Ink-jet head, ink-jet cartridge, and ink jet recording apparatus
Abstract
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Expired 21 April 2017, 9.4 years ago.
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11 claims: 4 independent, 7 dependent
- 1An ink-jet head comprising:an ejection outlet portion (108) which has an ejection outlet (101), and is convergent toward said outlet;an ink channel (104) communicating with said outlet;and an element substrate (23) disposed in said ink channel and having individually drivable first (102, 3) and second (103, 4) heaters;wherein: said first heater and said second heater have different heating powers and are spaced from each other;said ink-jet head being characterised in that the following formula: tan -1 S N S O (Sin θ 1 + Sin θ 2 ) S N 2 -S O 2 Sin θ 1 Sin θ 2 ≤5° is satisfied, where the area S N is the sectional area of the ink channel perpendicular to the ink-ejecting direction, the area S o is the area of the ejection outlet, and, within the plane which contains the center line of the ink channel and is parallel to the line connecting the areal center of the first heater to the areal center of the second heater, the angle θ 1 is the angle between the center line of the ink channel and the line between the areal center of the ejection outlet and the projection of the areal center of the first heater onto said plane and the angle θ 2 is the angle between the center line of the ink channel and the line between the areal center of the ejection outlet and the projection of the areal center of the second heater onto said plane.
- 7An ink-jet head comprising:an ejection outlet portion which has an ejection outlet, and is convergent toward said outlet;an ink chamber communicating with said outlet;and an element substrate (23) disposed in said ink chamber and having individually drivable first (102, 3) and second (103, 4) heaters;wherein: said first heater and said second heater have different heating powers and are spaced from each other;said ink-jet head being characterised in that the following formula: tan -1 S N S O (Sin θ 1 + Sin θ 2 ) S N 2 -S O 2 Sin θ 1 Sin θ 2 ≤5° is satisfied, where the area S N is the sectional area of the ink chamber perpendicular to the ink-ejecting direction, the area S o is the area of the ejection outlet, and, within the plane which contains the center line of the ink chamber and is parallel to the line connecting the areal center of the first heater to the areal center of the second heater, the angle θ 1 is the angle between the center line of the ink chamber and the line between the areal center of the ejection outlet and the projection of the areal center of the first heater onto said plane and the angle θ 2 is the angle between the center line of the ink chamber and the line between the areal center of the ejection outlet and the projection of the areal center of the second heater onto said plane.
Independent claims4
40 paragraphs in 7 sections, as filed
BACKGROUND OF THE INVENTION
Field of the Invention
The present invention relates to ink-jet heads and apparatuses used in printers, video printers and others serving as output terminal units for copying machines, facsimile machines, word processors, host computers and others. In particular, the present invention relates to an ink-jet head and an ink-jet apparatus having a base member comprising an electrothermal converting element which generates thermal energy utilized as recording energy. Incidentally, the term "recording" used here implies ink application and other activities (printing) onto any type of ink-receiving material such as cloth, thread, paper, and sheet materials, and the term "recording apparatus" implies various types of information-processing apparatuses and printers serving as output units used in such apparatuses. Accordingly, the present invention is applicable for these usages.
Description of the Related Art
Recently, ink-jet recording apparatuses are increasingly required to be of smaller size, lower price, and in addition, have abilities for color recording and higher image quality recording. Hitherto, since a precise and complex structure and control of the recording head was necessary for achieving high image quality, recording apparatuses were extremely expensive and of large size.
In relation to this, Japanese Examined Patent Publication No. 62-48585 discloses an ink-jet recording apparatus capable of modulating dot sizes while using a markedly simple mechanism in which two or more of electrothermal converting elements (including large one and small one) are disposed within one nozzle, and thus achieving high image quality. This invention is significant for gray-scale recording.
US Patent No. 5,172,139 also discloses an ink jet recording apparatus capable of producing graduated dot sizes by using two or more electrothermal converting elements which may be independently driven and which, either by means of varying the distance between the converting elements and the ejection outlet or by varying the power of each converting element, cause different sizes of ink droplets to be ejected.
