Method and apparatus for thermal ink jet drop volume control using variable prepulses

Information

  • Patent Grant
  • 6698862
  • Patent Number
    6,698,862
  • Date Filed
    Thursday, January 16, 2003
    21 years ago
  • Date Issued
    Tuesday, March 2, 2004
    20 years ago
Abstract
A method and apparatus are providing for extending the drop volume control of a thermal ink jet print head. The print head has a plurality of drop ejectors, each of the plurality of drop ejectors has a heating element actuatable in response to input signals to eject an ink droplet from the print head. The method includes the steps of applying a plurality of print signals to the print head, the plurality of print signals corresponding to an image for the ink jet assembly to create, applying at least one pulse signal to the print head, and sequentially using the at least one pulse signal and the plurality of print signals to activate the heating elements so that the change in current remains small. In addition, the apparatus has a print data storage element that receives print data from a printer controller, a pulse data delay element that receives pulse data from either a print head controller or a previous drop ejector and sends the pulse data to a next drop ejector after a predetermined delay, a heating element and a checksum element that, when the data storage element contains print data, and the pulse data delay element contains pulse data, activates the heating element according to the print data and the pulse data.
Description




BACKGROUND OF THE INVENTION




1. Field of Invention




This invention relates to methods and apparatus used in thermal ink jet printers.




2. Description of Related Art




A thermal ink jet print head selectively ejects droplets of ink from a plurality of drop emitters to create a desired image on an image receiving member, such as a sheet of paper. The print head typically comprises an array of the drop emitters that convey ink to the image receiving member. In a carriage ink jet print head, the print head moves back and forth relative to the image receiving member to print the image in swaths.




Alternatively, the array may extend across the entire width of the image receiving member to form a fullprint head. Fullprint heads remain stationary as the image receiving member moves in a direction substantially perpendicular to the array of drop emitters.




A thermal ink jet print head typically comprises a plurality of ink passageways, such as capillary channels. Each channel has a drop emitter and is connected to an ink supply manifold. Ink from the manifold is retained within each channel. Then, in response to an appropriate signal applied to a resistive heating element in each channel, the ink in a portion of the channel adjacent to the heating element is rapidly heated. Rapidly heating and vaporizing some of the ink in the channel creates a bubble that causes a quantity of ink, such as an ink droplet or a main ink droplet and smaller satellite drops, to be ejected from the emitter to the image receiving member. U.S. Pat. No. 4,774,530 to Hawkins, the disclosure of which is incorporated herein by reference in its entirety, shows a general configuration of a typical inkjet print head.




U.S. Pat. No. 4,791,435 to Smith et al., the disclosure of which is incorporated herein by reference in its entirety, discloses an ink jet system where a constant temperature of the print head is maintained by using the heating elements of the print head not only for ejecting ink but to maintain the temperature close to a predetermined value as well. The print head temperature is compared to thermal models of the print head to provide information for controlling the print head temperature. At low temperature, low energy pulses are sent to each channel, or nozzle, below the voltage threshold which would cause a drop of ink to be ejected. Alternatively, the print head is warmed by firing some droplets of ink into an external chamber or “spittoon,” rather than onto the surface of the image receiving member.




European Patent Application 0 496 525 A1, the disclosure of which is incorporated herein by reference in its entirety, discloses ink jet recording method and apparatus in which ink is ejected by thermal energy produced by a heat generating element of a recording head. In the EP 525 application, driving circuits apply plural driving pulses to the heat generating element for every ink droplet ejected. The plural driving pulses include a first driving pulse used to increase a temperature of the ink adjacent the heater without creating a bubble, and a second driving pulse subsequent to the first driving pulse to eject the ink. Additionally, a width of the first driving pulse is adjustable to change an amount of ejected ink.




European Patent Application 0 505 154 A2, the disclosure of which is incorporated herein by reference in its entirety, discloses thermal ink jet recording method and apparatus which control an ink ejection quantity by changing driving pulses supplied to the recording head based on a variation in the temperature of the recording head. A preheat pulse is applied to the ink to control the ink temperature and is set to a value which does not cause an ink bubble to form. After a predetermined time interval, a main heat pulse is applied which forms an ink bubble to eject one or more droplets, such as a main droplet and satellite droplets, of ink from the ink channel.




U.S. Pat. No. 5,519,417 to Stephany, the disclosure of which is incorporated herein by reference in its entirety, discloses a power control system for a printer which has at least one heating element for producing spots. The system includes a thermostat, disposed on a print head, that senses the temperature of the print head. The sensed temperature is used to vary pulses applied to the at least one heating element to maintain a constant spot size.




Thus, it is known to advance the firing of a print ejector by applying different pulses to a print ejector, advancing the firing after applying a firing pulse.




U.S. Pat. No. 5,917,509 to Becerra et al., the disclosure of which is incorporated herein by reference in its entirety, discloses methods and apparatus for interleaving multiple pre-pulses in a thermal ink jet printer. The pre-pulses are timed to use the periods between preheating a print head to pre-warm additional print ejectors.




SUMMARY OF THE INVENTION




This invention provides methods and apparatus for using a print head having a plurality of drop ejectors.




This invention separately provides a thermal ink jet print head circuit architecture that enables arbitrary multiple prepulsing signals to be used.




This invention separately provides systems and methods for varying the timing of pre-pulses, as well as the timing of a final or firing pulse to sequentially pre-warm and fire print ejectors.




In various exemplary embodiments, each ejector has a heating element actuatable in response to input signals to emit a quantity of ink from the print head toward an image receiving member. Pulse trains comprising of a series of pulses are used as the input signals. The pulse train can be determined based on, for example, the temperature of the print head.




In various exemplary embodiments, the sequential and cumulative firings of the prepulses and final or drop-forming pulses in the selected channels throughout the print head are performed in a manner such that the switching transients due to energizing and de-energizing drop ejectors are reduced to the level of those due to one heater element turning on or off. The transients are reduced in spite of substantial variations in print head temperature, the number of print jets used and the print image produced. The image data is loaded from the printer controller into a print data array. The heating elements are then fired in a sequence controlled by pulse trains originating in a print head controller. The pulse trains are clocked to sequence the firing of the heating elements in a manner that minimizes the change in current per unit of time.




