1. Field of the Invention
The present invention relates to charging devices with magnetic particles.
2. Description of the Related Art
Many image-forming apparatuses based on electrophotography or electrostatic recording have conventionally been created. The schematic structure of such an apparatus and its operation are briefly described below with reference to
When a copy-start signal is input to an image-forming apparatus shown in
A developing device 4 containing toner particles develops the electrostatic latent image into a toner image on the photosensitive drum 1. A transfer device 7 electrostatically transfers the toner image onto a transfer material which is then electrostatically separated and carried to a fusing device 6. The toner image is thermally fused onto the transfer material to output the image.
After the toner image is transferred, a cleaner 5 removes contaminants adhering to the surface of the photosensitive drum 1, including toner residue after the transfer. In addition, if necessary, the photosensitive drum 1 is exposed to light by a pre-exposure device 8 to eliminate the optical memory of the image exposure for repeated use in image formation.
Conventionally, charging devices for use in an image-forming process with an electrophotographic image-forming apparatus as described above are typically based on corona charging, as mentioned above. In recent years, however, contact charging has been intensively researched and developed, and has already been put into practical use. Contact charging has the advantages of yielding a small amount of ozone by discharge and low power consumption.
In contact charging, a charging member is brought into contact with a photosensitive member and is supplied with voltage to charge the photosensitive member. Examples of charging devices based on this method include charging rollers and magnetic brush charging devices. Among them, a magnetic brush charging device, in which a magnetic brush serves as a contact charging member, is used to achieve contact charging stability.
A magnetic brush charging device magnetically holds conductive magnetic particles directly on the surface of a magnet or on the surface of a sleeve including the magnet. The magnetic particles are brought into contact with the surface of a photosensitive member to charge the surface of the photosensitive member.
When a magnetic brush charging device is used to charge, for example, an organic photosensitive member having a surface layer in which fine conductive particles are dispersed (according to, for example, Japanese Patent Laid-Open No. 06-003921, which corresponds to U.S. Pat. No. 5,809,379) or an amorphous-silicon-based photosensitive member, the surface of the photosensitive member can be charged to a potential substantially equivalent to the DC component of a bias applied to a magnetic brush. Such a charging method is hereinafter referred to as magnetic brush injection charging. This method involves no discharging phenomenon as used in contact charging to provide ozone-free charging with low power consumption.
Unfortunately, however, a photosensitive member of an image-forming apparatus including a magnetic brush injection charging device has a shorter life than that of an image-forming apparatus including a corona charging device. The surface of the photosensitive member wears by friction against magnetic particles after repeated use. This problem is more serious when a sleeve and the photosensitive member are rotated in opposite directions to increase the possibility of contact between the magnetic particles and the photosensitive member for higher charging stability.
The life of the photosensitive member can be significantly increased by making a modification to the photosensitive member, such as a hard protective layer provided on the surface of the photosensitive member, or a modification to the charging device, such as the coating of the magnetic particles and the reduction of the pressure between the magnetic particles and the photosensitive member for lower friction against the magnetic particles.
The pressure between the magnetic particles and the photosensitive member can be reduced by, for example, extending the distance between the sleeve and the photosensitive member or reducing the amount of magnetic particles carried on the sleeve. Such approaches, however, also have adverse effects such as insufficient contact between the magnetic particles and the photosensitive member. This results in reduced charging stability and the adhesion of the magnetic particles from the sleeve to the photosensitive member.
The most serious effect among the adverse effects is the adhesion of the magnetic particles to the photosensitive member at the outermost ends of a magnetic particle carrying region of the sleeve. Magnetic particles adhering to the photosensitive member may undesirably intrude into a developing device to degrade image quality, cause transfer defects in a transfer device, and damage the photosensitive member at a cleaner.
The adhesion of the magnetic particles to the photosensitive member at the outermost ends of the magnetic particle carrying region of the sleeve results from an unstable magnetic particle carrying state. Such an unstable state occurs probably because the magnetic force of the magnet included in the sleeve is weak at the ends of the sleeve. In addition, the contact between the magnetic particles and the photosensitive member is poorer at the outermost ends of the sleeve than the center thereof. The photosensitive member is therefore insufficiently charged at the outermost ends of the sleeve to produce a potential difference between the sleeve and the photosensitive member. This potential difference can cause the magnetic particles to adhere to the photosensitive member. Some methods, including the insulation of the ends of the sleeve, have been proposed to prevent the problem of the potential difference between the sleeve and the photosensitive member.
