. For the reasons stated below, this phenomenon is especially pronounced in multiple jet printers. In a system with multiple printing jets positioned relatively close to one another, the electric field from a charging electrode (the charge field) may affect the drop charge of several printing jets, besides the jet associated with that particular charging electrode, i.e. crosstalk between different channels may occur. To reduce such crosstalk, it is conventional to arrange the separate charging elec¬ trodes in the manner shown in Fig. 1 of the accompanying drawings. One such electrode structure is described in, for example, IBM Technical Disclosure Bulletin, Vol. 20, No. 1, June 1977 and IBM Technical Disclosure Bulletin, Vol. 19, No. 8, January 1977. Fig. 1 shows a broken-away part of a charging elec¬ trode means 10 in an ink jet printing head with multiple printing jets 12. The electrode means 10 has, for each printing jet 12, a rectangular recess or slit in which a separate charging electrode 14 is formed. The shielded U profile thus imparted to each charging electrode 14 reduces the crosstalk between the separate charge fields. Furthermore, Fig. 1 illustrates schematically how a print signal 16 associated with each printing jet 12 and con- taining information about a desired drop charge in the printing jet is supplied to the respective charging elec¬ trode 14 via an amplifier 18. With an electrode structure as shown in Fig. 1, the risk is considerable that already a few drops deposited on the charging electrodes may clog the relatively small slits and form physical obstacles to the jets 12. To solve the problem of clogging, the above-mentioned IBM Technical Disclosure Bulletin, Vol. 20, No. 1, June 1977 proposes a charging electrode means which is movable in relation to the nozzle generating the printing jet. Upon start-up and shut-down, the charging electrode means is moved aside, such that uncontrolled printing jets and drops cannot be deposited on the charging electrodes. Similar constructions have been proposed for moving the deflection electrodes aside. In this manner, the undesired deposition of ink on the electrodes is avoided. However, moving the charging electrodes aside in this manner during start-up and shut-down is inadequate. For one thing, addi¬ tional space is required in the printing head to accommo- date the electrode means moved aside. Secondly, the move¬ ment of the charging electrodes may, in course of time, cause these electrodes to be incorrectly positioned in relation to the orifice plate and the drop formation points, resulting in an incorrect text. Thirdly, a movable electrode structure is more expensive to manufacture and requires more maintenance, and fourthly an undesired depo¬ sition of ink in the small slits may occur also during normal operation (i.e. between start-up and shut-down) of the electrode structure shown in Fig. 1. The crosstalk problem has previously been discussed by Robertson in US 4,074,278 which proposes a method of compensating for crosstalk between adjacent charging elec¬ trodes of an ink jet printer having multiple printing jets or channels, each with one charging electrode. More parti¬ cularly, Robertson proposes, in order to provide in a spe¬ cific channel X a drop charge suitable for printing, to apply to the corresponding charging electrode a charge potential V χ which is compensated for in response to any charge potentials V χ , and/or V χ+ . being applied to charg¬ ing electrodes of the nearest channel X-1 and X+l, respec¬ tively, on each side of the specific channel X. Thus, US 4,174,278 proposes (col. 4, lines 26-29), in order to obtain uncharged drops, i.e. drops providing a print, to selectively apply to the electrode of the specific channel X a potential of opposite polarity which is sufficient in magnitude to counteract the crosstalk effect. This known compensation technique can be explained by means of the Table below in which it is assumed that the printing function is normally controlled by switching the charge potential between V . and 0 volt (both taken in relation to the potential of the ink), and in which k is a constant less than 1, which is dependent upon the amount of crosstalk in the printer at issue. ELECTRODE X-1 ELECTRODE, ELECTRODE X+l 0 -kVcharge +Vcharge +Vc I harge -kVcharge 0 +Vcharge -2kVc.harge +Vcharge To avoid confusion with other known technique in the field of ink jet printers, it should be observed that both US 4,074,278 and the present invention are concerned with the compensation of channel-to-channel crosstalk, not with drop-to-drop crosstalk in a specific channel. The compensation technique proposed by US 4,074,278 is, as can be seen from Fig. 2 of this patent, intended to be used in conjunction with a slitted or U-shaped charging electrode structure as shown in Fig. 1 of the present application. As already mentioned, it is extremely diffi¬ cult with such an electrode structure always to maintain the printing jets fully stable so that they will not strike the charging electrode structure. Only a few drops need to be