In various exemplary embodiments of this invention, using multiple pre-pulse wave forms allows drop mass to be stable over substantial temperature and pulse train ranges. The print head circuit design accepts these arbitrary wave forms while decreasing switching noise, reducing fluidic cross-talk in the print head, and allowing maximal droplet ejection frequencies.




Other objects, advantages and features of the invention will become apparent from the following detailed description taken in conjunction with the attached drawings, which disclose exemplary embodiments of the invention.











BRIEF DESCRIPTION OF THE DRAWINGS




The invention will be described with reference to the following drawings in which like reference numerals refer to like elements and wherein:





FIG. 1

is a schematic view of an ink jet printer;





FIG. 2

is a crossview of a single ejector channel for a thermal ink jet print head;





FIG. 3

is a conventional timing diagram showing how single prepulses may be applied in a printing device to banks of emitters;





FIG. 4

is the temperature history at the inkelement interface for a single prepulse in a conventionally driven thermal ink jet printhead;





FIG. 5

is a table showing a first exemplary embodiment of a pulse train table according to this invention;





FIG. 6

is a table showing a second exemplary embodiment of a pulse train table according to this invention;





FIG. 7

is a block diagram of one exemplary embodiment of an ink jet emitter driver circuit according to this invention;





FIG. 8

is a block diagram of one exemplary embodiment of an ink jet emitter driver circuit according to this invention usable as a slice of the driver circuit of

FIG. 7

;





FIG. 9

shows a first exemplary embodiment of a pulse train according to this invention;





FIG. 10

shows one exemplary embodiment of a pulse train moving through a print head and the associated current according to this invention; and





FIG. 11

is a block diagram of a second exemplary embodiment of an ink jet emitter driver circuit according to this invention.











DETAILED DESCRIPTION OF EXEMPLARY EMBODIMENTS




For simplicity and clarification, the operating principles and design factors of various exemplary embodiments of the systems and methods according to this invention are explained with reference to one exemplary embodiment of a carriage-type ink jet printer


2


, as shown in

FIG. 1

, and one exemplary embodiment of a printhead


30


, as shown in FIG.


2


. The basic explanation of the operation of the ink jet printer


2


and the printhead


30


is applicable for the understanding and design of any fluid ejection system that incorporates this invention. Although the systems and method of this invention are described in conjunction with the ink jet printer


2


and the printhead


30


, the systems and methods according to this invention can be used with any other known or later-developed fluid ejection system.





FIG. 1

shows a carriage thermal ink jet printing device


2


. A linear array of droplet producing channels is housed in a print head


4


mounted on a reciprocal carriage assembly


5


. A number of ink droplets


6


are propelled towards a receiving medium


8


, such as a sheet of paper, that is stepped by a motor


10


a preselected distance in a process direction, indicated by the arrow


12


, each time the print head


4


traverses across the receiving medium


8


along the scan axis indicated by arrow


14


. The receiving medium


8


can be stored on a supply roll


16


and stepped onto a take up roll


18


by the motor


10


or other means well known to those of skill in the art.




The print head


4


is fixedly mounted on the support base


20


of the carriage


5


, which reciprocally moves along the two parallel guide rails


22


. The print head


4


may be reciprocally moved by a cable


24


and a pair of pulleys


26


, one of which is powered by a reversible motor


28


. The print head


4


is generally moved across the receiving medium


8


perpendicularly to the direction that the receiving medium


8


is moved by the motor


10


. Of course, any other known or later-developed structure usable to reciprocally move the carriage assembly


5


can be used in the thermal ink jet printing device


2


.




Alternatively, the linear array of droplet producing channels may extend across the entire width of the receiving medium


8


, as is well known to those of skill in the art. This is typically referred to as a fullarray. See, for example, U.S. Pat. No. 5,160,403 to Fisher et al. and U.S. Pat. No. 4,463,359 to Ayata et al., each of which is incorporated herein by reference in its entirety.





FIG. 2

shows one exemplary embodiment of an ink droplet emitter or ejector


30


of one embodiment of a typical ink jet print head


4


. A plurality of such emitters


30


are found in a typical thermal ink jet print head


4


. While

FIG. 2

shows a side emitter, other emitters, such as roofemitters, may similarly be used with the systems, the methods and the architectures according to this invention. In an exemplary embodiment, the emitters


30


are sized and arranged in linear arrays of 300 to 600 of the emitters


30


per inch. Other dimensions can be used in other exemplary embodiments, as known to those skilled in the art.




A silicon member having a plurality of ink channels is known as a “die module” or “chip”. Each die module can comprise hundreds of the emitters


30


, spaced 300 or more to the inch. An exemplary full-width thermal ink jet print head may have one or more die modules forming a fullarray extending across the full width of the receiving medium on which the image is to be printed. In print heads with multiple die modules, each die module may include its own ink supply manifold, or multiple die modules may share a common ink supply manifold.




Each emitter


30


includes a capillary channel


32


terminating in an orifice or nozzle


34


. The capillary channel


32


holds a quantity of fluid


36


, such as ink, but not limited to ink, maintained within the capillary channel


32


until such time as a droplet of fluid is to be emitted. Each capillary channel


32


is connected to a supply of fluid from a fluid supply manifold (not shown). An upper substrate


38


is located adjacent to a thick film layer


44


, which in turn is adjacent to a lower substrate


42


.




Addressing electrodes


52


are sandwiched between the thick layer


44


and the lower substrate


42


. The addressing electrodes


52


control and carry electrical current to one or more electrical heating elements


46


located within openings


54


in the thick film layer


44


. Each of the ejectors


30


in the print head may have its own heating element


46


and individual addressing electrode


52


. In various exemplary embodiments, the addressing electrode


52


may be protected by a passivation layer


40


and an insulating layer


50


. Each addressing electrode


52


and associated heating element


46


may be selectively controlled by control circuitry, as will be explained in detail below, to form and grow vapor bubbles in the fluid


36


due to heating the fluid


36


in contact with the heater element


46


, with droplets


56


of the ink being subsequently ejected from the print head


4


. Other embodiments of the fluid print head are well known to those skilled in the art and are also within the scope of this invention.




