1. Field of the Invention
The present invention relates to a driving circuit for driving a driven element, a driving apparatus including the driving circuit and the driven element, and an image forming apparatus including the driving apparatus.
2. Description of the Related Art
Driven elements such as light-emitting diodes (LEDs), organic electroluminescence elements (organic light-emitting diodes or OLEDs), and light-emitting thyristors generally have temperature dependencies. The LEDs used as light-emitting elements in the optical print heads (LED heads) of LED printers, which are a type of electrophotographic printer, emit less optical power as their temperature rises. Since the printing darkness of an LED printer varies depending on the emitted optical power, the LED drive current must be changed to compensate for variations in emitted optical power caused by such temperature changes.
As disclosed, for example, by Nagumo in U.S. Pat. No. 6,028,472 (Japanese Patent Application Publication No. H10-332494) and Japanese Patent Application Publication No. 2006-159472 (now Japanese patent No. 4498905), an LED printer has a plurality of LEDs, driver integrated circuits (ICs) for feeding drive current to the LEDs, and a reference voltage generating circuit for supplying a reference voltage to the driver ICs. The drive current fed to the LEDs is proportional to the reference voltage applied to the driver ICs, so for temperature compensation, the reference voltage generating circuit in the above disclosures operate with a positive temperature coefficient that causes the reference voltage to increase as the temperature rises.
The reference voltage generating circuit disclosed in U.S. Pat. No. 6,028,472 outputs a voltage substantially proportional to absolute temperature. The reference voltage generating circuit disclosed in JP 2006-159472 provides a temperature coefficient that can be set to different values by selection of suitable components.
An LED head must hold the emitted optical power of the LEDs at the prescribed level as the LED temperature rises even if the temperature rise is due to the driving of the LEDs. There is also a need for a temperature compensation circuit having a temperature coefficient that is flexibly settable according to the temperature characteristics and luminous efficiency of the LEDs, which vary depending on the crystalline material and emission wavelength.
For LEDs with some characteristics, the reference voltage generating circuit in U.S. Pat. No. 6,028,472, which outputs a reference voltage proportional to absolute temperature, is unable to perform appropriate temperature compensation.
JP 2006-159472 discloses a reference voltage generating circuit with an internal diode-generated forward voltage drop. The voltage drop has a temperature coefficient that compensates for the temperature coefficient of the LEDs, but if the voltage drop is made large enough to obtain an adequate range of compensation, the reference voltage supplied to the driver ICs is reduced to such a low value that voltage noise effects etc. become significant. In the presence of such noise effects, it becomes difficult to specify a reference voltage that produces the desired output from the LEDs.
An object of the present invention is to provide a driving circuit that can provide correct temperature compensation for a variety of driven elements, without suffering from noise effects.
The invention provides a driving circuit for driving a driven element. The driving circuit includes a reference voltage generating circuit for generating a reference voltage, and a driver circuit for driving the driven element at a level responsive to the reference voltage.
In some embodiments, the reference voltage generating circuit includes a regulating section that generates a first voltage, a temperature compensation section that generates a second voltage responsive to the first voltage, and a voltage amplifying section that generates the reference voltage by amplifying the second voltage.
The reference voltage generating circuit may include a bipolar transistor that operates with a temperature characteristic that compensates for the temperature characteristic of the driven element.
The amplification factor of the voltage amplifying section is high enough to provide a reference voltage resistant to noise voltage effects.
The temperature coefficient of the temperature compensation section and the amplification factor of the voltage amplifying section can be set independently, enabling the driving circuit to compensate for the temperature characteristics of various types of driven elements while maintaining a sufficiently high reference voltage level.
In an alternative embodiment, the driver circuit includes a control voltage generating circuit having a bipolar transistor that operates with a temperature characteristic that compensates for the temperature characteristic of the driven element. In this case the temperature compensation section and amplifying section of the reference voltage generating circuit may be omitted. The control voltage is generated from the reference voltage, and controls the driving level of the driven element.
The invention also provides a driving apparatus incorporating the invented driving circuit and the driven element, and an image forming apparatus incorporating this driving apparatus.
By providing temperature compensation without noise vulnerability, the invention reliably assures that the driven element provides uniform output as its temperature changes. In an image forming apparatus, this results in images of consistent quality, regardless of changes in driven element temperature.
In the attached drawings:
Embodiments of the invention will now be described with reference to the attached drawings, in which like elements are indicated by like reference characters.
