The present invention relates to a discharge apparatus.
An inkjet printing apparatus prints an image by discharging ink droplets which are an example of droplets. However, as the inkjet printing apparatus is continuously used, the ink droplet discharge speed can sometimes change due to individual differences of the printing apparatuses and printheads, the physical properties of the ink, and the state of use of the printing apparatus or the environmental influence on the printing apparatus. If the ink droplet discharge speed changes, when an image is to be printed by reciprocally scanning the printhead, the relationship between the ink droplet landing positions of ink droplets discharged in a forward scan direction and the ink droplet landing positions of ink droplets discharged in a backward scan direction will shift. As a result, the image quality will be affected.
Japanese Patent Laid-Open No. 2007-152853 discloses a registration adjustment method in which a printhead includes an optical detector for measuring the discharge speed of the ink to be discharged, and a discharge timing is appropriately set according to the movement speed of the printhead and the ink discharge speed based on the measurement result. In addition, Japanese Patent Laid-Open No. 2007-152853 also discloses, as an ink discharge speed measurement method, a method in which the time it takes for discharged ink to reach a light beam emitted by the optical detector is measured and a discharge speed is calculated based on the measurement result and the distance from the printhead to the light beam.
According to one embodiment of the present invention, there is provided a discharge apparatus comprising: a discharge head that includes an orifice surface in which orifices each configured to discharge a droplet are arrayed in a predetermined direction; a detecting unit that includes a light emitting element configured to emit light and a light receiving element configured to receive light emitted from the light emitting element, and configured to optically detect a droplet discharged from the orifice in a state in which the orifice surface of the discharge head is present between the light emitting element and the light receiving element in a predetermined direction; and a suppression unit that is arranged between the light emitting element and the orifice surface, and configured to suppress light emitted from the light emitting element from reaching the orifice surface by shielding at least some rays of light which is emitted from the light emitting element and propagates to the orifice surface.
Further features of the present invention will become apparent from the following description of exemplary embodiments (with reference to the attached drawings).
When ink discharged by a printhead is to be detected, some of the rays of light emitted from a light emitting element may be reflected by the printhead and enter into a light receiving element. If the rays of light reflected by the printhead enter into the light receiving element, the measurement accuracy may degrade when time it takes for the ink discharged from the printhead to reach a light beam emitted by an optical detector is measured. If the measurement accuracy degrades, it may influence the accuracy of specifying an ink droplet discharge speed which is obtained based on the time it takes for the ink to reach the light beam.
Embodiments of the present invention provide a technique that improves the accuracy of specifying a droplet discharge speed.
Hereinafter, embodiments will be described in detail with reference to the attached drawings. Note, the following embodiments are not intended to limit the scope of the claimed invention. Multiple features are described in the embodiments, but limitation is not made to an invention that requires all such features, and multiple such features may be combined as appropriate. Furthermore, in the attached drawings, the same reference numerals are given to the same or similar configurations, and redundant description thereof is omitted.
Note that in this specification, the term “printing” (to be also referred to as “print” hereinafter) not only includes the formation of significant information such as characters and graphics, regardless of whether they are significant or insignificant. Furthermore, it broadly includes the formation of images, figures, patterns, and the like on a print medium, or the processing of the medium, regardless of whether they are so visualized as to be visually perceivable by humans.
In addition, the term “print medium” not only includes a paper sheet used in common printing apparatuses, but also broadly includes materials, such as cloth, a plastic film, a metal plate, glass, ceramics, wood, and leather, capable of accepting ink.
Furthermore, the term “ink” (to also be referred to as a “liquid” hereinafter) should be extensively interpreted similarly to the definition of “printing (print)” described above. That is, “ink” includes a liquid which, when applied onto a print medium, can form images, figures, patterns, and the like, can process the print medium, or can process ink (for example, solidify or insolubilize a coloring material contained in ink applied to the print medium).
Further, a “nozzle” generically means an orifice or a liquid channel communicating with it, and an element for generating energy used to discharge ink, unless otherwise specified.
<Overall Outline of Printing Apparatus>
The printing apparatus 100 shown in
The printhead 201 discharges ink to print an image on the print medium 203. The printhead 201 includes an orifice surface 201a (
The printhead 201 also includes a distance detecting sensor 204 for detecting the distance between the printhead 201 and the print medium 203 on the platen 212. The distance detecting sensor 204 includes a light emitting unit 702 (
A droplet detecting unit 205 is a sensor for detecting droplets, that is, ink droplets in this case, discharged from the printhead. The droplet detecting unit 205 is an optical sensor that includes a light emitting element 401 (
A main rail 206 supports the carriage 202. The carriage 202 performs reciprocal scanning along the main rail 206 in the X direction (a direction perpendicular to the conveyance direction of the print medium). The scanning by the carriage 202 is performed by driving a carriage motor 208 via a carriage conveyance belt 207. A linear scale 209 is arranged in the scanning direction, and an encoder sensor 210 mounted in the carriage 202 obtains position information by detecting the linear scale 209. In addition, the printing apparatus 100 includes a lift cam (not shown) for changing, in a stepwise manner, the height of the main rail 206 that supports the carriage 202, and a lift motor 211 that drives this lift cam. By driving the lift cam by the lift motor 211, it will be possible to make the printhead 201 move up and down as well as increase/decrease the distance between the printhead 201 and the print medium 203. The printing apparatus 100 according to this embodiment can change the height of the printhead to multiple levels with a predetermined accuracy based on the stop position of the lift cam. Since the amount of change of this height is driven relatively with respect to the height of a predetermined level, a distance corresponding to the change between the levels can be set accurately.
