Automatic modulation control for ESV modulators

Information

  • Patent Grant
  • 6504376
  • Patent Number
    6,504,376
  • Date Filed
    Wednesday, November 29, 2000
    25 years ago
  • Date Issued
    Tuesday, January 7, 2003
    22 years ago
Abstract
Method and apparatus for modulating the vibrations of an object with a constant amplitude has a sensor, e.g., a piezoelectric transducer, for sensing the vibrations. A light source, e.g., an LED, receives the sensed signal and illuminates a light dependent resistor (LED) In turn, a control circuit controls the vibration amplitude in accordance with the LDR resistance. A full wave bridge rectifier can be used between the sensor and the LED.
Description




CROSS-REFERENCES TO RELATED APPLICATIONS




This application is related to U.S. Pat. No. 6,381,426.




STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT




Not Applicable




BACKGROUND OF THE INVENTION




1. Field of the Invention




The present invention relates to vibration amplitude control, and more particularly, to such control when used with ESVs (electrostatic voltmeters) in xerographic copying machines.




2. Description of the Related Art Including Information Disclosed Under 37 CFR 1.97 and 1.98




In xerographic copying machines it is desired to measure the potential on a photoreceptor to achieve better copy quality. This is done using an ESV. However, the standard “feedback” ESV is a second order feedback system. The “speed of response” of the ESV is dependent on the open loop gain of the system, which in dependent on both the spacing between a sense head and the mechanical vibration modulation (change in this spacing). If the system gain is “high”, the output will overshoot the final value. If it is “low”, it will be slow or underdamped. If it is “optimized”, it is “critically” damped, i.e., it is going as fast as possible without overshooting. In practice, there is an electronic gain control that is adjusted in the factory setup procedure to give the desired output response at the calibration spacing and the assumption is made that the amount of modulation stays constant.




In fact, vibration modulation is dependent on a stable modulating structure, such as the standard tuning fork and the newer ASIC (application specific integrated circuit) ESV “vibrating beam”. Also needed is a stable mounting system for that structure with enough rigidity and mass that the energy supplied by the driver, which causes the modulator to move, goes entirely into moving the modulator and is not absorbed by the mounting structure or by vibrating a complete probe or modulator assembly.




It is noted that a large modulating amplitude is desired for a high modulating frequency and high signal-to-noise ratio. While a good mount resolves this problem, it is difficult and expensive to achieve in a mass-produced product.




While it is known to use a feedback circuit to maintain a constant amplitude, such circuits typically have a fast time constant in order to measure a peak voltage. In the present application, this results in the feedback voltage being a function of frequency which is undesirable. Increasing the value of capacitors and/or resistors has the effect of increasing only the discharging time. This is undesirable since for ESVs it is desired to have both charging and discharging times equal.




It is therefore desirable to have a frequency independent constant amplitude mechanical vibration modulation in order to reduce the requirements on a mount and achieve optimum gain, and thus a constant optimum response speed.




BRIEF SUMMARY OF THE INVENTION




A method of modulating the vibrations of an object with a substantially constant mechanical amplitude comprises providing an electrical signal in accordance with the amplitude of said mechanical vibrations; applying the provided signal to a light source; applying the light emitted by said source to a light dependent resistor having a slow response time compared to the modulating frequency; and using the resistance of said resistor to control the amplitude of said mechanical vibrations to a substantially constant value.




Apparatus for modulating the vibrations of an object with a substantially constant mechanical amplitude comprises a transducer providing an electrical signal in accordance with the amplitude of said vibrations; a light source receiving the provided signal; a light dependent resistor having a slow response time compared to the modulating frequency receiving the light emitted by said source; and a control circuit coupled to said resistor controlling the amplitude of said vibrations to a substantially constant value.




It is noted that the basic system of LED/LDR control has been adopted by the audio industry many years ago as means of preventing signal overload; by proper circuit choices, limiting can be made “rounded” or “soft” which is tolerated by the ear much better than the “harsh” limiting of a solid state system.











BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWING(S)





FIG. 1

shows a general view of a copying apparatus;





FIG. 2

is a schematic drawing of a first embodiment of the invention;





FIGS. 2A and 2B

show modifications of

FIG. 2

; and





FIG. 3

is a schematic drawing of a second embodiment of the invention.











