Image forming apparatus

An image forming apparatus comprising a charging section for uniformly charging a surface of a photoconductive body; an image forming section for forming an image on the photoconductive body charged by the charging section; a detecting section for detecting an influx current flowing to the photoconductive body when the photoconductive body is charged by the charging section; and a control section for controlling the image forming section so as to stabilize a quality of images formed by the image forming section.

BACKGROUND OF THE INVENTION 
(1) Field of the Invention 
This invention relates to an image forming apparatus equipped with a 
photoconductive body which is gradually worn away as an image forming 
procedure is repeated many times (for example, a photoconductive drum 
having a surface formed of an organic photoconductive layer), especially 
to an image forming apparatus for compensating the sensitivity of the 
photoconductive body which would be deteriorated as the photoconductive 
body is worn away. 
(2) Description of the Related Art 
In a conventional copier equipped with a photoconductive drum, a surface 
thereof formed of an organic photoconductive layer is gradually worn away 
by a friction when a cleaning blade scratches off the residual toner on 
the surface after an image is transferred onto a copying paper. 
Such a phenomenon deteriorates the sensitivity of the photoconductive drum 
for the following reason. 
A surface potential V.sub.0 of the drum applied by a main charger and a 
thickness d of the organic photoconductive layer of the drum have the 
following relationship: 
##EQU1## 
where Q: charge amount applied to the photoconductive drum per a unit area 
C: capacitance per a unit area of the organic photoconductive layer 
.epsilon..sub.0 : dielectric constant in vacuum 
.epsilon..sub.r : relative dielectric constant in the organic 
photoconductive layer 
As apparent from Equation (1), if the photoconductive drum is charged with 
the same surface potential V.sub.0 before and after the thickness d is 
reduced, the charge is accumulated in a larger amount in the latter case. 
Accordingly, even if the photoconductive drum is exposed by the same light 
amount after the repetition of the image forming procedure as on the 
initial stage, the potential at the exposed portion is not lowered enough. 
In the normal development, such a phenomenon adheres an unnecessary toner 
on the exposed portion, as a result of which the copying paper gets 
fogging in a blank area. In the reverse development such as in a laser 
copier, the image density is lowered. In other words, the sensitivity of 
the photoconductive drum is lowered. 
When the photoconductive drum is worn away much more and completes a life 
thereof, black streams appear on the copying paper or half-tone images are 
blurred. Since the life expectancy cannot be determined accurately in a 
conventional copier, the drum is renewed when the drum is still in a good 
condition or after the above problems occur. 
Japanese Patent Publication No. 61-29505 has disclosed a copier for 
compensating the sensitivity of the photoconductive drum. The number of 
copies, the paper size and the exposure time are detected, and the copying 
conditions such as the light amount are adjusted in accordance with the 
predetermined relationship between each detected value and the 
characteristics of the photoconductive layer of the drum. In this 
construction, wherein a change in the thickness of the photoconductive 
layer is not directly detected, the compensation precision is not high. 
According to U.S. Pat. No. 3,961,193, an influx current I.sub.pc, which 
flows to the photoconductive layer from the back side thereof and has the 
same amount as a charging current from the main charger to the surface of 
the photoconductive layer, is measured, and the output of the main charger 
is adjusted by comparing the measured I.sub.pc and the predetermined 
reference value. In such a construction, the surface potential V.sub.0 of 
the photoconductive layer can be kept at a certain level as long as the 
thickness of the photoconductive layer is kept the same. However, the 
reduction in the thickness d accompanies the decline in the surface 
potential V.sub.0. As a result, the image density is not high enough in 
the normal development while the copying paper gets fogging in the reverse 
development. 
SUMMARY OF THE INVENTION 
Accordingly, this invention has an object of offering an image forming 
apparatus for remarkably improving the image quality by preventing fogging 
or fluctuations in the image density which occur when the photoconductive 
layer is worn away. 
The above object is fulfilled by an image forming apparatus comprising a 
charging section for uniformly charging a surface of a photoconductive 
body; an exposure section for exposing an image of a document on the 
photoconductive body; a developing section for developing the image formed 
on the photoconductive body; a detecting section for detecting an influx 
current flowing to the photoconductive body when the photoconductive body 
is charged by the charging section; and a control section for controlling 
the exposure section and/or the developing section based on a detecting 
result of the detecting section so as to stabilize a quality of images 
formed on the photoconductive body. 
