In an inkjet printing system, an inkjet printhead prints an image by ejecting drops of a fluid (e.g., printing fluid) through a plurality of fluid nozzles onto a print medium, such as a sheet of paper. In other cases, the printing system ejects another fluid, such as a fluid for additive manufacturing (e.g., three-dimensional (3D) printing) onto a surface. The nozzles may be arranged in arrays or columns such that properly sequenced ejection of fluid from the nozzles causes characters and/or images to be formed on the print medium as the printhead and print medium move relative to each other. Thermal inkjet (TIJ) printheads eject the fluid drops by passing electrical current through a heating element, which serves as an actuator for the nozzle, to generate heat and vaporize a small portion of the fluid within a firing chamber. The rapidly expanding vapor bubble forces a small fluid drop out of the firing chamber. When the heating element cools, the vapor bubble quickly collapses, drawing more fluid from a reservoir into the firing chamber in preparation for ejecting another drop from the nozzle. Other printheads, such as piezo inkjet (PIJ) printheads, eject fluid drops by providing an electrical current to a piezoelectric element behind the nozzle, which ejects fluid from the nozzle.
Regardless of the type of printhead, during printing operations, a flow rate of fluid is controlled or regulated to maintain consistent print quality as well as consistent operation of the printhead. Thus, the inkjet printing system needs to determine the flow rate of fluid through its printhead.
Various examples will be described below referring to the following figures:
In the figures, certain features and components disclosed herein may be shown exaggerated in scale or in somewhat schematic form, and some details of certain elements may not be shown in the interest of clarity and conciseness. In some of the figures, in order to improve clarity and conciseness, a component or an aspect of a component may be omitted.
In the following discussion and in the claims, the terms “including” and “comprising” are used in an open-ended fashion, and thus should be interpreted to mean “including, but not limited to . . . .” Also, the term “couple” or “couples” is intended to be broad enough to encompass both indirect and direct connections. Thus, if a first device couples to a second device, that connection may be through a direct connection or through an indirect connection via other devices, components, and connections.
As explained above, during printing operations, a flow rate of fluid is controlled or regulated to maintain consistent print quality as well as consistent operation of an inkjet printhead, which includes a fluidic die or, in some examples, a fluidic module comprising a plurality of fluidic dies. In some examples, the flow rate of fluid through the printhead is controlled for various reasons. For example, nozzle deprime may occur when the flow rate is too high, which causes a meniscus in the nozzle to be pulled down into the firing chamber, causing air ingestion and thus image quality and reliability issues. As another example, a too-low flow rate may cause the die temperature to increase more than is desired, which increases drop weight variation and/or consequent image quality variation. As another example, a too-low flow rate may lead to the formation of plugs (e.g., “decap”) in the nozzle area of the printhead; as a result, when the actuator is fired, initial drops of fluid are either not delivered (e.g., no fluid is expelled from the actuator) or misdirected toward the print medium. Further, in TIJ architectures, it is common to have some amount of air accumulate in the firing chamber, which is swept out of the chamber by the flow of fluid through the chamber; however, if the flow rate is too low, then the ability to clear air out of the firing chamber is reduced, which can result in degradation of print quality. Still further, spreading of fluid on the nozzle layer (e.g., “puddling”) may occur when a too-low flow rate increases the likelihood of meniscus overshoot from the firing chamber. In such a situation, increasing the flow rate increases the back pressure on the nozzle, which reduces the likelihood of meniscus overshoot, and thus puddling.
In addition to the above, other issues may be caused by irregular or poorly-regulated fluid flow rates. Thus, it is beneficial to determine and control the flow rate of fluid through a printhead. However, using a dedicated flow meter device to determine a flow rate of fluid through a printhead has several drawbacks, including being relatively expensive and bulky, which adds to the cost and packaging constraints of thermal inkjet printers.