deposited on the charging electrode surface to render the printing jet inoperative. On the other hand, a planar charging electrode struc¬ ture as shown in Fig. 2 of the accompanying drawings is far less sensitive to wrongly deposited drops, and also is easier to make. However, since such a planar charging electrode structure has no crosstalk shielding, the amount of crosstalk will nevertheless be so considerable that the compensation technique proposed by US 4,074,278 does not suffice to give a compensation with adequate accuracy of the drop charges. Therefore, there is need for a technique capable of producing an accurate and satisfactory compensation for charging electrode structures having intense crosstalk between adjacent channels. The present invention meets this requirement and proposes, for this purpose, an improvement of the com¬ pensation technique described in US 4,074,278. The dis¬ tinctive features of the inventive method of compensating for crosstalk between channels are stated in the appended claims. The inventive method of compensating for crosstalk gives a far better compensation than US 4,074,278. The compensation according to the invention is so efficient that it becomes practically possible to use the type of planar charging electrode structures illustrated in the accompanying Fig. 2 in applications with a relatively small distance between printing jets, i.e. in applications with fairly considerable crosstalk. A number of embodiments of the invention are describ¬ ed in more detail below, reference being had to the accom¬ panying drawings. Fig. 1 is a broken-away schematic view of a known slitted charging electrode structure; Fig. 2 is a broken-away schematic sectional view of a planar charging electrode structure and the associated compensation electronics; Fig. 3 is a schematic perspective view of a first embodiment of an ink jet printing head; Fig. 4 is a schematic perspective view of a second embodiment of an ink jet printing head; Fig. 5 is a broken-away schematic cross-sectional view of an electrode configuration in the printing head of Fig. 3, including suitable dimensions; Fig. 6 corresponds to Fig. 2 and illustrates in block form the structure of a signal correction means; Fig. 7 is an electric block diagram of a first method of realising the signal correction means of Fig. 1; and Fig. 8 illustrates a circuit solution for a second method of realising the signal correction means of Fig. 6. The charging electrode means 10 of Fig. 1 with its separate charging electrodes 14 has been described above in conjunction with the prior art technique. In the fol- lowing description, use is made, as far as possible, of the same reference numerals as in Fig. 1. Reference is now made to Fig. 3 which illustrates a highly schematic perspective view of an ink jet printing head with multiple channels. The printing head comprises a drop formation means in the form of a plate 24 having a row of orifices (not shown) communicating with a liquid container (not shown) containing electrically conductive ink. The ink in the liquid container is of fixed poten¬ tial. The orifices of the plate 24 divide the ink into a number of separate printing jets 12 which are divided, each at one drop formation point 20, into separate drops. Initially, the printing jets 12 are dispersed in a plane 26 perpendicular to the plate 24. The printing head further comprises a charging elec¬ trode means 10 having a separate charging electrode 14 for each printing jet 12. The charging electrodes 14 lie in the immediate vicinity of the drop formation points 20 in a main surface 28 of the charging electrode means 10, parallel to the plane 26. As can be seen from the corre¬ sponding schematic sectional view of Fig. 2, the main sur¬ face 28 is at a distance from the plane 26, i.e. the charging electrodes 14 lie entirely outside the plane in which the printing jets 12 are dispersed. The printing head of Fig. 3 is adapted to be sup¬ plied from outside with a printing signal 16 associated with each printing jet 12 and corresponding to the print- ing signals 16 in Fig. 1. On the basis of these printing signals 16, separate charge fields are generated at each charging electrode 14 for selectively charging the drops 22. The drops 22 are dispersed in the form of drop trains, as shown by the dotted line 30, in between sche¬ matically shown deflection electrodes 32 and 34. Uncharg¬ ed drops pass straight ahead through the deflection field, as shown at 36. Charged drops, on the other hand, are deflected in known manner and caught by a catching means 38, as indicated at 39. The printing signals 16 are not directly supplied to the charging electrodes 14, as in Fig. 1. Instead, the printing signals 16 which are assumed to be binary sig¬ nals, are supplied in parallel into a signal correction means 40 in which the printing signals 16 are processed in a predetermined manner to generate a corresponding number of output signals 42. After suitable amplification in amplifiers 18, there are obtained, on the basis of these output signals 42, charge-controlling