Aspects of the invention relate to hard imaging apparatus charging devices, imaging assemblies, imaging assembly charging methods, and hard imaging device image bearing member charging methods.
Charge rollers (CRs) are used to charge a photoconductor in hard imaging systems (e.g., laser-printer imaging systems). Similar to Scorotron/Corona charging, charge rollers use air ionization to charge a photoconductor. However, a charge roller has increased charging efficiency (close to 100% charging efficiency) and uses lower voltages (˜1500V) compared with Scorotron charging (˜6500V). Physical contact of a charge roller with a photoconductor may cause print quality defects that are mainly driven by the interaction of the charge roller with materials remaining on the photoconductor after cleaning operations of the photoconductor. Materials remaining on the photoconductor may create sticky polymers which coat the photoconductor. These interactions are even more intensive with liquid electrophotographic processes where, after cleaning the photoconductor, imaging oil comprising dissolved materials and charge directors may still be present on the photoconductor surface giving rise to several print quality issues.
In general, a charge roller contacting a photoconductor may interact with a remaining image formed on the photoconductor, thereby creating ghosting effects (e.g., with the circumference of the charge roller). Further, the charge roller contacting the photoconductor may also interact with other materials (e.g., imaging oil) that remain on the photoconductor, contaminate the photoconductor with leak materials (e.g., conductive ions from the charge roller rubber), and create pin holes in the photoconductor in the charge roller/photoconductor nip. The above drawbacks may contribute to photoconductor quality issues by interfering with the photoconductor/blanket image transfer, interfering with image development, and interfering with cleaning of the photoconductor. The above drawbacks may also cause problems relating to photoconductor lateral conductivity, and uneven photoconductor charging. As a result, lifetime of consumables may decrease and the printing cost per page may increase. Other problems with liquid electrophotographic processes using a photoconductor with a seam area include print quality defects due to accumulation of imaging fluid in defects or wrap-over sections (e.g., seam regions) on the photoconductor. Movement of the charge roller over a section of the photoconductor may elevationally attract some of the accumulated materials and duplicate them into an image area. The extra imaging oil may not only cause disturbance of normal imaging processes but also cause disruption of the Paschen curve and the photoconductor charging voltages, thereby leading to permanent photoconductor damage.
At least some embodiments of the invention relate to hard imaging apparatus charging devices, imaging assemblies, imaging assembly charging methods, and hard imaging device image bearing member charging methods.
In one aspect, a hard imaging apparatus charging device is disclosed. The charging device may include first and second end members, and an intermediate member connecting the first and second end members. The intermediate member may have a length corresponding to an imaging area of the image bearing member. The intermediate member may be configured to charge the imaging area used to form latent images on the image bearing member during hard imaging operations of the hard imaging apparatus. The first and second end members of the charging device may be configured to maintain a predetermined spaced charging clearance between the intermediate member and the imaging area of the image bearing member. The first and second end members and the intermediate member of the charging device may include a monolithic layer. The charging device may include an outer layer configured to charge the image bearing member. The layer may be formed such that the first and second end members have a larger radius than a radius of the intermediate member.
In another aspect, an imaging assembly charging method is described. The charging method may include first providing a photoconductor having a plurality of portions of different radii, second providing a charging device configured to charge the photoconductor, rotating the photoconductor adjacent the charging device to charge the photoconductor, and third providing a clearance between the photoconductor and the charging device during charging of the photoconductor, wherein the clearance may be provided using at least one of the photoconductor or the charging device. The charging method may include configuring the photoconductor to have first and second end portions and an intermediate portion. The first and second end portions may be configured to have a larger radius than a radius of the intermediate portion, the radii measured from a central axis of the photoconductor.
Other aspects of the invention are disclosed herein as is apparent from the following description and figures.
Referring to
Referring to
The controller 202 may be configured to control operations of individual components (e.g., 204, 205, 210) of the hard imaging device 100. Exemplary operations of controller 202 include image data processing operations (e.g., rasterization) of data received from an external source (not shown), internally generated, or otherwise accessed. Further details of controller 202 are described below at
The scanning apparatus 204 may be configured to scan information formatted by controller 202 onto a photoconductor 206 to form latent images. Apparatus 204 may comprise a laser or other light source configured to output a light beam to scan the information in one embodiment.
The imaging assembly 205 includes photoconductor 206 and a charging device 208 in one embodiment. Photoconductor 206 is alternately referred to herein as an image bearing member. Charging device 208 may also be referred to as a charge roller.
