The introduction of electrophotography revolutionized the handling of printed information. With the mere click of a button, a copy can be made onto paper or other recording media. This convenience has led to electrophotography devices becoming an indispensable part of the home and office landscape. However, while electrophotography is commonplace, some conventional electrophotography devices are too slow, costly, and/or too bulky.
In the following detailed description, reference is made to the accompanying drawings which form a part hereof, and in which is shown by way of illustration specific embodiments in which the subject matter of the present disclosure may be practiced. In this regard, directional terminology, such as “top,” “bottom,” “front,” “back,” “leading,” “trailing,” etc., is used with reference to the orientation of the Figure(s) being described. Because components of embodiments of the present disclosure can be positioned in a number of different orientations, the directional terminology is used for purposes of illustration and is in no way limiting. It is to be understood that other embodiments may be utilized and structural or logical changes may be made without departing from the scope of the present disclosure. The following detailed description, therefore, is not to be taken in a limiting sense, and the scope of the present disclosure is defined by the appended claims.
Embodiments of the present disclosure are directed to electrophotography devices tuned to facilitate a faster response from a photoconductor. In one embodiment, an electric field applicator is positioned adjacent to a photoconductor between a light source for exposing a latent image on a photoconductor and a development station for developing the latent image. In other embodiments, the field applicator is positioned between a charging station and the light source or is interposed directly between the light (from the light source) and the photoconductor.
In one aspect, the externally controller field applicator induces a substantially uniform electric field in an outer portion of a photoconductor to quickly drive components (e.g., positive holes) of a charge pair to a top surface of the outer portion of the photoconductor. This arrangement reduces the relaxation period of the photoconductor, while simultaneously using less energy for discharging targeted regions of the photoconductor. This arrangement also reduces unwanted dot gain (of the type associated with slow discharge of a photoconductor), thereby producing sharper images from the electrophotography device. These effects, in turn, facilitate smaller sized electrophotography devices by permitting smaller photoconductors and facilitate more energy efficient electrophotography devices by permitting the use of lower intensity light sources.
In another aspect, the externally controlled electric field enables greater uniformity of the discharge level (caused by the exposure to a light source) regardless of the discharge region size. In one aspect, this arrangement also results in a reduction in the discharge voltage, thereby increasing the longevity of a photoconductor.
These embodiments, and additional embodiments, are described in association with
In one embodiment, photoconductor 12 comprises an outer portion 15 that includes outer charge transport layer 20, inner conductive layer 24, and charge generating layer 22 sandwiched between the conductive layer 24 and the outer charge transport layer 20. In one aspect, outer portion 15 comprises a top surface 14 defined by outer charge transport layer 20.
Charging station 30 applies a charge on outer portion 15 of photoconductor 12 and in one embodiment, comprises a corona charger or other known charging devices. Light source 32 comprises a direct light source (e.g., LEDs) or a laser system including directional mirrors to emit a beam of light (as represented by directional arrow B) onto outer portion 15 of photoconductor 12.
In operation, as photoconductor 12 rotates, charging station 30 applies a charge on outer portion 15 of photoconductor 12 and then beam of light (B) from light source 32 exposes the charged outer portion 15 of photoconductor 12 to form a latent image on top surface 14 of photoconductor 12. Development station 34 develops the latent image via application of toner (or charged ink) to the outer surface 14 of photoconductor drum and transfer station 36 acts to transfer the developed image onto medium 35 (e.g., paper) that moves between surface 14 of outer portion 15 of photoconductor 12 and transfer station 36. In one embodiment, a rubber roller or belt is used to facilitate transfer of the developed image from the photoconductor 12 to the paper or other medium.