The photoconductive body may be organic. 
According to the above constructions, the detecting section detects the 
influx current flowing to the photoconductive body being charged by the 
charging section, and then the control section controls the light amount 
emitted from the exposure section and/or the developing bias voltage of 
the developing section. In this way, the sensitivity of the 
photoconductive body is surely compensated. 
Another object of this invention is to offer an image forming apparatus for 
assuring an excellent sensitivity compensation of the photoconductive 
layer regardless of temperature change or humidity change. 
The above object is fulfilled by an image forming apparatus comprising a 
scorotron type charger for uniformly charging a surface of a 
photoconductive body; a switching section for selecting one of at least 
two grid voltages of the charger; an exposure section for exposing an 
image of a document on the photoconductive body; a developing section for 
developing the image formed by the exposure section; a detecting section 
for detecting influx currents flowing to the photoconductive body when the 
photoconductive body is charged by the charger with the respective grid 
voltages being switched over; a calculating section for calculating 
thickness of a photoconductive layer of the photoconductive body based on 
a detecting result of the detecting section; and a control section for 
controlling an amount of the light used in the exposure section and/or the 
developing bias voltage of the developing section. 
According to the above constructions, the exposure section and/or the 
developing section is controlled based on the influx currents 
corresponding to at least two grid voltages. Even if an offset current is 
included in the influx current by the temperature change, the sensitivity 
compensation of the photoconductive body is not affected by the offset 
current. 
Still another object of this invention is to offer an image forming 
apparatus for appropriately renewing the photoconductive drum in 
accordance with the life expectancy of the photoconductive layer judged by 
the reduction of the thickness thereof. 
The above object is fulfilled by an image forming apparatus comprising a 
charging section for uniformly charging a surface of a photoconductive 
body; an image forming section for forming an image on the photoconductive 
body charged by the charging section; a detecting section for detecting an 
influx current flowing to the photoconductive body when the 
photoconductive body is charged by the charging section; a calculating 
section for calculating a thickness of a photoconductive layer of the 
photoconductive body based on a detecting result of the detecting section; 
and an estimating section for estimating a life expectancy of the 
photoconductive layer based on a calculating result of the calculating 
section. 
According to the above constructions, the calculating section calculates 
the thickness of the photoconductive body based on the influx current, and 
the estimating section estimates the life expectancy of the 
photoconductive layer to warn an operator when the photoconductive layer 
completes the life thereof or inform an operator how many more copies can 
be made. The photoconductive body can be renewed appropriately.

DESCRIPTION OF THE PREFERRED EMBODIMENTS 
Embodiment I 
A first embodiment according to this invention will be described referring 
to FIGS. 1 through 4. 
Overall construction and operation of the copier 
A copier as the first embodiment has a construction as shown in FIG. 1. 
When a document D is set on a glass document table 21 and a print key (not 
shown) is turned on, a light from an exposure lamp 2 illuminates the 
document D, and a photoconductive drum 1 is exposed by the reflected light 
through an optical system 20 comprising mirrors and a lens. 
A light amount to be emitted from the exposure lamp 2 is adjusted by a 
voltage applying section 14 in the following way. 
As shown in FIG. 2, the voltage applying section 14 comprises a triac 16 
interposed between the exposure lamp 2 and an AC power source 15, and a 
phase angle control circuit 17. The triac 16 is turned on or off by the 
phase angle control circuit 17 in accordance with a timing signal of a 
phase angle corresponding to a control signal sent from a control section 
22, whereby an AC power sent from the AC power source 15 to the exposure 
lamp 2 is adjusted. 
The photoconductive drum 1, which is rotatable in a direction of an arrow A 
(FIG. 1), comprises a conductive base (formed of Al or the like) and an 
organic photoconductive layer coated thereon. The organic photoconductive 
layer comprises a CGL (charge generating layer) and a CTL (charge 
transporting layer). A main charger C opposed to the drum 1 uniformly 
charges negative a surface of the photoconductive drum 1 prior to 
exposure. Then, an electrostatic latent image is formed on the surface of 
the drum 1 through the exposure. The electrostatic latent image is 
provided with a toner which is friction-charged positive by a developing 
device 4 which has a bias voltage applied by a power supply 30, whereby a 
toner image is formed on the drum 1. 
