In order for a printer to create high-quality images, movement of paper and other types of media through the printer should be precisely measured and controlled. An optical sensor configured to capture images and calculate distances can be used to measure advancement of media in the printer.
The accompanying drawings illustrate various embodiments and are a part of the specification. The illustrated embodiments are merely examples and do not limit the scope of the claims. Throughout the drawings, identical reference numbers designate similar, but not necessarily identical elements.
The same part numbers designate the same or similar parts throughout the figures.
In some printers an optical sensor that measures media advances operates in an environment in which there are significant temperature changes and high temperatures. For example, a printer utilizing latex inks may utilize internal heaters to heat media so as to dry and cure ink on the media. Heating the media can cause the optics of the optical sensor in the printer to deform, resulting in errors in calculated distances. Such distance calculation errors in turn may result in erroneous media advances. The erroneous media advances can lead to gaps, overlaps and banding in printed output and other quality issues.
Embodiments of a method and apparatus to adjust distance calculations were developed in an effort to reduce distance calculation errors attributable to optics deformation in an optical sensor. Embodiments are described with reference to an inkjet printer. The embodiments shown in the accompanying drawings and described below, however, are non-limiting examples. Other embodiments are possible and nothing in the accompanying drawings or in this Detailed Description of Embodiments should be construed to limit the scope of the disclosure, which is defined in the Claims.
An optical sensor 18 is situated beneath an opening in the platen 6, such that there is a line of sight between the optical sensor 18 and a target 22 on the media 4 to be tracked. In an embodiment a physical aspect of the media 4 constitutes the target 22, such that no printed tracking patterns or artificial marks are required to be made on the media 4. Such physical aspects of the media 4 may include small scale (e.g. microscopic) features in the surface of the media 4. The optical sensor 18 is configured to capture a series of digital images of the target 22 at known intervals that can be sent to a controller 20 for calculating a distance that the target 22 advances. The optical sensor 18 according to this exemplary embodiment includes an optical module 24, a window 26 and an image sensor module 28.
In the exemplary embodiment the optical module 24 includes a first portion 16 and a second portion 30, the first portion 16 being closer to a heat source 10 than the second portion 30. Both the first and second portions hold optics 32 to focus images onto an image sensor 34. The optical module 24 also includes an array of light-emitting diodes (LEDs) to provide adjustable and uniform illumination to the target 22. The window 26 is a hardened transparent surface that allows the LEDs' light to reach the target 22, and allows reflected light to reenter the optical sensor 18. The hardened transparent surface may be in contact with the side of the media 4 that is opposite of the media side that faces the printhead 8. The image sensor module 28 holds an image sensor 34, and electronics that control the operation of the optics 32, the LEDs and the image sensor 34. The image sensor 34 is configured for high-speed digital imaging and fast data transfer. In an embodiment a second temperature sensor 36 is embedded in the image sensor module 28, to take temperature measurements of the second portion 30 of the optical sensor 18. In the exemplary embodiment illustrated in
In the exemplary embodiment, the optical sensor 18 electronically connects to the controller 20. The controller 20 is configured to compensate for non-uniform optics deformation by adjusting distance calculations regarding the distance the target 22 travels by a compensation factor that is a function of temperatures measured by the first and second temperature sensors at the time of the distance calculation. The controller 20 in turn utilizes the adjusted distance calculations to precisely control the printer's media advance mechanism 2. As used in this specification and the appended claims, “controller” suggests a processor 38 and a memory 40. The processor 38 may represent multiple processors, and the memory 40 may represent multiple memories. In an embodiment, the controller may include a number of software components that are stored in a computer-readable medium, such as memory, and are executable by processor. In this respect, the term “executable” means a program file that is in a form that can be directly (e.g. machine code) or indirectly (e.g. source code that is to be compiled) performed by the processor. An executable program may be stored in any portion or component of memory.
In the preceding paragraphs embodiments are described with reference to an inkjet printer. Other embodiments are possible. In an embodiment the apparatus may be incorporated in a laser printer or any other printer. In an embodiment, the apparatus may be incorporated in a sheet-fed scanning device having a media advance mechanism. In an embodiment, the apparatus may be incorporated in a flatbed scanning device having a mechanism for advancing a scan head. In an embodiment the apparatus may be incorporated in a microscope having a mechanism for advancing a slide or an object to be viewed or measured. In an embodiment the apparatus may be incorporated in a precision microelectronic assembly machine having a mechanism for advancing an assembly or components to be placed, assembled or measured.
The exemplary embodiment depicted in
In the exemplary embodiment a second controller 44 electronically connects to the first controller 42, to the first temperature sensor 12 and to the media advance mechanism 2. The second controller 44 is configured to receive a distance calculation regarding the distance the target 22 travels, and temperature measurements of the second portion 30 of the optical sensor 18, from the first controller 42. The second controller 44 is also configured to receive temperature measurements of the first portion 16 of the optical sensor 18 from the first temperature sensor 12. The second controller 44 is configured to compensate for non-uniform optics deformation by adjusting the distance calculation by a compensation factor that is a function of temperatures measured by the first and second temperature sensors at the time of the distance calculation. The second controller 44 is additionally configured to in turn utilize the adjusted distance calculations to precisely control the printer's media advance mechanism 2.
In an embodiment, the first temperature sensor could be external to the optical sensor 18, for example coupled to a platen 6, to take temperature measurements of a first portion 16 of the optical sensor 18. In an embodiment, the first temperature sensor could be coupled to, or embedded in, the optical sensor 18. In an embodiment, the second temperature sensor 36 could be coupled to, or embedded in, or external to the optical sensor 18.