In one embodiment, device 10 comprises an electric field applicator 50 positioned adjacent outer portion 15 of photoconductor 12 between light source 32 and development station 34. Electric field applicator 50 induces an electric field in the charge transport layer 20 of the photoconductor 12 to draw charges (e.g., positive holes) migrating from charge generation layer 22 toward top surface 14 of outer portion 15 of photoconductor 12, as described more fully in association with
In one aspect, a first negative charge potential (Vp1) is present at top surface 14 of photoconductor 12 due to charging by charging station 30. Upon light (from light source 32) impinging on and exposing outer portion 15 of photoconductor 12, top surface 14 of photoconductor 12 is partially discharged in a pattern to form a latent image. During this exposure, charge pairs are created in charge generation layer 22 with the charge pairs 63 including positive charges 64 and negative charges 66. In one aspect, many of the positive charges 64 (i.e., holes) recombine with the negative charges 66 within dielectric portion 21 while some positive charges 64 migrate toward top surface 14 of outer portion 15 of photoconductor 12 because of the first negative voltage potential (Vp1) at the top surface 14 of photoconductor 12 which attracts the positive charges 64. Positive charges 64 reaching top surface 14 discharge a portion of the charged top surface 14. In another aspect, negative charges 66 that do not recombine with positive charges 64 flow to the ground 62 via conductive layer 24.
In another aspect,
In one embodiment, dielectric layer 54 of field applicator 50 has a thickness (T2) which is selected as small as possible and at least comparable to (T1) of the dielectric portion 21 of the outer portion 15 of photoconductor 12. This arrangement facilitates keeping the voltage used to maintain the electric field E (in the dielectric portion 21 of photoconductor 12) to be at a sufficient level without resorting to high values of Vp2.
In one embodiment, the electric field E is defined by at least the following parameters: (1) the thickness (T1) of the dielectric portion 21 of photoconductor 12; (2) the thickness (T2) of the dielectric layer 54 of the field applicator 50; (3) the dielectric constant (e1) of the dielectric portion 21 of photoconductor 12; and (4) the dielectric constant (e2) of the dielectric layer 54 of the field applicator 50. Using these parameters, the electric field E created in the outer portion 15 of photoconductor 12 by field applicator 50 is given by the equation Vp2/(T1+(e1/e2)T2).
In one embodiment, using these same notations, the total electric field E in the dielectric portion 21 of photoconductor 12 is expressed as:
where ρs is the surface charge density deposited by the charging station 30.
With this relationship, the gain to the electric field E caused by the action of field applicator 50 (compared to surface charging alone via charging station 30) immediately after exposure of photoconductor 12 to field applicator 50 is expressed as:
Accordingly, the effect of the original charge caused by the charging station 30 (as represented by first negative voltage potential Vp1) and of the second negative voltage (Vp2) applied by the field applicator 50 on the dielectric portion 21 of photoconductor 12 is represented by a surface charge distribution ρs on charge transport layer 20, which adds up an external potential driving the electric field E. The field E generated by field applicator 50 provides a generally consistent attractive force regardless of the number of, or speed at which, positive charges 64 reach top surface 14 of photoconductor 12, and therefore the electric field E induced by the externally controlled field applicator 50 generally does not dissipate over time.
Moreover, because the electric field E generated by the second voltage (Vp2) applied via the field applicator 50 in combination with the original charge (represented by first negative voltage potential Vp1) provides a stronger attractive force than the first negative voltage potential (Vp1) alone, more positive charges 64 are pulled to top surface 14 of photoconductor 12 before they have a chance to re-combine with negative charges 66 in the charge generation layer 22. In addition, the positive charges 64 pulled to top surface 14 of photoconductor 12 are pulled faster than without the field applicator 50, thereby reducing transit time for the positive charges 64. This reduced transit time, in turn, reduces the time taken to discharge the top surface 14 of the photoconductor 12 in the pattern of the desired latent image. Together, these effects caused by field applicator 50 result in a sharper latent images on surface 14 of photoconductor 12 as well as a substantial reduction in the relaxation time between light exposure of the photoconductor 12 (at light source 32) and development of the latent image at development station 34. In one embodiment, a relaxation time is reduced to about one-half the conventional relaxation time. In another embodiment, the relaxation time is reduced more than one-half the conventional relaxation time when higher voltages are applied by the field applicator 50.
In addition, this arrangement also results in a reduction in the amount of light needed to discharge the outer portion 15 of the photoconductor 12, thereby reducing the size and cost of the light source 32. Moreover, by using less light over a shorter time period, this arrangement also uses less energy, making electrophotography device 60 more energy efficient.
In another aspect, this external electric field (E) also pulls deeper positive charges 64 up to top surface 14 of photoconductor 12 by overcoming a masking effect of shallower positive charges that would otherwise occur in the absence of the electric field E. In other words, the external electric field E induced and maintained via field applicator 50 facilitates migration of deep positive charges 64, independent of the position and migration of shallower positive charges 64.
