Electrophotographic printers include photo imaging members such as photoconductive drums. The photoconductive drums are electrically charged and discharged to attract inks in a particular pattern. The photoconductive drums deposit the inks directly onto a print substrate or via an offset drum, and the inks are then fixed to the substrate to output a hard image.
Wherever possible, the same reference numbers will be used throughout the drawing(s) and accompanying written description to refer to the same or like parts.
In electrophotographic printers, a photo imaging plate (also referred to as a photo imaging surface or a photo imaging member) is charged with a uniform charge by a charge roller. Known charge rollers are consumable products, and may have lifespans less than 750,000 impressions. Some known charge rollers use ionic conduction to evenly transfer charge from the charge roller to the photo imaging plate. The materials that provide the ionic conduction are affected by currents that alter the physical properties of the material over time and eventually alter the charge applied to the photo imaging plate and/or cause the charge to be applied unevenly, at which point the charge roller must be replaced. Some known charge rollers use conductive materials to transfer the charge to the photo imaging plate. Concentrated electrical currents tend to follow particular paths through the material in these charge rollers, which causes local hot spots in the material. These hot spots result in pinholing on the photo imaging plate, which reduces the life of the photo imaging plate, and the image quality. Some known charge rollers use somewhat less conductive materials to coat the roller (having resistivities up to about 109 Ohm-centimeters (cm)) to reduce the likelihood of pinholing but tend to suffer from poor charging uniformity.
Example charge rollers and apparatus disclosed herein include a conductive inner layer and a dielectric outer layer to provide a uniform or substantially uniform electric charge to a photo imaging plate. Some example charge rollers disclosed herein include the dielectric outer layer, the conductive inner layer, and a conductive core. Example conductive cores disclosed herein are constructed using a metal such as aluminum or stainless steel. Example conductive inner layers disclosed herein are constructed using a conductive rubber (e.g., a conductive rubber doped with carbon) having a resistivity between about 1×10−6 Ohm-cm and about 1×105 Ohm-cm, although other resistivities may be used. By using a material having a lower resistivity (e.g., a higher conductivity) for the inner layer and a dielectric outer layer, example charge rollers disclosed herein provide a more uniform charge or voltage distribution to an external surface to be charged.
Example dielectric outer layers disclosed herein have an inner surface (e.g., adjacent the inner layer) and an outer surface (e.g., opposite the inner surface) and are constructed of a dielectric material having a high electrical breakdown strength (e.g., greater than about 100 Volts per micrometer (V/μm)) and/or a high resistivity (e.g., greater than about 5×1012 Ohm-cm). By using a material having high electrical breakdown strength, disclosed example outer layers prevent undesirable pinholing when using a conductive inner layer. By using a material having a high resistivity, disclosed example outer layers also prevent or substantially prevent currents that may cause depletion of the inner layer and/or substantial reduction in print quality. In some disclosed examples, the outer layer prevents more than 1 percent of current used to charge an external surface from transferring through the outer layer. Additionally, unlike known charge rollers, some example charge rollers disclosed herein do not depend on a voltage applied to the conductive inner layer or core of the charge roller to establish the voltage to which the photo imaging member is charged.
Example image forming apparatus disclosed herein include a charge roller, a bias roller, and a photo imaging plate. Some disclosed examples further include a direct current (DC) source and/or alternating current (AC) source to charge the bias roller based on a desired voltage to be applied to the photo imaging plate. Some disclosed examples include a DC source and/or AC source to charge the conductive core of the charge roller. In some examples, the bias roller applies charge to the outer surface of the charge roller during operation of the image forming apparatus. The example charge roller transfers the charge to the photo imaging member to provide a substantially uniform charge to the photo imaging plate. In some examples, an external surface is considered to have a uniform charge if the upper peak-to-peak voltage difference between charged portions of the surface is less than 20 Volts (V).
Some example charge rollers disclosed herein substantially prevent electrical current from flowing between the outer surface and the inner surface of the charge roller outer layer. In some examples, the outer layer is considered to substantially prevent current flow if the current traversing the outer layer is less than about 1 percent of the current transferred from a first external surface to a second external surface via the charge roller during operation. As a result, example charge rollers disclosed herein substantially prevent current flow between the conductive core and/or the inner layer and the bias roller, and between the core and/or the inner layer and the photo imaging plate.