electrode potentials which are applied each to one charging electrode 14. Before the function of the signal correction means 40 is described, reference is made to Fig. 4 which illu¬ strates a second embodiment of a printing head. Like the printing head of Fig. 3, the printing head shown in Fig. 4 comprises a drop formation means in the form of an orifice plate 24, a charging electrode means 10 with separate charging electrodes 14, deflection electrodes 32, 34, a collecting means 38, and a signal correction means 40. In the embodiment of Fig. 4, the separate charging electrodes 14 are, however, applied directly to the side of the plate 14 facing the deflection electrodes 32, 34. Each charging electrode 14 has an orifice oppo¬ site a corresponding orifice in the plate 24. Thus, in this embodiment, the potential of the printing jets 12 discharged from the plate 24 is controlled. The separate charge fields are established between, on the one hand, the separate charging electrodes 14 and the associated printing jet 12 and, on the other hand, a common elec¬ trode 46 having a fixed potential and substantially coin¬ ciding with the main surface 28 shown in Fig. 3. The function of the correction electronics 40 in Figs. 2-4 will now be described with reference to Fig. 6 which at the top schematically shows a section of the charging electrode means 10 in Fig. 3. The reference numerals in Fig. 6 are indexed X-2, X-1, X, X+l and X+2, respectively, indicating the channel position among the channels of the printing head. The amount of crosstalk between channels is repre¬ sented by schematically drawn capacitances C„. The contri¬ bution to the charging of the drops in a specific channel X (the centre channel in Fig. 6) deriving from the charg- ing electrode 14_ is given by C„V„ wherein V„ is the charge potential applied to the charging electrode 14 . It is assumed that the drops in the printing jet 12 χ for the specific channel X should be either uncharged (printing) or sufficiently charged for deflection and catching (no printing). The charge of the drops 22 χ in specific channel X is then obtained from the following equation Q χ =C χ V χ +∑C n V n (n≠X ) (equation 1) wherein C χ V χ is the direct charge contribution to the drops 22 χ for the charging electrode 14 χ , and wherein ∑CnVn is the crosstalk contribution from the other elec- trodes. Since the value of Ci |n-X„|ι decreases when |ιn-X„|ι increases (i.e. the farther one gets away from the speci¬ fic channel X), one needs to include only so many terms that sufficient charge accuracy is obtained. If it is assumed that the system is symmetrical, the crosstalk from a given channel on one side of the channel X will equal the crosstalk from the corresponding channel on the other side, i.e. C χ-n =C X + n ( equation 2 ) To further simplify this model, it is assumed that sufficient charge accuracy for the drops is obtained if only the crosstalk from the two nearest adjoining chan¬ nels on each side is taken into consideration. It should be stressed, however, that the invention is in no way restricted to this selection, and that the model is entirely generic, i.e. the number of further adjoining channels to be considered - in addition to the two near¬ est on each side - may be optional and should be deter¬ mined by the required charge accuracy. The required charge accuracy is in turn determined int. al. by the deflection obtained by a possible "mischarge", and by the resolution desired in the printed text. If only crosstalk from the two nearest channels on each side is taken into consideration, equation 1 may be simplified as Q X =C X V X +C X + l (V X + l +V X-l )+C X + 2 V X + 2 +V X-2 ) ( equation 3 ) From equation 3, V γ can be calculated by iteration as fol- lows V(new) χ =V(old) χ +K-[Q(ideal) χ -Q χ ]/C χ (equation 4) wherein Q(ideal) χ is the desired drop charge, Q χ is the calculated value from equation 3, and K is a constant affecting the convergence of the iteration. For example, K is 0.5, preferably less than 1.0. If the iteration con- verges, the charge error (Q(ideal) χ -Q χ ) will be minimised. In a system without crosstalk, V χ merely need assume two different values, viz. V QN to generate the drop charge 0 upon printing, and QFF to generate the drop charge Q 0FF upon deflection. According to equation 3, however, the system which has been described and which thus exhibits 4 crosstalk, requires sixteen (2 ) different potentials to generate the drop charge 0, and a further 16 potentials to generate the drop charge Q OFF , because of the necessary compensation for the crosstalk of the four nearest chan¬ nels. 5 These thirty-two (2 ) different potentials will here¬ inafter be identified as [V(0), V(l), ...V(30), V(31)]. The index I associated with the potentials V(I) (0≤I≤31) is determined as follows I=2 Z χ _ 2 +2 3 Z χ _ 1 +2 2 Z χ +2 1 Z χ+1 +2 C χ+2 (equation 5) wherein Z v assumes the value 0 if channel X is printing (i.e. generating uncharged drops), and Z χ assumes the value 1 if the specific channel X is deflecting (i.e. generating charged drops). The