Image data transmitted from a host apparatus 1 is converted into a discharge signal by the CPU 301, and printing is performed by discharging the ink from the printhead 201 to a print medium 203 in accordance with the discharge signal. The CPU 301 is formed by including a I/O control unit and driver unit 306 (to be referred to as the driver unit 306 hereinafter), a sequence control unit 307, an image processing unit 308, a timing control unit 309, and a head control unit 310. The sequence control unit 307 controls the general printing control operations and controls, more specifically, the activation and suspension of the image processing unit 308, the timing control unit 309, and the head control unit 310 as the respective functional blocks, controls the conveyance of a print medium, controls the scanning of the carriage 202, and the like. The control of the functional blocks is executed by causing the sequence control unit 307 to read out various kinds of programs from the memory 303 and execute the programs. The driver unit 306 generates, based on an instruction from the sequence control unit 307, control signals to the sensor/motor control unit 302, the memory 303, the head control circuit 305, and the like, and transmits input signals from the blocks to the sequence control unit 307.
The image processing unit 308 performs image processing by performing color separation/conversion on the image data input from the host apparatus 1 to convert the data into print data that is printable by the printhead 201. The timing control unit 309 transfers, in synchronization with the position of the carriage 202, the print data converted/generated by the image processing unit 308 to the head control unit 310. The timing control unit 309 also controls the ink discharge timing based on the print data. The timing control unit 309 controls this timing in accordance with the discharge timing that is determined based on a discharge speed calculated by discharge speed calculation processing which is to be described later. The head control unit 310 functions as a discharge signal generation unit by converting the print data input from the timing control unit 309 into a discharge signal and outputting the discharge signal. In addition, the head control unit 310 controls the temperature of the printhead 201 by outputting, based on an instruction from the sequence control unit 307, a control signal which will not cause the ink to be discharged. The head control circuit 305 functions as a driving pulse generation unit, and generates a driving pulse in accordance with the discharge signal input from the head control unit 310 and applies the driving pulse to the printhead 201.
The discharge timing adjustment will be described next with reference to
Xa=(H/Va)×Vcr (1)
Furthermore, a distance Xb, in the X direction, from an ink droplet discharge position to an ink droplet landing position on the print medium 203 during a scanning operation in the backward direction is calculated as follows.
By using the above equations, an appropriate discharge timing with respect to a position in the X direction of the printhead 201 detected by the encoder sensor 210 can be obtained. In this embodiment, the default discharge speed Va and the discharge timing with respect to the default discharge speed Va are stored in advance in the memory 303. An adjustment value of the discharge timing with respect to this default discharge speed Va is set as 0, and the adjustment value is adjusted between −4 to +4 in accordance with the discharge speed. The adjustment is performed at 1,200 dpi. A table in which the adjustment values of the discharge timing and the discharge speeds have been associated with each other is stored in advance in the memory 303. Subsequently, an adjustment value of the discharge timing corresponding to the speed obtained by the discharge speed calculation processing of
In addition,
Xa′=(H/Va′)×Vcr (3)
If it is assumed that the discharge speed Va′ of the ink droplet until the ink droplet discharged from the printhead 201 lands on the print medium 203 has attenuated by 10% from the discharge speed Va, the distance from the discharge position to the landing position in the X direction can be obtained as follows.
As described above, when the discharge speed decreases, the landing position will shift in the scanning direction of the printhead 201. In this manner, even in a case in which the landing position has already shifted, an appropriate discharge timing adjustment value can be obtained based on the discharge speed, in a manner similar to
The method of calculating the discharge speed of ink droplets to be discharged from the printhead 201 according to this embodiment will be described next with reference to
As shown in
When the detection time T1 and the detection time T2 have been detected in the states of
V1=(H2−H1)/(T2−T1) (5)
After the discharge speed V1 has been calculated, the sensor/motor control unit 302 will drive the lift motor 211 to further increase the distance, in the height direction, between the orifice surface 201a and the light 404 from the distance H2 to a distance H3. This state is shown in
V2=(H3−H2)/(T3−T2) (6)
After the calculation of the discharge speed V2, the sensor/motor control unit 302 will further drive the lift motor 211 to further increase the distance, in the height direction, between the orifice surface 201a and the light 404 from the distance H3 to a distance H4. This state is shown in
V3=(H4−H3)/(T4−T3) (7)
As described above, the distance between the printhead 201 and the droplet detecting unit 205 is changed, and the detection time at each distance is detected to calculate a discharge speed V (the discharge speeds V1 to V3 in the example described above) of an ink droplet. Although the detection time is detected sequentially from a shorter distance in the above described example, the detection order is not limited to this. For example, the detection time may be detected sequentially from a longer distance. Note that in this embodiment, the separation distance H is a distance between 1.2 mm to 2.2 mm.
In addition, the discharge speed may be calculated by measuring the detection time at many more distances with respect to the distance between the printhead 201 and the droplet detecting unit 205. Since a discharge speed that corresponds to many distances can be calculated, it will be possible to obtain the attenuation influence of the discharge speed (whether the discharge remains constant or changes depending on the distance). As a result, it will be possible to obtain the discharge speed and the attenuation influence of the ink droplet more accurately.
In the graph shown in
In the graph shown in
In addition, depending on the individual differences of the printheads, the differences of the physical properties of the respective ink colors, and the state of use and the environmental influence on the printing apparatus, data that changes linearly may be obtained.
In addition, even in a case in which the discharge speed changes nonlinearly, the calculation of the approximation curve need not be performed if printing is to be performed only when the distance between the orifice surface 201a and the print medium 203 is constant. In such a case, the detection times at two distances that include the distance to be used during printing can be detected.
First, in step S601, the sequence control unit 307 drives the lift motor 211 to separate the printhead 201 and the droplet detecting unit 205 from each other by predetermined distances. The separation distances are set in advance in the memory 303 and are the distances H1 to H4 described in
Next, the process advances to step S602, and preprocessing necessary for detecting the discharge speed is executed. More specifically, presetting of discharge control suitable for detecting the discharge speed, a preliminary discharge operation for stable discharge of ink droplets, a suction fan stopping operation to stabilize air current control in the printing apparatus, and the like can be performed as preprocessing.