Practically, when ink-ejecting quantity is modulated for achieving high image quality while using two electrothermal converting elements within one nozzle, each of the parallel-disposed electrothermal converting elements is generally individually driven. It has been revealed, however, that merely disposing the electrothermal converting elements in parallel cannot achieve an optimum ink-impacting position accuracy in some cases though a considerable accuracy can be achieved. In relation to this, the Inventors found that alteration of design parameters such as the distances between the electrothermal converting elements and an orifice, the size of the orifice, and others causes deterioration of the ink-impacting position accuracy, and therefore, the design must be wholly reformed in order to attain desired image quality. More specifically, alteration of some design parameters as described above leads to failure in satisfying practical levels, which may be attributed to complex factors arising from provision of two electrothermal converting elements within one nozzle and concerning nozzle designing for achieving high levels of ink-ejecting quantity and stability of the ejecting quantity. Further, the Inventors conducted the following examination in addition to examination of problems in related arts on designing the above-described electrothermal converting elements and the ink-impacting point. Ordinarily, factors on designing a nozzle and its periphery for achieving desired ink-impacting position accuracy are the orifice area, the nozzle length, the size and disposition of the electrothermal converting element, and others. The inventors examined designs of nozzles which contain a plurality of electrothermal converting elements while focusing the attention on the orifice area and the nozzle length among the above-listed factors, and found that a desired ink-impacting position accuracy can rarely be stably achieved possibly due to influence of other predominant factors. Meanwhile, among the parameters on designing a nozzle and its periphery, sizes of the electrothermal converting elements are determined at the point when a photomask used in a patterning step in a process for manufacturing a semiconductor substrate is designed. When the sizes of the electrothermal converting elements are altered aiming at achieving a desired ink-impacting position accuracy, the head must be produced almost newly. Accordingly, since the size and position of each electrothermal converting element should be altered at the last point of nozzle designing, there are considerable losses in view of time and workload. In contrast, only if the sizes and positions of the electrothermal converting elements can be determined beforehand, other ink-ejecting properties can easily be adjusted. For example, the orifice area can be minutely altered since methods for controlling the energy from a laser or the like for forming the orifice have been developed, and such an alteration is less causative of time loss and work inefficiency since forming the orifice is a relatively later step. Consequently, for a head having a plurality of electrothermal converting elements within one nozzle, it is particularly important to properly determine positions of the orifice and the electrothermal converting elements and others at an initial stage of nozzle designing.
As described above, requirements on structure of a head having a plurality of heaters within one nozzle for achieving a high image quality have not yet been considered in detail in view of the relationship between the orifice and the electrothermal converting elements. Based on the above findings, the present invention is directed to solve difficulties in achieving a high image quality while using a head having a plurality of heaters within one nozzle, and to achieve recording with a higher image quality.
The Inventors examined the parameters on head designing in order to improve ink-impacting position accuracy aiming at achieving high image quality recording, and found that stable achievement of a high image quality requires considering tendency of the influence upon ink-impacting position accuracy by the orifice area and positions of the two electrothermal converting elements relative to the orifice. The present invention has been accomplished based on this finding.
SUMMARY OF THE INVENTION
Accordingly, an object of the present invention is to provide an ink-jet recording head, an ink-jet head cartridge and an ink-jet recording apparatus capable of achieving highly fine recording by specifying a head structure in which the positional relationship between a plurality of heaters and the areal center of an ejection outlet is carefully considered.
According to a first aspect of the present invention, there is provided an ink-jet head as set out in claim 1.
According to a second aspect of the present invention, there is provided an ink-jet head as set out in claim 7.
According to a third aspect of the present invention, there is provided an ink-jet recording apparatus as set out in claim 10.
According to a fourth aspect of the present invention, there is provided an ink-jet recording apparatus as set out in claim 11.
According to a fifth aspect of the present invention, there is provided an ink-jet head cartridge as set out in claim 9.
Based on the above constructions, , ink-impacting position accuracy can be improved by inhibiting irregularity in the ink-impacting position in a case where each heater is individually driven, and thus gray-scale recording can be achieved with a high image quality.
BRIEF DESCRIPTION OF THE DRAWINGS
<ul id="ul0001" list-style="none" compact="compact"><li>Fig. 1 is a schematic sectional view illustrating the structure around the ink channel of an ink-jet recording head according to the present invention;</li><li>Fig. 2 is a schematic sectional view illustrating the structure around the ink channel of another ink-jet recording head according to the present invention; Fig. 3 is a schematic sectional view illustrating the structure of an ink channel in detail;</li><li>Fig. 4 contains schematic diagrams showing the relationship between an ejection outlet portion and a sectional area of an ink channel in the present invention;</li><li>Fig. 5 is a schematic diagram showing an equivalent circuit on an element substrate equipped with heaters;</li><li>Fig. 6 is a schematic view illustrating the structure of a nozzle and its periphery in an ink-jet recording head of the present invention;</li><li>Fig. 7 is a schematic view illustrating an ink-jet recording apparatus of the present invention;</li><li>Fig. 8 is a schematic sectional view showing another example of an ink-jet recording head according to the present invention; and</li><li>Fig. 9 is a schematic sectional view showing another example of an ink-jet recording head according to the present invention.</li></ul>
DESCRIPTION OF THE PREFERRED EMBODIMENT
EXAMPLE 1
Fig. 1 is a schematic sectional view of an ink-jet recording head and its periphery most properly showing the feature of the present invention. In this figure, 101 indicates an ejection outlet; 108 indicates an ejection outlet portion having the ejection outlet; 102 indicates an electrothermal converting element as a first heater generating a thermal energy according to application of a predetermined electric current; and 103 indicates an electrothermal converting element as a second heater.