Examples of the present disclosure address the foregoing with a fluidic die, for example, a printhead, that includes a thermal sensor (e.g., a thermal sense resistor (TSR)). A processor is coupled to the TSR and receives temperature data from the TSR. The processor determines a flow rate of fluid through the fluidic die based on both the temperature data and an operating parameter for the fluidic die. The operating parameter may include a target warming temperature for the fluidic die, a warming frequency for the fluidic die, or other attributes of the fluidic die during operation. In some cases, the fluidic die includes multiple TSRs and the processor determines the flow rate based on temperature data from a subset of the TSRs. In other examples, the printhead includes a fluidic module, which itself comprises a plurality of fluidic dies. Continuing this example, the processor may determine the flow rate through the fluidic module as a sum of flow rates through the fluidic dies of the module, which are determined as described above.
In some examples, the fluidic die includes a silicon substrate having a membrane region between a back side flow channel and a front side of the substrate. The membrane region facilitates positioning a TSR near the flow of fluid through the substrate. For example, by forming the membrane region in the silicon substrate of the fluidic die, a TSR is able to be positioned on the membrane region in much closer proximity to the flow of fluid through the fluidic die than is possible in arrangements where a membrane region is not present.
In some examples, the disclosed fluidic die includes a TSR disposed on a membrane region of the substrate of the fluidic die. The fluidic die may also include TSRs disposed on the substrate away from the membrane regions. During operation, the processor determines the flow rate of fluid through the fluidic die based on temperature data from a subset of the TSRs, which may include the TSR disposed on the membrane region, which is more closely thermally coupled to the fluid flowing through the fluidic die.
In some examples, the temperature measured on the fluidic die is proportional to the inverse of fluid flow rate through the fluidic die. For example, as fluid flow rate increases through the fluidic die, the temperature of the fluidic die decreases. However, the relationship between a measured temperature (e.g., by a TSR on the fluidic die) and a flow rate of fluid through the fluidic die may be dependent on operating parameters of the fluidic die, such as a target warming temperature for the fluidic die, a warming frequency for the fluidic die, or other attributes of the fluidic die during operation.
The described examples also pertain to establishing a working relationship between measured or sensed temperature (e.g., temperature data from TSRs) and fluid flow rate. In particular, a target warming temperature is established and a level of power is supplied to the fluidic die that is insufficient to reach that target warming temperature (e.g., below a threshold level needed to reach the target warming temperature). This ensures that power is constantly supplied to the fluidic die and also that no fluid is ejected from nozzles of the fluidic die, which simplifies the thermal system being considered (e.g., because no heat is dispelled from the system as fluid is ejected). A target warming temperature is selected that provides a large range of average flow rates and/or average TSR temperatures as a function of warming frequency, for example, relative to the ranges of average flow rates and/or average TSR temperatures as a function of warming frequency available for other target warming temperatures. Subsequently, for the selected target warming temperature, a warming frequency is selected that maximizes a range of corresponding flow rates for a given range of temperatures. Further, while reference is made to an example thermal inkjet printing system, certain examples of the present disclosure may also apply to other fluidic printing technologies, such as piezo inkjet and others.
Fluid supply assembly 104 supplies fluid to printhead assembly 102 and includes a reservoir 120 for storing fluid, such as printing fluid or fluid for additive manufacturing. Fluid flows from reservoir 120 to printhead assembly 102. Fluid supply assembly 104 and printhead assembly 102 can form a one-way fluid delivery system or a recirculating fluid delivery system. In a one-way fluid delivery system, substantially all of the fluid supplied to printhead assembly 102 is consumed during printing. In a recirculating fluid delivery system, however, a portion of the fluid supplied to printhead assembly 102 is consumed during printing. Fluid not consumed during printing is returned to fluid supply assembly 104.