Determining a thermal state may include a comparison of rates of temperature change within the first and second portions. In an example, temperature readings of the first portion 46 and the second portion 48 of an optical sensor may be analyzed to determine that the optical sensor is in one of the following thermal states: a start-up state 50, a first transient state 52, a steady state 54, a cool-down state 56 and a second transient state 58.
In an embodiment, the start-up state 50 is a state in which the temperatures of the both the first and second portions are lowest and closest to ambient temperature in comparison to the other states, suggesting a device incorporating the optical sensor has just been turned on. In an embodiment, the first transient state 52 is a state following start-up in which the temperatures of the both the first and second portions are increasing, the temperature of the first portion 46 is greater than that of the second portion 48, and the temperature of the first portion 46 is increasing more rapidly than that of the second portion 48. In an embodiment, the steady state 54 is a state in which the temperatures of both the first and second portions are increasing, the temperature of the first portion 46 is greater than that of the second portion 48, and the temperatures of the first and second portions are increasing at approximately the same rate. In an embodiment, the cool-down state 56 is a state in which the temperatures of both the first and second portions are decreasing, suggesting that a device incorporating the optical sensor is in a standby mode in which no heat is being applied and a distance is not being calculated. In an example the temperatures reach a floor of approximately thirty-seven degrees C. during the cool-down state 56. In an embodiment, the second transient 58 is like the first transient state 52 except that it follows a cool-down state 56 rather than start-up, and therefore the difference in the rates of change as between the first and second portions is not as large as in the first transient state 52.
In an embodiment, knowledge of the previous thermal state may be helpful in identifying a current thermal state. For example, when determining whether an optical sensor is in a first transient or a second transient state 58, it may be helpful to have the knowledge that the previous state was a start-up state. In this example, such knowledge of the previous state may help lead to a conclusion that increasing temperature measurements in the first and second portions indicate a first transient state 52.
In an embodiment, a printer's controller may be configured to consider thermal states in applying a compensation factor to adjust distance calculations. In the exemplary embodiment such a controller might utilize a first transient state 52, a steady state 54, and a second transient state 58 to generalize temperature characteristics of the optical sensor at different times as these are states in which printing processes may take place. In this embodiment the controller may not utilize the start-up and cool-down thermal states in applying a compensation factor, as the start-up and cool-down states suggest that the printer that incorporates the optical sensor is in a standby mode.
Starting with
Continuing with the flow diagram of
Continuing with the flow diagram of
The compensation factor should take into account that deformation of the optics may be not be uniform, and that the deformation can be predicted in light of the first and second temperature measurements. At least two phenomena may change magnification in an optical system: non-uniform thermal expansion of distances along the optical axis, and the lenses changing their refractive index or curvature by temperature. While the type and degree of such optics deformation may vary depending upon the thermal state that the optical sensor is in, it is possible to utilize an approximation that does not consider multiple thermal states to simplify implementation. In one example, a linear compensation factor (CF) may be used CF=A·(Tu−ε·Tb)+B. where Tu is the temperature in first portion of optical sensor, Tb is the temperature in second portion of optical sensor, and A, B and ε are constants for stateless approximation.
Moving on to
Continuing with
Continuing with the flow diagram of
In one example, a compensation factor for a first transient state is developed:
is time derivative, Tu is the temperature in first portion of optical sensor, Tb is the temperature in second portion of optical sensor, and K1, and D1 are constants. Such a compensation factor considers that optics magnification in this first transition state is changing mainly due to different expansions in the first portion and the second portion. Such a compensation factor also considers that the biggest magnification change occur at the beginning of this thermal state, when Tu-Tb changes most rapidly.
In one example, a compensation factor for a steady state is developed: CFSS(Tu,Tb)=Ks·Tu+Ds, where Tu is the temperature in first portion of optical sensor, Tb is the temperature in second part of optical sensor, and Ks, and Ds are constants. Such a compensation factor considers that while the optics' focal distances may not change significantly in the steady state, the optics lenses' refractive index and curvature may still be changing, at a rate proportional to that of temperatures Tb or Tu.
In one example, a compensation factor for a second transient state, after a device's operation is stopped and resumed, is developed
is time derivative, Tu is the temperature in first portion of optical sensor, Tb is the temperature in second portion of optical sensor, and K2, and D2 are constants. Such a compensation factor is similar to the compensation factor for the first transient state, but the second transient state starts at higher temperatures than the first transient state, and with Tb very close to Tu throughout as compared to the first transient state.
Although the flow diagrams of
The preceding description has been presented only to illustrate and describe embodiments and examples of the principles described. This description is not intended to be exhaustive or to limit these principles to any precise form disclosed. Many modifications and variations are possible in light of the above teaching.
Number | Name | Date | Kind |
---|---|---|---|
6657650 | Omelchenko et al. | Dec 2003 | B1 |
6863363 | Yabuta | Mar 2005 | B2 |
7055929 | Yabuta | Jun 2006 | B2 |
7391525 | Chapman et al. | Jun 2008 | B2 |
7556333 | Mitsuzawa | Jul 2009 | B2 |
20080253782 | Honguh | Oct 2008 | A1 |
20090009751 | Taniguchi | Jan 2009 | A1 |
Number | Date | Country | |
---|---|---|---|
20110074855 A1 | Mar 2011 | US |