Example charge rollers and image forming apparatus described herein charge a surface to a negative voltage (e.g., −1000 V) with respect to a ground. As used herein, a “higher” voltage refers to a voltage that is farther from a 0 V reference than another “lower” voltage. Thus, −200 V would be described below as “higher” than −100 V because there is a larger difference in potential between −200 V and 0 V than −100 V and 0 V.
The example inner layer 102 illustrated in
The example inner layer 102 illustrated in
The example outer layer 104 in constructed using a dielectric material. In the illustrated example of
To charge an external surface (e.g., a photo imaging plate in a printer), charges are first deposited onto the outer surface 108 (e.g., by an external source). The deposited charge(s) may be negative or positive, and example apparatus and methods to deposit charge onto the outer surface 108 are described in more detail below. In some examples, charge is transferred to the outer surface 108 using a Paschen discharge, in which a voltage difference between the outer surface 108 and the surface of the external source of charge is larger than a Paschen breakdown voltage of an intermediate medium (e.g., air). This causes charges to deposit on the outer surface 108 and an adjacent external surface. Example charge transfers are also described in more detail below.
In contrast to known charge rollers, the example charge roller 100 of
Parylene-N is advantageously used to implement the outer layer 104 in the example of
The example core 202 of
The example inner layer 204 of
While the example charge roller 200 of
The example image forming apparatus 300 further includes a photo imaging member 302 (e.g., a photoconductor, a photo-imaging plate), a bias roller 304, and electrical sources 306 and 308. As illustrated in
The example photo imaging member 302 may be a photoconductor, and/or any other type of electrophotographic surface that may be repeatedly charged and/or discharged. The photo imaging member 302 may be configured as a rotating drum and/or as an electrophotographic surface that travels along a path defined by multiple rollers. The example photo imaging member 302 of
The example bias roller 304 is constructed using a metal roller. For example, the bias roller 304 may be constructed using aluminum, stainless steel, copper, and/or other metal and, thus, has substantial rigidity. The illustrated bias roller 304 of
The example electrical source 306 of
In the illustrated example of
In the illustrated example of
The electrical source 308 applies to the core 202 a DC voltage bias of −1000 V and a peak-to-peak AC voltage of 1400 V at a frequency of 8 kilohertz (kHz). The example DC voltage offset is selected to be the voltage to which the charge roller 200 is to charge the example photo imaging member 302 (e.g., −1000 V). However, other DC voltage offsets may be selected based on the choice of charging configuration as described in more detail below and/or the thickness of the outer layer 104.
In some examples where the electrical source 308 applies an AC voltage to the core 202, the inner layer 204 is constructed to have a sufficiently high AC response time (e.g., a relatively low RC time constant). For example, when the electrical source 208 provides an AC voltage to the core 202, the inner layer 204 is about 5 mm thick, and the inner layer 204 is constructed using a material having a resistivity of about 1×105 Ohm-cm, the example inner layer 204 is also constructed to have a dielectric constant (static relative permittivity) of about 10,000 or higher. For example, the inner layer 204 may be constructed of Polyurethane rubber doped with a relatively small amount (e.g., a few percent) of carbon black, which provides short-distance conductivity without significantly changing the DC resistivity of the example Polyurethane.
As the charge roller 200 rotates, an example section 314 of the outer layer 104 approaches the nip 312 (e.g., a charge roller-bias roller interface). As the section 314 approaches the nip 312, the charge density at the section 314 increases due to the decrease in distance between the section 314 and the charged bias roller 304. Additionally, the distance between the section 314 and the bias roller 304 approaches the distance for the Paschen minimum breakdown voltage between the outer layer 104 and the bias roller 304. The Paschen minimum breakdown voltage is the lowest voltage between two surfaces with a fluid between them. A Paschen discharge may occur at or above the Paschen minimum breakdown voltage, which is the breakdown voltage at a corresponding Paschen minimum breakdown distance.
The voltage of the example core 202 changes according to the AC component of the electrical source 308. When the voltage of the example core 202 and, due to the electrical conductivity of the inner layer 204, the voltage of the inner surface 106 are higher than (e.g., farther from 0 V when the bias roller 304 is biased to a negative voltage) the voltage of the bias roller 304, the example section 314 attracts negative charges 316 onto the outer layer 104, thereby causing corresponding positive charges 318 to be attracted to the inner surface 106 from the core 202 and/or the inner layer 204.