In synchronization with the formation of the toner image, a copying paper P 
is sent to a transferring section, whereby a reverse side of the paper P 
is charged in the opposite polarity to the toner by a transfer charger 51. 
In this way, the toner image on the drum 1 is transferred on the paper P. 
The paper P has the charge thereon removed by a separation charger 52 (AC 
corotron) and is separated from the drum 1 due to the paper's own 
firmness. Then, the paper P is sent to a fixing device 18 by a 
transporting device 53, whereby the toner image is fixed on the paper P 
and delivered outside. 
The residual toner on the drum 1 is scratched off by a cleaning blade 6, 
and the residual charge on the drum 1 is removed by an eraser lamp 7. 
Construction and operation of the main charger C and its vicinity 
The main charger C of the scorotron type comprises a charging wire 9 
connected to a high-voltage power supply 8, a casing 10 which is a 
rectangular box with a bottom thereof open and accommodates the charging 
wire 9, and a grid electrode 11 interposed between the charging wire 9 and 
the photoconductive drum 1. The grid electrode 11 is provided for keeping 
a potential V.sub.0 of the surface of the drum 1 at a certain level. The 
grid electrode 11 is connected in series to two varistors 12a and 12b, and 
an end of the varistor 12b is grounded. The varistors 12a and 12b are 
resistance elements whose voltage-current characteristics are non-linear. 
A grid voltage V.sub.g of the grid electrode 11 is kept at a level 
determined by the combination of the varistors 12a and 12b. Since this 
means the potential V.sub.0 of the surface of the drum 1 is substantially 
the same as the grid voltage V.sub.g, Formula (2) is obtained. 
EQU V.sub.0 .apprxeq.V.sub.g =V.sub.a +V.sub.b (2) 
where 
V.sub.a : voltage across both ends of the varistor 12a 
V.sub.b : voltage across both ends of the varistor 12b 
Sensitivity compensation 
In this embodiment, the sensitivity of the photoconductive drum 1 is 
compensated by detecting the change in the thickness of the 
photoconductive layer of the drum 1 and thus adjusting the light amount 
emitted from the exposure lamp 2. The thickness of the photoconductive 
layer is assumed by an influx current I.sub.pc. 
The influx current I.sub.pc is detected by a detecting section 21 with the 
drum 1 being rotated and the main charger C and the eraser lamp 7 being 
driven. As shown in FIG. 3, the detecting section 21 comprises a 
resistance 21a and an A/D converter 21b. The resistance 21a grounds the 
conductive base of the drum 1, and the A/D converter 21b converts voltages 
generated at both ends of the resistance 21a and sends the converted 
voltages to the control section 22. 
The control section 22, which comprises an input interface 22a, a CPU 22b, 
a ROM 22c, a RAM 22d and an output interface 22e (FIG. 4), obtains an 
optimum light amount to be emitted from the exposure lamp 2 and the 
thickness d of the photoconductive layer based on the voltages sent from 
the A/D converter 21b. 
The principle of the sensitivity compensation of the photoconductive drum 1 
will be explained hereinafter. 
The influx current I.sub.pc supplied to the photoconductive layer and the 
charge amount Q accumulated in the photoconductive layer, both per a unit 
area, have the following relationship: 
EQU Q.apprxeq.k.sub.1 .multidot.I.sub.pc (3) 
where k.sub.1 is a constant determined by a length of the drum 1 in an 
axial direction thereof and the rotating speed of the drum 1. 
From Equations (1), (2) and (3), the thickness d and the influx current 
I.sub.pc have the following relationship: 
##EQU2## 
where k.sub.2 is a constant (=.epsilon..sub.0 .multidot..epsilon..sub.r 
/k.sub.1). The grid voltage V.sub.g is kept at a certain level for the 
above reasons in the scorotron type main charger C. 
As apparent from Equation (4), the thickness d is obtained by the influx 
current I.sub.pc although indirectly. 
The thickness d and the sensitivity of photoconductive layer have the 
following relationship: 
##EQU3## 
".alpha.", which is a constant obtained from the relationship between a 
carrier generation efficiency in the CGL and an electric field strength 
(V.sub.0 /d), varies in accordance with the kind of the photoconductive 
layer. In the organic photoconductive layer used in this embodiment (a 
lamination of a disazo system charge generating layer and a hydrazone 
system charge transporting layer), .alpha.=0.8. 