In an electrophotographic printer (an LED printer, for example), an optical print head (an LED head, for example) selectively illuminates the surface of a photosensitive drum according to print information to form a latent electrostatic image on the drum surface. The latent image is developed by application of toner to form a toner image, which is then transferred from the drum surface to paper and fixed onto the paper by heat and pressure.
Referring to
The printing control unit 11 includes a microprocessor, a read-only memory (ROM), a random access memory (RAM), input-output ports, timers, and other well-known facilities (not shown). The printing control unit 11 forms part of a printing unit (not shown) that uses the LED printer to execute printing operations. The printing control unit 11 controls the printing operations of the LED printer in response to a control signal SG1, a data signal SG2, etc. received from an image processing unit (not shown), and sends the LED head 100 a print data signal HD-DATA, clock signal HD-CLK, latch signal HD-LOAD, and negative-logic strobe signal HD-STB-N. The data signal SG2 is sometimes referred to as a video signal because it supplies dot-mapped data one-dimensionally.
When the printing control unit 11 receives a printing command by means of control signal SG1, it checks the fuser temperature sensor 15b to determine whether the fuser 15 is at the necessary temperature for printing. If it is not, current is fed to the heater 15a to raise the temperature of the fuser 15. Next, the printing control unit 11 commands motor driver 14a to turn the develop/transfer process motor 14 and concurrently turns on the high-voltage charging power source 12a by means of a charge signal SGC to charge the developing unit 12.
Next, the printing control unit 11 checks the paper sensor 19 to confirm that paper is present in a cassette (not shown), checks the paper size sensor 20 to determine the type of the paper, and commands the motor driver 16a to turn the paper transport motor 16. The paper transport motor 16 turns in the reverse direction bring a sheet of paper out of the cassette, and stops turning when the pick-up sensor 17 detects the paper. Next, the paper transport motor 16 turns in the forward direction to transport the paper into the printing mechanism in the LED printer.
When the paper is in position for printing, the printing control unit 11 sends the image processing unit a timing signal SG3 (including a main scanning synchronization signal and a sub-scanning synchronization signal) and receives the video signal SG2. The image processing unit responds by sending edited dot data for one page in the video signal SG2. The printing control unit 11 sends corresponding dot data (HD-DATA) to the LED head 100 in synchronization with the clock signal (HD-CLK). The LED head 100 comprises a linear array of LEDs for printing respective dots (also referred to as picture elements or pixels). After receiving data for one line of dots in the video signal SG2 and sending the data to the LED 100, the printing control unit 11 sends the LED head 100 the latch signal (HD-LOAD), causing the LED head 100 to store the print data (HD-DATA). The print data stored in the LED head 100 can then be printed while the printing control unit 11 is receiving the next print data from the image processing unit in the video signal SG2.
The video signal SG2 is transmitted and received one printing line at a time. For each line, the LED head 100 forms a latent image of dots with a comparatively high electric potential on the photosensitive drum (not visible), which is negatively charged. In the developing unit 12, negatively charged toner is electrically attracted to the dots, forming a toner image. The drum and toner are both charged by the high-voltage charging power source 12a.
The toner image is then transported to the transfer unit 13. The printing control unit 11 activates the high-voltage transfer power source 13a by sending it a transfer signal SG4, and the toner image is transferred to the sheet of paper as it passes between the photosensitive drum and transfer unit 13. The sheet of paper carrying the transferred toner image is transported to the fuser 15, where the toner image is fused onto the paper by heat generated by the heater 15a. Finally, the sheet of paper carrying the fused toner image is transported out of the printing mechanism, passing the exit sensor 18, and ejected from the printer.
The printing control unit 11 controls the high-voltage transfer power source 13a according to the information detected by the pick-up sensor 17 and size sensor 20 so that voltage is applied to the transfer unit 13 only while paper is passing through the transfer unit 13. When the paper passes the exit sensor 18, the printing control unit 11 stops the supply of voltage from the high-voltage charging power source 12a to the developing unit 12, and halts the turning of the photosensitive drum and various rollers (not shown) driven by the develop/transfer process motor 14. The above operations are repeated to print a series of pages.