Next, the process advances to step S603, and a discharge operation for discharging an inspection ink droplet from the printhead 201 to the light 404 emitted by the light emitting element 401 of the droplet detecting unit 205 is performed. More specifically, the detection time, which is a period from when the printhead 201 starts to discharge an ink droplet from a predetermined nozzle to when the light receiving element 402 of the droplet detecting unit 205 has detected that the ink droplet has passed the light 404, is detected with respect to the separation distance set in step S601. A plurality of detection times will be detected in regards to the detection time by using a plurality of nozzles of the printhead 201. In order to accurately detect the discharge speed, it is desirable to select, as target nozzles to be used for detection time measurement, a wide range of nozzles including those at both ends and the center.
Next, the process advances to step S604, and data processing of the detection times obtained in step S603 is executed to calculate the detection time with respect to the set separation distance of step S601. More specifically, to stabilize the detection time measurement, data processing operations such as performing averaging based on a necessary obtained sample number, deleting data outside the upper and lower limits of the error range to prevent mixing of abnormal values in the data, and the like are executed.
Next, the process advances to step S605, and whether the detection time has been detected for all of the separation distances set in the memory 303 is determined. In this embodiment, this is determined by determining whether the current distance between the orifice surface 201a and the light 404 of the droplet detecting unit 205 is the distance H4 which is the final separation distance. If it is determined that the distance is not the distance H4, the process returns to step S601, an operation is performed to separate the printhead and the droplet detecting unit 205 by the next set separation distance, and the subsequent data obtainment and processing are executed. If it is determined in step S605 that the current distance is the distance H4, it will be determined that the detection time has been obtained with respect to all of the distances, and the process advances to step S606.
In step S606, discharge speed calculation is executed. More specifically, as described with reference to
Next, the process advances to step S608 to execute a termination process. More specifically, since the discharge speed calculation has been completed, the printhead 201 is returned to a predetermined position or shifted to a standby state for the next printing operation process. Furthermore, a cleaning process is performed on the printhead 201 based on the obtained discharge speed information and the like. Subsequently, the processing ends.
After the completion of the discharge speed calculation processing of
As described above, according to this embodiment, the distance between the printhead 201 and the droplet detecting unit 205 is changed, and the time from the discharge of ink droplets to the detection of the ink droplets is detected for each of the plurality of distances. Subsequently, the discharge speed is calculated based on the difference between the distances and the difference between the detection times. As a result, the ink droplet discharge speed can be calculated accurately even if the apparatus has not been accurately assembled. In addition, by detecting the detection times of four or more distances, it will be possible to more accurately obtain the attenuation influence of the discharge speed with respect to the individual differences of the printing apparatuses or the printheads, the physical properties of the respective ink colors, the state of use of the printing apparatus or the environmental influence on the printing apparatus, and each separation distance. Furthermore, the degradation of image quality due to a landing position shift can be suppressed by adjusting the discharge timing based on the discharge speed.
Note that although the above-described embodiment has an arrangement in which the distance is changed by moving the printhead 201 with respect to the droplet detecting unit 205, it is sufficient as long as the distance between the droplet detecting unit 205 and the printhead 201 in the Z direction is changed in a relative manner. Hence, for example, it may be arranged so that the distance will be changed by moving the droplet detecting unit 205 in the Z direction.
In relation to the discharge speed calculation by the droplet detecting unit 205, a method in which the discharge speed is calculated based on the difference between the distances and the difference in the detection times has been described in the above-described embodiment. However, a method in which detection times are obtained for a plurality of distances and the discharge speed is calculated based on each distance and the detection time corresponding to the distance may also be employed.
In addition, in the above-described embodiment, it was arranged so that a wider range of target nozzles will be set for measuring the detection time for discharge speed calculation. However, it may be arranged so that discharge speed measurement will be performed by setting, in accordance with the state of use by the user, nozzles with a higher ratio of use in printing as the target nozzle.
The second embodiment will be described next. In the first embodiment, the thickness of a print medium 203 was not considered. However, since the print medium 203 has a thickness in reality, the distance between a orifice surface 201a and a platen 212 will be different from the distance between the orifice surface 201a and the print medium 203. In particular, in a case in which printing is to be performed by using a thick print medium 203, using an adjustment value determined based on the distance between the orifice surface 201a and the platen 212 may cause the discharge position to shift due to the fact that the distance between the orifice surface 201a and the print medium 203 is different from that between the orifice surface and the platen. Hence, in this embodiment, discharge timing adjustment is performed based on the distance between the orifice surface 201a and the print medium 203.
The distance between the orifice surface 201a and the print medium 203 is measured by a distance detecting sensor 204. The discharge timing control is performed based on the distance between a printhead 201 and the print medium 203 detected by the distance detecting sensor 204 and the discharge speed information calculated in the discharge speed calculation processing.
Furthermore, the intensity of reflected light obtained by each of the light receiving units 703 and 704 is converted into an output signal based on a current value or a voltage value, predetermined arithmetic processing is performed on the output signal, and the obtained result is stored in a memory 303. For example, distance information data that indicates the relationship between the value of the ratio of output signals obtained by the light receiving units 703 and the light receiving unit 704 and the distance from the printhead 201 to the print medium 203 is stored in the memory.
As shown in
Note that the relationship between a position on the irradiation surface to be a reference and an output signal ratio value of the distance detecting sensor 204 may be obtained in advance and stored in the memory 303. For example, a value detected for a printing medium of a predetermined thickness can be held as a reference value. In addition, the positions of the printhead 201 when the distance from the printhead 201 to the print medium 203 changes between the distances M1 to M5 and the distance from the printhead 201 to a droplet detecting unit 205 for each distance can also be stored in advance.