Further, O indicates the areal center of the ejection outlet 101, and HC<sub>A</sub> and HC<sub>B</sub> indicate the areal centers of the electrothermal converting elements 102 and 103, respectively. Incidentally, the centers of the effective heating areas, which especially directly contribute to generation of bubbles, may also be regarded as areal centers.
Additionally, Fig. 3 is a detailed view of the principal portion for further illustration of the present invention. In this figure, only the first heater among the above-mentioned heaters is shown in order to simplify illustration of the present invention, θ<sub>1</sub> is an angle of the line O-HC<sub>A</sub> relative to the center line of the ink channel, and θ<sub>A</sub> is an angle between the ink-ejecting direction and the center line of the ink channel when ink drops are ejected based on such an ink channel structure.
Moreover, Figs. 4A and 4B are schematic drawings showing the ejection outlets and the sections of ink channels employed in this example. In these figures, S<sub>O</sub> indicates the area of the ejection outlet, and S<sub>N</sub> indicates the cross sectional area in the direction perpendicular to the longitudinal direction of the ink channel.
Here, the relationship between θ<sub>1</sub> and θ<sub>A</sub> will be determined with reference to Fig. 3. The angle θ<sub>A</sub> is formed between the center line of the ink channel and the direction of F which is the resultant force of the pressure F<sub>d</sub> in the θ<sub>1</sub> direction and the pressure F<sub>O</sub> along the center line of the ink channel. Accordingly, θ<sub>A</sub> can be determined by determining the ratio between F<sub>O</sub> and F<sub>d</sub>.
Additionally, when F<sub>X</sub> is defined as the ink-ejecting-directional component of the bubbling pressure derived from the electrothermal converting element 102, F<sub>X</sub> substantially equals F, and therefore the pressure F<sub>d</sub> upon the area S<sub>O</sub> of the ejection outlet can be expressed according to the following formula.<maths id="math0001" num=""><math display="block"><mrow><msub><mrow><mtext>F</mtext></mrow><mrow><mtext>d</mtext></mrow></msub><mtext> = </mtext><mfrac><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub></mrow><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub></mrow></mfrac><msub><mrow><mtext> · F</mtext></mrow><mrow><mtext>X</mtext></mrow></msub></mrow></math><img file="EP0803361B1_D0001.tif" /></maths> Meanwhile, the other pressure can be expressed as F<sub>O</sub> as follows.<maths id="math0002" num=""><math display="block"><mrow><msub><mrow><mtext>F</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><mtext> = </mtext><mfrac><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msub><mrow><mtext>-S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub></mrow><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub></mrow></mfrac><msub><mrow><mtext>F</mtext></mrow><mrow><mtext>X</mtext></mrow></msub></mrow></math><img file="EP0803361B1_D0002.tif" /></maths>
Accordingly, the F<sub>d</sub>/F<sub>O</sub> ratio can be expressed by S<sub>O</sub>/(S<sub>N</sub> - S<sub>O</sub>). Using this ratio, θ<sub>1</sub> and θ<sub>2</sub>, the equation relative to the direction of the resultant force F can be expressed as follows.<maths id="math0003" num=""><math display="block"><mrow><msub><mrow><mtext>tan θ </mtext></mrow><mrow><mtext>A</mtext></mrow></msub><mtext> = </mtext><mfrac><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msub><mrow><mtext> sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub></mrow><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msub><mrow><mtext>-S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msub><mrow><mtext>(1-cosθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><mtext>)</mtext></mrow></mfrac></mrow></math><img file="EP0803361B1_D0003.tif" /></maths> Hereupon, according to the ordinary rules on designing nozzles (ink channels), θ<sub>1</sub> is less than 12°, and therefore, the value of [1 - cosθ<sub>1</sub>] is substantially zero. Accordingly, the above equation can be expressed as follows.<maths id="math0004" num=""><math display="block"><mrow><msub><mrow><mtext>tan θ </mtext></mrow><mrow><mtext>A</mtext></mrow></msub><mtext> = </mtext><mfrac><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub></mrow><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub></mrow></mfrac><msub><mrow><mtext> sin θ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub></mrow></math><img file="EP0803361B1_D0004.tif" /></maths>