When a signal is applied from a power source to the addressing electrode


52


using the control circuitry, the heating element


46


is energized. If the signal is of a sufficient magnitude and/or duration, the heat from the resistive heating element


46


will cause the fluid


36


immediately adjacent to the heating element


46


to vaporize, creating a bubble


57


of vaporized fluid. The force of the expanding bubble


57


ejects a fluid droplet


56


, which includes a main droplet


56


and may include one or more smaller satellite drops from the orifice


34


onto the surface of the receiving medium. For a given heating pulse, or pulse train, length, the minimum voltage which causes a droplet of the fluid


36


to be ejected in response to the heating pulse or pulse train being applied to the heating element


46


is called the threshold voltage.




The thermal ink jet print head


4


may apply a plurality of pulses to the heating element


46


for each fluid droplet


56


to be ejected. One or more precursor pulses, i.e., warming pulses or prepulses, may be applied by the heating element


46


to warm the fluid


36


adjacent to the heating element


46


. Subsequently, a print pulse, i.e., a drive pulse, a firing pulse or a main pulse, may be applied to the heating element


46


. The print pulse causes the fluid droplet


56


to be ejected. The prepulses may be used to raise the temperature of the fluid


36


adjacent to the heating element


46


and additionally may be used to control the volume of the fluid droplet


56


. The prepulses do not contain enough energy to cause the fluid droplet


56


to be emitted.




More particularly, in the thermal ink jet printing process according to this invention, a short duration voltage pulse may be applied to the heating element


46


. This short duration voltage pulse very rapidly raises the temperature of the heating element


46


, as well as the temperature of the fluid


36


that is in physical contact with the heater element


46


. In the absence of an extant liquid/gas interface, the fluid


36


in the neighborhood of the heating element


46


may be superheated, i.e., heated beyond the normal boiling temperature of the fluid


36


.




The vapor bubble


57


subsequently nucleates and grows at the surface of the heating element


46


. The vapor bubble


57


begins to expand under the influence of the high initial vapor pressure, which can be, in various exemplary embodiments, several tens of atmospheres, and continues to expand due to inertial effects. As the size of the vapor bubble


57


grows, the pressure in the vapor bubble


57


decreases, due in part to the increase in the volume of the vapor bubble


57


. However, the pressure in the vapor bubble


57


decreases as well due to cooling caused by the fluid


36


lying at the initially-expanding interface with the vapor bubble


57


. This cooling occurs due to the fluid


36


evaporating at the bubble-fluid interface, as well as to heat conducting from the vapor bubble


57


into the surrounding fluid


36


.




Following initial growth of the vapor bubble


57


, the heating element


46


loses contact with the fluid


36


. Accordingly, subsequent growth of the vapor bubble


57


is essentially unaffected by the temperature of the heating element


46


. Thus, the eventual size of the vapor bubble


57


, and thus the size of the droplet


56


of the fluid


36


ejected from the nozzle


34


, depends on the energy stored in the layer of superheated fluid


36


which was in contact with the heating element


46


when the vapor bubble


57


nucleated. With higher print head and ink temperatures, there is more energy stored in the superheated fluid


36


next to the heater element


46


when the ink temperature reaches the nucleation value.




In addition, the viscosity of the fluid depends on the temperature of the fluid. In particular, higher fluid temperatures lead to lower viscosity, and similarly reduced resistance to flow. Thus, high temperatures cause more energy to be stored in the superheated layer in the fluid


36


, and cause lower resistance to the impulsive flow involved in ejecting the fluid droplets


56


. As a result, drop volumes increase with print head temperature.




In addition, only a small fraction of the energy dissipated in the heater element


46


is utilized in nucleating the vapor bubble


57


and producing the fluid droplet


56


. The remainder of the heat flows into the die and subsequently into a heat sink, raising their temperature. Thus, continued use of the thermal inkjet print head causes the temperature of the thermal inkjet print head to increase. Unless some device, structure or apparatus is provided to prevent drop masses from changing, drop masses will increase with continued use of the thermal inkjet print head, thus degrading print quality. In addition, thermal inkjet print heads may be used within a range of ambient temperatures. Variations in the ambient temperature may exacerbate the variations in droplet masses due to the self-heating effect described above.




Simply changing pulse width or voltage in response to changes in print head temperature is a relatively ineffective method of maintaining a constant drop volume as the temperature of the thermal inkjet print head changes. This occurs due to the de-coupling of the heater element


46


from the fluid


36


by the vapor bubble


57


once the vapor bubble


57


forms and due to the requirement for a minimal or threshold voltage below which no droplet


56


is produced.




The energy input to the heating element


46


can be varied to provide different energy amounts stored in the layer of superheated fluid


36


at the time of vapor bubble nucleation, by breaking the heating pulses into two or more segments. Following this technique, energy is supplied to the heater element


46


and the fluid


36


via one or more pre-pulses which locally heat the fluid


36


. In various exemplary embodiments, the fluid


36


is heated to temperatures above the normal boiling point of the fluid


36


, to provide some superheat in the fluid


36


, but not to the temperature required for a vapor bubble


57


to form and grow. With the fluid


36


next to the heater element


46


thus pre-heated, a relatively short off, or soak, time allows the heat to diffuse deeper into the fluid


36


, while the temperature of the fluid


36


next to the heater decreases. A subsequent main or firing pulse, possibly having a longer duration, is then provided to the heater element


46


to re-heat the fluid


36


next to the heater element


46


to the nucleation temperature, where a vapor bubble


57


forms, causing a droplet


56


of the fluid


36


to be ejected.





FIG. 3

is a timing diagram showing how conventional prepulse and firing signals are applied to the emitters


30


or banks of the emitters


30


, in a thermal inkjet print head. A precursor pulse


58


, having a duration T


1


, is applied to an emitter, or an emitter bank, A, to warm the fluid


36


and/or to control a size of the fluid droplet


56


to be ejected. This is followed by a relaxation time interval


64


having a duration T


2


. Then, a print pulse


60


having a duration T


3


is applied to a specific emitter or the emitter bank A. Subsequently, a second precursor pulse


58


followed by a second relaxation time interval


64


and a print pulse


60


are applied to an emitter, or an emitter bank, B. This process continues across the print head in serial fashion until all the emitters


30


, or all of the emitter banks, required to eject drops of fluid have been addressed.