The LED head 100 according to the first embodiment will be described with reference to
The driver ICs all have the same internal circuit configuration. In this configuration, a shift resister circuit 31 receives the clock signal HD-CLK and serially transfers the print data. A latch circuit 32 latches data signals output from the shift resister circuit 31 in parallel according to the latch signal (HD-LOAD). An inverter 33 receives the strobe signal (HD-STB-N). A NAND circuit 34 receives the outputs of the latch circuit 32 and the inverter circuit 33. An LED drive circuit 35 supplies drive current from a power source node VDD to the LED array chips (CHP1 etc.) according to signals output from the NAND circuit 34. A control voltage generating circuit 36 for generates a control voltage that controls the drive currents output from the LED drive circuit 35 so that they remain constant despite possible fluctuations in the power source potential.
In this embodiment, the driven elements are the LEDs (not shown) in the LED arrays CHP1 to CHP26. The driving circuit includes the driver ICs IC1 to IC26 and the reference voltage generating circuit 40. The LED head 100 as a whole is the driving apparatus:
The LED head 100 in
Referring to
The driving circuit receives a first power source potential at various nodes denoted VDD in the drawings, and a second power source potential various nodes denoted by the ground symbol and the letters GND. The VDD nodes will be referred to collectively as the power source VDD; the ground (GND) nodes will be referred to simply as ground. In the embodiments described herein, the first power source potential (also denoted Vdd) is positive with respect to the second power source potential. These power source potentials are supplied to all the driver ICs in
The regulator circuit 41 has a power terminal 41a connected to the power source VDD, an output terminal 41b connected to the control terminal or base terminal 42b of the npn bipolar transistor 42, and a ground terminal 41c connected to ground. The npn bipolar transistor 42 has its first main terminal or emitter terminal 42e connected to ground through resistor 43, and its second main terminal or collector terminal 42c connected to the power source VDD. The npn bipolar transistor 42 and resistor 43 constitute an emitter-follower circuit. The emitter terminal 42e of the npn bipolar transistor 42 is also connected to the non-inverting input terminal 46a of the operational amplifier 46. One terminal of resistor 44 and one terminal of resistor 45 are connected to the inverting input terminal 46b of the operational amplifier 46. The other terminal of resistor 44 is grounded, and the other terminal of resistor 45 is connected to the output terminal 46c of the operational amplifier 46. The output terminal 46c of the operational amplifier 46 is connected to the output terminal VREF of the reference voltage generating circuit 40.
The output voltage V1 of the regulator circuit 41 remains substantially constant, with respect to ground, despite variations in the first power source potential. The regulator circuit 41 may also be designed so that its output voltage V1 remains substantially constant despite temperature variations, that is, so that V1 has a zero temperature coefficient. The value of the output voltage V1 is a design choice that can be made by selecting appropriate components for the regulator circuit 41, if the regulator circuit 41 is configured using discrete components, or by selecting an appropriate type of regulator circuit 41, if the regulator circuit 41 is obtained as an integrated circuit from an IC manufacturer. In either case, the optimum output voltage V1 should be selected according to the other design conditions of the driving apparatus.
The operation of the first embodiment will now be described. Referring to the timing diagram in
For comparison with the reference voltage generating circuit 40 in
As noted above, the output voltage of the regulator circuit 41 is substantially independent of the potential Vdd of the power source VDD. If the output voltage of the regulator circuit 41 is denoted V1, the base-emitter potential of the npn bipolar transistor 42 is denoted Vbe, the potential at the emitter terminal 42e of the npn bipolar transistor 42 is denoted V2, and the resistance values of resistors 61 and 62 are denoted R61 and R62, respectively, the emitter potential V2 is given by the following equation (1)
V2=V1−Vbe (1)
hand the reference voltage Vra output at the VREFa terminal is given by the following equation (2).
V1 is the known output voltage of the regulator circuit 41. The base-emitter voltage Vbe is a known characteristic of the npn bipolar transistor 42 and can be considered to be approximately 0.6 V. The base-emitter voltage Vbe of the npn bipolar transistor 42 has a negative temperature dependency, that is, Vbe decreases as the temperature increases. The temperature coefficient of Vbe is approximately minus two millivolts per degree Celsius (−2 mV/° C.). It will be assumed below that resistors 61 and 62 are of identical type or material and have identical temperature dependencies. Their temperature dependencies then cancel in the term R61/(R61+R62) on the right in equation (2), so this term can be ignored when the temperature dependency of the output voltage Vra is considered.