In one example, printhead assembly 102 and fluid supply assembly 104 are housed together in an inkjet cartridge or pen. In another example, fluid supply assembly 104 is separate from printhead assembly 102 and supplies fluid to printhead assembly 102 through an interface connection, such as a supply tube. In either case, reservoir 120 of fluid supply assembly 104 may be removed, replaced, and/or refilled. In one example, where printhead assembly 102 and fluid supply assembly 104 are housed together in an inkjet cartridge, reservoir 120 may include a local reservoir located within the cartridge as well as a larger reservoir located separately from the cartridge. The separate, larger reservoir serves to refill the local reservoir. Accordingly, the separate, larger reservoir and/or the local reservoir may be removed, replaced, and/or refilled.
Mounting assembly 106 positions printhead assembly 102 relative to media transport assembly 108, and media transport assembly 108 positions print medium 118 relative to printhead assembly 102. Thus, a print zone 122 is defined adjacent to nozzles 116 in an area between printhead assembly 102 and print medium 118. In one example, printhead assembly 102 is a scanning type printhead assembly. In a scanning type printhead assembly, mounting assembly 106 includes a carriage for moving printhead assembly 102 relative to media transport assembly 108 to scan print medium 118. In another example, printhead assembly 102 is a non-scanning type printhead assembly. In a non-scanning printhead assembly, mounting assembly 106 fixes printhead assembly 102 at a prescribed position relative to media transport assembly 108. Thus, media transport assembly 108 positions print medium 118 relative to printhead assembly 102.
Electronic controller 110 may include a processor, firmware, and other printer electronics for communicating with and controlling printhead assembly 102, mounting assembly 106, and media transport assembly 108. Electronic controller 110 receives host data 124 from a host system, such as a computer, and includes memory for temporarily storing host data 124. Host data 124 may be sent to fluid ejection system 100 along an electronic, infrared, optical, or other information transfer path. Host data 124 represents, for example, a document and/or file to be printed. Using host data 124, electronic controller 110 controls printhead assembly 102 to eject fluid drops from nozzles 116. Thus, electronic controller 110 defines a pattern of ejected fluid drops which form characters, symbols, and/or other graphics or images on print medium 118. The pattern of ejected fluid drops is determined by the print job commands and/or command parameters from host data 124.
In one example, printhead assembly 102 includes one fluid ejection assembly 114. In another example, printhead assembly 102 is a wide-array or multi-head printhead assembly having multiple fluid ejection assemblies 114. In one wide-array example, printhead assembly 102 includes a carrier that carries fluid ejection assemblies 114, provides electrical communication between fluid ejection assemblies 114 and electronic controller 110, and provides fluidic communication between fluid ejection assemblies 114 and fluid supply assembly 104. In one example, fluid ejection system 100 is a drop-on demand TIJ printing system wherein fluid ejection assembly 114 is a TIJ printhead, such as described further below.
In the example of
During operation, a fluid drop is ejected from a firing chamber 314 through a corresponding nozzle 116 and the firing chamber 314 is then refilled with fluid circulating from flow channel 302 through a fluid feed hole (identified in
In accordance with an example of this disclosure, the membrane regions 204a, 204b are positioned between the flow channel 302 and a front side 303 of the fluidic die substrate 200. The fluid feed holes 316 extend through the membrane regions 204a, 204b and are in fluidic communication with one of the flow channel 302 and the front side 303 of the fluidic die substrate 200. For example, the fluid feed holes 316 permit the flow of fluid from the flow channel 302 into the firing chambers 314, and permit the return of unused fluid from the firing chambers 314 to the flow channel 302. In other examples, there may be more than two membrane regions 204a, 204b, or one membrane region may extend substantially across the flow channel 302 (e.g., the membrane regions 204a and 204b are connected). For example, a single membrane region 204 including fluid feed holes may span the flow channel 302 to provide fluid communication from the flow channel 302 to the front side 303 of the fluidic die substrate 200.