FIG. 4

shows a typical temperature vs. time evolution curve


140


for the fluid


36


next to the heater element


46


of a print head driven by the single-pre-pulse waveform shown in FIG.


3


.

FIG. 4

also shows corresponding plots of the energy


150


delivered to the fluid


36


, and the amount of energy


160


stored in the layer of superheated fluid


36


. The superheat energy is that energy stored in the layers of the fluid


36


having temperatures above the normal boiling point for the fluid


36


. For the water-based inks used in a thermal ink jet, the normal boiling point of the fluid is slightly over 100° C.




By using the pre-pulse


58


and the delay interval


64


prior to the application of the main or firing pulse


60


, the local temperature, i.e., the temperatures of the heater element


46


and of the fluid


36


within a few micrometers of the heater element


46


, as well as the energy stored in the superheated fluid


36


at nucleation, are similar to those temperatures for the same print head at an elevated temperature. Therefore, utilizing a pre-pulse makes the drop volume increase relative to that for the same print head with a single drop-ejecting pulse.




By varying the durations of the pre-pulses


58


at a constant operating temperature, the drop volume can be changed, where longer pre-pulses


58


result in larger drop volumes. Alternatively, by varying the durations of the pre-pulses


58


in response to changes in print head temperature, the drop volume may be held constant as the print head temperature changes. With suitable adjustments to the durations of the pre-pulse


58


as well as to the main pulse


60


in response to changes in print head temperature, the drop volumes as well as the operating point for the print head, relative to the threshold voltage, may be held constant in spite of the changes in temperature.




There are limitations to the amount of control over drop volume that can be achieved by using a single pre-pulse


58


if the operating voltage of the print head is to be fixed. One such limitation is due to the onset of interference. Interference occurs when the pre-pulse duration is so long that small, localized vapor bubbles


57


form on the heater element


46


near the end of the pre-pulse


58


. These vapor bubbles


57


may fail to grow sufficiently to eject a droplet


56


by themselves. However, the presence of these small localized vapor bubbles


57


disturbs the desired uniform pre-heated layer of fluid


36


next to the heater element


46


. Additionally, any residual vapor bubbles


57


on the surface of the heater element


46


, when the main pulse has heated the fluid


36


to the nucleation temperature, may adversely affect the desired subsequent explosive growth of a drop-ejecting vapor bubble


57


. In practical terms, for a single pre-pulse drive waveform, drop volume increases with pre-pulse duration, but the duration of the single pre-pulse


58


is limited by the onset of interference. When used in a drop volume stabilization scheme as described above, drop volumes may be held constant over a temperature range of about 15° C. by using a single pre-pulse


58


, when constrained by the effects of interference as well as the additional requirement that the threshold voltage remain constant.




The advantages of a multiple prepulse waveform according to this invention, relative to a single prepulse waveform, arise because the relatively low average power level resulting from using a relatively large number of short, appropriately-spaced pre-pulses allows a thicker layer of fluid


36


to be pre-heated, which provides a higher level of superheat energy in the fluid


36


at the time of the explosive growth of the vapor bubble


57


when the firing pulse


60


is applied to the heater element


46


. This increase in the superheat energy available to drive the growth of the vapor bubble


57


and the drop ejection is achieved with the multiple pre-pulse waveform according to this invention without the damaging effects of interference by pre-heating a thicker layer of the fluid


36


to a lower peak temperature than would be obtainable if a single pre-pulse wave form were used to achieve the same superheat energy.




Because the probability that interference bubbles will form depends on the peak fluid temperature during the pre-heating process, the lower peak temperature due to the multiple pre-pulse wave form according to this invention allows greater energy to be stored into the fluid


36


without forming interference vapor bubbles


57


. The ability of the multiple pre-pulse waveforms, according to this invention, to achieve greater superheat energy levels without the deleterious effects of interference enables a larger range of temperatures over which the drop volumes may be held constant by varying the number of pre-pulses in the multiple pre-pulse pulse train.




The multiple prepulse waveforms according to this invention limit the temperature rise in the fluid


36


with each prepulse


58


by utilizing short heating pulses as the prepulses


58


. Intervals between these short prepulses


58


allow the heat to diffuse into the fluid


36


somewhat before a next heating prepulse


58


or main pulse


60


is applied. This is approximately equivalent to preheating the fluid


36


with a long duration, but low power-density, heating prepulse


58


.




However, it should be appreciated that it is important to drive the fluid temperature through the nucleation level briskly and continuously. Thus, an exemplary multiple prepulse waveform according to this invention has a relatively large number of short prepulses


58


, and a relatively long main pulse


60


at the end of the pulse train. The relatively long main pulse


60


assures that the fluid temperature is taken briskly and continuously through the nucleation temperature during the relatively long main pulse


60


in spite of variations in circuit parameters.




The multiple prepulsing methods according to this invention substantially increase the temperature range over which the drop volume can be controlled. It has been determined that the superheat content of the fluid


36


plays an important role in determining the droplet volume. The superheat content of the fluid


36


changes either because of prepulsing, because the die temperature rises due to heat build-up in the die, or because of a combination of both factors. Even though the superheat may be the same under different combinations, the droplet volume will depend upon how that superheat is accumulated.




At a given die temperature, the droplet volume can be increased by increasing the superheat using different pulsing patterns. In various exemplary embodiments according to this invention, a larger number of prepulses


58


is used to drive the print head when the print head is at its lowest temperature. The number of prepulses


58


decreases as the temperature of the print head increases to hold the drop volumes constant. In practice, a schedule of pulse trains can be used over different ranges of temperatures, such that the drop volumes and threshold voltages are maintained essentially constant in spite of the changes in the temperature of the print head.