Accordingly, 
##EQU4## 
where d.sup.0 : initial thickness 
d.sup.1 : thickness after image forming repetition 
E.sub.0.sup.0 : initial optimum light amount 
E.sub.0.sup.1 : optimum light amount after image forming repetition 
The initial optimum light amount, which is set when the photoconductive 
drum 1 is mounted in the copier, is stored in a non-volatile memory 
provided in the copier. 
The optimum light amount after image forming repetition is also expressed 
by: 
##EQU5## 
where I.sub.pc.sup.0 : initial influx current 
I.sub.pc.sup.1 : influx current after image forming repetition 
I.sub.pc.sup.0 is measured when the photoconductive drum 1 is mounted in 
the copier and stored in the non-volatile memory. Based on the measured 
influx current I.sub.pc.sup.1, the control section 22 executes the 
operation of Equation (7) to obtain E.sub.0.sup.1. Then, the control 
section 22 sends a predetermined control signal to the voltage applying 
section 14, whereby E.sub.0.sup.1 is set in the exposure lamp 2. 
The control section 22 also determines the life expectancy of the 
photoconductive drum 1 based on the thickness d which has been obtained 
through the operation of Equation (4). The operator is notified that the 
photoconductive drum 1 should be renewed. When the photoconductive drum 
completes a life thereof, black streams appear on the copying paper or 
half-tone images are blurred. These problems are conspicuous when a 22 
.mu.m thick photoconductive layer gets 12 .mu.m thick, for example. 
How to determine the life expectancy will be described hereinafter. 
If the present thickness d.sup.1, which is estimated from Equation (4), 
exceeds the predetermined value, the control section 22 drives a warning 
display 23 to display a warning message or illuminate a warning lamp. 
In another conceivable construction, the number of copies which have been 
made so far is stored, and the stored number and the present thickness 
d.sup.1 are used to obtain how much thickness is taken away from the 
photoconductive layer per copy. Based on the obtained thickness, how many 
more copies can be made is determined and displayed. 
Where the number of copies which have been made is C.sub.1, the thickness 
which is taken away per copy is: 
EQU (d.sup.0 -d.sup.1)/C.sub.1 
Where the total number of copies is C.sub.TOTAL and the least possible 
thickness necessary for image forming is d.sub.E, 
##EQU6## 
How many more copies can be made (C.sub.r) is expressed 
##EQU7## 
Cr is also obtained from Equations (4) and (9) based on the influx current 
I.sub.pc. 
Embodiment II 
In the first embodiment, the optimum light amount E.sub.0.sup.1 is obtained 
based on the measured influx current I.sub.pc. A second embodiment 
concerns a copier equipped with a photoconductive drum 1' including a 
organic photoconductive layer which generates an offset current I.sub.po 
(a kind of a lamination of a disazo system charge generating layer and a 
hydrazone system charge transporting layer). 
As shown in FIG. 5, the offset current I.sub.po, which does no contribution 
to the charging of the drum 1', is varied in accordance with the ambient 
temperature or humidity of the photoconductive layer. In such a case, the 
influx current I.sub.pc and the surface potential V.sub.0 do not have the 
relationship mentioned in the first embodiment. The thickness d cannot 
obtained accurately unless the offset current I.sub.po is considered. 
As shown in FIG. 5, the influx current I.sub.pc and the surface potential 
V.sub.0 are in proportion to each other both at 32.5.degree. C. and 
14.0.degree. C. where the surface potential V.sub.0 is a certain level 
(200 V in this case) or above. In other words, the surface potential 
V.sub.0, the grid voltage V.sub.g and the influx current I.sub.pc have the 
following relationship, with the same slope regardless of the temperature: 
##EQU8## 
It is said from Equation (11) that the slope of the line indicating the 
relationship between the surface potential V.sub.0 and the influx current 
I.sub.pc is obtained by measuring the influx current I.sub.pc at least at 
two points in the area where the surface potential V.sub.0 and the influx 
current I.sub.pc are in proportion to each other regardless of the amount 
of the offset current. The thickness d is estimated by that slope. 