If, additionally, the pressure between the magnetic particles and the photosensitive member is reduced to inhibit the wear of the photosensitive member, the magnetic particle carrying state becomes unstable at the ends of the magnetic particle carrying region of the sleeve. This is more likely to result in an insufficient effect of preventing the magnetic particles carried at the ends of the sleeve from adhering to the photosensitive member.
The present invention is directed to a charging device that has a stable amount of magnetic particles carried at the ends of a magnetic particle carrying member, that can prevent the magnetic particles on the magnetic particle carrying member from adhering to a member to be charged, and that can inhibit the wear of the member to be charged.
In one aspect of the present invention, a charging device for charging a member to be charged includes magnetic particles; a magnetic particle carrying member that magnetically carries the magnetic particles into contact with the member to be charged, the magnetic particle carrying member having end regions in a longitudinal direction and a central region in the longitudinal direction; and a magnetic particle adjusting unit configured to adjust an amount per unit area of magnetic particles carried on the magnetic particle carrying member so that the amount per unit area of magnetic particles is larger in the end regions than in the central region. The end regions of the magnetic particle carrying member are regions outside of a region of the member to be charged where an electrostatic latent image is formed in the longitudinal direction. The central region of the magnetic particle carrying member is a region inside the region of the member to be charged where the electrostatic latent image is formed in the longitudinal direction.
Further features and advantages of the present invention will become apparent from the following description of exemplary embodiments with reference to the attached drawings.
Referring to
A magnetic brush charging device is described below. Conductive magnetic particles are magnetically held directly on a magnet or on a sleeve including the magnet. The magnet or the sleeve is fixed or rotatable with respect to a photosensitive member. The magnetic particles are brought into contact with the photosensitive member, which is supplied with a voltage through the magnetic particles, so as to start a charging process.
The magnetic brush charging device 30A used in this embodiment has a rotatable, nonmagnetic charging sleeve (magnetic particle carrying member) 31 containing a fixed magnet 32. The magnetic particles 34 are carried on the charging sleeve 31 in a brush form by a magnetic field. The magnetic particles 34 are controlled by a magnetic particle control member 33A, and are carried as the charging sleeve 31 rotates.
The charging sleeve 31 rotates in the direction opposite to the rotational direction of the photosensitive member 1 in the area between the charging sleeve 31 and the photosensitive member 1. The charging sleeve 31 is supplied with the charging voltage to charge the photosensitive member 1 through the magnetic particles 34 to nearly the potential corresponding to the charging voltage. The charging sleeve 31 may be rotated in the direction opposite to the rotational direction of the photosensitive member 1 in the area between the charging sleeve 31 and the photosensitive member 1 to improve injection charging properties.
The magnetic particles 34 used may have an average particle size of 10 to 100 μm, a saturation magnetization of 20 to 250 emu/cm3, and a resistance of 102 to 1010 Ω·cm. Although the lowest resistance possible offers better charging properties, the resistance may be 106 Ω·cm or more in consideration of insulation defects of the photosensitive member 1, such as pin holes. In this embodiment, the resistance of the magnetic particles 34 is adjusted by oxidation and reduction of the ferrite surfaces, and the magnetic particles 34 are then subjected to coupling. The magnetic particles 34 used for charging in this embodiment have an average particle size of about 25 μm, a saturation magnetization of about 200 emu/cm3, and a resistance of about 5×106 Ω·cm.
The resistance of the magnetic particles 34 used in this embodiment is measured by placing 2 g of the magnetic particles 34 into a metal cell having a bottom area of 228 cm2, applying a load of 6.6 kg/cm2, and applying a voltage of 100 V.
In this embodiment, a test described below is carried out to determine the amount of wear of the photosensitive drum 1 and the amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeve 31 relative to the amount of magnetic particles carried on the charging sleeve 31.