FIGS. 5 and 6

show two exemplary pulse and interval signal profile tables usable to keep the exemplary print emitter″s drop volume constant over a range of temperatures while maintaining threshold voltages relatively constant according to this invention. The tables in

FIGS. 5 and 6

show pulse and interval times in microseconds (μs), with the main pulses given subscripts of zero, and preceding pre-pulses and intervals identified with successively larger subscripts. For example, as shown in the profile table shown in

FIG. 5

, when the temperature of the print head is 30 degrees C., an initial prepulse P


5


lasts for 0.3 microseconds. A second prepulse P


4


then lasts for 0.3 microseconds after a first 0.6 microsecond interval S


5


. A third prepulse P


3


then lasts for 0.3 microseconds after a second 0.6 microsecond delay S


4


. A fourth prepulse P


2


then lasts for 0.2 microseconds after a third 0.6 microsecond interval S


3


. A fifth or final prepulse P


1


then lasts 0.2 microseconds after a fourth 0.6 microsecond interval S


2


. A main pulse P


0


then lasts 2.0 microseconds after a fifth or final interval S


1


that lasts for 0.6 microseconds. Means for measuring or estimating the temperature of the printhead are provided so that the printhead controller can select which pulse train to utilize for a given printing area.




While calculations indicate that pulse-train schedules incorporating initial pre-pulse segments with longer pulse duration and relatively shorter intervals between pulses should provide even larger temperature control ranges, experiments have shown those to result in relatively unstable droplet velocities, apparently due to interference-like phenomena.




One potential disadvantage of using longer pulse trains for the multiple pre-pulse trains disclosed above is that the time required to apply the full pulse train to the heater elements


46


increases. To enable an adequate electrical operating frequency limit for a print head utilizing a multiple pre-pulse wave form according to this invention, larger numbers of heater elements


46


need to be on at any single time if the total time for moving the pulse train through the print head should remain below a threshold time. This has implications for electrical transients due to simultaneously switching the currents to all the heater elements


46


that are addressed at the same time, and for the fluidic transients resulting from simultaneously forming and growing large numbers of the vapor bubbles


57


. In addition, the relatively complex and variable nature of the pulse trains prevents using known print head circuit architectures. In various exemplary embodiments, a print head circuit architecture according to this invention that avoids these performance-limiting factors allows the multiple pre-pulse wave forms according to this invention to be effectively utilized.





FIG. 7

is a schematic diagram of one exemplary embodiment of a circuit


250


according to this invention usable to control a thermal ink jet emitter array that avoids these performance limiting defects. The circuit


250


includes a digital delay line


252




a


to allow serial loading of print data, a print data storage array


252




b,


a digital delay line for the pulse train


254


, an array of AND gates, pre-drivers and drivers


256


, and an array of heater elements


258


. One element in each of the arrays


252


,


254


,


256


and


258


is associated together into a slice, such as slice


260


.




Print data from a printer controller, such as a computer, a network or a copier, is input to the print data storage array


252


. In an exemplary embodiment, the data bits are serially shifted into the digital delay line


252




a,


and then simultaneously latched into the print data storage array


252




b.


The print data delay line


252




a


can be implemented as an array of D-type flip-flop circuits, or any other known or later-developed circuitry usable to latch and propagate the print data down the print data delay line


252




a.


In various exemplary embodiments, the print data storage array


252




b


stores the print data for a predetermined time period. Alternately, in various exemplary embodiments, the print data delay line


252




a


simply forwards appropriate information to the array


256


of AND gates, pre-drivers and drivers.




The contents of print data storage array


252




b


determine whether the associated ink jet emitters are to be fired in a particular stroke. If the print data bit is set for a particular slice


260


, the print data storage array


252




b


forwards a positive signal to the AND gate of the array


256


of AND gates associated with the slice


260


.




The digital delay line for the pulse train


254


receives a serial pulse train from the print head controller and shifts it down the array in accordance with a clock signal. The contents of each cell of the digital delay line for the pulse train are also provided to the associated elements of the array of AND gates


256


.




The array


256


of AND gates combines the print data signals from print data storage array


252




b


and the pulse train on the digital delay line


254


. When both signals are positive for a particular slice


260


, the AND gate of the array


256


of heater elements associated with that slice


260


forwards a positive signal to the heater element of that slice


260


of the array


258


. The heater element of the array


258


then heats the ink using current I.





FIG. 8

is a schematic diagram of one exemplary embodiment of a device circuit


200


used to implement a slice


260


, and that, individually, can be used to control an individual thermal emitter


30


. The drive circuit


200


includes a heater resistor


210


, a driver or power transistor


208


, a number of D-type flip-flop circuits


202


,


204


and


212


, and an AND gate


206


.




Each slice


260


can include a latch


212


that is one element of a chain of latches forming a serial data register implementing the print data delay array


252




a.


This register loads and stores the print data. The input of each latch “n” takes data from the previous serial data latch “n−1” and sends it to the next latch “n+1.” The output of the Nth latch is also fed forward to another latch


202


which forms one element of a large parallel data register, used to implement the print data storage array


252




b


with N


T


stages. The collection of all serial data latches in


252




a


forms a serial data register with N


T


stages with one primary data input to the thermal print head.




The set of latches which comprise the parallel data register, or print data storage


252




b,


can store the data to be printed while new data is simultaneously loaded into the serial data register


252




a.


The output of latch


202


is connected to the input of the logical AND circuit


206


.




A latch may also be used as an element of a chain of latches forming the pulse train digital delay line


254


. This register stores the pulse train to be used to energize the heater


210


shown in FIG.


8


. Latch


204


takes its input from the pulse train latch of the previous stage n−1 and sends it to the next stage n+1. The output of the nth stage is also connected to the input of the logical AND circuit


206


. The collection of all pulse train delay latches can form a digital delay line


254


with N stages, and with one primary pulse train input to the thermal ink jet circuit.




The print data from a printer controller, such as a computer, a network or a copier, is loaded into the D-type flip-flop circuit


212


, along with a clock signal from a first clock signal CLOCK


1


. The D-type flip-flop circuit


212


stores the print data for a predetermined time period. The D-type flip-flop circuit


212


acts in concert with the neighboring D-type flip-flop circuit


212


of the next slice along the circuit


250


. The D-type flip-flop circuits


212


form a long shift register which is loaded with the data in a series fashion.




Once all the data is loaded into the D-type flip-flop circuits


212


in each slice of circuit


250


, the D-type flip-flop circuits


202


are clocked by a second clock signal CLOCK


2


, which loads all of the data stored in the D-type flip-flop circuits


212


into the array of D-type flip-flop circuits


202


. The D-type flip-flop circuits


202


then retain this print data and present it to the AND gate


206


.