FIG. 6 shows a construction of such a copier. In addition to the elements 
of the first embodiment, the copier has a bypass circuit 13 for grounding 
a connecting point A of the varistors 12a and 12b. The bypass circuit 13 
includes a switching section 13a, which de-electrifies the bypass circuit 
13 by a command from a control section 22.degree. in the normal copying 
mode. When the bypass circuit 13 is de-electrified, the grid electrode 11 
of the main charger C is grounded through the varistors 12a and 12b, 
whereby the surface potential V.sub.0 =V.sub.a +V.sub.b. When the bypass 
circuit 13 is electrified, the surface potential V.sub.0 =V.sub.a. In this 
way, the surface potential V.sub.0 is switched over two steps, whereby 
detecting two levels of the influx current I.sub.pc. 
The detailed explanation will follow. The grid voltage V.sub.g is switched 
to V.sub.a or V.sub.a +V.sub.b to detect the influx current I.sub.pc(a) or 
I.sub.pc(a+b) of each case. The relationship among the grid voltages 
V.sub.a and V.sub.a+b and the influx currents I.sub.pc(a) and 
I.sub.pc(a+b) is expressed by: 
##EQU9## 
The thickness d, which is assumed from Equation (14), is expressed by: 
##EQU10## 
From Equations (5) and (13), the optimum light amount E.sub.0.sup.1 for the 
above thickness is expressed by: 
##EQU11## 
where I.sub.pc(a+b).sup.0 : initial influx current corresponding to the 
grid voltage of V.sub.a +V.sub.b 
I.sub.pc(a+b).sup.0 : initial influx current corresponding to the grid 
voltage of V.sub.a 
The control section 22' sends a predetermined control command signal to the 
voltage applying section 14 in accordance with Equation (16), whereby the 
light amount emitted from the exposure lamp 2 is adjusted. 
I.sub.pc(a).sup.0 and I.sub.pc(a+b).sup.0 are set when the photoconductive 
drum 1' is mounted in the copier and stored in the nonvolatile memory. 
In the first and second embodiments, the sensitivity compensation is done 
by adjusting the light amount emitted from the exposure lamp 2. Such a 
compensation method stabilizes the high quality of images since the 
surface potential V.sub.0 before exposure, the potential V.sub.i of the 
exposed portion and the developing bias voltage V.sub.B are kept the same. 
Embodiment III 
The sensitivity compensation can also be done by adjusting a developing 
bias voltage V.sub.B. 
FIG. 7 shows the principle of compensating the sensitivity by adjusting the 
developing bias voltage V.sub.B. 
As described in detail before, when the photoconductive layer is worn away, 
the potential at the exposed portion of the layer is not lowered enough. 
Practically, the surface potential at the exposed portion is not lowered 
down to V.sub.i but only to V.sub.i ', which is higher than the developing 
bias voltage V.sub.B. 
In a copier as the third embodiment shown in FIG. 8, a control section 22" 
sends a developing bias voltage setting signal based on the measured 
influx current I.sub.pc to a power supply 30". Based on the signal, the 
power supply 30" changes the developing bias voltage to be applied the 
developing device 4 from V.sub.B to V.sub.B ', which is higher than 
V.sub.i '. 
In this embodiment, it is not necessary that the exposure lamp 2 allows the 
light amount to be increased or that the heat generated by the exposure 
lamp 2 is considered, as distinct from the first and the second 
embodiments. 
The sensitivity compensation may also be done by adjusting the surface 
potential. The thickness d of the photoconductive layer is assumed based 
on the measured influx current I.sub.pc, and a control section controls 
the output of a main charger based on the measured influx current 
I.sub.pc, whereby the surface potential after exposure is lowered than the 
surface initial potential. 
Or the light amount emitted from the exposure lamp, the developing bias 
voltage and the surface potential may all be adjusted. 
This invention is also applicable to a copier equipped with an inorganic 
photoconductive layer as far as the layer is worn away by repeated image 
forming procedure. Needless to say, other image forming apparatuses such 
as an LED printer and a laser printer are covered, in which case, the 
output level of the print head or the laser diode is adjusted. 
Although the present invention has been fully described by way of 
embodiments with references to the accompanying drawings, it is to be 
noted that various changes and modifications will be apparent to those 
skilled in the art. Therefore, unless such changes and modifications 
depart from the scope of the present invention, they should be construed 
as being included therein.