To determine the discharge timing adjustment value, first, the print medium 203 is conveyed onto the platen 212, and the distance detecting sensor 204 measures the distance between the conveyed print medium 203 and the orifice surface 201a. Subsequently, a speed corresponding to the measured distance between the orifice surface 201a and the print medium 203 is obtained from the discharge speed approximation curve. In this manner, a more accurate discharge speed can be calculated by calculating the ink droplet discharge speed from the actually measured distance between the orifice surface 201a and the print medium 203.
A measurement point is indicated by a hatched circle in
For example, assume that the discharge speed has been calculated for a case in which the distance between the orifice surface 201a and the droplet detecting unit 205 is 1.0 mm, and the discharge speed has been calculated for a case in which the distance between the orifice surface 201a and the droplet detecting unit 205 is 1.5 mm. In this case, if the distance between the orifice surface 201a and the print medium 203 measured by the distance detecting sensor 204 is 1.1 mm, the discharge speed of the case in which the distance is 1.1 mm can be calculated by executing linear complementation on the calculated discharge speeds.
Although the distance between the orifice surface 201a and the print medium 203 is measured by the distance detecting sensor 204 in the above description, another method may be used. For example, it may be arranged so that the thicknesses of various kinds of print media which are to be set as targets will be stored in the memory 303, and the user may select a target print medium from the operation panel on the printing apparatus 100 to set a corresponding distance. The distance detecting sensor may not be included in the printing apparatus if such an arrangement is to be employed.
When the discharge speed for the distance between the orifice surface 201a and the print medium 203 is calculated, the discharge timing adjustment value is obtained from the table held in the memory 303 and the calculated discharge speed in a manner similar to the first embodiment.
As described above, a more accurate discharge speed can be calculated by calculating the ink droplet discharge speeds based on the distances between the orifice surface 201a of the printhead 201 and the print medium 203. By adjusting the discharge timing based on such an accurate discharge speed, it will be possible to suppress a landing position shift.
The third embodiment will be described next. The ink droplet discharge speed can gradually decrease if a printhead is used over a long period. If the discharge speed has decreased from when the detection time adjustment value was set, the ink droplet landing position may shift if the set adjustment value is maintained when printing is to be performed by reciprocally moving the printhead. Hence, this embodiment will describe a mode in which the discharge timing adjustment value is reset at a predetermined timing after the discharge timing adjustment value has been set once. A description of parts similar to those of the above described embodiments will be omitted in this embodiment.
First, in step S1101, a discharge timing adjustment pattern inspection is performed. More specifically, printing of an adjustment pattern for obtaining a discharge timing adjustment value is performed, and the adjustment value is determined from the adjustment pattern.
The process advances to step S1102, and the discharge speed at the point of time when the adjustment pattern was printed is calculated based on the adjustment value obtained in step S1101. A discharge speed at the time of printing of the adjustment pattern will be referred to as a reference discharge speed hereinafter. The calculation method of the reference discharge speed will be described with reference to
First, after the adjustment value has been determined, a landing position shift amount from the adjustment value (“0” in this case) from the reference discharge timing can be determined. The shift amount is shift amount=Xa′−Xa as described in
As described in
Va′=(H×Vcr)/Xa′ (8)
A distance detecting sensor 204 will measure a distance H between an orifice surface 201a and a print medium 203. In addition, a scanning speed Vcr of a printhead 201 is already stored in the memory 303. The distance Xa′ from the discharge position to the landing position according to the current reference discharge speed is calculated, as described above, based on the distance Xa and the shift amount obtained from the adjustment value determined from the adjustment pattern. By substituting each value in the equation, the current reference discharge speed Va′ can be calculated. The current reference discharge speed Va′ that has been calculated is stored in the memory 303. In this embodiment, the line patterns when the distance between the orifice surface 201a and the print medium 203 are at a distance M1, a distance M3, and a distance M5 are printed, and a discharge speed is calculated for each distance. The adjustment value is determined by the above-described processing, and a reference discharge speed is calculated from the adjustment pattern.
The discharge speed will decrease with time as the printhead 201 is used. If the discharge speed decreases, the landing position will shift when printing is performed based on the adjustment value determined by the adjustment pattern. Hence, an attenuation factor of the discharge speed after the previous discharge speed calculation will be obtained by performing discharge speed calculation by using a droplet detecting unit 205, described in the first and second embodiments, at a predetermined timing after the adjustment pattern has been printed. The discharge speed adjustment value will be set based on this attenuation factor. This process will be described in detail with reference to
Each value indicated by a white circle in
Next, at a predetermined timing, in a manner similar to the first embodiment, the detection times at the distances H1 to H5 are indicated as detection times T1′ to T5′ that have been detected by the droplet detecting unit 205 by using hatched circles each surrounded by a solid line in
First, in step S1201, the calculation of discharge speeds of the ink droplets to be discharged from the printhead 201 is performed by processing similar to the discharge speed detection processing of
Next, in step S1202, whether the discharge speed has changed is determined by comparing each reference discharge speed obtained by the processing of
If the process advances to step S1203, the attenuation factor of the ink droplet discharge speed obtained in step S1201 with respect to the reference discharge speed is calculated.
Next, the process advances to step S1204, and the correction processing of the discharge timing adjustment value is executed based on the reduction ratio with respect to the reference discharge speed calculated in step S1203. The adjustment value can be corrected by calculating, based on the attenuation factor, how much the adjustment value is to be shifted from the adjustment value of a case in which the ink droplet discharge speed is at the reference discharge speed.