In one aspect, the dielectric layer 54 of field applicator 50 is maintained in contact with top surface 14 of photoconductor 12 during application of the field E. In one aspect, this contact is maintained by the strong attractive electric force created between the conductive layer 52 of field applicator 50 and the inner conductive layer 24 of the photoconductor 12, which pulls the dielectric layer 54 of the field applicator 50 into contact (e.g., sliding contact) against surface 14 of photoconductor 12. In one aspect, this attractive force is present even when there is no discharge of outer portion 15 of photoconductor 12.
Once energized, the conductive foil 120 induces an electric field E in the charge transport layer 20 (shown in
In one aspect, dielectric layer 122 of conductive sheet 108 of field applicator 102 comprises a thickness (T3), which is substantially the same as a thickness (T1) of the dielectric portion 21 of outer portion 15 of photoconductor 12 (including charge generation layer 22 and charge transport layer 20), as previously described in association with
In a manner substantially the same as previously described for electrophotography devices 10 in association with
In one embodiment, device 150 comprises a single, generally larger roller 161. In another embodiment, device 150 comprises a plurality of generally smaller rollers 161 aligned in series to extend about a portion of the circumference of the outer portion 15 photoconductor 12. In another aspect, multiple rollers 161 are used instead of a single roller to maximize the amount of surface area in rolling contact against the outer surface 14 of photoconductor 12 while simultaneously minimizing the height of the rollers 161 relative to outer portion 14 of photoconductor 12. This latter aspect contributes to reducing the overall size or volume of the electrophotography device 150.
As illustrated in the enlargement, each filament 186 comprises a conductive core 190 (extending from conductive core 186) and an outer dielectric layer 192 surrounding the conductive core 190. The conductive core 190 in the array of filaments 186 induces the electric field in the charge transport layer 20 of the photoconductor 12 while the outer dielectric layer 192 comprises an insulating member that electrically isolates the conductive core 190 of each filament 186 from the outer portion 15 of photoconductor 12 (to substantially prevent conductive core 190 from depositing charges on photoconductor 12).
In one embodiment, device 175 comprises a single, generally larger brush 180. In another embodiment, in a manner substantially similar to the multiple rollers 160,161 of device 150 as previously described in association with
In one embodiment, device 200 comprises a single, generally larger electrode 202. In another embodiment, device 200 comprises a plurality of generally smaller electrodes 202. In one embodiment, metal electrode 202 has a generally straight shape while in another embodiment, metal electrode 202 has a generally curved shape arranged to substantially match a curvature of outer portion 14 of photoconductor 12.
In one aspect, a charge transport layer 20 of outer portion 14 of photoconductor 12 of electrophotography device 230 is formed with a capacitance sufficient (via its relaxation time) to sustain the electric field induced by the field applicator 232 during and after exposure to light source 32.
Accordingly, in one embodiment, the field applicator 252 is implemented in a manner substantially the same as one of the metal electrode of electrophotography device 200 as previously described in association with
In another embodiment, field applicator 252 having the location illustrated in
In one embodiment, application of a field applicator (as in the embodiments described in association with
Embodiments of the present disclosure are directed to electrophotography devices tuned to facilitate a faster response from a charged photoconductor. In one embodiment, a field applicator is positioned between a charging station and a development station to provide a substantially uniform electric field in an outer portion of a photoconductor. This arrangement drives components of a charge pair to a surface of the outer portion of the photoconductor to substantially decrease a transit time for the charge components (e.g. a positive hole). This arrangement substantially reduces the relaxation time of the photoconductor, while simultaneously using less energy, and producing sharper images from the electrophotography devices. These effects, in turn, facilitate smaller sized electrophotography devices by permitting smaller light sources and smaller photoconductors.
Although specific embodiments have been illustrated and described herein, it will be appreciated by those of ordinary skill in the art that a variety of alternate and/or equivalent implementations may be substituted for the specific embodiments shown and described without departing from the scope of the present disclosure. This application is intended to cover any adaptations or variations of the specific embodiments discussed herein. Therefore, it is intended that the claimed subject matter be limited by the claims and the equivalents thereof.