The D-type flip-flop circuit


204


in slice


260


is loaded with a bit from the pulse train which is supplied by the print head controller to the D-type flip-flop circuit


204


in the first slice of the circuit


250


, and shifted into the corresponding circuit


204


of slice


260


from the previous slice with the timing controlled by the clock signal CLOCK


1


. The pulse train will typically include a series of prepulses and a main pulse. In accordance with the timing of the CLOCK


1


signal, the D-type flip flop circuit


204


then forwards its bit from the pulse train to the AND gate


206


and to the corresponding D-type flip-flop circuit


204


of the next slice.




The separate first and second clock signals CLOCK


1


and CLOCK


2


allow a next set of data to be loaded into the D-type flip-flop circuit


212


while the data stored in the D-type flip-flop circuit


202


is utilized for a current firing stroke. Thus, the circuits according to this invention can load data into the D-type flip-flop circuit


212


timed by Clock


1


, while simultaneously pulsing the data from the D-type flip-flop circuit


204


. This above described procedure continues until there is no more data and no more clocks. At this point the carriage has completed its scan across the paper, and it will then be reinitialized for the next pass.




The AND gate


206


combines the signals from the D-type flip-flop circuits


202


and


204


. When both signals are positive, the AND gate


206


forwards a drive signal to driver or power transistor


208


. The driver or power transistor


208


allows the current I


n


to flow through the heater resistor


210


in response to the drive signal. As a result the heater resistor


210


resistively heats.




A heater element of the heater array


258


in a particular slice


260


is energized when the data input and the pulse train are both active for that slice


260


. It should be noted that if the data bit corresponding to slice


260


is set, the heater power in that slice will vary from clock cycle to clock cycle in accordance with the sequence of pulses in the pulse train as the pulse train is shifted through slice


260


.




It is obvious to anyone skilled in the art that the printhead circuit architecture as described above allows the pulse train to be any complex sequence of pulses and intervals. Therefore, for a pulse train of P “time slots”, it is possible to provide 2


P


unique heating profiles of temperature versus time. This approach allows the heating profiles to be flexible and extend the range of possible power versus time profiles and temperature versus time profiles. In contrast, analog techniques enabling similar power and temperature profiles would be expensive and complex to implement on the thermal print head.




In various exemplary embodiments, the pulse train schedules shown in

FIGS. 5 and 6

are usable in the systems, methods and circuit architectures according to this invention to make the size of the ink drops emitted by the thermal ink jet emitters


30


more constant. It can be seen that within the pulse train schedules shown in

FIGS. 5 and 6

, there are variations in number and length of prepulses, length of the main pulse, and overall length of the pulse train. Alternatively, the pulse trains shown in

FIGS. 5 and 6

can be used in various exemplary embodiments of the systems methods and circuit architectures according to this invention to controllably vary the size of the ink drops emitted by the thermal inkjet emitters


30


in selected ways.




It is likewise obvious to anyone skilled in the art that the printhead circuit architecture described above reduces the instantaneous variations in total current flow to the heaters in the printhead to a value equal to that of the current flow to a single heater element. This minimized current transient results from the bit-by-bit insertion and advancement of the pulse train into and through the serial shift register formed by the D-type flip-flops


204


in each of the slices


260


in the printhead. The overall current flow to the heaters in the printhead—subject of course to the previously loaded and latched data bits—thus incrementally increases as the pulse train enters delay line


254


and incrementally decreases as the pulse train leaves delay line


254


.





FIG. 9

shows a time plot of an exemplary multiple-pre-pulse pulse train which has five pre-pulses followed by a main pulse. If the tic-marks on the abscissa indicate 0.5 μsec intervals, we see that the first pre-pulse


502


is 1.5 μsec long, whereas all succeeding pre-pulses (


506


,


510


,


514


&


518


) are 0.5 μsec long. We see further that intervals


504


,


508


,


512


,


516


&


520


are 0.5 μsec, and that the main pulse


522


is 2.0 μsec. The overall length of the pulse train T is simply the sum of all the on and off times: 8 μsec.





FIG. 10

shows a combined graph of one embodiment of the circuit architecture performing the multiple prepulse method according to the present invention and the total heater current at each instant in time during the passage of the pulse train through the printhead. The exemplary printhead circuit has an effective length as indicated by the arrow on FIG.


10


. The input signal is the pulse train shown in

FIG. 9

, composed of desired pre-pulse and main pulse signals, and shown here at various locations


604


-


610


on the timing diagram. Clock


602


controls the advancement of the pulse train through the pulse train shift register or delay line. For the purposes of this example, we assume that the data has been pre-loaded, and that that data calls for each channel in the exemplary printhead to fire a droplet of ink. The pulse train is supplied to the printhead″s pulse train shift register or delay line, and at the instant indicated by the location of pulse train


604


, the lead edge of the first pre-pulse is just about to enter the first stage of the pulse train shift register. One clock period later, the pulse train is as indicated by number


606


, and the overall heater current waveform


620


shows an incremental increase in current. Following a second clock pulse, the pulse train is at the location indicated as


608


, and we see that at that time, the heater current has incremented again. With each period of the clock, the pulse train advances into and through the pulse train shift register, and the heaters corresponding to each of the slices in the head in which the pulse train bit is high are activated. In

FIG. 10

, the overall heater current (the sum of the currents flowing through all the heaters) increases in a step-wise manner in response to each clock pulse so long as the incoming pulse train bit is set. After the full pulse train has been shifted into the printhead″s pulse train shift register, and until the first pre-pulse begins to be shifted out of the shift register, the overall heater current is constant. Finally, at a time indicated by the location of pulse train


612


, the pulse train begins to be incrementally shifted out of the printhead shift register, and the overall current decreases in increments of the current that flows through a single heater.