Next, the process advances to step S1205, and each calculated discharge speed and the correction processing result are stored in the memory 303. Subsequently, a termination process is performed in step S1206. The termination process is a process similar to the process of step S608 of
As described above, by correcting the discharge timing adjustment value, it will be possible to set an appropriate discharge timing adjustment value for the current ink droplet discharge speed. As a result, image quality degradation can be suppressed.
In addition, the discharge speed calculation using the droplet detecting unit 205 may be performed at a timing after a predetermined time has further passed from the completion of the processing of
In step S1204 of the processing of
Although it has been described above that the initial reference discharge speed is calculated based on the adjustment pattern, the discharge speeds may be calculated by using the droplet detecting unit 205 at the timing of the printing of the adjustment pattern. In addition, it may be arranged so that an adjustment value will be determined first based on the discharge speeds calculated by using the droplet detecting unit 205, and the adjustment value will be updated by subsequently printing a pattern.
Furthermore, if it is arranged so that the initial adjustment value will be set based on the discharge speeds calculated by using the droplet detecting unit 205, it will be possible to apply this embodiment to an arrangement which does not have a function for printing the adjustment pattern for obtaining a discharge timing adjustment value.
(Arrangement Examples of Periphery of Droplet Detection Unit)
A method of specifying an ink droplet discharge speed based on the detection results of the droplet detecting unit 205 has been mainly described with reference to
(Arrangement Example 1 (
The droplet detecting unit 205 is formed by a light emitting element 401, a light receiving element 402, a control circuit substrate 403 (see
Here, as described in
This detection time may sometimes include a large error due to the physical arrangement of the droplet detecting unit 205 and its periphery. For example, the light beam 404 formed by the opening 1401 may include a ray of light that linearly propagates, that is, propagates in a straight line parallel to the Y-axis from the light emitting element 401 to the light receiving element 402, and a ray of light that propagates diagonally with respect to the Y-axis. In the example of
When the diffused light 1405 enters the orifice surface 201a after passing the opening 1401, reflected light 1406 which is a part of light irregularly reflected by the orifice surface 201a will enter the light receiving element 402. Particularly, in the detection of an ink droplet that is discharged from an orifice at the center position of the orifice surface 201a in the Y direction, an angle of incidence of the diffused light 1405 will have a value close to an angle of reflection of the reflected light 1406, thus allowing the reflected light 1406 to easily enter the light receiving element 402. This can cause a detection error to be generated. More specifically, if the diffused light 1405 or its reflected light 1406 is shielded by an ink droplet, the received light amount of the light receiving element 402 will decrease in a state in which the ink droplet is present in a region higher than the region of the straight light 404a. Hence, a detection time error will be obtained because the detection time will be shorter than that in the case in which the straight light 404a is shielded by the ink droplet.
Therefore, from the point of view of reducing a detection time error, it is preferable to suppress a state in which the light receiving element 402 will receive the reflected light 1406 emitted from the light emitting element 401 and reflected by the orifice surface 201a. Hence, the shapes, the dimensions, and the like of the housing 2051 and its opening 1401 to be used for this will be described below.
Here, in
At this time, the distance H_GAP can be obtained based on the relation between the ratios of the distance La, the distance L_MID, and a radius da of the opening 1401 from the center of the light beam. That is,
H_GAP: da=(La+L_MID): La (9)
Hence,
H_GAP=da×{(La+L_MID)/La} (10)
On the other hand, in a case in which
H_Lo>H_GAP (11)
is satisfied, the diffused light 1405 will not reach the center position of the orifice surface 201a in the Y direction. In other words, it will be possible to suppress, while using the housing 2051 and the opening 1401 formed thereof to shield a part of the light emitted from the light emitting element 401 to form the light beam 404, a state in which the light emitted from the light emitting element 401 will enter the center portion of the orifice surface 201a in the Y direction. Hence, it will be possible to suppress the reflected light 1406 from entering the light receiving element 402 and reduce the generation of a detection time error. From a certain aspect, the housing 2051 and the opening 1401 thereof function as a suppression unit that suppresses the light receiving element 402 from receiving light that has been emitted from the light emitting element 401 and has been reflected by the orifice surface 201a.
To offer a more specific description in accordance with the example of
H_Hi>H_GAP (12)
will naturally be satisfied as long as equation (11) is satisfied. In addition, since the difference between the distance H_Hi and the distance H_GAP will be greater than that between the distance H_Lo and the distance H_GAP in a case in which both equations (11) and (12) are satisfied, the ratio of the diffused light 1405 that will directly enter the center portion of the orifice surface 201a in the Y direction will decrease more than in the case of the distance H_Lo. Hence, the generation of a detection time error can be reduced.
As described with reference to
Note that this arrangement example described an example in which a part of the light emitted from the light emitting element 401 is shielded so as to suppress the diffused light 1405 from entering the center position of the orifice surface 201a in the Y direction. However, it is also possible to employ an arrangement in which the shapes and the like of the housing 2051 and its opening 1402, formed on the side of the light receiving element 402, are set so as to suppress the light receiving element 402 from receiving the reflected light 1406. For example, it is possible to shield the reflected light 1406 that propagates toward the light receiving element 402 by decreasing the radius of the opening 1402, increasing the distance from the light receiving element 402 to the far-end portion, with respect to the light receiving element 402, of the opening 1402 in the Y direction, and the like.
In addition, this arrangement example showed equation (11) as a condition in which the diffused light 1405 will not enter the center position of the orifice surface 201a in the Y direction. However, it may be arranged so the diffused light 1405 will not enter the orifice surface 201a over the entire region of the orifice surface 201a in the Y direction. More specifically, by using a width LN of the orifice surface 201a in the Y direction, the shape and the dimension of each portion may be set so as to satisfy
H_Lo>da×{(La+L_MID+LN/2)/La} (13)
As a result, the generation of a detection time error can be reduced more effectively.