potentials calculated for the specific channel X are correct for all channels except the two outermost channels of the printing head. For these two channels either a separate calculation model must be established, or two additional channels with charging electrodes, but without associated printing jets, must be provided as outermost channels on each side. To make the calculations manageable, the following standardisations are introduced " Q χ (l> = (equa¬ tion 6 The value 1 corresponds to the charge which, in an equi¬ valent system without crosstalk, is required for deflect¬ ing a drop sufficiently to ensure that it is caught. The value 0 corresponds to a zero charge. The capacitances C_ are standardised as follows C " C X' " C X+1' " c x+2 ] ' [1 ' C X+1 C X' c x+ 2 / c χl (equa¬ tion 7 For the iteration, the following standardised values are given as starting values for the V(I) matrix "V = wherein 0 corresponds to the potential of the printing jets, and the value 1 corresponds to the potential which, in an equivalent system without crosstalk, gives suffi¬ cient deflection. With these standardisations, equations 3 and 4 can be standardised as follows " Q X = " C x" V X +C X+l^ V X+l + " V X-l> + " C X+2<" C V+2 + " V X-2 Ration 9 ,, V(new) χ ="V(old) χ +0.5[ ,, Q(ideal) χ -"Q χ ]/"C χ (equation 1 By means of equations 9 and 10, new values are calcu¬ lated for all components of the matrix. By taking these new values as new input values, and by repeating the cal¬ culation, it is possible to arrive by iteration at a solu- tion of V χ . Whether the iteration converges, depends upon the values of [C χ , C χ ., C χ \ , but in actual practice it has been found that the iteration converges in most cases. The capacitance values can be measured as follows. The charging electrode systems is combined with a nozzle having but one printing jet; this channel is designated X hereinafter. By introducing an electrically conductive plate in the path of the drop train and connecting this plate via an ammeter to the liquid forming the printing jet, the current carried by the charged drops can be measured. By applying a potential E to the charging electrode of chan¬ nel Z, while maintaining all of the other charging elec¬ trodes at the same potential as the printing jets, a cur¬ rent I_ is measured on the ammeter. By repeating this pro¬ cedure for all of the channels, a set of current values is obtained. These current values are proportional to the capacitances C„ previously mentioned. By dividing the cur- rent values by the value I χ , the standardised capacitances "C„ are obtained. For the converging values of V χ equation 9 can be used for calculating the drop charges given by the system. The matrix component among the uncharged conditions which has the greatest deviation from the ideal matrix (equation 6) is compared with the permissible "mischarge". If the deviation is too large, further adjoining channels must be included in the calculation, in the case here concerned also the third nearest channel on each side. The standardised values in the V(I) matrix are con- verted into actual potentials by multiplying by V QFF for all matrix components, i.e. the potential which, in an equivalent system without crosstalk, gives sufficient deflection. It is especially pointed out that equation 9 uses one and the same V(I) matrix for selecting the values of the variables ["V χ _ 2 , "V χ+1 , "V χ+2 ] . For the cal¬ culation in accordance with equation 9, one does not know the exact value of the potentials C"V χ _ 2 , "V χ _,, " v x+1 , "V χ 2 3 because these potentials (which also have been com- pensated for crosstalk) also depend on the state of chan¬ nels outside the channel group ["V χ _ 2 , "V χ _ l "V χ , "V χ+1 , "V χ 2 ] . This can be solved by calculating the drop charge for every conceivable situation and using a mean value in the calculation of the charge error in equation 10. In the analysis of whether adequate charge accuracy has been achieved, this should be taken into consideration. A computer program should be formulated to carry out the large number of calculations required for obtaining V χ and for analysing the "mischarge" caused by the matrix. The above iteration technique has been used for a case in which ["C χ , "C χ+1 , " χ + 2- != - 1 ' °- 274 / 0.032], which gave the following V(I) matrix The values in the above matrix can be interpreted as follows. If it is assumed that all five channels are printing, i.e. situation 1=0 (00000), the charge potential V γ for channel X should be 0.00 according to the above matrix. If one then proceeds to sitation 1=4 (00100), i.e. if only the channel X is changed from printing to deflec¬ tion, it will be seen that the requisite voltage change ΔV χ is +1.23. This voltage change ΔV χ of +1.23 must be carried out whenever only the channel X is changed from printing to deflection, regardless of the states of the remaining four channels. This corresponds to the following row changes in the matrix, while retaining the same column: 1 to 2, 3 to 4, 5 to 6 and 7 to 8. For example, if one proceeds