In the absence of the membrane regions 204a, 204b in accordance with some examples of this disclosure, a fluid slot may extend through the fluidic die substrate 200. Such a fluid slot extending through the fluidic die substrate 200 prevents a TSR from being positioned near the flow channel 302 through the fluidic die substrate 200. For example, with the fluid slot extending through the fluidic die substrate 200, it is not possible to locate the TSRs 206a, 206b as shown, proximate to the flow of fluid through the flow channel 302, the fluid feed holes, the firing chambers 314, and out through the nozzles 116. While it would still be possible to locate the TSRs 202a, 202b, 202c as shown, if the fluid slot extends through the fluidic die substrate 200, the TSRs 202a, 202b, 202c are positioned away from the flow of fluid through the flow channel 302, the fluid feed holes, the firing chambers 314, and out through the nozzles 116. As a result, the TSRs 202a, 202b, 202c are relatively distant from the fluid flow, and thus data from those TSRs 202a, 202b, 202c may be at least partially uncorrelated to actual fluid temperature.
Thus, in accordance with examples of this disclosure, the membrane regions 204a, 204b facilitate the location of the TSRs 206a, 206b with greater proximity to the flow of fluid through the flow channel 302, the fluid feed holes, the firing chambers 314, and out through the nozzles 116. As a result, temperature data generated by the TSRs 206a, 206b is more closely coupled or correlated to the temperature of the fluid flowing through the fluid ejection assembly 114, and thus related to the flow of the fluid through the fluid ejection assembly 114 as well.
While
As explained above, the temperature measured on a fluidic die 114 may be inversely proportional to the fluid flow rate through the fluidic die 114. For example, as fluid flow rate increases through the fluidic die 114, the temperature of the fluidic die 114 decreases. However, the relationship between a measured temperature (e.g., by TSRs 202, 206 on the fluidic die 114) and a flow rate of fluid through the fluidic die 114 may be dependent on operating parameters of the fluidic die 114, such as a target warming temperature for the fluidic die 114, a warming frequency for the fluidic die 114, or other attributes of the fluidic die 114 during operation.
Thus, in certain examples, it is beneficial to establish a working relationship between measured or sensed temperature (i.e., temperature data from TSRs 202, 206) and fluid flow rate. In particular, a target warming temperature is established and a level of power is supplied to the fluidic die 114 insufficient to reach that target warming temperature (e.g., below a threshold level needed to reach the target warming temperature). This ensures that power is constantly supplied to the fluidic die 114 and also that no fluid is ejected from nozzles 116 of the fluidic die 114, which simplifies the thermal system being considered (e.g., because no heat is dispelled from the system as fluid is ejected). A target warming temperature is selected that provides high sensitivity of fluid flow rate to changes in measured temperature. Subsequently, for the selected target warming temperature, a warming frequency is selected that maximizes a range of corresponding flow rates for a given range of temperatures.
Turning to
To aid in establishing a relationship between data from the TSRs 202, 206 and fluid flow rates through a fluidic die 114 or a fluidic module 400, a target warming temperature may be selected for which average TSR temperatures and average flow rates demonstrate variability as a function of, for example, warming frequency. For example, a target warming temperature for which average TSR temperatures and average flow rates show little variability as warming frequency changes results in difficulty correlating TSR temperatures with average flow rates, since one or both values remain relatively constant even under varying operating parameters. In situations where average TSR temperatures and average flow rates show little variability as warming frequency varies, it is more difficult to relate measured TSR temperatures to flow rate. For example, when the warming frequency is sufficiently high that the measured TSR temperature reaches the target warming temperature, warming of the fluidic die 114 is turned off. When the warming of the fluidic die 114 is turned off, the fluidic die 114 begins to gradually cool until its temperature falls below a threshold temperature (e.g., 1 degree below the target warming temperature), at which point warming of the fluidic die 114 turns on again. This closed loop process continues for as long as warming is enabled. Under these conditions, the slope of average flow rate as a function of warming frequency (e.g., grams/min/kHz) will be approximately zero, because the warming power supplied to the fluidic die 114 is sufficiently high to reach and maintain the target warming temperature. For the purposes of the examples described herein, where temperature data from the TSRs 202, 206 is correlated to a flow rate through the fluidic die 114, a target warming temperature for which flow rate varies little as a function of warming frequency is not useful in determining the relationship, or correlation, between temperature data from the TSRs 202, 206 and the flow rate through the fluidic die 114.