(Arrangement Example 2 (
According to Arrangement Example 1, as a method of suppressing the light emitted from the light emitting element 401 from entering the center position of the orifice surface 201a in the Y direction, the distance H_Lo, the radius da of the opening, and the distance La may be set to satisfy a state in which distance H_Lo>distance H_GAP.
On the other hand, since this embodiment has an arrangement in which the printhead 201 operates in the height direction and the scanning directions, due to the shape of the droplet detecting unit 205, there may be restrictions on the positional relationship between the printhead 201 and the droplet detecting unit 205, and the like. For example, if the distance La from the light emitting element 401 to the far end of the opening 1401 is increased, there is a concern that this will interfere with the operation region of the printhead 201. In addition, to facilitate the optical design of the sensor and to ensure a necessary light amount while using a low-cost arrangement, the droplet detecting unit 205 may need to be arranged as close to the light emitting element 401 and the light receiving element 402 as possible. Furthermore, to satisfy the ink droplet detection performance, the distance between the printhead 201 and the droplet detecting unit 205 may need to be brought particularly closer in the height direction (Z) or the longitudinal direction (Y), or the radius da of the opening 1401 may need to be increased. However, it may be difficult to simultaneously satisfy both these restrictions and the condition of equation (11) in some cases. Hence, in Arrangement Example 2, the diffused light 1405 will be suppressed from entering the orifice surface 201a by arranging a light shielding portion 1501 (to be described later) in the droplet detecting unit 205.
The light shielding portion 1501 is arranged between the opening 1401 and the orifice surface 201a to shield at least some of the rays of light that propagate toward the orifice surface 201a. In this arrangement example, the light shielding portion 1501 is fixed to a position, of the housing 2051, which is near the opening 1401. The light shielding portion 1501 includes a fixing portion 1501a, an extending portion 1501b, and a hangover portion 1501c. The light shielding portion may be made of the same material as the housing 2051 or be made of a different material.
The fixing portion 1501a is a portion that fixes the light shielding portion 1501, separately prepared from the housing, to the housing 2051, and is fixed to the housing 2051 by, for example, a known arrangement such as an adhesive, a screw, or the like. The extending portion 1501b is arranged to extend from the fixing portion 1501a to the side of the printhead 201 in the Y direction. The hangover portion 1501c is arranged in an end, of the extending portion 1501b, opposite to the side of the fixing portion 1501a, so as to protrude downward from the extending portion 1501b.
In this arrangement example, the light beam 405 is formed as follows. That is, a light beam is formed when a part of light emitted from the light emitting element 401 passes the opening 1401. The light beam 405 is formed by the light shielding portion 1501 shielding, among the rays of the light beam formed by the opening 1401, at least some of the rays of light that propagate toward the orifice surface 201a. That is, in this arrangement example, the light beam 405 is formed when the light shielding portion 1501 shields some of the rays of light included in the light beam formed by the opening 1401. In addition, of the light included in the light beam 405 formed in such a manner, diffused light 1505 on the upper side of the light beam 405 in the vertical direction will propagate in a straight line to the side of the orifice surface 201a.
In this arrangement example, the distance between the printhead 201 and the light beam 405 is set to H_Lo. On the other hand, a distance, in the Z direction, between the diffused light 1505 and the optical axis 406 at a position identical to the center position of the orifice surface 201a in the Y direction is indicated as a distance H′ GAP. In other words, the distance H′ GAP is a Z value of the diffused light 1505 when Y=La+L_MID in a case in which the light emission position of the light emitting element 401 is the origin.
At this time, the distance H′_GAP can be obtained based on the relation between the ratios of the distance La, the distance L_MID, a distance Ga, and a radius d′a of the opening 1401 from the center of the light beam. That is,
H′_GAP:d′a=(La+L_MID):(La+Ga) (14)
Hence,
H′_GAP=d′a×{(La+L_MID)/(La+Ga)} (15)
Here, the distance Ga is a distance from the far end of the opening 1401 to the end of the light shielding portion 1501 in the +Y direction.
Hence, in a manner similar to
H_Lo>H′_GAP (16)
is established, the light shielding portion 1501 can effectively shield the diffused light 1505 that enters the center position of the orifice surface 201a in the Y direction. Thus, it will be possible to reduce the influence of an error in the measurement of the detection time which is the time it takes for a discharged ink droplet to reach the light beam 405. In addition, even in a case in which the distance between the printhead 201 and the light beam 405 is set to the height of H_Hi which is greater than H_Lo, the light shielding portion 1501 joined to the opening 1401 will be able to effectively shield the diffused light 1505 that can enter the orifice surface 201a.
As described above, according to this arrangement example, emitted light is partially shielded by the opening 1401 arranged near the light emitting element, and the light beam 405 is formed by further using the light shielding portion 1501, which is joined to the opening 1401, to shield the light which passed through the opening 1401. This will decrease the distance H′_GAP of the diffused light 1505 and suppress the diffused light 1505 from entering the orifice surface 201a. As a result, it will be possible to reduce an error when the time it takes for an ink droplet that has been discharged from the printhead 201 to reach the light beam 405 is measured. Furthermore, it will be possible to form, while avoiding interference with the operation range of the printhead 201 in the height direction and the scanning directions, the light shielding portion 1501 for effectively shielding the light emitted from the light emitting element 401.
Also, as described above, from a certain aspect, the opening 1401 functions as a formation unit that forms a light beam. The light shielding portion 1501 also functions as a light shielding unit that is arranged between the opening 1401 as the formation unit and the orifice surface 201a to shield some of the rays of light, among the rays of light formed by the opening 1401, which propagate to the orifice surface 201a. Hence, the opening 1401 and the light shielding portion 1501 function as a suppression unit that suppresses the light receiving element 402 from receiving the light which has been emitted from the light emitting element 401 and has been reflected by the orifice surface 201a.