Photoconductor 206 includes a rotating imaging surface (e.g., reference numeral 408 of
The charge roller 208 may be configured to charge photoconductor 206 to enable forming of latent images on the photoconductor 206. The charge roller 208 may be rotatably positioned adjacent photoconductor 206 to charge the photoconductor 206. Following charging of photoconductor 206, latent images are formed upon photoconductor 206 using scanning apparatus 204. Further details of exemplary charge rollers 208 are set forth below at FIGS. 4, 5A-5C.
The developer/fusing assembly 210 may be configured to develop information written onto the photoconductor 206 using a marking agent (e.g., toner), and transfer and fuse the developed image to media 212 (e.g., hard-imaging media such as paper, transparencies, etc.).
Processing circuitry 302 may be configured to output data to scanning apparatus 204 and to issue command signals to photoconductor 206 and charge roller 208 to control respective operations thereof (e.g., charging of photoconductor 206 using charge roller 208, forming of latent images on the photoconductor 206, etc.).
In one embodiment, processing circuitry 302 may comprise circuitry configured to execute provided programming. For example, processing circuitry 302 may be implemented as a microprocessor or other structure configured to execute executable instructions of programming including, for example, software and/or firmware instructions. Other exemplary embodiments of processing circuitry 302 include hardware logic, PGA, FPGA, ASIC, and/or other structures. These examples of processing circuitry 302 are for illustration and other configurations are possible for implementing operations discussed herein.
The storage device 304 may be configured to store electronic data, file systems having one or more electronic files, programming such as executable instructions (e.g., software and/or firmware for use by processing circuitry 302), and/or other digital information and may include processor-usable media. For example, electronic data and/or file systems may be stored in the form of a table in database 306 of the storage device 304, and stored information may be configured for retrieval by the processing circuitry 302. Processor-usable media includes any article of manufacture which can contain, store, or maintain programming, data and/or digital information for use by or in connection with an instruction execution system including processing circuitry in the exemplary embodiment. For example, exemplary processor-usable media may include any one of physical media such as electronic, magnetic, optical, electromagnetic, infrared or semiconductor media. Some more specific examples of processor-usable media include, but are not limited to, a portable magnetic computer diskette, such as a floppy diskette, zip disk, hard drive, random access memory, read only memory, flash memory, cache memory, and/or other configurations capable of storing programming, data, or other digital information.
Interface 308 may be configured to communicate electronic data externally of the controller 202, for example, with respect to external devices of hard imaging device 100, to communicate control signals to form latent images on the photoconductor 206, etc.
As discussed further below in accordance with some embodiments, photoconductor 206 may include a plurality of different regions. The plural regions may correspond to imaging and non-imaging regions 408, 406 (
The charge roller 208 may be positioned adjacent photoconductor 206 and configured to rotate about an axis to charge the photoconductor 206. The charge roller 208 may include a core member 403 (e.g., comprising a conductive material) and a layer of material 404 (e.g., high resistivity rubber) formed on the core member 403. The core member 403 may be configured to receive a voltage from voltage supply apparatus 410 to enable charging of the photoconductor 206. In one embodiment, the charge roller 208 is positioned such that a predetermined clearance “h” is provided between the charge roller 208 and the photoconductor 206 during charging of the photoconductor 206.
A Paschen curve describes air ionization breakdown voltages as a function of the clearance “h” between exposed electrodes. In one embodiment, layer 404 of charge roller 208 and layer 409 of photoconductor 206 act as the electrodes for charging the photoconductor 206. A voltage Vg in the clearance “h” depends on the splitting of charge roller voltage VCR between the photoconductive material layer 409 and the clearance “h”. The voltage Vg is provided by the following equation:
where “Vcr” is the metal core voltage of charge roller 208; “Vphoto” is the charge voltage of photoconductor 206; “Velastomer” is the voltage drop across elastomer or rubber layer 404; “h” is a clearance between exposed electrodes (e.g., a gap between electrodes comprising photoconductive material layer 409 and the charge roller 208); “∈” is the dielectric constant of layer 409 of the photoconductor 206; and L is the thickness of photoconductive material layer 409 of the photoconductor 206.