A graphical example of the foregoing is demonstrated by the graph 500. In the graph 500, at a target warming temperature of 45 C, the range of average flow rates and range of average TSR temperatures as a function of warming frequency are both relatively small (e.g., a range of 20 C and 2 grams/minute over a range of warming frequencies). In particular, at a target warming temperature of 45 C, the average flow rates as a function of warming frequency are nearly constant, only varying by about 2 grams/minute from 72-74 grams/minute at varying warming frequencies. At a target warming temperature of 50 C, the range of average flow rates and the range of average TSR temperatures increase relative to those displayed at the target warming temperature of 45 C. However, at a target warming temperature of 55 C, the range of average flow rates as a function of warming frequency is the largest. Similarly, at the target warming temperature of 55 C, the range of average TSR temperatures as a function of warming frequency is the largest. Thus, in one example, a target warming temperature (e.g., 55 C) is selected that provides the largest range of average flow rate and/or average TSR temperatures across a range of warming frequencies, or as a function of warming frequency. By selecting a target warming temperature for which the average TSR temperatures and average flow rate values demonstrate greater variability as a function of warming frequency, a warming frequency may be selected (as described further below) that provides a relationship between sensed TSR values and flow rates having greater correlation and increased sensitivity (e.g., of sensed TSR values to changes in flow rate).
Turning to
As demonstrated by the graph 600, at a warming frequency of 24 kHz, the range of temperatures that correspond to a range of fluid flow rates from 30-75 grams/minute is relatively small, while the corresponding slope of temperature as a function of flow rate is also relatively small. For example, the temperature of the TSR 206a is nearly constant (e.g., a slope of approximately zero, and thus a correspondingly small range of temperatures that correspond to the range of flow rates) across the fluid flow rate range, while the temperature ranges of the other TSRs for that fluid flow rate range are relatively small. At a warming frequency of 18 kHz, the temperature ranges and slopes of temperature as a function of flow rate of the TSRs increase for the fluid flow rate range of 30-75 grams/minute. However, at a warming frequency of 12 kHz, the temperature ranges and slopes of temperature as a function of flow rate of the TSRs for the fluid flow rate range of 30-75 grams/minute through the fluidic module 400 are the largest. That is, at the warming frequency of 12 kHz, the temperature data from the TSRs is more sensitive to changes in flow rate through the fluidic module 400, which improves the accuracy of determining flow rate based on the temperature data from the TSRs.
Regardless of the particular target warming temperature selected (e.g., as explained above with respect to
As explained above, the fluidic die 114 and its associated TSRs 202, 206 shown in
Turning to
The method 700 continues in block 704 with determining a fluid flow rate for the fluidic die based on the temperature data and an operating parameter for the fluidic die. As explained above, the relationship between a measured temperature (e.g., by TSRs 202, 206 on the fluidic die 114) and a flow rate of fluid through the fluidic die 114 may be dependent on operating parameters of the fluidic die 114, such as a target warming temperature for the fluidic die 114, a warming frequency for the fluidic die 114, or other attributes of the fluidic die 114 during operation. As a result, and as explained above, particular with regard to
Referring back to
As used herein, including in the claims, the word “or” is used in an inclusive manner. For example, “A or B” means any of the following: “A” alone, “B” alone, or both “A” and “B.”
The above discussion is meant to be illustrative of the principles and various examples of the present disclosure. Numerous variations and modifications will become apparent to those skilled in the art once the above disclosure is fully appreciated. It is intended that the following claims be interpreted to embrace all such variations and modifications.
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/US2020/015669 | 1/29/2020 | WO |