In this embodiment, an image assurance width refers to the longitudinal width of the region of the charging sleeve 31 corresponding to a region of the photosensitive member 1 in which an image is formed (a region in which a toner image is formed by a developing device). A magnetic particle carrying width refers to the width of a region of the charging sleeve 31 in which the magnetic particles 34 are carried by magnetic force. In this embodiment, the magnetic particle carrying width equals to the width of the magnet 32 in the charging sleeve 31. The ends of the charging sleeve 31 are insulated by resin coating to eliminate potential differences at the ends of the charging sleeve 31. An injection charging width refers to the width of the uninsulated region of the charging sleeve 31, in which the magnetic particles 34 are brought into contact with the photosensitive member 1 to perform injection charging. The injection charging width is adjusted to a width larger than the image assurance width and smaller than the magnetic particle carrying width. The resin coating has a thickness of about 50 μm. The relationship between the above widths in the longitudinal direction is shown in
In this embodiment, as shown in
The above arrangement poses no serious problem in the test because magnetic particles adhering to the photosensitive member 1 within the image assurance width are recovered by the charging sleeve 31.
The pre-exposure lamp 8 used is an LED with a wavelength of about 660 nm. The pre-exposure lamp 8 is supplied with a voltage of 20 V from a pre-exposure power supply 81 to expose the photosensitive member 1 to light at about 370 lux-sec.
The photosensitive member 1 has a diameter of 80 mm and a rotational speed of 400 mm/sec. The charging sleeve 31 has a diameter of 16 mm and a rotational speed of 180 mm/sec, and the surface thereof is processed by blasting with alundum (180 mesh). A charging container contains 100 g of the magnetic particles 34. In charging, a charging bias device 35 supplies the charging sleeve 31 with a charging bias with a DC voltage of 600 V, an AC voltage of 300 Vpp, and a frequency of 1 kHz.
The amount of magnetic particles carried on the charging sleeve 31 at the nip between the photosensitive member 1 and the charging sleeve 31 is measured with a measurement jig 40 (shown in
The amount of wear of the photosensitive member 1 is determined by measuring the thickness of the surface layer thereof before and after a durability test and then calculating the difference. The thickness of the surface layer is measured with an interference thickness gauge at a total of 20 spots (all in the image assurance region), namely 5 spots at intervals of 4 cm from the center to the ends of the photosensitive member 1 in the longitudinal direction by 4 spots in the circumferential direction of the photosensitive member 1. The measured values are averaged to determine the thickness of the surface layer of the photosensitive member 1.
As described above, the magnetic particles 34 adhere to the photosensitive member 1 mainly at the ends of the charging sleeve 31, and few magnetic particles 34 adhere to the photosensitive member 1 in the center of the charging sleeve 31. Accordingly, the amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeve 31 may be measured to determine whether the adhesion of the magnetic particles 34 is acceptable for the photosensitive member 1. As shown in
Comparative Example 1-1 is described below as a specific comparative example for the first embodiment. In this example, the magnetic particle control member 33A used was a nonmagnetic plate (control blade) 331 shown in
The distance between the control blade 331 and the charging sleeve 31 was adjusted so that the amount of magnetic particles carried in the central region of the charging sleeve 31 in the longitudinal direction was about 50, 100, 150, and 200 mg/cm2. The distance between the charging sleeve 31 and the photosensitive member 1 was adjusted to about 300, 400, 500, 600, and 700 μm. For each combination of the above conditions, an idling durability test equivalent to 10,000 copies of A4 sheets was carried out to measure the amount of wear of the photosensitive member 1 and the amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeve 31.
According to the test results, a longer distance between the charging sleeve 31 and the photosensitive member 1 or a smaller amount of magnetic particles carried on the charging sleeve 31 results in a smaller amount of wear of the photosensitive member 1, but also results in a larger amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeve 31.
Next, the potential at the development position was measured for each condition using an electrostatic voltmeter (Model 344, manufactured by Trek, Inc.).
According to the above results, a longer distance between the charging sleeve 31 and the photosensitive member 1 or a smaller amount of magnetic particles carried on the charging sleeve 31 results in a smaller amount of wear of the photosensitive member 1, but also results in a larger amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeve 31 and lower charging properties of the charging device 30A.
Accordingly, the amount per unit area of magnetic particles carried in the central region of the charging sleeve 31 in the longitudinal direction, namely M (mg/cm2), and the distance between the charging sleeve 31 and the photosensitive member 1 in the central region of the charging sleeve 31 in the longitudinal direction, namely S (μm), may be controlled such that M<0.35S in view of the amount of wear of the photosensitive drum 1 and M≧0.125S in view of the maintenance of the charging properties. Hence, a reduction in the amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeve 31 is desired within the above range.