In addition, in this arrangement, the extending portion 1501b and the hangover portion 1501c as portions that do not overlap the printhead 201 in the Z direction are arranged extending in the Y direction in light shielding portion 1501. Hence, the light shielding portion 1501 can shield, while avoiding interference with the printhead 201, the light that propagates to the orifice surface 201a.
Note that in this arrangement example, the light shielding portion 1501 and the opening 1401 are separate components, and the light shielding portion 1501 is fixed to the opening 1401. The necessary size of the suppression changes depending on the distance to the orifice surface 201a and the distance between the light emitting element 401 and the light receiving element 402. By setting an arrangement in which the light shielding portion 1501 is attached to the opening 1401, only the light shielding portion 1501 will be the component whose arrangement needs to be changed if the apparatus arrangement is to be changed, and the same arrangement can be used for the housing 2051.
On the other hand, the light shielding portion 1501 may be formed as a part of the housing 2051. This will reduce the number of components and the number of assembly processes.
Note that the light shielding portion 1501 may not be arranged in the droplet detecting unit 205, but may be supported and arranged in, for example, another portion in the printing apparatus 100. However, it is preferable for the relative positional relationship between the light shielding portion 1501 and the light shielding portion 1501 to be defined by fixing the light shielding portion 1501 to the housing 2051 which is provided with the opening 1401 as in
In addition, by fixing the light shielding portion 1501 to the housing 2051 or by integrally forming the light shielding portion 1501 with the housing 2051, the amount of the light beam 404 that can be shielded by the light shielding portion 1501 can be kept constant. Hence, it will be possible to stabilize the detection accuracy even when the height of the printhead 201 is brought closer to or separated from the light beam 404 during the measurement of the ink droplet discharge speed.
In addition, according to this arrangement example, by installing the light shielding portion 1501 immediately after or near the opening 1401 in the direction of propagation of the light beam 405, it will be possible to ensure the light shielding performance of the light shielding portion 1501 while minimizing its size. Since this will allow the droplet detecting unit 205 to be brought closer to the printhead 201, the distance between the light emitting element 401 and the light receiving element 402 can be shortened, and the distance of the droplet detecting unit 205 in the Y direction can be shortened. Hence, the performances of the light emitting element 401 and the light receiving element 402 can be ensured by a low-cost arrangement. Furthermore, it will be possible to maintain the necessary light amount without increasing the distance from the light emitting element to the light receiving element, and to optimize the shape of the light shielding portion.
Note that when the relation shown in equation (16) is viewed from another point of view, the light shielding portion 1501 suffices to be arranged to shield a virtual line VL that connects the light emitting element 401 and the center position of the orifice surface 201a in the Y direction. Also, in order to further improve the light shielding performance of the light shielding portion 1501, the light shielding portion 1501 may be arranged to shield a virtual line (not shown) that connects the light emitting element 401 and the far-end portion, with respect to the light emitting element, of the orifice surface 201a.
In this numerical example, the distance, in the height direction (Z direction), between the orifice surface 201a of the printhead 201 and the light 404 emitted by the light emitting element 401 is set to H_Lo=2.0 mm. Also, in this numerical example, the light emitting element 401 is a φ5 light-emitting LED, the light receiving element 402 which includes a light receiving unit of 3 mm, and the opening 1401 which shields a part of the light 404 emitted from the light emitting element 401 is formed to have a width of 2 mm, and the light beam 405 is formed by partially shielding light from these elements. Also, the opening 1402 further shields some of the rays of the light beam 405 and guides the remaining rays of light to the light receiving element 402. In addition, the droplet detecting unit 205 is formed by setting the distance from the light emitting element 401 to the far-end portion, with respect to the light emitting element 401, of the opening 1401 to approximately 10 mm and the distance from the light emitting element 401 to the light receiving element 402 to approximately 70 mm.
In addition, in this numerical example, the distance from the center position of the orifice surface 201a, provided in the printhead 201, to the end of the orifice surface 201a in the Y direction is approximately 13.5 mm. Also, in this numerical example, the light shielding portion 1501 is arranged so that the distance d′a between the leading edge of the hangover portion 1501c and the optical axis 406 will be 0.3 mm. The light shielding portion 1501 forms the light beam 405 by using the extending portion 1501b and the hangover portion 1501c to shield some of the rays of light emitted by the light emitting element 401. Hence, the angle of the diffused light 1505, which propagates to a side higher than (the +side of the Z direction) the optical axis 406, with respect to the optical axis 406 can be decreased.
When the arrangement shown by this numerical example is checked against the relations indicated by equations (14), (15), and the like, the distance H′_GAP, at the center position of the orifice surface 201a in the Y direction, of the diffused light 1505 that entered from the light beam 405 is approximately 0.8 mm. Hence, since the distance H′_GAP will be sufficiently smaller than the distance H_Lo, it will be possible to suppress the diffused light 1505 from entering the center position of the orifice surface 201a. Therefore, the detection time error due to the droplet detecting unit 205 can be reduced. At this time, the relation between the distance La+Ga and the distance L_MID+La is (La+Ga):(L_MID+La)=(10+4.4):(30+10)=1:2.7.
The numerical example described above is an example of a case in which the diffused light 1505 is suppressed from entering the center position of the orifice surface 201a. However, the dimensions and the shapes of the components are not limited to this example. Increasing the distance La+Ga can further minimize the angle of the diffused light 1505 with respect to the optical axis 406. However, since increasing the distance La+Ga will increase the distance between the light emitting element 401 and the light receiving element 402, the received light amount will decrease. Thus, it is preferable for the distance La+Ga to be smaller than ½ of the distance L_MID+La. Here, the distance La+Ga is a Y-directional component of the distance from the light emitting element 401 to the far-end portion, with respect to the light emitting element 401, of the light shielding portion 1501 in the Y direction. The distance L_MID+La is a Y-directional component of the distance from the light emitting element 401 to the center position of the orifice surface 201a in the Y direction.