from situations 1=16 (line 5: 10000) to situation 1=20 (line 6: 10100), the charge potential V χ must be changed from 0.05 to 1.28, i.e. with ΔV χ =+1.23. If, on the other hand, it is assumed - proceeding from situation 1=0 (00000) - that the nearest right-hand channel X+l begins to deflect (i.e. a positive potential is applied to the electrode V χ . ), this will mean a change-over to situation 1=2 (00010). As will appear from the above matrix, the charge potential V χ of channel X must then be compensated for from 0.00 to ΔV χ . by -0.34, which should be compared to the prior art technique of US 4,074,278 in which the compensation was given as -kV . However, if one studies the compensation effect of potential changes in channels X-2 and X+2, an unexpected change of signs can be seen. For example, by proceeding once more from the charge situation 1=0 (00000) and letting the next nearest channel X+2 to the right of the channel X start deflecting, which implies a change-over to the charge situation 1=1, it will be seen from the above matrix that, for channel X, the voltage change required for compensation is ΔV χ 2 =+0.05. In other words, the vol¬ tage change for channel X must be positive if the next nearest channel goes from printing to deflection, and this is an unexpected result. For comparison, the compensation technique proposed by US 4,074,278 may be studied. If one tries to use this prior art technique to compensate for more than the two nearest channels, this change of signs would not be obtained, i.e. the prior art technique pro¬ posed by this patent would not give a correct result if applied to the compensation for crosstalk from two or more channels on each side of a given channel. According to the above matrix, the charge error for printing drops lies between 0.88% and -0.79% of the stan¬ dardised deflection charge. An interesting observation is that V χ may purely be expressed additively as follows V X =ΔV X Z X +ΔV X+l Z X-l +ΔV X+l Z X+l +ΔV X+2 Z X-2 +ΔV X+2 Z X+2 wherein Z assumes the value 0 if channel X is printing (i.e. generating uncharged drops), and Z χ assumes the value 1 if channel X is deflecting (i.e. generating charg¬ ed drops). For example, for a change-over from situation I=(00000) to situation 1=27(11011), the potential V of the electrode 14 χ of channel X must, according to equation 10, be changed from V χ =0.00 to V χ =+1.23«0+(-0.34)•(1+1)+ (+0.05) ' (1+1)=-0.58, which corresponds to V(27) in the above matrix. Fig. 7 illustrates a possible realisation of the com¬ pensation electronics for channel X with ΔV χ - positive. By means of five resistors R1-R5, of which R1=R5 and R2=R4, the previously calculated table values can be rea- lised. The printing signals from the two nearest channels X-1 and X+l are inverted before they are coupled, like the printing signals for channel X and for the two next nearest channels X-2 and X+2, to the corresponding resis- tors. The output signal 42 χ from the resistor network 48 is then connected, like before, to the charging electrode 14 via an amplifier 18. Fig. 8 illustrates a more generic solution. In this alternative, the function generating unit 48 comprises an electronic memory 50, such as a ROM or RAM memory, con¬ taining the previously calculated values for every con¬ ceivable input signal state. The memory 50 is addressed by the printing signals supplied in parallel and consisting for the X channel of the printing signals 16 χ _ 2 , 16 χ _ 1 , !6 χ , 1( 5χ + ι an *^ 1 ^χ + 2* w ^ en 'the memor Y 50 is addressed in this manner, the correctly stored value is supplied in digital form, as indicated by reference numeral 52. This digital output signal can then be supplied to a digital- to-analog converter 54 converting the digital value 52 into an analog output signal 42 χ whose voltage is propor¬ tional to the binary value 52. The analog output signal 42 χ is then transferred to the charging electrode 14 χ via an amplifier 18. It should be observed that the above-mentioned unex- pected change-over of signs for the next nearest channels is not absolutely necessary. Geometries giving a negative voltage change for channel X when the next nearest channel X-2 or X+2 goes from printing to deflection, can also be physically realised. The above method of compensating for crosstalk, according to the present invention, is so effective that it can be used with advantage in combination with a planar charging electrode structure of the type shown in Fig. 2, in spite of the fairly considerable crosstalk of such a structure. This is a considerable advantage as compared with the slitted structure which is shown in Fig. 1 and which has the above-mentioned inconvenience of clogging. It should also be mentioned that the invention is applicable also to the case when the printing signals 16 have more than two state levels. For the above-mentioned compensation for two channels on each side of a specific channel, this would mean that the V(I) matrix contains more than 32 values. However, the calculation thereof could be carried out in basically the same manner.