Example 1-1 is described below as a specific example of the first embodiment. Instead of the plate 331 used in Comparative Example 1-1, a control blade 332 was used as the magnetic particle control member (magnetic particle adjusting unit) 33A to increase the amount of magnetic particles carried at the ends of the magnetic particle carrying region of the charging sleeve 31.
The above control blade 332 was confirmed to provide a larger amount of magnetic particles carried at the ends of the magnetic particle carrying region of the charging sleeve 31 in the longitudinal direction than the amount of magnetic particles carried in the center by about 40 mg/cm2. In addition, the above control blade 332 was visually confirmed to allow the stabilization of the magnetic particle carrying state as well as the increase in the amount of magnetic particles carried at the ends of the magnetic particle carrying region of the charging sleeve 31. Such a larger amount of magnetic particles carried had greater opportunity for contact with each other. This made it difficult for the photosensitive member 1 to remove the magnetic particles 34 from the charging sleeve 31 when the magnetic particles 34 were brought into contact with the photosensitive member 1, thus inhibiting carrier adhesion.
The same test as in Comparative Example 1-1 was carried out using the above control blade 332. The test results are shown in
The results in
In this case, the amount of wear of the photosensitive drum 1 may increase at the ends of the charging sleeve 31. This increase, however, is negligible for practical use if the amount of magnetic particles carried is increased outside the image assurance region in the longitudinal direction.
As described in Comparative Example 1-1, the conditions of the charging sleeve 31 may be controlled such that M<0.35S in view of the amount of wear of the photosensitive drum 1 and M≧0.125S in view of the maintenance of the charging properties.
An image-forming apparatus used in a second embodiment has substantially the same structure as that used in the first embodiment except for a magnetic brush charging device 30B.
In
An a-Si-based photosensitive member is produced by converting gas into plasma with high frequencies or microwaves and solidifying and depositing it on an aluminum cylinder. This type of photosensitive member therefore has the problem that nonuniform plasma causes variations in thickness and composition in the circumferential direction.
An a-Si-based photosensitive member exhibits a significantly larger amount of potential decay in a dark state after charging than an organic photosensitive member. In addition, the amount of potential decay increases by optical memory in image exposure. Thus, a pre-exposure device is required to erase the optical memory in a previous cycle. Accordingly, the amount of potential decay between charging and development is extremely large, namely about 100 to 200 V. In such a state, the variations in thickness described above result in potential variations of about 10 to 20 V in the circumferential direction.
An a-Si-based photosensitive member is more susceptible to such potential variations than an organic photosensitive member because an a-Si-based photosensitive member has a higher electrostatic capacity and lower contrast than an organic photosensitive member, thus exhibiting more significant variations in density.
For example, multiple charging of the photosensitive member is effective against the above problem. The increase in dark decay due to optical memory described above can be reduced by multiple charging in which first charging greatly reduces the optical memory to provide a smaller amount of dark decay after second charging. Multiple charging can therefore greatly reduce potential ghosts and potential variations.
The effect described above is the advantage of the double charging.
The magnetic brush charging device 30B used in this embodiment has a first charging sleeve 310 and a second charging sleeve 311 that are rotatable and nonmagnetic and each contain a fixed magnet 32. Charging magnetic particles 34 are held on the charging sleeves 310 and 311 in a brush form by a magnetic field. The magnetic particles 34 are controlled by a magnetic particle control member 33B, and are carried as the charging sleeves 310 and 311 rotate.
The magnetic particles 34 are kept away from the vicinity of adjacent repelling poles, which are the same pole, of the charging sleeves 310 and 311. In this embodiment, the adjacent repelling poles are positioned so that the magnetic particles 34 move around the charging sleeves 310 and 311 rather than enter the space between the charging sleeves 310 and 311.
The charging sleeves 310 and 311 rotate in the direction opposite to the rotational direction of the photosensitive member 1 in the area between the charging sleeves 310 and 311 and the photosensitive member 1. The charging sleeves 310 and 311 are supplied with charging voltage to charge the photosensitive member 1 through the magnetic particles 34 to nearly the potential corresponding to the charging voltage.
The photosensitive member 1 has a diameter of 80 mm and a rotational speed of 400 mm/sec. The first and second charging sleeves 310 and 311 have a diameter of 16 mm and a rotational speed of 180 mm/sec, and the surfaces thereof are processed by blasting with alundum (180 mesh). A charging container contains 100 g of the magnetic particles 34. In charging, a charging bias device 36 supplies the first charging sleeve 310 with a charging bias with a DC voltage of 600 V, an AC voltage of 300 Vpp, and a frequency of 1 kHz while another charging bias device 35 supplies the second charging sleeve 311 with a charging bias with a DC voltage of 500 V, an AC voltage of 300 Vpp, and a frequency of 1 kHz.