Referring to
Photoconductor 206 may be made by forming a plurality of layers (not shown) on a cylindrical drum. Exemplary layer 409 of material coated on the cylindrical drum to form the photoconductor 206 may include Mylar, aluminum, a charge generating layer, and/or a charging transport layer. The plurality of regions (e.g., imaging and non-imaging regions 408, 406, respectively) of the photoconductor 206a may be made from a continuous monolithic layer of material (e.g., layer 409 (
In one embodiment, end portions 502 and intermediate portion 504 of layer 404 of charge roller 208 may be formed as a continuous layer (e.g., a monolithic layer of high resistivity rubber) of material about a core member 403. For example, the charge roller 208 may include a monolithic layer 404 configured to charge the photoconductor 206, and the layer 404 may be formed such that the end portions 502 have a larger radius than a radius of the intermediate portion 504.
Referring to
Continuing to refer to
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As illustrated in the exemplary embodiments of
As shown in the graph, the inventors have observed that no ionization occurred for VCR=500V for all clearances “h”. Minimal VCR where ionization occurred was found to be 573V with an associated clearance h=19 microns, referred to herein as the charging clearance, for exemplary photoconductors described herein. The charging clearance corresponds to a maximum spaced distance “h” between charge roller 208 and the photoconductor 206 wherein the charging efficiency is substantially the same as if the charge roller 208 contacts the photoconductor 206. Typically, the charging clearance is about 19 microns with minor variations depending on such factors as the characteristics of the photoconductor layer 409, and air pressure and humidity in the charging environment, etc. Charging efficiency decreases in arrangements wherein the distance “h” exceeds this charging clearance.
For VCR=700V, the inventors have observed that ionization started at a clearance “h” of 50 microns and continued until the clearance “h” was decreased to about 8 microns. Once ionization begins, the surface of the photoconductor 206 attracts charges and counter charges, thereby increasing its surface voltage. However, surface voltage of the charge roller 208 was not found to have significantly changed due to the attraction of counter charges as charge roller 208 was made conductive. Hence, the voltage Vg within the clearance “h” may be reduced until the voltage reaches the Paschen value for a given clearance “h”. As the clearance “h” is reduced for different designs of the photoconductor and charge roller, increased ionization occurs (e.g., due to lower Paschen voltage limit) thereby increasing charge on photoconductor 206 until the charging clearance is reached. The voltage Vg was found to be pinned to the Paschen curve until the clearance “h” reached a predetermined clearance (e.g., charging clearance). As mentioned previously, the charging clearance was observed to be about 19 microns in exemplary embodiments.
In one exemplary case, the inventors have observed that if the clearance “h” drops below the charging clearance, no additional charging of the photoconductor 206 occurred as the VCR split drops Vg below the Paschen curve due to accumulated charges on the surface of the photoconductor 206. In one example, the charge roller 208 was observed to charge the photoconductor 206 to a maximum voltage only up to the charging clearance, and no additional charging of the photoconductor 206 occurred with clearances below the charging clearance. For the above-noted example, charging efficiency of the photoconductor 206 obtained at the charging clearance remained the same for all clearances “h” less than the charging clearance (e.g., from 19 microns to 0 microns), and the photoconductor 206 has been charged to its maximum potential (e.g., Charge Roller voltage −573V) at about the charging clearance.
The charging efficiency of the photoconductor 206 with clearance “h” between the charge roller 208 and the photoconductor 206 may be compared with the charging efficiency where the charge roller 208 contacts the photoconductor 206, and the results are shown in the below table:
As can be seen from the above Table I, even though no contact is established between the charge roller 208 and the photoconductor 206 and a clearance “h” is maintained between the charge roller 208 and the photoconductor 206, the charging efficiency of the photoconductor 206 remained uniform. Moreover, the charging uniformity is improved by maintaining a clearance “h” between the charge roller 208 and the photoconductor 206 compared to approaches wherein the charge roller contacts the photoconductor.
Exemplary advantages of some embodiments include providing a clearance between a charge roller and a photoconductor to reduce chances of damage to the charge roller due to contact with the photoconductor. Since no direct charging of the photoconductor occurs in embodiments having a clearance between the charge roller and the photoconductor, increased charging uniformity in both in-scan and cross-scan directions may be possible. Solutions provided by some embodiments provide a charging system which is more robust to misalignments and material defects during manufacturing. Other advantages of using a spaced charge roller to charge a photoconductor include efficiencies related to cost, size, and Ozone generation rate.
The protection sought is not to be limited to the disclosed embodiments, which are given by way of example only, but instead is to be limited only by the scope of the appended claims.