In the figures corresponding elements have been given corresponding reference numbers.




DETAILED DESCRIPTION OF THE INVENTION




It will become evident from the following discussion that the present invention is equally well-suited for use in a wide variety of printing systems including ionographic printing machines and discharge area development systems, as well an other more general non-printing systems providing multiple or variable outputs such that the invention is not necessarily limited in its application to the particular system shown herein.




Turning initially to

FIG. 1

, before describing the particular features of the present invention in detail, an exemplary electrophotographic copying apparatus will be described. The exemplary electrophotographic system may be a multicolor copier, as for example, the recently introduced Xerox Corporation “5775” copier. To initiate the copying process, a multicolor original document


38


is positioned on a raster input scanner (RIS), indicated generally by the reference numeral


10


. The RIS


10


contains document illumination lamps, optics, a mechanical scanning drive, and a charge coupled device' (CCD array) for capturing the entire image from original document


38


. The RIS


10


converts the image to a series of raster scan lines and measures a set of primary color densities, i.e. red, green and blue densities, at each point of the original document. This information is transmitted as an electrical signal to an image processing system (IPS), indicated generally by the reference numeral


12


, which converts the set of red, green and blue density signals to a set of colorimetric coordinates.




The IPS contains control electronics for preparing and managing the image data flow to a raster output scanner (ROS), indicated generally by the reference numeral


16


. A user interface (UI), indicated generally by the reference numeral


14


, is provided for communicating with IPS


12


. UI


14


enables an operator to control the various operator adjustable functions whereby the operator actuates the appropriate input keys of UI


14


to adjust the parameters of the copy. UI


14


may be a touch screen, or any other suitable device for providing an operator interface with the system. The output signal from UI


14


is transmitted to IPS


12


which then transmits signals corresponding to the desired image to ROS


16


.




ROS


16


includes a laser with rotating polygon mirror blocks. The ROS


16


illuminates, via mirror


37


, a charged portion of a photoconductive belt


20


of a printer or marking engine, indicated generally by the reference numeral


18


. Preferably, a multi-facet polygon mirror is used to illuminate the photoreceptor belt


20


at a rate of about 400 pixels per inch. The ROS


16


exposes the photoconductive belt


20


to record a set of three subtractive primary latent images thereon corresponding to the signals transmitted from IPS


12


.




One latent image is to be developed with cyan developer material, another latent image is to be developed with magenta developer material, and the third latent image is to be developed with yellow developer material. These developed images are subsequently transferred to a copy sheet in superimposed registration with one another to form a multicolored image on the copy sheet which is then fused thereto to form a color copy. This process will be discussed in greater detail hereinbelow.




With continued reference to

FIG. 1

, marking engine


18


is an electrophotographic printing machine comprising photoconductive belt


20


which is entrained about transfer rollers


24


and


26


, tensioning roller


28


, and drive roller


30


. Drive roller


30


is rotated by a motor or other suitable mechanism coupled to the drive roller


30


by suitable means such as a belt drive


32


. As roller


30


rotates, it advances photoconductive belt


20


in the direction of arrow


22


to sequentially advance successive portions of the photoconductive belt


20


through the various processing stations disposed about the path of movement thereof.




Initially, a portion of photoconductive belt


20


passes through a charging station, indicated generally by the reference letter A. At charging station A, a corona generating device


34


or other charging device generates a charge voltage to charge photoconductive belt


20


to a relatively high, substantially uniform voltage potential. The corona generator


34


comprises a corona generating electrode, a shield partially enclosing the electrode, and a grid disposed between the belt


20


and the unenclosed portion of the electrode. The electrode charges the photoconductive surface of the belt


20


via corona discharge. The voltage potential applied to the photoconductive surface of the belt


20


is varied by controlling the voltage potential of the wire grid.




Next, the charged photoconductive surface is rotated to an exposure station, indicated generally by the reference letter B. Exposure station B receives a modulated light beam corresponding to information derived by RIS


10


having a multicolored original document


38


positioned threat. The modulated light beam impinges on the surface of photoconductive belt


20


, selectively illuminating the charged surface of photoconductive belt


20


to form an electrostatic latent image thereon. The photoconductive belt


20


is exposed three times to record three latent images representing each color.