In the illustrated example, the bias roller 304 deposits the negative charges 316 on the outer layer 104 (e.g., on the outer surface 108) via plasma discharge 320. The plasma discharge 320 of the illustrated example is an avalanche breakdown of the air between the charge roller 200 and the bias roller 304 that occurs when the voltage difference between the charge roller 200 and the bias roller 304 is greater than the Paschen minimum breakdown voltage between the outer layer 104 and the bias roller 304 at a given distance. As a result, the section 314 of the illustrated example is charged by the bias roller 304 via the plasma discharge 320 prior to reaching the nip 312. When the section 314 is sufficiently charged, the voltage difference between the section 314 and the bias roller 304 becomes less than the Paschen minimum breakdown voltage and the charging stops. At this time, the section 314 is considered charged. In some examples, multiple plasma discharges may occur before the section 314 is charged. Due to the dielectric properties of the example outer layer 104, the negative charges 316 transferred to the outer layer 104 do not dissipate, and instead remain on the section 314 as the charge roller 200 rotates.
Turning to an example photo imaging member 302 charging process, as an example charged section 322 of the outer layer 104 approaches the nip 310 (e.g., between the charge roller 200 and the photo imaging member 302), the charged section 322 approaches the Paschen minimum breakdown distance between the outer layer 104 and the photo imaging member 302. Additionally, while the example charge roller 200 rotates, the AC component of the example electrical source 308 increases and decreases the difference in voltage between the charged section 322 and the photo imaging member 302. When the charged section 322 is at or near the Paschen minimum breakdown distance, the voltage between the charged section 322 and the photo imaging member 302 becomes higher than the Paschen breakdown voltage (e.g., for the distance between the charged section 322 and the photo imaging member 302) and the charged section 322 discharges to charge the photo imaging member 302 via a Paschen discharge 324.
The discharge of the example charged section 322 and the charging of the example photo imaging member 302 reduces the voltage between them. In the illustrated example, the AC component of the example electrical source 308 also reduces the voltage between the charged section 322 and the photo imaging member 302. As a result, the example charged section 322 of
The net flow of charge between the example bias roller 304 and the example photo imaging member 302 of the illustrated example results in a current of about −0.6 mA at a photo imaging member speed of 1.2 m/s. Due to the high resistivity of the example outer layer 104, the charge transfer between the inner 106 and outer 108 surfaces of the outer layer 104 is less than 0.2 microamperes (μA), or less than 0.04 percent of the current transferred between the example bias roller 304 and the example photo imaging member 302. The example outer layer 104 may be considered to prevent or substantially prevent current flow when transferring between the surfaces 106 and 108 less than 1 percent of the current transferred between the bias roller 304 and the photo imaging member 302 in operation.
While example voltages and frequencies are described, other voltages and frequencies may be used to charge the photo imaging member 302 to a desired voltage based on the materials used and/or the geometries of the respective rollers 200, 302, 304. For example, the electrical source 306 may charge the bias roller 304 to a higher (e.g., more negative) DC voltage to increase (e.g., make more negative) the voltage to which the example photo imaging member 302 is charged.
The example Paschen breakdown voltage 404 is the same voltage-to-distance relationship, but is shown in
In the pre-nip area 408, the example photo imaging member 302 has a DC voltage of about −50 V (e.g., left by a charge eraser) and the DC component of the charge roller 200 is −1000 V. Accordingly, the example difference voltage 402 has a DC component of about −950 V. As the example section of the photo imaging member 302 moves through the pre-nip area 408, the Paschen breakdown voltage 404 decreases. When the voltage difference 402 between the photo imaging member 302 and the charge roller 200 increases above the Paschen breakdown voltage 404 in either the positive or negative directions, the charge roller 200 charges the photo imaging member 302 (e.g., when the voltage of the charge roller 200 is more negative than the voltage of the photo imaging member 302 as shown at reference numerals 414) or discharges the photo imaging member 302 (e.g., when the voltage of the photo imaging member 302 is more negative than the voltage of the charge roller 200 as shown at reference numerals 416) until the charge density of the example photo imaging member 302 is equal or approximately equal to the charge density on the outer surface 108 of the example charge roller 200. As the charge roller 200 charges the photo imaging member 302, the voltage 406 on the photo imaging member 302 increases (e.g., becomes more negative) until the voltage of the photo imaging member 302 is equal to or approximately equal to the desired voltage of −1000 V. The voltage 406 of the photo imaging member 302 is a function of the charge density and the thickness of the photo imaging member.