As in the first embodiment, additionally, the ends of the first and second charging sleeves 310 and 311 are insulated by resin coating so that the width of the uninsulated region is larger than the image assurance width and is smaller than the magnetic particle carrying width. The resin coating has a thickness of about 50 μm.
Comparative Example 2-1 is described below as a specific comparative example for the second embodiment. In this example, as in Comparative Example 1-1, the magnetic particle control member 33B used was the nonmagnetic plate (control blade) 331 shown in
The distance between the control blade 331 and the charging sleeve 31 was adjusted so that the amount of magnetic particles carried in the central region of the charging sleeve 31 in the longitudinal direction was about 50, 100, and 150 mg/cm2. The distances between the charging sleeves 310 and 311 and the photosensitive member 1 were adjusted to about 300 and 500 μm. For each combination of the above conditions, an idling durability test equivalent to 10,000 copies of A4 sheets was carried out to measure the amount of wear of the photosensitive member 1 and the amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeves 310 and 311.
The amount of wear of the photosensitive member 1 and the amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeves 310 and 311 were measured by the same methods as in Comparative Example 1-1.
According to the test results, longer distances between the charging sleeves 310 and 311 and the photosensitive member 1 or a smaller amount of magnetic particles carried on the charging sleeves 310 and 311 results in a smaller amount of wear of the photosensitive member 1, but also results in a larger amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeves 310 and 311.
Two charging sleeves were used in this example, though the amount of wear was similar to that for a single charging sleeve. The second charging sleeve 311 is positioned upstream in the movement direction of the magnetic particles 34 in the area (nips) between the charging sleeve 310 and 311 and the photosensitive member 1. The second charging sleeve 311 has a great effect on the amount of wear, while the first charging sleeve 310 has no significant effect on the amount of wear. The pressure between the first charging sleeve 310 and the photosensitive member 1 is lower than that between the second charging sleeve 311 and the photosensitive member 1 because only magnetic particles passing through the nip between the second charging sleeve 311 and the photosensitive member 1 pass through the nip between the first charging sleeve 310 and the photosensitive member 1.
In addition, the amount of magnetic particles carried on the second charging sleeve 311 has a great effect on the amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeves 310 and 311. The second charging sleeve 311 is positioned downstream in the rotational direction of the photosensitive member 1 to recover magnetic particles detached from the first charging sleeve 310, which is positioned upstream in the rotational direction of the photosensitive member 1. The upstream and downstream sides in the rotational direction of the photosensitive member 1 are defined with respect to the position of a developing device; the downstream side is defined as the side near the developing device.
Example 2-1 is described below as a specific example of the second embodiment.
The above control blade 333 was visually confirmed to increase the amount of magnetic particles carried at the ends of the magnetic particle carrying region of the charging sleeves 310 and 311 and stabilize the magnetic particle carrying state. Subsequently, the same test as in Comparative Example 2-1 was carried out.
As in the case of Example 1-1, the test results show that the amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeves 310 and 311 may be inhibited with no increase in the amount of wear of the photosensitive drum 1 by increasing only the amount per unit area of magnetic particles carried in the end regions of the charging sleeves 310 and 311 relative to that of magnetic particles carried in the central regions.
In this example, as in Comparative Example 2-1, the second charging sleeve 311 has a great effect on the amount of wear. As described in Comparative Example 1-1, additionally, at least the conditions of the second charging sleeve 311 may be controlled such that M<0.35S in view of the amount of wear of the photosensitive drum 1 and M≧0.125S in view of the maintenance of the charging properties. Within the above range, the second charging sleeve 311 provides a satisfactorily small amount of wear of the photosensitive drum 1 and excellent charging properties.
In this case, the amount of wear of the photosensitive drum 1 may increase at the ends of the charging sleeves 310 and 311. This increase, however, is negligible for practical use if the amount of magnetic particles carried is increased outside the image assurance region in the longitudinal direction.
An image-forming apparatus used in a third embodiment has substantially the same structure as that used in the first embodiment except that a positively charged organic photosensitive member is used as the photosensitive member 1 instead of an a-Si-based photosensitive member.