Similarly, the relationship between θ<sub>B</sub> and θ<sub>2</sub> can be expressed as follows, wherein θ<sub>B</sub> is the ink-ejecting direction according to bubbling by the non-illustrated second electrothermal converting element, and θ<sub>2</sub> is the angle formed between the center line of the ink channel and the line O-HC<sub>B</sub>.<maths id="math0005" num=""><math display="block"><mrow><msub><mrow><mtext>tan θ </mtext></mrow><mrow><mtext>D</mtext></mrow></msub><mtext> = </mtext><mfrac><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub></mrow><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub></mrow></mfrac><msub><mrow><mtext> sin θ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub></mrow></math><img file="EP0803361B1_D0005.tif" /></maths>
Consequently, when ink is ejected according to bubbling by both first and second electrothermal converting elements, the narrowed angle θ<sub>f</sub> in the ink-ejecting direction calculated by θ<sub>A</sub> + θ<sub>B</sub> can be determined as follows.<maths id="math0006" num=""><math display="block"><mrow><msub><mrow><mtext>tan θ</mtext></mrow><mrow><mtext>f</mtext></mrow></msub><msub><mrow><mtext> = tan (θ</mtext></mrow><mrow><mtext>A</mtext></mrow></msub><mtext> + </mtext><msub><mrow><mtext mathvariant="italic">θ</mtext></mrow><mrow><mtext>B</mtext></mrow></msub><mtext>)</mtext><mspace linebreak="newline" /><mtext> =</mtext><mfrac><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msub><mrow><mtext>(Sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext>+Sinθ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub><mtext>)</mtext></mrow><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msup><mrow><mtext></mtext></mrow><mrow><mtext>2</mtext></mrow></msup><msub><mrow><mtext>-S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msup><mrow><mtext></mtext></mrow><mrow><mtext>2</mtext></mrow></msup><msub><mrow><mtext>Sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext>Sinθ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub></mrow></mfrac></mrow></math><img file="EP0803361B1_D0006.tif" /></maths><maths id="math0007" num=""><math display="block"><mrow><msub><mrow><mtext>θ</mtext></mrow><mrow><mtext>f</mtext></mrow></msub><msup><mrow><mtext> = tan</mtext></mrow><mrow><mtext>-1</mtext></mrow></msup><mtext></mtext><mfrac><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msub><mrow><mtext>(Sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext>+Sinθ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub><mtext>)</mtext></mrow><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msup><mrow><mtext></mtext></mrow><mrow><mtext>2</mtext></mrow></msup><msub><mrow><mtext>-S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msup><mrow><mtext></mtext></mrow><mrow><mtext>2</mtext></mrow></msup><msub><mrow><mtext>Sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext>Sinθ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub></mrow></mfrac></mrow></math><img file="EP0803361B1_D0007.tif" /></maths>
Here, ink-impacting position error levels required for various image qualities are shown in Table 1 below. <tables id="tabl0001" num="0001"><table frame="all"><title>Table 1</title><tgroup cols="4" colsep="1" rowsep="0"><colspec colnum="1" colname="col1" colwidth="39.37mm" /><colspec colnum="2" colname="col2" colwidth="39.37mm" /><colspec colnum="3" colname="col3" colwidth="39.37mm" /><colspec colnum="4" colname="col4" colwidth="39.37mm" /><thead valign="top"><row rowsep="1"><entry namest="col1" nameend="col1" align="center">Picture Element Density (dpi)</entry><entry namest="col2" nameend="col2" align="center">Picture Element Pitch (µm)</entry><entry namest="col3" nameend="col3" align="center">Ink-impacting Position Error for One Picture Element at 1.0 mm Distance (deg)</entry><entry namest="col4" nameend="col4" align="center">Ink-impacting Position Error for Half Picture Element at 1.0 mm Distance (deg)</entry></row></thead><tbody valign="top"><row><entry namest="col1" nameend="col1" align="center">300</entry><entry namest="col2" nameend="col2" align="center">84.7</entry><entry namest="col3" nameend="col3" align="center">4.9</entry><entry namest="col4" nameend="col4" align="center">2.4</entry></row><row><entry namest="col1" nameend="col1" align="center">360</entry><entry namest="col2" nameend="col2" align="center">70.5</entry><entry namest="col3" nameend="col3" align="center">4.0</entry><entry namest="col4" nameend="col4" align="center">2.0</entry></row><row rowsep="1"><entry namest="col1" nameend="col1" align="center">400</entry><entry namest="col2" nameend="col2" align="center">63.5</entry><entry namest="col3" nameend="col3" align="center">3.6</entry><entry namest="col4" nameend="col4" align="center">1.8</entry></row></tbody></tgroup></table></tables>
As shown in Table 1, in a case where ink drops are ejected from one ejection outlet, the ink-impacting position error level should fall within 4.9° when the maximum ink-impacting position error is assumed as one picture element value. Further, when the maximum ink-impacting position error is assumed as half picture element value, the ink-impacting position error level should fall within 2.4°. Accordingly, the above-determined θ<sub>f</sub> should satisfy 0° < θ<sub>f</sub> ≤ 5°, and more preferably, 0° < θ<sub>f</sub> ≤ 3°.