While the sections of the example charge roller 200 and the photo imaging member 302 travel through the nip area 410, the photo imaging member 302 is not charged or discharged. When the sections of the example charge roller 200 and the example photo imaging member 302 exit the nip area 410 and travel through the post-nip area 412, the charge roller 200 may again charge and/or discharge the photo imaging member 302. As illustrated in the example graph 400, the section of the photo imaging member 302 is charged to the desired voltage (e.g., −1000 V) prior to entering the nip area 410 and, thus, little or no additional charging or discharging occurs in the post-nip area 412 in the illustrated example.
Due to the Paschen discharge mechanism used by the example configuration illustrated in
Continuing with the example, the example section 326 carries the positive charges toward the bias roller 304 as the charge roller 200 rotates. An example charged section 328, carrying positive charges 318 transferred from the photo imaging member 302, has a lower voltage than the example core 202 as a result of the positive charges 318 and, thus, the voltage difference between the charged section 328 and the bias roller 304 is larger than the Paschen minimum breakdown voltage. As the example charged section 328 approaches the bias roller 304, the charged section 328 discharges the positive charges 318 to the bias roller 304 via a Paschen discharge. In this manner, the example charge roller 200 charges the photo imaging member 302 by removing positive charges to the bias roller 304 instead of depositing negative charges onto the photo imaging member 302.
In another example configuration, the electrical source 306 of
Continuing with the example, the portion 326 of the charge roller 200 receives positive charges 318 from the photo imaging member 302 (e.g., via a first Paschen discharge) as the portion 326 exits the nip 310. The example charged section 328, which has positive charges 318 transferred from the photo imaging member 302, carries the positive charges 318 toward the bias roller 304. The positive charges 318 increase the voltage difference between the bias roller 304 and the charge roller 200 beyond the Paschen minimum breakdown voltage. As a result, a Paschen discharge occurs and the positive charges 318 are removed from the example charged section 328 to the bias roller 304 (e.g., via a second Paschen discharge).
While some example charging configurations are described above, other configurations may additionally or alternatively be used. For example, the DC bias applied to the charge roller core 202 by the electrical source 208 (if any) is described in the examples above as between the voltage to which the photo imaging member 302 is charged and the bias voltage of the bias roller 304. However, in some other example configurations the DC bias applied to the charge roller core 202 is less than the charged voltage of the photo imaging member 302 or greater than the DC bias of the bias roller 304. Such configurations may result in more uniform charging of the photo imaging member 302.
The example outer layer 104 of
Pinholes are more likely to form in materials having lower resistances. An example outer layer constructed using Parylene-N has a resistivity of at least 1016 Ohm-cm, which is a sufficiently high resistivity to prevent pinholing when the outer layer is 10 μm thick, as demonstrated by the example results 500, or when the outer layer is 3 μm thick. The example 3 μm-thick layer of Parylene-N used in the example outer layer 104 of
The example charge roller 200 of
The example image forming apparatus 800 will be discussed with reference to an example section 802 of the outer layer 104 to be charged by the bias roller 304 and an example charged section 804 of the outer layer 104 to be discharged to charge the photo imaging member 302. As in the example image forming apparatus 300 of
As the section 802 rotates toward the nip 312, the distance between the section 802 and the bias roller 304 approaches the Paschen minimum breakdown distance. Due to the relatively high voltage between the (discharged) section 802 and the bias roller 304, a Paschen discharge may occur prior to the section 802 reaching the Paschen minimum breakdown distance. The Paschen discharge charges the section 802 to a negative voltage approximately equal to the voltage of the bias roller (e.g., −2300 V), less the Paschen breakdown voltage between the bias roller 304 and the outer layer 104. The voltage of the example section 802 is further reduced by a voltage drop between the inner 106 and outer 108 surfaces of the outer layer 104 at the section 802 during charging. While charging of the section 802 may begin before the section 802 reaches the Paschen minimum breakdown distance, the charging is generally completed by the time the section 802 passes the Paschen minimum breakdown distance.