Referring to
The photosensitive member 1 has a diameter of 80 mm and a rotational speed of 400 mm/sec. A charging sleeve 312 has a diameter of 24 mm and a rotational speed of 180 mm/sec, and the surface thereof is processed by blasting with alundum (180 mesh). The distance between the charging sleeve 312 and the photosensitive member 1 is adjusted to about 300 μm. A charging container contains 100 g of magnetic particles 34. The distance between a control blade 33C and the charging sleeve 312 is adjusted so that the amount of magnetic particles carried in the central region of the charging sleeve 312 in the longitudinal direction is about 50 mg/cm2. In charging, a charging bias device 35 supplies the charging sleeve 312 with a charging bias with a DC voltage of 600 V, an AC voltage of 300 Vpp, and a frequency of 1 kHz.
A charging sleeve having a larger diameter provides a larger contact area between the magnetic particles 34 and the photosensitive member 1 to achieve better charging properties. In addition, the magnetic particle control member 33C used is a magnetic control blade or a nonmagnetic control blade to which a magnetic plate is bonded. The positions of poles of the control blade 33C and a magnet 32 contained in the charging sleeve 312 may be adjusted so that the amount of magnetic particles carried can be further stabilized by a combination of mechanical and magnetic control forces.
As in the first embodiment, additionally, the ends of the charging sleeve 312 are insulated by resin coating so that the width of the uninsulated region is larger than the image assurance width and is smaller than the magnetic particle carrying width. The resin coating has a thickness of about 50 μm.
Comparative Example 3-1 is described below as a specific comparative example for the third embodiment. In this example, the magnetic particle control member 33C used was a control blade 334 shown in
Under the above conditions, an idling durability test equivalent to 10,000 copies of A4 sheets was carried out to measure the amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeve 312. The measured amount was about 3.9 g.
Example 3-1 is described below as a specific example of the third embodiment.
The above control blade 335 was visually confirmed to increase the amount of magnetic particles carried at the ends of the magnetic particle carrying region of the charging sleeve 312 and stabilize the magnetic particle carrying state. Subsequently, the same test as in Comparative Example 3-1 was carried out. The measured amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeve 312 was about 0.3 g.
According to the above results, even if the amount of magnetic particles carried in the central region of the charging sleeve 312 in the longitudinal direction is relatively small, namely about 50 mg/cm2, the amount of magnetic particles adhering to the photosensitive member 1 at the ends of the charging sleeve 312 may be reduced by increasing the amount of magnetic particles carried in the end regions of the charging sleeve 312 to stabilize the magnetic particle carrying state.
As described above, a magnetic brush charging device charges a photosensitive member by sliding magnetic particles thereon. The amount of magnetic particles carried at the ends of a magnetic particle carrying region of a magnetic particle carrying member may be increased by, for example, modifying a magnetic particle control member to stabilize the magnetic particle carrying state. Such a stable state can inhibit the magnetic particles from adhering to the photosensitive member at the ends of the magnetic particle carrying region of the magnetic particle carrying member. This allows long-term stable operation.
The amount of magnetic particles carried may be increased in the regions outside the image assurance width in the longitudinal direction in consideration of the wear of the photosensitive member. In addition, the optimum method for modifying the magnetic particle control member and the optimum dimensions thereof may be selected according to the design of the charging device.
Photosensitive members have been described as an example of a member to be charged in the above embodiments, though the member to be charged may have no photosensitivity. In addition, the amount of magnetic particles carried at the ends of a charging sleeve is increased by modifying a control blade in the above embodiments, though the present invention is not limited to such methods. For example, the amount of magnetic particles carried at the ends of the charging sleeve may be increased by enhancing the magnetic force of a magnet contained in the charging sleeve only at the ends thereof.
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 embodiments. On the contrary, the invention is intended to cover various modifications and equivalent arrangements included within the spirit and scope of the appended claims. 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 priority from Japanese Patent Application No. 2004-165915 filed Jun. 3, 2004, which is hereby incorporated by reference herein.
Number | Date | Country | Kind |
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2004-165915 | Jun 2004 | JP | national |
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5809379 | Yano et al. | Sep 1998 | A |
6298206 | Toyoshima et al. | Oct 2001 | B1 |
6381431 | Kinoshita et al. | Apr 2002 | B1 |
7035575 | Ikeguchi et al. | Apr 2006 | B2 |
Number | Date | Country | |
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20050271419 A1 | Dec 2005 | US |