After the electrostatic latent images have been recorded on photoconductive belt


20


, the belt is advanced toward a development station, indicated generally by the reference letter C. However, before reaching the development station C, the photoconductive belt


20


passes subjacent to a voltage monitor, preferably an electrostatic voltmeter


33


, for measurement of the voltage potential at the surface of the photoconductive belt


20


.




The electrostatic voltmeter


33


(as described in detail below) of the present invention provides the measuring condition in which an electrostatic field between a probe electrode and the belt


20


is sensed as known in the art. The voltage potential measurement of the photoconductive belt


20


is utilized to determine specific parameters for maintaining a predetermined potential on the photoreceptor surface.




The development station C includes four individual developer units indicated by reference numerals


40


,


42


,


44


, and


46


. The developer units are of a type generally referred to in the art as “magnetic brush development units”. Typically, a magnetic brush development system employs a magnetizable developer material including magnetic carrier granules having toner particles adhering triboelectrically thereto. The developer material is continually brought through a directional flux field to form a brush of developer material. The developer material is constantly moving so as to continually provide the brush with fresh developer material. Development is achieved by bringing the brush of developer material into contact with the photoconductive surface. Developer units


40


,


42


, and


44


, respectively, apply toner particles of a specific color corresponding to the compliment of the specific color separated electrostatic latent image recorded on the photoconductive surface.




Each of the toner particle colors is adapted to absorb light within a preselected spectral region of the electromagnetic wave spectrum. For example, an electrostatic latent image formed by discharging the portions of charge on the photoconductive belt corresponding to the green regions of the original document will record the red and blue portions as areas of relatively high charge density on photoconductive belt


20


, while the green areas will be reduced to a voltage level ineffective for development. The charged areas are then made visible by having developer unit


40


apply green absorbing (magenta) toner particles onto the electrostatic latent image recorded on photoconductive belt


20


. Similarly, a blue separation is developed by developer unit


42


with blue absorbing (yellow) toner particles, while the red separation is developed by developer unit


44


with red absorbing (cyan) toner particles.




Developer unit


46


contains black toner particles and may be used to develop the electrostatic latent image formed from a black and white original document. In

FIG. 3

, developer unit


40


is shown in the operative position with developer units


42


,


44


, and


46


being in the non-operative position.




After development, the toner image is moved to a transfer station, indicated generally by the reference letter D. Transfer station D includes a transfer zone, generally indicated by reference numeral


64


, defining the position at which the toner image is transferred to a sheet of support material, which may be a sheet of plain paper or any other suitable support substrate. A sheet transport apparatus, indicated generally by the reference numeral


48


, moves the sheet into contact with photoconductive belt


20


. Sheet transport


48


has a belt


54


entrained about a pair of substantially cylindrical rollers


50


and


52


. A friction retard feeder


58


advances the uppermost sheet from stack


56


onto a pre-transfer transport


60


for advancing a sheet to sheet transport


48


in synchronism with the movement thereof so that the leading edge of the sheet arrives at a preselected position, i.e. a loading zone. The sheet is received by the sheet transport


48


for movement therewith in a recirculating path. As belt


54


of transport


49


moves in the direction of arrow


62


, the sheet is moved into contact with the photoconductive belt


20


, in synchronism with the toner image developed thereon.




In transfer zone


64


, a corona generating device


66


sprays ions onto the backside of the sheet so as to charge the sheet to the proper magnitude and polarity for attracting the toner image from photoconductive belt


20


thereto. The sheet remains secured to the sheet gripper so as to move in a recirculating path for three cycles. In this manner, three different color toner images are transferred to the sheet in superimposed registration with one another.




Each of the electrostatic latent images recorded on the photoconductive surface is developed with the appropriately colored toner and transferred, in superimposed registration with one another, to the sheet for forming the multi-color copy of the colored original document.




After the last transfer operation, the sheet transport system directs the sheet to a vacuum conveyor, indicated generally by the reference numeral


68


. Vacuum conveyor


68


transports the sheet, in the direction of arrow


70


, to a fusing station, indicated generally by the reference letter E, where the transferred toner image is permanently fused to the sheet. The fusing station includes a heated fuser roll


74


and a pressure roll


72


. The sheet passes through the nip defined by fuser roll


74


and pressure roll


72


. The toner image contacts fuser roll


74


so as to be affixed to the sheet. Thereafter, the sheet is advanced by a pair of rolls


76


to a catch tray


78


for subsequent removal therefrom by the machine operator. The last processing station in the direction of movement of belt


20


, as indicated by arrow


22


, is a cleaning station, indicated generally by the reference letter F.