Based on the above-described designing rule, the positions of the electrothermal converting elements and the orifice area were determined, and several types of ink-jet heads were manufactured. The design parameters and the resulting image qualities of the practically manufactured ink-jet heads are shown in Table 2 below. <tables id="tabl0002" num="0002"><table frame="all"><title>Table 2</title><tgroup cols="7" colsep="1" rowsep="0"><colspec colnum="1" colname="col1" colwidth="22.50mm" /><colspec colnum="2" colname="col2" colwidth="22.50mm" /><colspec colnum="3" colname="col3" colwidth="22.50mm" /><colspec colnum="4" colname="col4" colwidth="22.50mm" /><colspec colnum="5" colname="col5" colwidth="22.50mm" /><colspec colnum="6" colname="col6" colwidth="22.50mm" /><colspec colnum="7" colname="col7" colwidth="22.50mm" /><thead valign="top"><row rowsep="1"><entry namest="col1" nameend="col1" align="center">Type</entry><entry namest="col2" nameend="col2" align="center">θ<sub>1</sub> (deg)</entry><entry namest="col3" nameend="col3" align="right">θ<sub>2</sub> (deg)</entry><entry namest="col4" nameend="col4" align="right">S<sub>o</sub> (µm)</entry><entry namest="col5" nameend="col5" align="center">S<sub>N</sub> (µm)</entry><entry namest="col6" nameend="col6" align="center">θ<sub>f</sub> (deg)</entry><entry namest="col7" nameend="col7" align="center">Quality</entry></row></thead><tbody valign="top"><row><entry namest="col1" nameend="col1" align="center">A</entry><entry namest="col2" nameend="col2" align="center">2</entry><entry namest="col3" nameend="col3" align="right">4</entry><entry namest="col4" nameend="col4" align="right">900</entry><entry namest="col5" nameend="col5" align="center">2500</entry><entry namest="col6" nameend="col6" align="center">2.2</entry><entry namest="col7" nameend="col7" align="center">Very Good</entry></row><row><entry namest="col1" nameend="col1" align="center">B</entry><entry namest="col2" nameend="col2" align="center">4</entry><entry namest="col3" nameend="col3" align="right">6</entry><entry namest="col4" nameend="col4" align="right">900</entry><entry namest="col5" nameend="col5" align="center">2500</entry><entry namest="col6" nameend="col6" align="center">3.6</entry><entry namest="col7" nameend="col7" align="center">Good</entry></row><row><entry namest="col1" nameend="col1" align="center">C</entry><entry namest="col2" nameend="col2" align="center">6</entry><entry namest="col3" nameend="col3" align="right">8</entry><entry namest="col4" nameend="col4" align="right">900</entry><entry namest="col5" nameend="col5" align="center">2500</entry><entry namest="col6" nameend="col6" align="center">5.0</entry><entry namest="col7" nameend="col7" align="center">Good</entry></row><row rowsep="1"><entry namest="col1" nameend="col1" align="center">D</entry><entry namest="col2" nameend="col2" align="center">8</entry><entry namest="col3" nameend="col3" align="right">10</entry><entry namest="col4" nameend="col4" align="right">900</entry><entry namest="col5" nameend="col5" align="center">2500</entry><entry namest="col6" nameend="col6" align="center">6.4</entry><entry namest="col7" nameend="col7" align="center">Bad</entry></row><row><entry namest="col1" nameend="col1" align="center">E</entry><entry namest="col2" nameend="col2" align="center">6</entry><entry namest="col3" nameend="col3" align="right">8</entry><entry namest="col4" nameend="col4" align="right">400</entry><entry namest="col5" nameend="col5" align="center">2500</entry><entry namest="col6" nameend="col6" align="center">2.2</entry><entry namest="col7" nameend="col7" align="center">Very Good</entry></row><row><entry namest="col1" nameend="col1" align="center">F</entry><entry namest="col2" nameend="col2" align="center">6</entry><entry namest="col3" nameend="col3" align="right">8</entry><entry namest="col4" nameend="col4" align="right">700</entry><entry namest="col5" nameend="col5" align="center">2500</entry><entry namest="col6" nameend="col6" align="center">3.9</entry><entry namest="col7" nameend="col7" align="center">Good</entry></row><row rowsep="1"><entry namest="col1" nameend="col1" align="center">G</entry><entry namest="col2" nameend="col2" align="center">6</entry><entry namest="col3" nameend="col3" align="right">8</entry><entry namest="col4" nameend="col4" align="right">1000</entry><entry namest="col5" nameend="col5" align="center">2500</entry><entry namest="col6" nameend="col6" align="center">5.6</entry><entry namest="col7" nameend="col7" align="center">Bad</entry></row></tbody></tgroup></table></tables>