Claims: 18 CLAIMS 1. A method of compensating for crosstalk between adjacent charging electrodes (14) in an ink jet printer having multiple printing jets (12) or channels, each with one charging electrode (14), said method comprising the step of applying, in order to provide a desired drop charge in a specific channel X, to the corresponding charging electrode (14 χ ) a charge potential V χ which is compensated for in response to any charge potentials V χ _.. and V χ . being applied to charging electrodes (14 χ _., 14 .) of the nearest channel X-1 and X+l, respectively, on each side of the specific channel X, c h a r a c ¬ t e r i s e d by the step of compensating for said charge potential V χ for the specific channel X in response also to at least charge potentials V χ _ 2 and V χ 2 applied to charging electrodes (14 2 , 14 χ+2 ) of the next nearest channel X-2 and X+2, respectively, on each side of the specific channel X, said channel X, said nearest channels X-1 and X+l and said next nearest channels X-2 and X+2 jointly forming a channel group, said compensation being achieved by selecting, for a given charge situation I of said channel group, V as equalling a value V(I) asso¬ ciated with the charge situation I and included in a matrix of compensated predetermined potential values compiled by an iterative, or equivalent, technique accord¬ ing to which there is calculated, in each iteration step and for every possible charge situation I of the said channel group, a new value of V(I) as a function of, on the one hand, the value of V(I) calculated in the imme¬ diately preceding iteration step and, on the other hand, a deviation of the desired charge in the charge situation I for the specific channel X from the charge Q χ (I) which, for the charge situation I, is obtained in the specific channel X according to the formula X+2 ι=X-2 wherein C. is a capacitance between the printing jet (12 v ) for the specific channel X and the charging electrode for channel No. "i" of the said channel group, and wherein V.(I) is a charge potential value which, for channel No. "i" of the said channel group, is determined by means of the values of V(I) calculated in the immediately pre- ceding iteration step. 2. A method as claimed in claim 1, c h a r a c ¬ t e r i s e d in that binary printing signals (16) are supplied in parallel to an electronic memory means (50) for jointly forming successive digital address signals to said memory means; that data concerning the said compen¬ sated potential values V(I) for every possible combination of the binary printing signals (16), i.e. every possible address signal, are stored in predetermined memory spaces of said electronic memory means (50); and that charge potentials for said charging electrodes are formed on the basis of these data, when said memory means is addressed by said address signals. 3. A method as claimed in claim 1, c h a r a c ¬ t e r i s e d in that the printing signals (16) are sup- plied in parallel to a network of inverters and resistors (R1-R5) to form said charge potentials. 4. A method as claimed in claim 1, c h a r a c ¬ t e r i s e d in that said printing jets (12) are caused to disperse in a common geometrical plane (26), and that said charging electrodes (14) are arranged entirely outside said plane (26). 5. A method as claimed in claim 4, c h a r a c ¬ t e r i s e d in that said charging electrodes (14) are arranged in a surface (28) parallel to said plane (26) and facing the printing jets (12), to form a planar charging electrode structure. 6. A method as claimed in claim 1, c h a r a c ¬ t e r i s e d in that each charging electrode (14) is arranged in direct contact with its printing jet (12) to control the potential thereof. 7. A method as claimed in claim 1, c h a r a c ¬ t e r i s e d in that the said charge potential V χ of the specific channel X is also compensated for in response to any charge potentials applied to charging electrodes of further adjacent channels (X-w, X+w, w>2) on each side of said specific channel X.

Inventors: BJOERKENGREN ULF, BJOERKENGREN, ULF
Applicants: PLOTCON HB
Application year: 1990
Main classification: B41J2
IPC codes: B41J2