In the exemplary embodiment shown in

FIGS. 7 and 8

, the digital delay array


254


uses one digital delay element for each slice, where each slice


260


contains one heater element. In the exemplary embodiments shown in

FIGS. 7 and 8

, the digital delay line delays the pulse train data from the printer controller by a time interval “t” in each slice


260


. This time interval “t” is determined by the period of the clock signal input to the delay elements of the digital delay array


254


. Accordingly, power is switched to the enabled heaters synchronously in each time slot having this same duration “t”. In various exemplary embodiments, the exemplary input multiple prepulse waveform has a duration of K*t. That is, the multiple prepulse waveform applied to each slice


260


extends over K time slots. In such a multiple prepulse waveform, the total time required to select all of the N heaters shown in

FIG. 7

is (K+N)*t. In contrast, in a sequential circuit that applies the multiple pre-pulse waveform sequentially and serially to each individual heater element, the total time to select all N heater elements


46


is K*t*N which, for practical values of K and N is greater than (K+N)*t. Therefore, the circuit architecture shown in

FIGS. 7 and 8

is faster than serial sequential circuits, and the shorter cycle time enabled by the improved circuit architecture allows the printhead to fire droplets at higher operating frequencies.




Of course, it would be apparent to one skilled in the art that the speed of an architecture using serial sequential addressing can be improved, for example, by addressing groups or banks of heaters


46


simultaneously. For example, by associating and simultaneously activating groups or banks containing P heater elements each, the total selection time would be reduced to K*t*N/P for the conventional serial-sequential architecture. However, the simultaneous application of power to banks of P heater elements


46


requires switching P times as much current I at a given time. A 320-jet printhead with the circuit architecture as shown in

FIGS. 7 and 8

would require 48 μsec to address all the heaters with a 64-bit pulse train and a 8 MHz clock frequency. In order to achieve the same cycle time with the same pulse train, the serial-sequential circuit would need to address groups or banks containing 53 heaters each.




As is well known in the art, abrupt changes in current can cause voltage spikes in the power supply connection V


SS,


based on the conductance in the circuit. This voltage spike is undesirable, and as well known, can reduce the reliability of the print head circuit architecture. In general, relative to a bank-fired serial-sequential circuit architecture that provides current to P different heater elements


46


, the circuit architecture shown in

FIGS. 7 and 8

will have a switching noise amplitude only 1/P as large. Thus, the print head circuit architecture shown in

FIGS. 7 and 8

significantly reduces the electrical switching noise as the heaters are energized and de-energized relative to conventional circuit designs with the same or similar cycle times.




In general, due to fluidic cross-talk between the capillary channels associated with adjacent slices


260


, it is generally desirable to increase the temporal difference in firing times for physically adjacent slices


260


. The print head circuit architecture shown in

FIGS. 7 and 8

can be designed to allow specific slices


260


to be enabled in a given pass through the printhead. Thus, it is not necessary to address all adjacent slices in the same pass, although if all are not addressed in each pass, multiple passes must be made to address all the slices. Because non-adjacent slices


260


can be energized in a single pass, the distance between the near-simultaneously energized heaters can be increased. This tends to reduce the instantaneous fluid flow at any point in the fluid supply circuit that supplies fluid to the heater elements


46


, and it also tends to reduce the heater current density in the print head circuit leads and other circuit elements in the print head.




The temporal difference between the firing times of physically adjacent slices


260


can be increased by appropriately arranging the digital delay for pulse train


254


in multiple segments and providing the appropriate interconnectections within the printhead. In this way, the physical spacing between simultaneously active slices is controlled. For example, an embodiment of the circuit architecture


250


shown in

FIGS. 7 and 8

operates particularly well when the active slices


260


are physically separated by three inactive slices


260


, so that all the slices


260


in the circuit architecture


250


shown in

FIGS. 7 and 8

can be addressed in four distinct passes or ripples.




In this way, each ripple addresses one-fourth of the total number of slices


260


in the circuit architecture


250


shown in

FIGS. 7 and 8

. Therefore after four passes or ripples, each of the slices


260


will have been addressed and the cycle can begin again. Thus, in various other exemplary embodiments, the circuit architecture


250


shown in

FIG. 7

can have, instead of the single delay line array


254


, a connected pair of digital delay line arrays positioned along the heater array as shown in FIG.


11


.

FIG. 11

shows an architecture in which the digital delay line for pulse train


254


is broken into two half-length sections


254




a


and


254




b,


wherein the pulse train from the controller is fed to the cell at one end of


254




a


and the output from the last cell of


254




a


is fed to the first cell of


254




b.


As was the case in

FIG. 7

, in

FIG. 11

the print data is supplied by the controller to the digital delay line for print data


252




a,


and the print data bits are latched into the print data storage elements


252




b.


A preferred 320-jet, 4-ripple printhead architecture of the current type has a 160-bit digital delay line for print data


252




a,


a 160-bit latch array for the print data


252




b,


two connected 80-bit digital delay lines for pulse train


254




a


&


254




b,


a heater array


258


with 320 heaters, and an AND circuit, a pre-driver and a driver for each heater. The outputs of the delay elements of the digital delay line for the pulse train


254




a


&


254




b


are then connected as inputs to the corresponding elements in the AND array


256


, as are the outputs of the print data storage latch


252




b.


An internally-generated but pre-settable odd/even signal provides a third input to each of the AND gates, while the outputs of the AND gates provide the drive signals to the pre-drivers and drivers


208


.




The preferred architecture″s physically-folded, 160-bit digital delay line for the pulse train


254




a


&


254




b


enables easier interconnects within the printhead″s logic circuitry, and requires only a single injection of the pulse train from the controller to enable addressing of half the ejector channels in the printhead in two ripples. By sequentially scheduling two ripples each of odd-numbered and even-numbered channels, the preferred architecture provides maximally-spaced channel firings within each 4-channel group, and allows easy 50% area-coverage, checkerboard-type printing for fast, ink-conserving draft printing modes.




The preferred 320-jet, 4-ripple printhead architecture of the current type would address all the 320 channels in four ripples in the following manner, in the case where we start with the odd-numbered channels, and at the low-numbered-channels end of the printhead: With the odd-channel data bits loaded into digital delay line for data


252




a


and latched into the print data storage array


252




b,


the pulse train is injected into and through the digital delay line for pulse train


254




a


and


254




b


in synchronism with Clock


1


to address:




Ripple 1: Heaters


1


,


5


,


9


, . . .


317


(the AND gates select the heaters with odd numbers), and




Ripple 2: Heaters


3


,


7


,


11


, . . .


318


(the AND gates select the heaters with odd numbers).