Incidentally, when nozzles are designed according to the ordinary designing rule, the distance between the first and second electrothermal converting elements is required to be 2 µm or more in view of deposition performance, and the width of each electrothermal converting element requires an additional 2 µm or more around the effective heating zone, namely, 4 µm or more in total.
Further, the distance between the areal center of each electrothermal converting element and that of the ejection output is at most 300 µm, and therefore, the angle θ between the areal centers of the first and second electrothermal converting elements via the areal center of the ejection outlet is determined as follows.<maths id="math0008" num=""><math display="block"><mrow><msup><mrow><mtext>θ = tan</mtext></mrow><mrow><mtext>-1</mtext></mrow></msup><mtext>(3/300) = 0.6°</mtext></mrow></math><img file="EP0803361B1_D0008.tif" /></maths><maths id="math0009" num=""><math display="block"><mrow><msub><mrow><mtext>θ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext> = θ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub><mtext> = θ/2 = 0.3°</mtext></mrow></math><img file="EP0803361B1_D0009.tif" /></maths>
Moreover, when the sectional area S<sub>N</sub> of the ink channel is set as 2500 µm<sup>2</sup>, the area S<sub>O</sub> of the ejection outlet requires at least 400 µm<sup>2</sup>. Accordingly, the minimum value of the narrowed angle θ<sub>f</sub> in the ink-ejecting direction is calculated at 0.1° by substitution of the above-described values, namely, 0.1° ≤ θ<sub>f</sub>.
Next, the practical structure of the above-described heads will be illustrated below. The structure around the nozzles is shown in Fig. 6. Ink in an ink-ejecting nozzle 104 is heated for bubble generation by electrothermal converting elements 3 and 4, and ejected from a laterally opened ejection outlet 101. The reference number 1 indicates an common lead wire 1 electrically connected to each heater, and 6 and 7 indicate selective lead wires for individually driving each heater. A substrate 23 is stuck to a base plate 41, and nozzle walls 5 are formed so as to be integrated with a grooved member 105.
Fig. 7 is a perspective view of an example ink-jet recording apparatus carrying an ink-jet recording head which has the above-described structure. This ink-jet recording apparatus IJRA has a leading screw 2040 whose rotation is interlocked with front or reverse rotation of a driving motor 2010 through driving-force-transmitting gears 2020 and 2030. A carriage HC carrying an ink-jet cartridge IJC comprising an ink-jet recording head integrated with an ink tank is supported with a carriage shaft 2050 and the leading screw 2040, has a pin (not illustrated) engaged to a spiral groove 2041 on the leading screw 2040, and moves left and right, namely, in the directions of arrows a and b in accordance with rotation of the lead screw 2040. The referential number 2060 indicates a sheet-pressing plate which presses a paper sheet P against a platen roller 2070 over the range where the carriage moves. The referential numbers 2080 and 2090 indicate parts of a photo-coupler which function as home-position-detecting means for processes such as switching the rotating direction of the motor 2010 according to recognition of the presence of a lever 2100 joined to the carriage HC when the lever comes to the position of the coupler. The referential number 2110 indicates a cap member to cap the entire surface of the recording head, and the member is supported by a supporting member 2120. The referential number 2130 indicates a sucking means for sucking the inside of the cap, and the recording head is sucked for recovery by the sucking means through an opening in the cap. A cleaning blade 2140 which cleans the end face of the recording head is disposed on a member 2150 so as to be capable of moving forward and backward, and these blade and member are supported by a main-body-supporting plate 2160. As a matter of course, the form of the blade 2140 is not limited to the above, and any type of publicly-known cleaning blade can be used in this example. Additionally, a lever 2170 functioning to recover the suction for recovery of the recording head is disposed so as to move in accordance with movement of a cam 2180 engaged with the carriage HC, and according to such a mechanism, the driving force derived from the driving motor 2010 is controlled by a publicly-known transmitting means such as clutch switching.