A lamp


80


illuminates the surface of photoconductive belt


20


to remove any residual charge remaining thereon. Thereafter, a rotatably mounted fibrous brush


82


is positioned in the cleaning station and maintained in contact with photoconductive belt


20


to remove residual toner particles remaining from the transfer operation prior to the start of the next successive imaging cycle.




The foregoing description should be sufficient for purposes of the present application for patent to illustrate the general operation of an electrophotographic printing machine incorporating the features of the present invention. As described, an electrophotographic printing system may take the form of any of several well-known devices or systems. Variations of specific electrophotographic processing subsystems or processes may be expected without affecting the operation of the present invention.





FIG. 2

shows a first embodiment of the ESV


33


. A vibrating beam


200


, preferably made of Ph bronze, is disposed near belt


20


and has rigidly mounted beam web ends


202


. On a first end is mounted an L-shaped bracket


204


, which is disposed between belt


20


and an electrode


206


. At a second end of beam


200


is a counterweight


208


. If beam


200


is made of a non-magnetic material, then weight


208


must be of a magnetically susceptible material, e.g., Fe, to close a magnetic drive path. Disposed adjacent weight


208


is a permanent magnet core drive coil


210


. The permanent magnet biases the position of beam


200


. As shown in the art, AC current through coil


210


causes beam


200


and thus bracket


204


to vibrate. In turn, this causes a change in the capacitance between belt


20


and electrode


206


. From this, the voltage of belt


20


can be determined.




In order to keep the vibration amplitude constant, a feedback circuit is used. It comprises a piezoelectric crystal sensor


212


is mounted on beam


200


, preferably at the left to right center as viewed in

FIG. 2

thereof for maximum sensitivity. For clarity sensor


212


is also shown in the schematic portion of the drawing.




The output voltage from sensor


212


is provided to a current-to-voltage converter of operational amplifier A


1


and feedback resistor R


1


. The output voltage from A


1


is applied to a level shifting circuit of R


3


, R


4


, R


5


, R


6


, and then to push-pull amplifier of A


3




a


and A


3




b.


In turn, amplifier A


3


drives coil


210


.




The output voltage of A


1


is also applied to rectifier


214


. As shown, rectifier


214


is preferably a full wave bridge type for greatest sensitivity, accuracy, faster start time, and LED (described below) lifetime, but a half wave type can also be used. Variable resistor R


2


adjusts a bias current through rectifier


214


and hence through a light source, e.g., light emitting diode (LED)


216


.




A light dependent resistor (LDR) R


9


is optically coupled to LED


216


and electrically coupled to resistor R


10


. Resistors R


9


and R


10


form a voltage divider than biases the gate of field effect transistor (FET) Q


3


. If desired, Q


3


can be a bipolar transistor. The gate bias voltage sets the source-drain current of Q


3


. This current is applied to a current mirror including R


7


, R


8


, Q


1


, and Q


2


, which mirror is in turn coupled to the power input pin


218


of A


3




b.


As known in the art, this limits the power from A


36


to coil


210


to that of said Q


3


source-drain current.




In operation, if the vibration amplitude decreases from a value determined by R


2


, then this is sensed by amplifier A


1


to cause a greater current to be applied to pin


218


. This causes greater current in coil


210


so that the vibrational amplitude increases. Similarly, if the amplitude increases from the value determined by R


2


, a lesser current is applied to pin


218


. This causes lesser current in coil


210


so that the vibration amplitude decreases.




It will be appreciated that the use of an LDR in the feedback circuit results in an accurate, reliable, frequency independent vibration amplitude control with a high signal-to-noise ratio. This is true since it has a slow response time compared to the frequency, e.g., 1 KHz, of the modulating signal, which results in measuring the average power rather than the peak value of the feedback voltage. It also results in a large control range since it has a dynamic range of about three decades. Further since LED


216


and LDR R


9


are electrically isolated from each other, the circuit design is simplified by eliminating ground loops.