On this basis, the temperature coefficient Tc of the output voltage Vra of the conventional reference voltage generating circuit in
Assuming that the temperature coefficient of the output voltage of the regulator circuit 41 is negligible, the temperature coefficient Tc of the reference voltage Vra at the VREFa terminal of the reference voltage generating circuit 90 in
From equations (1) and (4), comparative examples 1 to 4 can be obtained for the temperature coefficient Tc and reference voltage Vra in
If V1 is 1.4 V (V1=1.4 V), the temperature coefficient Tc is:
If R61 is zero, the reference voltage Vra at the VREFa terminal is:
If V1 is 1.2 V (V1=1.2 V), the temperature coefficient Tc is:
If R61 is zero, the reference voltage Vra at the VREFa terminal is:
If V1 is 0.9 V (V1=0.9 V), the temperature coefficient Tc is:
If R61 is zero, the reference voltage Vra at the VREFa terminal is:
If V1 is 0.8 V (V1=0.8 V), the temperature coefficient Tc is:
If R61 is zero, the reference voltage Vra at the VREFa terminal is:
Different types of LEDs are used to obtain different wavelengths of emitted light, and these different types have different temperature characteristics. To provide temperature compensation, the different types of LEDs therefore require different drive current temperature coefficients. An aluminum gallium arsenide (AlGaAs) LED requires a drive current temperature coefficient of approximately 0.25%/° C. A gallium arsenide (GaAs) LED requires a drive current temperature coefficient of approximately 0.6%/° C. An aluminum gallium indium phosphorus (AlGaInP) LED requires a drive current temperature coefficient of approximately 1%/° C.
These differing requirements are met by changing the output voltage value V1 for the regulator circuit 41, but as comparative examples 1-4 indicate, to obtain a temperature coefficient as high as +1.0%/° C., the reference voltage Vra must be reduced to the value of 0.2 V. A reference voltage this low is highly vulnerable to noise voltage effects in the driver ICs and the wiring traces by which they are connected to the reference voltage generating circuit. A low reference voltage is particularly undesirable if, as in
Referring again to
In
Vr={1+(R2/R1)}×V2 (5)
According to equation (1),
V2=V1−Vbe
From equations (1) and (5), the following equation (6) is obtained.
Vr={1+(R2/R1)}×(V1−Vbe) (6)
These equations indicate that the voltage amplifying section 53 generates the reference voltage Vr by amplifying the voltage V2 generated in the temperature compensation section 52 by a factor of (1+R2/R1), and can therefore increase the reference voltage Vr by this factor (1+R2/R1) without changing the temperature coefficient of the voltage V2. As an example, if the ratio of R1 to R2 is one to five (1:5), a reference voltage Vr equal to six times the value of V2 can be obtained.
This provides the following example of the temperature coefficient Tc and reference voltage Vr in the first embodiment.
If V1 is 0.8 V (V1=0.8 V), the temperature coefficient Tc is:
If R2/R1 is five (R2/R1=5), the reference voltage Vr at the VREF terminal is:
Whereas the reference voltage Vra is only 0.2 V in the corresponding comparative example (4) for the conventional reference voltage generating circuit 90 in
The presence of the operational amplifier 46 in the voltage amplifying section 53 adds to the cost of the reference voltage generating circuit 40 in the first embodiment. Even if reference voltage generating circuit 40 is manufactured as a monolithic integrated circuit chip, the operational amplifier 46 occupies relatively large chip area, increasing the chip cost. However, as seen from Example 5 above, to obtain the temperature coefficient of +1.0%/° C. needed for temperature compensation of AlGaInP LEDs, the reference voltage generating circuit 40 in the first embodiment is preferable despite the additional cost.
To summarize the first embodiment, the regulating section 51 (regulator circuit 41) used in the reference voltage generating circuit 40 (
In the voltage amplifying section 53, any desired voltage amplification factor can be obtained by selecting resistance values R1 and R2 that produce a suitable ratio (R1/R2). Moreover, the temperature coefficient of the voltage amplifying section 53 itself is negligibly small. As a result, the temperature coefficient Tc of the reference voltage Vr can be set by selecting a regulating section 51 with a suitable output voltage, and the value of the reference voltage Vr can be set independently from the temperature coefficient Tc, by selecting suitable resistance values in the voltage amplifying section 53.
