Reference is made to commonly-assigned, U.S. patent application Ser. No. 12/333,340, entitled “PRESSURE MODULATION CLEANING OF JETTING MODULE NOZZLES”, filed concurrently herewith.
This invention relates generally to the field of digitally controlled printing devices, and in particular to techniques for cleaning individual nozzles of a jetting module.
Debris, for example, dust or dirt, when present in or around nozzles of a printhead can cause ink drops ejected from the nozzle to be misdirected or have inconsistencies in drop size or drop shape which may result in reduced print quality. Various techniques for removing debris located in or around the nozzles of a printhead are known and include, for example, utilizing a cleaning fluid and/or a mechanical cleaning assembly to clean the nozzles of the printhead.
According to one aspect of the present invention, a liquid ejection device includes a jetting module including an array of nozzles, a thermal stimulation device associated with each nozzle of the array of nozzles, and a controller in electrical communication with each thermal stimulation device. The controller is configured to provide a first activation waveform to each thermal stimulation device and to provide a second activation waveform to each thermal stimulation device to clean the associated nozzle with liquid emitted from the associated nozzle. The second activation waveform has a higher activation component when compared to the first activation waveform.
According to another aspect of the invention, a method of cleaning a liquid ejection device includes providing a jetting module including an array of nozzles; providing a thermal stimulation device associated with each nozzle of the array of nozzles; using a controller in electrical communication with each thermal stimulation device to provide a first activation waveform to each thermal stimulation device; and using the controller to provide a second activation waveform to each thermal stimulation device to clean the associated nozzle with liquid emitted from the associated nozzle, the second activation waveform having a higher activation component when compared to the first activation waveform.
In the detailed description of the preferred embodiments of the invention presented below, reference is made to the accompanying drawings, in which:
The present description will be directed in particular to elements forming part of, or cooperating more directly with, apparatus in accordance with the present invention. It is to be understood that elements not specifically shown or described may take various forms well known to those skilled in the art. In the following description and drawings, identical reference numerals have been used, where possible, to designate identical elements.
The example embodiments of the present invention are illustrated schematically and not to scale for the sake of clarity. One of the ordinary skills in the art will be able to readily determine the specific size and interconnections of the elements of the example embodiments of the present invention.
As described herein, the example embodiments of the present invention provide a printhead and/or printhead components typically used in inkjet printing systems. However, many other applications are emerging which use inkjet printheads to emit liquids (other than inks) that need to be finely metered and deposited with high spatial precision. As such, as described herein, the terms “liquid” and/or “ink” refer to any material that can be ejected by the printhead and/or printhead components described below.
Referring to
Recording medium 32 is moved relative to printhead 30 by a recording medium transport system 34, which is electronically controlled by a recording medium transport control system 36, and which in turn is controlled by a micro-controller 38. The recording medium transport system shown in
Ink is contained in an ink reservoir 40 under pressure. In the non-printing state, continuous ink jet drop streams are unable to reach recording medium 32 due to an ink catcher 42 that blocks the stream and which may allow a portion of the ink to be recycled by an ink recycling unit 44. The ink recycling unit reconditions the ink and feeds it back to reservoir 40. Such ink recycling units are well known in the art. The ink pressure suitable for optimal operation will depend on a number of factors, including geometry and thermal properties of the nozzles and thermal properties of the ink. A constant ink pressure can be achieved by applying pressure to ink reservoir 40 under the control of ink pressure regulator 46. As shown in
The ink is distributed to printhead 30 through an ink channel 47. The ink preferably flows through slots and/or holes etched through a silicon substrate of printhead 30 to its front surface, where a plurality of nozzles and drop forming mechanisms, for example, heaters, are situated. When printhead 30 is fabricated from silicon, drop forming mechanism control circuits 26 can be integrated with the printhead. Printhead 30 also includes a deflection mechanism (not shown in
Referring to
Liquid, for example, ink, is emitted under pressure through each nozzle 50 of the array to form filaments of liquid 52. In
Jetting module 48 is operable to form liquid drops having a first size or volume and liquid drops having a second size or volume through each nozzle. To accomplish this, jetting module 48 includes a drop stimulation or drop forming device 28, for example, a heater or a piezoelectric actuator, that, when selectively activated, perturbs each filament of liquid 52, for example, ink, to induce portions of each filament to breakoff from the filament and coalesce to form drops 54, 56.
In
Typically, one drop forming device 28 is associated with each nozzle 50 of the nozzle array. However, a drop forming device 28 can be associated with groups of nozzles 50 or all of nozzles 50 of the nozzle array.