In the above-described structure, each process of capping, cleaning, and suction for recovery of the head is carried out desirably at a position corresponding to the process by action of the lead screw 2040 when the carriage HC enters a zone near the home position. Needless to say, any type of structure in which desired processes are carried out with known timing can be employed for this example.
EXAMPLE 2
Fig. 2 is a schematic sectional view illustrating the structure around the ink channel of another ink-jet recording head according to the present invention. Although the distance between HC<sub>A</sub> and the front end of the nozzle was different from that between HC<sub>B</sub> and the same, results similar in Example 1 could be obtained by properly determining θ<sub>1</sub> and θ<sub>2</sub>.
EXAMPLE 3
In this example, as shown in Figs. 8 and 9, an ejection outlet 101 is formed in parallel to the surface of an element substrate 23 equipped with heating resistors 3 and 4, namely, opposite to the heating resistors. Similar to Fig. 3, Fig. 8 is a schematic view illustrating the ink-ejecting angle. Although an ink inlet is disposed in the direction perpendicular to the longitudinal direction of the heating resistors in this figure, it does not influence the results of this example if the inlet is disposed lying in a direction parallel to the heating resistors. Fig. 9 is a schematic perspective sectional view showing the structure of nozzles and their peripheries in this example.
According to the same calculation as illustrated in Example 1, the following equation expressing the relationship between the positions of the heating resistors and ink-ejecting direction can be obtained.<maths id="math0010" num=""><math display="block"><mrow><msub><mrow><mtext>θ</mtext></mrow><mrow><mtext>f</mtext></mrow></msub><msup><mrow><mtext> = tan</mtext></mrow><mrow><mtext>-1</mtext></mrow></msup><mtext></mtext><mfrac><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msub><mrow><mtext>(Sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext>+Sinθ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub><mtext>)</mtext></mrow><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msup><mrow><mtext></mtext></mrow><mrow><mtext>2</mtext></mrow></msup><msub><mrow><mtext>-S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msup><mrow><mtext></mtext></mrow><mrow><mtext>2</mtext></mrow></msup><msub><mrow><mtext>Sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext>Sinθ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub></mrow></mfrac></mrow></math><img file="EP0803361B1_D0010.tif" /></maths> Based on this equation, an inequality 0° < θ<sub>f</sub> ≤ 5° should be satisfied in order to achieve the optimum ink-impacting position error.
As described above, false ink-impacting position when ink bubbles are generated by two electrothermal converting elements can be prevented and high image quality can be achieved in such a case where the following formula is satisfied with the angle θ<sub>1</sub> of the areal center of a first heating resistor member relative to the areal center of an orifice in a ejection outlet portion; the angle θ<sub>2</sub> of the areal center of a second heating resistor member relative to the same; the sectional area S<sub>N</sub> of an ink channel when the channel is sectioned perpendicular to the ink-ejecting direction; and the area S<sub>O</sub> of the orifice.<maths id="math0011" num=""><math display="block"><mrow><msup><mrow><mtext>0° < tan</mtext></mrow><mrow><mtext>-1</mtext></mrow></msup><mtext></mtext><mfrac><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msub><mrow><mtext>(Sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext>+Sinθ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub><mtext>)</mtext></mrow><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msup><mrow><mtext></mtext></mrow><mrow><mtext>2</mtext></mrow></msup><msub><mrow><mtext>-S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msup><mrow><mtext></mtext></mrow><mrow><mtext>2</mtext></mrow></msup><msub><mrow><mtext>Sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext>Sinθ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub></mrow></mfrac><mtext> ≦ 5°</mtext></mrow></math><img file="EP0803361B1_D0011.tif" /></maths> More preferably, such effects can be obtained when the following formula is satisfied.<maths id="math0012" num=""><math display="block"><mrow><msup><mrow><mtext>0° < tan</mtext></mrow><mrow><mtext>-1</mtext></mrow></msup><mtext></mtext><mfrac><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msub><mrow><mtext>(Sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext>+Sinθ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub><mtext>)</mtext></mrow><mrow><msub><mrow><mtext>S</mtext></mrow><mrow><mtext>N</mtext></mrow></msub><msup><mrow><mtext></mtext></mrow><mrow><mtext>2</mtext></mrow></msup><msub><mrow><mtext>-S</mtext></mrow><mrow><mtext>O</mtext></mrow></msub><msup><mrow><mtext></mtext></mrow><mrow><mtext>2</mtext></mrow></msup><msub><mrow><mtext>Sinθ</mtext></mrow><mrow><mtext>1</mtext></mrow></msub><msub><mrow><mtext>Sinθ</mtext></mrow><mrow><mtext>2</mtext></mrow></msub></mrow></mfrac><mtext> ≦ 3°</mtext></mrow></math><img file="EP0803361B1_D0012.tif" /></maths>
Although two heating resistor members are disposed within one nozzle in the above examples, similar results can also be achieved, needless to say, in cases where three or more of heating resistor members are disposed within one nozzle by determining the maximum θ<sub>f</sub> value.