Accordingly, whereas in the configuration in the example in
Referring to
Referring to
The second main terminal or drain terminal 82d of PMOS transistor 82 is connected to ground through resistor 83. The drain terminal 82d of PMOS transistor 82 is connected to the output (VREF) terminal. The resistance values of resistors 43, 83 are denoted R11, R12, respectively, the potential at the output terminal 41b of the regulator circuit 41 is again denoted V1, the potential at the emitter terminal 42e of the npn bipolar transistor 42 is again denoted V2, and the potential at the VREF terminal is again denoted Vr. The emitter current of the npn bipolar transistor 42 is denoted Ie. The drain current of PMOS transistor 82 is denoted Iy. Overall, reference voltage generating circuit 70a is divided into three blocks: a regulating section 71 including the regulator circuit 41, a temperature compensation section 72 including the npn bipolar transistor 42 and resistor 43, and a voltage amplifying section 73 including the PMOS transistors 81, 82 and resistor 83.
Referring to
In
To calculate the drain potential V0 of PMOS transistor 101, first current I1 will be determined. Electronics theory teaches that the following equation (7) holds between the emitter current Ie and base-emitter voltage Vbe of an npn bipolar transistor.
Ie≅Is*exp(qVbe/(kT)) (7)
In this equation, Is indicates saturation current, which is a constant proportional to the device area of an npn bipolar transistor; the asterisk indicates multiplication; exp( ) indicates the exponential function; q indicates the electron charge, which is 1.6*10−19 C; k is the Boltzmann constant, which is 1.38*10−23 J/K; and T indicates absolute temperature, which is approximately 298 K at a room temperature of 25° C.
From equation (7), the following equation (8) is obtained.
Vbe=(kT/q)*ln(Ie/Is) (8)
In this equation, ln( ) indicates the natural logarithm function. If Vbe1 and Vbe2 are the base-emitter voltages, Ie1 and Ie2 are the emitter currents, and Is1 and Is2 are the saturation currents of npn bipolar transistors 104 and 105, respectively, then equation (8) gives the following equations (9) and (10) for npn bipolar transistors 104 and 105.
Vbe1=(kT/q)*ln(Ie1/Is1) (9)
Vbe2=(kT/q)*ln(Ie2/Is2) (10)
In
ΔVbe=Vbe1−Vbe2 (11)
If equations (9) and (10) are substituted into equation (11) and the result is rearranged, the following equation (12) is obtained.
Since the ratio between the emitter areas of the npn bipolar transistors 104 and 105 is 1:N, where N>1, and the saturation current of a bipolar transistor is proportional to its emitter area, the following equation (13) is true.
Is2=Is1×N (13)
PMOS transistors 101 and 102 constitute a current mirror circuit. If their drain currents I1 and I2 have the same value, then the base-emitter currents Ie1 and Ie2 of the npn bipolar transistors 104 and 105 become identical and the following equation (14) is true.
ΔVbe=(kT/q)×ln(N) (14)
The drain current I1 of PMOS transistor 101 substantially equals the current passing through the resistor 106 with resistance value R21, so the following equation (15) is true.
Since drain current I1 flows through the resistor 106 with the resistance value R22, the drain potential value V0 is obtained from the following equation (16).
The first term (I1×R22) on the right side of equation (16) indicates a positive temperature coefficient with respect to absolute temperature. The second term (Vbe1) on the right side indicates the temperature coefficient of the base-emitter voltage of an npn bipolar transistor, which is approximately −2 mV/° C., exhibiting a negative dependency. As a result, the temperature dependency of the potential V0 can be set to a positive or negative value or a substantially zero value by proper selection of the ratio of resistance values R22 and R21.
To estimate the voltage Vreg at the VREG terminal in
If I3 equals I1 (I3=I1), the voltage Vreg is given by the following equation (18).
Since Vreg is proportional to the absolute temperature T, its temperature coefficient is 1/T, equal to approximately +0.33%/° C. at room temperature.
The graph in
Assuming that the base-emitter voltage Vbe1 is 0.6 V, the temperature coefficient Tc is obtained from the following equation (19).
Point Pe in
Tc=+0.33%/° C. (20)
In
The temperature compensation section 72 in
The current amplification ratio of npn bipolar transistor 42 is large and its base current is smaller than its emitter-collector current. As a result, the collector current of the npn bipolar transistor 42 in
Ie≅Iy (22)
The emitter current Ie of npn bipolar transistor 42 is expressed by the following equation (23).
Ie=V2/R11 (23)
The reference voltage is given by the following equation.
Vr=Iy×R12 (24)
From equations (23) and (24), the following equation (25) is obtained.
Vr=(R12/R11)×V2 (25)
From equation (25), it is clear that the voltage amplifying section 73 generates an output voltage Ve that is R12/R11 times the V2 potential. As a specific example, if the ratio of resistance values R11 and R12 in
From equation (1),
V2=V1−Vbe
Thus the potential Vr at the VREF terminal can be obtained by the following equation (26).