When printhead 30 is in operation, drops 54, 56 are typically created in a plurality of sizes or volumes, for example, in the form of large drops 56, a first size or volume, and small drops 54, a second size or volume. The ratio of the mass of the large drops 56 to the mass of the small drops 54 is typically approximately an integer between 2 and 10. A drop stream 58 including drops 54, 56 follows a drop path or trajectory 57.
Printhead 30 also includes a gas flow deflection mechanism 60 that directs a flow of gas 62, for example, air, past a portion of the drop trajectory 57. This portion of the drop trajectory is called the deflection zone 64. As the flow of gas 62 interacts with drops 54, 56 in deflection zone 64 it alters the drop trajectories. As the drop trajectories pass out of the deflection zone 64 they are traveling at an angle, called a deflection angle, relative to the undeflected drop trajectory 57.
Small drops 54 are more affected by the flow of gas than are large drops 56 so that the small drop trajectory 66 diverges from the large drop trajectory 68. That is, the deflection angle for small drops 54 is larger than for large drops 56. The flow of gas 62 provides sufficient drop deflection and therefore sufficient divergence of the small and large drop trajectories so that catcher 42 (shown in
When catcher 42 is positioned to intercept large drop trajectory 68, small drops 54 are deflected sufficiently to avoid contact with catcher 42 and strike the print media. As the small drops are printed, this is called small drop print mode. When catcher 42 is positioned to intercept small drop trajectory 66, large drops 56 are the drops that print. This is referred to as large drop print mode.
Referring to
Drop stimulation or drop forming device 28 (shown in
Positive pressure gas flow structure 61 of gas flow deflection mechanism 60 is located on a first side of drop trajectory 57. Positive pressure gas flow structure 61 includes first gas flow duct 72 that includes a lower wall 74 and an upper wall 76. Gas flow duct 72 directs gas flow 62 supplied from a positive pressure source 92 at downward angle θ of approximately a 45° relative to liquid filament 52 toward drop deflection zone 64 (also shown in
Upper wall 76 of gas flow duct 72 does not need to extend to drop deflection zone 64 (as shown in
Negative pressure gas flow structure 63 of gas flow deflection mechanism 60 is located on a second side of drop trajectory 57. Negative pressure gas flow structure includes a second gas flow duct 78 located between catcher 42 and an upper wall 82 that exhausts gas flow from deflection zone 64. Second duct 78 is connected to a negative pressure source 94 that is used to help remove gas flowing through second duct 78. An optional seal(s) 84 provides an air seal between jetting module 48 and upper wall 82.
As shown in
Gas supplied by first gas flow duct 72 is directed into the drop deflection zone 64, where it causes large drops 56 to follow large drop trajectory 68 and small drops 54 to follow small drop trajectory 66. As shown in
Alternatively, deflection can be accomplished by applying heat asymmetrically to filament of liquid 52 using an asymmetric heater 51. When used in this capacity, asymmetric heater 51 typically operates as the drop forming mechanism in addition to the deflection mechanism. This type of drop formation and deflection is known having been described in, for example, U.S. Pat. No. 6,079,821, issued to Chwalek et al., on Jun. 27, 2000.
As shown in
Referring to
Referring to
Controller 26 is also configured to provide a second activation waveform 102 to each thermal stimulation device, for example, heater 51. The second activation waveform 102 functions to clean the nozzle associated with each thermal stimulation device, or heater, with the liquid emitted through the nozzle. When the second activation waveform form is used for cleaning, the set of pulses has a larger activation component than is employed for drop formation. Additionally, the second activation waveform can be sized to cause stream deflection when applied to one of the two heater sections of heater 51 when heater 51 is an asymmetric heater. The controller 26 can be configured to provide the second activation waveform 102 to individual thermal stimulation devices, for example, to a thermal stimulation device associated with a nozzle that has been identified as not functioning properly. Example embodiments of the second activation waveform 102 are described below with reference to
The second activation waveform 102 used for cleaning has at least one activation component (frequency, amplitude, duty cycle, etc.) that is higher than the corresponding activation component of the first activation waveform used while printing. As used herein, the term activation component is defined to be at least one of a frequency, an amplitude, a duty cycle (ratio of pulse width to period) of the activation waveform, and a steady state voltage level. The steady state voltage level includes, for example, DC offset with activation pulses (as shown in
Referring to
Referring to
Referring to
Referring to
In the example embodiments described above, each set of activation pulses comprised an increase in a single activation component which increased average heater power. It should be recognized that increases to more than one activation component can be incorporated into the set of activation pulses for cleaning. For example, the second activation waveform can comprise an increased pulse frequency and increased pulse amplitude. In other words, multiple activation components can be increased, when compared to the activation components used for a normal printing state, to help improve printhead nozzle cleaning.