In addition, the angle, formed by the diffused light 1505 and the optical axis 406, which allows the detection time error of the droplet detecting unit 205 to be effectively reduced has been discovered by the experiment by the present inventor. As shown in
tan θ1=d′a/(Ga+La) (17)
tan θ2=H_Lo/(L_MID+La) (18)
In the numerical example of
Examples of the dimensions and shapes of the respective components when the angle θ1 is 1.2° to 1.4° will be described. For example, if the distance d′a from the optical axis 406 to the hangover portion 1501c in the numerical example of
Note that the numerical value of the above-described angle θ1 is merely an example, and the angle of θ1 is not limited to this. The angle θ1 suffices to be less than the angle θ2. Such an arrangement will allow the light shielding portion 1501 to shield a predetermined amount of light that propagates toward the center position of the orifice surface 201a in the Y direction.
In addition, the angle θ1 may be less than an angle formed by the optical axis 406 and a line that connects the light emitting element 401 and the far-end portion, with respect to the light emitting element 401, of the orifice surface 201a. Even in such a case, it will be possible to effectively shield the light that propagates to the orifice surface 201a. By arranging so as to form such an angle, it will be possible to more accurately detect ink droplets which are discharged from all of the orifices including an orifice arranged at a far position, with respect to the light emitting element 401, of the orifice surface 201a.
In addition, although the above embodiments described a condition for improving the detection accuracy of an ink droplet discharged from an orifice positioned at the center of an orifice array, the components may be arranged under another condition if an end of the orifice array is to be detected. For example, when detecting an ink droplet which is discharged from an orifice arranged at a close position, with respect to the light emitting element 401, of the orifice surface 201a, the angle θ1 can be arranged to be less than an angle formed by the optical axis 406 and a line that connects the light emitting element 401 to the orifice arranged at the close position, with respect to the light emitting element 401, of the orifice surface 201a.
(Arrangement Example 3 (
In contrast to the example shown in
In a similar manner, an opening 1802, which is arranged near the light receiving element 402, is formed so that the distance to its lower end portion from the optical axis 406 will be longer by 0.5 mm than the case shown in
According to this arrangement, the light beam 1803 which has a width of 2 mm can pass through the opening 1802 in a manner unchanged from
Furthermore, irregularly reflected light that cannot be shielded by the hangover portion 1501c may sometimes be generated depending on the degree of the diffusion of the light emitted from an LED used as the light emitting element 401 or depending on the member of the opening 1801. This irregularly reflected light will influence the detection if it enters the light receiving element 402 upon being reflected by the orifice surface 201a. By shortening the distance from the optical axis 406 to the upper end portion of the opening 1802 by 0.5 mm less than the case shown in
According to this arrangement example, even in a case in which the opening 1801 and the light shielding portion 1501 are arranged in consideration to the measurement accuracy of the ink droplet discharge speed, the opening 1802 can be enlarged in the lower side of the optical axis of the light beam to supplement the reduction in the amount of light received by the light receiving element 402.
Note that the specification method of the ink droplet discharge speed of the printhead 201 based on the detection results of the droplet detecting unit 205 to be used in a case in which each arrangement example described in (Arrangement Examples of Periphery of Droplet Detection Unit) is to be applied is not limited to the methods described above in the first to third embodiments. For example, the discharge speed may be calculated by dividing the distance (height) between the orifice surface 201a and the print medium 203, which has been detected by the distance detecting sensor 204, by the detection time from the ink droplet discharge by the printhead 201 to the detection of the ink droplet by the droplet detecting unit 205. In addition, for example, a table in which the detection time and the discharge speed has been associated for each height (for example, H1 to H4 of
Embodiment(s) of the present invention can also be realized by a computer of a system or apparatus that reads out and executes computer executable instructions (e.g., one or more programs) recorded on a storage medium (which may also be referred to more fully as a ‘non-transitory computer-readable storage medium’) to perform the functions of one or more of the above-described embodiment(s) and/or that includes one or more circuits (e.g., application specific integrated circuit (ASIC)) for performing the functions of one or more of the above-described embodiment(s), and by a method performed by the computer of the system or apparatus by, for example, reading out and executing the computer executable instructions from the storage medium to perform the functions of one or more of the above-described embodiment(s) and/or controlling the one or more circuits to perform the functions of one or more of the above-described embodiment(s). The computer may comprise one or more processors (e.g., central processing unit (CPU), micro processing unit (MPU)) and may include a network of separate computers or separate processors to read out and execute the computer executable instructions. The computer executable instructions may be provided to the computer, for example, from a network or the storage medium. The storage medium may include, for example, one or more of a hard disk, a random-access memory (RAM), a read only memory (ROM), a storage of distributed computing systems, an optical disk (such as a compact disc (CD), digital versatile disc (DVD), or Blu-ray Disc (BD)™), a flash memory device, a memory card, and the like.
While the present invention has been described with reference to exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.
This application claims the benefit of Japanese Patent Application No. 2020-123149, filed Jul. 17, 2020, which is hereby incorporated by reference herein in its entirety.
Number | Date | Country | Kind |
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2020-123149 | Jul 2020 | JP | national |
Number | Name | Date | Kind |
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9676182 | Kiyokawa | Jun 2017 | B2 |
20060139392 | Fernandez | Jun 2006 | A1 |
20120139982 | Abe | Jun 2012 | A1 |
Number | Date | Country |
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2007-152853 | Jun 2007 | JP |
2010131800 | Jun 2010 | JP |
Entry |
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Miyata, MachineTranslationofJP-2010131800-A, 2010 (Year: 2010). |
Number | Date | Country | |
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20220016889 A1 | Jan 2022 | US |