Compared to the example AC configuration of
In the illustrated example, the voltage of the section 802 after charging is approximately equal to the sum of: the desired voltage to which the photo imaging plate is to be charged; the Paschen breakdown voltage between the outer layer 104 and the photo imaging member 302; the Paschen breakdown voltage between the outer layer 104 and the bias roller 304; and the voltage drop between the inner 106 and outer 108 surfaces of the outer layer 104 at the section 802 resulting from deposited charges 316 and 318. Thus, to charge the example photo imaging plate 302 to −1000 V, the example section 802 is charged by the bias roller 304 to approximately −2260 V.
When the example charged section 804 approaches the nip 310, the distance between the charged section 804 and the photo imaging member 302 approaches the Paschen minimum breakdown distance. Similar to the charging of the example section 802 by the bias roller 304, the example charged section 804 begins charging the photo imaging member 302 prior to the Paschen minimum breakdown distance due to the voltage between the charged section 804 and the photo imaging member 302 being higher than the Paschen minimum breakdown voltage. In the illustrated example, the charged section 804 discharges to charge the photo imaging member 302 and completes charging the section 806 by the time the charged section 804 passes the Paschen minimum breakdown distance.
Compared to the AC configuration described with reference to
While charging is described as occurring prior to the photo imaging member 302 and the section 802 entering the respective nips 310 and 312, the example photo imaging member 302 and the example section 802 may also be charged after exiting the nips 310 and 312. For example, as the charge roller 200 continues to rotate, the distance between the section 802 and the bias roller 304 again approaches the Paschen minimum breakdown distance after the section 802 exits the nip 312. If the section 802 and/or portions of the section 802 are undercharged, additional Paschen discharge may occur to further charge the section 802 to the appropriate voltage. The example photo imaging member 302 may be similarly charged by the charged section 804 after exiting the nip 310.
While the examples described above include example materials and operate at example voltages, currents, and/or frequencies, the materials, voltages, currents, and/or frequencies may be modified to suit a particular application. For example, while the charge rollers described above are discussed with reference to charging a photo imaging member to −1000 V, the charge roller may be used to provide other voltages and/or charge densities to other external surfaces, in which case any of the sizes, voltages, currents, frequencies, materials, and/or other aspects of the example charge rollers may be modified. As another example, constructing the example outer layer of the example charge roller using a different material may cause a change in the Paschen breakdown voltage between the outer layer and the external surface. In such a case, any of the sizes, voltages, currents, frequencies, materials, and/or other aspects of the charge roller may be modified to charge the external surface to a desired voltage.
The above-disclosed example charge rollers and image forming apparatus including the charge rollers provide a substantially uniform charge to a photo imaging member surface. While the example AC configuration described in conjunction with
Although certain example methods, apparatus and articles of manufacture have been described herein, the scope of coverage of this patent is not limited thereto. On the contrary, this patent covers all methods, apparatus and articles of manufacture fairly falling within the scope of the claims of this patent.
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/US2011/023825 | 2/4/2011 | WO | 00 | 7/25/2013 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2012/105987 | 8/9/2012 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
4371252 | Uchida et al. | Feb 1983 | A |
4380384 | Ueno et al. | Apr 1983 | A |
5745820 | Iwakura et al. | Apr 1998 | A |
5768653 | Fare | Jun 1998 | A |
5970302 | Yamane | Oct 1999 | A |
5974277 | Yamane et al. | Oct 1999 | A |
6381432 | Hattori | Apr 2002 | B1 |
6909859 | Nakamura et al. | Jun 2005 | B2 |
7298993 | Lee et al. | Nov 2007 | B2 |
7756439 | Kosuge et al. | Jul 2010 | B2 |
20080166154 | Watanabe et al. | Jul 2008 | A1 |
20100092204 | Askren et al. | Apr 2010 | A1 |
20100166459 | Kawashima | Jul 2010 | A1 |
20100296851 | Toyooka et al. | Nov 2010 | A1 |
20100296852 | Higaki | Nov 2010 | A1 |
Number | Date | Country |
---|---|---|
64-073367 | Mar 1989 | JP |
6222649 | Aug 1994 | JP |
H087485 | Jan 1996 | JP |
2001-034040 | Feb 2001 | JP |
Entry |
---|
International Bureau, “International Search Report”, issued in connection with PCT application No. PCT/US2011/023825, mailed Oct. 28, 2011, (3 pages). |
Number | Date | Country | |
---|---|---|---|
20130308982 A1 | Nov 2013 | US |