Contents7
28 sheets
Sheet 1 Sheet 2 Sheet 3 Sheet 4 Sheet 5 Sheet 6 Sheet 7 Sheet 8 Sheet 9 Sheet 10 Sheet 11 Sheet 12 Sheet 13 Sheet 14 Sheet 15 Sheet 16 Sheet 17 Sheet 18 Sheet 19 Sheet 20 Sheet 21 Sheet 22 Sheet 23 Sheet 24 Sheet 25 Sheet 26 Sheet 27 Sheet 28
Every citation, both waysCites: the store holds 8 of 9
| Document | Relation | Office |
|---|---|---|
| EP0124312A | Cites | European Patent Office (EPO) |
| EP0613781A | Cites | European Patent Office (EPO) |
| EP0707963A | Cites | European Patent Office (EPO) |
| EP0707964A | Cites | European Patent Office (EPO) |
| EP0747221A | Cites | European Patent Office (EPO) |
| US4317124A | Cites | United States of America |
| US5121143A | Cites | United States of America |
| US5172139A | Cites | United States of America |
| PATENT ABSTRACTS OF JAPAN vol. 12, no. 141 (M-691), 28 April 1988 & JP 62 261452 A (CANON INC), 13 November 1987, | Non-patent | – |
| PATENT ABSTRACTS OF JAPAN vol. 13, no. 565 (M-907), 14 December 1989 & JP 01 235652 A (RICOH CO LTD), 20 September 1989, | Non-patent | – |
8 members in 4 offices
Priority claims4
| Document | Office | Kind | Date |
|---|---|---|---|
| 10017296 | Japan | A | |
| 10017296 | Japan | – | |
| 10017296 | – | – | – |
| JP19960100172 | – | – | – |
Members8
| Document | Office | Kind | |
|---|---|---|---|
| EP0803361A2 | European Patent Office (EPO) | A2 | |
| JPH09286105A | Japan | A | |
| EP0803361A3 | European Patent Office (EPO) | A3 | |
| US6290335B1 | United States of America | B1 | |
| EP0803361B1This record | European Patent Office (EPO) | B1 | |
| DE69723758D1 | Germany | D1 | |
| DE69723758T2 | Germany | T2 | |
| JP3559647B2 | Japan | B2 |
31 legal events, as 4 offices reported them to INPADOC
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Numbers
- Publication
- 0803361
- Publication, DOCDB
- 0803361
- Publication, EPODOC
- EP0803361
- Application
- 97302703
- Application, DOCDB
- 97302703
- Application, EPODOC
- EP19970302703
Titles3
- German
- Tintenstrahlkopf, Tintenstrahlkassette und Tintenstrahlaufzeichnungsapparat
- English
- Ink-jet head, ink-jet cartridge, and ink jet recording apparatus
- French
- Tête à jet d'encre, cartouche à jet d'encre et appareil d'enregistrement à jet d'encre
Classification
- CPC, 8
- B41J2/04533
- B41J2/04541
- B41J2/04543
- B41J2/04546
- B41J2/0458
- B41J2/1404
- B41J2/14056
- B41J2/14112
- IPC, 3
- B41J2 175
- B41J2 05
- B41J2 14
Designated states1
- Contracting states, 1
- Italy