During the addressing of the 160 odd-numbered channels, the even-channel print data are injected into the digital delay line for print data


252




a


in synchronism with Clock


1


, latched into the print data storage latch


252




b,


and then the pulse train is injected into and through the digital delay line for pulse train


254




a


and


254




b


in synchronism with Clock


1


to address:




Ripple 3: Heaters


2


,


6


,


10


, . . .


319


(the AND gates select the heaters with even numbers), and




Ripple 4: Heaters


4


,


8


,


12


, . . .


320


(the AND gates select the heaters with even numbers).




Bi-directional printing is desirable in printers with scanning print heads. The preferred 320-jet, 4-ripple architecture would allow the pulse train to move upward or downward through the digital delay line for pulse train


254




a


&


254




b


by utilizing a bi-directional shift register design and including a data director to present the pulse train to the lower or upper end of the pulse train delay line


254




a


&


254




b.


In order to symmetrically reverse the firing sequence of the preferred architecture, means are provided as well to set the odd/even bit, so that if the odd-numbered channels are fired first in the ripple-up printing direction, the even-numbered jets can be fired first in the ripple-down direction. In a preferred embodiment of the preferred printhead architecture, a print mode latch is provided in the printhead to receive mode bits controlling shift direction and odd or even channels first which are sent by the controller via the print data line prior to the first set of print data. In the preferred embodiment, the odd/even bit is automatically toggled following the completion of each 160-channel addressing sequence. Therefore, in the preferred embodiment, the bits controlling ripple direction and odd/even first need be sent only once per printing swath.




While the invention has been described in relation to preferred embodiments, many modifications and variations are apparent from the description of the invention, and all such modifications and variations are intended to be within the scope of the present invention as defined in the appended claims.



Claims
  • 1. A method of using a thermal ink jet assembly having at least one print head, the print head having a plurality of drop ejectors, each of the plurality of drop ejectors having a heating element actuatable in response to input signals to eject an ink droplet from the print head, the method comprising the steps of:applying a plurality of print signals to the print head, the plurality of print signals corresponding to an image for the ink jet assembly to create; applying at least one pulse signal to the print head; storing the print signal and the at least one pulse signal in multiple connected delay circuit elements prior to sequentially using the at least one pulse signal to activate the heating elements; and sequentially using the at least one pulse signal and the plurality of print signals to activate the heating elements so that a change in a current remains small.
  • 2. The method of claim 1 wherein the change in the current is kept small by increasing or decreasing the number of heating elements activated by no more than one per clock cycle.
  • 3. The method of claim 1, wherein the at least one pulse signal comprises:at least one prepulse that does not fire the drop ejector; and at least one firing pulse that fires the drop ejector.
  • 4. The method of claim 3, wherein the at least one prepulse is determined based on at least one of a temperature of the print head, a type of ink used, a type of printing to be done and at least one physical characteristic of the print head.
  • 5. The method of claim 1, further comprising the step of controlling characteristics of the at least one pulse signal based on a desired volume of the ink droplet to be ejected from the print head.
  • 6. The method of claim 1, wherein at least one of the timing and duration of the at least one pulse signal is selected such that a volume of the ink droplet is substantially constant over a temperature range of at least 20° C.
  • 7. The method of claim 1, wherein the change in current is kept small by increasing or decreasing the number of heating elements activated by no more than one per cycle of the controlling clock.
  • 8. The method of claim 1, wherein the at least one pulse signal simultaneously activates non adjacent heater elements.
  • 9. The method of claim 8, wherein one or more pulse signals activates non adjacent heater elements.
  • 10. The method of claim 1, wherein the at least one pulse signal comprises:a main pulse for firing the drop ejector.
  • 11. A thermal ink jet drop ejector, comprising:a print data storage element that receives print data from a printer controller; a pulse data element that that receives pulse data from either a print head controller or a previous drop ejector; a heating element; and multiple connected delay circuit elements that store the print data and the pulse data prior to sequentially using the print data and pulse data to activate the heating elements.
  • 12. The ejector of claim 11 wherein a change in a current is kept small by the pulse data delay element sending the pulse data to the next drop ejector after a one clock cycle delay.
  • 13. The ejector of claim 11, wherein the pulse data comprises:at least one prepulse that does not fire the drop ejector; and at least one firing pulse that fires the drop ejector.
  • 14. The ejector of claim 13, wherein the at least one prepulse is determined based on at least one of the temperature of the ejector, a type of ink used, a type of printing to be done and a physical characteristic of the ejector.
  • 15. The ejector of claim 11, wherein the pulse data is based on a desired volume of a ink droplet to be ejected from the print head.
  • 16. The ejector of claim 11, wherein at least one of the timing and duration of the at least one pulse signal is selected such that a volume of a ink droplet is substantially constant over a temperature range of at least 20° C.
  • 17. The ejector of claim 11, wherein the combinational elements simultaneously activate non adjacent heater elements.
  • 18. The ejector of claim 11, wherein the pulse data comprises:at least one main pulse that fires the drop ejector.
  • 19. A method of using a thermal ink jet assembly having at least one print head, the print head having a plurality of drop ejectors, each of the plurality of drop ejectors having a heating element actuatable in response to input signals to eject an ink droplet from the print head, the method comprising the steps of:applying a plurality of print signals to the print head, the plurality of print signals corresponding to an image for the ink jet assembly to create; applying at least one pulse signal to the print head according to a pulse and interval signal profile table; storing the print signal and the at least one pulse signal in multiple connected delay circuit elements prior to sequentially using the at least one pulse signal to activate the heating elements; and sequentially using the at least one pulse signal and the plurality of print signals to activate the heating elements so that a drop volume is relatively constant over a range of temperatures.
  • 20. The method of claim 19, wherein the threshold voltage is additionally maintained relatively constant.
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Number Name Date Kind
4463359 Ayata et al. Jul 1984 A
4791435 Smith et al. Dec 1988 A
5519417 Stephany et al. May 1996 A
5917509 Becerra et al. Jun 1999 A
5969730 Inose et al. Oct 1999 A
6375295 Ghozeil et al. Apr 2002 B1
6565177 Corrigan, III May 2003 B1
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Number Date Country
0 496 525 Jul 1992 EP
0 505 154 Sep 1992 EP