Providing the non-printing second activation waveform 102 to the electrical heaters can be useful when removing debris lodged in or near a nozzle. The agitation created by second activation waveform 102 at the location of the debris can dislodge the debris and help to straighten a crooked or otherwise improperly functioning jet.
One advantage of the cleaning technique described above is that the fluid does not need to be turned off during the cleaning cycle. When compared to other cleaning techniques that involve stopping the flow of fluid from the nozzles and then restarting the flow and reestablishing the liquid jets require a significant amount of time, the cleaning technique of the present invention that uses a second activation waveform having an increased activation components can reduce cleaning cycle time. Other advantages of the cleaning technique of the present invention include avoiding the mechanical wear associated with wiping techniques and reducing the ineffectiveness associated with techniques that oscillate or eject cleaning fluids throughout the nozzles themselves without increasing the temperature of the fluid and/or the temperature of the area around the nozzle.
While this cleaning technique can be used when ink is being jetted from the nozzles, it can also be used when other liquids are being jetted from the nozzles, for example, a cleaning fluid having a lower boiling point than the ink normally emitted from the nozzles. These types of cleaning fluids should be resistant to producing coagulation on the nozzle. Furthermore, when specially designed, this type of fluid can amplify the effects of agitating the debris and therefore provide an increased ability to remove debris.
Additionally, the cleaning effectiveness of the second activation waveform can be enhanced by the use of an additional heater internal to the drop generator or in the fluid lines supplying ink to the drop generator to heat the fluid before it reaches the nozzles. Preheating the fluid in this manner can further allow the fluid to agitate, shrink and remove debris from the inside of the orifice base and the area surrounding the ink channel.
As the cleaning technique of the present invention supplies activation pulses to the thermal stimulation device associated with the individual nozzles, the cleaning technique of the present invention can be employed on a nozzle by nozzle basis. For example, the controller 26 can provide the second activation waveform to only the thermal stimulation device associated with a nozzle identified as not functioning properly. Nozzles not functioning properly can include clogged nozzles, partially obstructed nozzles, nozzles producing crooked jets, and nozzles with debris located around the bore. Identification of the improperly functioning nozzle(s) can be achieved using cameras, examination of print samples, or any other method known in the art. Alternatively, the second activation waveform can be applied to one or more thermal stimulation devices on a pre-determined time schedule or upon direction by the user as part of a precautionary or regularly scheduled maintenance or cleaning. Furthermore, in printheads with nozzles having asymmetric heaters, the second activation waveform can be selectively applied only one of the heater segments or a second activation waveform can be applied to one of the heater segments for a period of time followed by applying a second activation waveform to another heater segment associated with the nozzle.
In the example embodiments shown in
In the embodiments described above, the second activation waveform 102 used for cleaning is different from the first activation waveform 100 used for printing. This can cause drop formation that occurs during cleaning to be different from drop formation that occurs during printing. These changes in drop formation can cause the deflection of the drops to be affected. For example, in the embodiment in which the frequency of activation pulses is increased, drops can be produced that are smaller than the drops produced while printing. As smaller drops are more easily deflected by a gas flow drop deflection, these drops can be deflected sufficiently to enter a gas flow duct which can lead to premature printhead failure. To reduce this risk, it is desirable to deactivate or adjust the operation of the drop deflection mechanism while using the second activation waveform for nozzle cleaning in order to reduce the likelihood of excessive drop deflection.
When the frequency of activation pulse is high enough that the activation pulses don't induce drop breakoff, then the liquid stream tends to breakup into drops of random size and the breakoff typically occur at a distance that is farther away from the nozzles (when compared to the distance that breakoff typically occurs during printing). This can result in drops that are not being deflected enough to strike the catcher which can lead to print defects and reduced image quality. To reduce this risk, when using the second activation waveform for cleaning the nozzles, it is desirable to employ a conventional eyelid that seals against the bottom of the catcher and diverts the drops into the fluid return channel of the catcher. Examples of eyelids that are suitable for sealing with the catcher include, but are not limited to, those described in U.S. Pat. No. 4,928,115; U.S. Pat. No. 5,475,410; and U.S. Pat. No. 6,247,781.
The invention has been described in detail with particular reference to certain preferred embodiments thereof, but it will be understood that variations and modifications can be effected within the scope of the invention.
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Number | Date | Country | |
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