FIG. 2A

shows a modification of

FIG. 2

wherein resistor R


2


comprises a series circuit of a fixed resistor R


2




a


and digitally variable potentiometer resistor R


2




b,


the remainder of the circuit being the same as in FIG.


2


.

FIG. 2B

shows a second modification of

FIG. 2

wherein resistor R


2


comprises a series circuit of a fixed resistor R


2




a


and an LDR R


2




b,


which is optically coupled to an LED


220


. The modifications of

FIGS. 2A and 2B

easily lend themselves to remote adjustment of R


2


.





FIG. 3

shows a second embodiment of the invention. For simplicity, belt


20


, L-shaped bracket


204


, and electrode


206


are not shown in

FIG. 3

, but are actually present as shown in FIG.


2


. This second embodiment takes advantage of the electrical isolation from the optical coupling to eliminate Q


1


, Q


2


, R


7


and R


8


and replace them with just a zener diode D


5


. Diode D


5


provides protection to prevent destruction of Q


3


. As with the first embodiment of

FIG. 2

, resistor R


2


can be a series circuit of a fixed resistor and either a digital potentiometer or LED and LDR.




While the present invention has been particularly described with respect to preferred embodiments, it will be understood that the invention is not limited to these particular preferred embodiments, the process steps, the sequence, or the final structures depicted in the drawings. On the contrary, it is intended to cover all alternatives, modifications, and equivalents as may be included within the spirit and scope of the invention defined by the appended claims. In particular, the scope of the invention is intended to include, for example, those devices and methods. In addition, other methods and/or devices may be employed in the method and apparatus of the instant invention as claimed with similar results.



Claims
  • 1. A method of modulating the vibrations of an object with a substantially constant mechanical amplitude, said method comprising:providing an electrical signal in accordance with the amplitude of said mechanical vibrations; applying the provided signal to a light source; applying the light emitted by said source to a light dependent resistor having a slow response time compared to the modulating frequency; and using the resistance of said resistor to remotely control the amplitude of said mechanical vibrations to a substantially constant value.
  • 2. The method of claim 1, wherein said object comprises a vibrating beam disposed adjacent a photoreceptor of a xerographic device.
  • 3. The method of claim 1, wherein said providing step comprises piezoelectrically transducing said vibrations.
  • 4. The method of claim 1, wherein said light source comprises an LED.
  • 5. The method of claim 1, wherein said applying step comprises full wave rectifying said electrical signal.
  • 6. The apparatus of claim 1, wherein said variable resistor comprises a digital potentiometer.
  • 7. Apparatus for modulating the vibrations of an object with a substantially constant mechanical amplitude, said apparatus comprising:a transducer providing an electrical signal in accordance with the amplitude of said vibrations; a light source receiving the provided signal; a light dependent resistor having a slow response time compared to the modulating frequency receiving the light emitted by said source; a control circuit coupled to said resistor controlling the amplitude of said vibrations to a substantially constant value; a rectifier coupled between said transducer and said light source; and a variable resistor coupled to said rectifier.
  • 8. The apparatus of claim 7, further comprising said object.
  • 9. The apparatus of claim 8, wherein said object comprises a vibrating beam disposed adjacent a photoreceptor of a xerographic device.
  • 10. The apparatus of claim 7, wherein said transducer comprises a piezoelectric one.
  • 11. The apparatus of claim 7, wherein the light source comprises an LED.
  • 12. The apparatus of claim 7, wherein said control circuit comprises an amplifier coupled to said resistor and a coil adapted to be disposed proximate said object and coupled to said amplifier.
  • 13. The apparatus of claim 7, wherein said variable resistor comprises a light dependent resistor.
  • 14. The apparatus of claim 12, wherein said amplifier comprises a push-pull amplifier.
  • 15. The apparatus of claim 12, wherein said control circuit comprises a current mirror coupled to said amplifier.
  • 16. The apparatus of claim 7, wherein said recitifer comprises a full wave rectifier.
US Referenced Citations (5)
Number Name Date Kind
3851247 Vosteen et al. Nov 1974 A
5243292 Borton et al. Sep 1993 A
5489850 Werner, Jr. et al. Feb 1996 A
5754918 Mestha et al. May 1998 A
5950040 Mestha et al. Sep 1999 A