Vr=(R12/R11)×(V1−Vbe) (26)
Next, the temperature coefficient of the reference voltage Vr for the combination of the configurations in
Equation (27) can be rewritten as the following equation (28).
In the regulator circuit output voltage Vreg at the VREG terminal in
If Vreg is set to 1.2 V (Vreg=1.2 V) by selection of a suitable R23 value in
From equation (21), the temperature coefficient is expressed as follows.
Then from equation (26),
Vr=(R12/R11)×(Vreg−Vbe)
Therefore, if R12/R11 is equal to two (R12/R11=2), the following reference voltage Vr can be obtained:
If Vreg is set to 1.8 V (Vreg=0.8 V) by selection of a suitable R23 value in
From equation (21), the temperature coefficient Tc is expressed as follows.
From equation (26), it follows that:
Vr=(R12/R11)×(Vreg−Vbe)
Accordingly, by setting R12/R11 to unity (R12/R11=1), the following reference voltage Vr is obtained.
As described above, a reference voltage Vr with a comparatively large temperature coefficient can be obtained by taking the output of the regulator circuit 41 from the drain 103d of PMOS transistor 103 as in
An advantage of the reference voltage generating circuit in the second embodiment is that it can fit in a small chip area, because it does not include any large for component such as an operation amplifier.
The circuits in a driver IC in the second embodiment that are concerned with the printing of one dot by driving one LED are shown in
The control voltage generating circuit 36 shown in
The ground terminal 34b of the NAND gate 34 is accordingly connected to the output terminal 114c of the operational amplifier 114, while the power source terminal 34a of the NAND gate 34 is connected to the power source VDD. When the output terminal 34c of the NAND gate 34 is at the high logic level, its output potential is substantially equal to the potential Vdd of the power source VDD; when the output terminal 34c is at the low logic level, its output potential is substantially equal to the control voltage Vcont. The gate length of PMOS transistor 116 is proportional to the gate length of PMOS transistor 112.
The VREF terminal is connected to the inverting input terminal 114a of the operational amplifier 114, and receives the reference voltage Vr generated by the reference voltage generating circuit 70a shown in
Ir=Vr/Rr (29)
As noted above, PMOS transistors 112 and 116 have proportional gate lengths. When the LED 113 is driven, the gate potentials of PMOS transistors 112 and 116 are both equal to the control voltage Vcont, and both transistors operate in their saturation regions, so they form a current mirror and the drive current supplied to the LED 113 is proportional to the reference current Ir, which is proportional to the reference voltage Vr input at the VREF terminal. The drive currents supplied to the LEDs are therefore all adjusted in unison by means of the reference voltage Vr.
As described above, the configuration of the driving circuit in the second embodiment makes it possible to set both the voltage value and the temperature coefficient of the reference voltage Vr to desired values. In particular, regardless of the temperature coefficient, the voltage value of the reference voltage Vr can be high enough to make noise voltages negligible by comparison, thereby avoiding noise-induced variations in LED drive current. Moreover, this effect is obtained with a reference voltage generating circuit 70a that does not require a large component such as an operation amplifier. The cost of the reference voltage generating circuit 70a is correspondingly low.
The second embodiment permits variations in the configurations of the temperature compensation section 52 and voltage amplifying section 53 of the reference voltage generating circuit. Two variations will be described below; other variations are possible as well.
Referring to
The resistance values of the resistors 43, 83, 84 in
The resistor 84 added to the reference voltage generating circuit 70b in
The current Ir mainly depends on the output voltage V1 of the regulator circuit 41 and the resistance values R13 and R11 of resistors 84 and 43, so its temperature dependency can be reduced to a small value. The base current of the npn bipolar transistor 42 is negligibly small, so the collector current is substantially equal the emitter current Ie. As the PMOS transistors 81 and 82 constitute a current mirror circuit, their drain currents can be made substantially identical to each other. If this is done, the drain current Iy of PMOS transistor 82 equals the drain current of PMOS transistor 81, which is the collector current of npn bipolar transistor 42, and is therefore substantially equal to the emitter current Ie. If the resistance value R13 of resistor 84 is reduced and current Ir is increased, current Ie is reduced by an equal amount, and current Iy is likewise reduced, but the reference voltage Vr can be kept at the prescribed level by increasing the resistance value R12 of resistor 83. Since the temperature dependent current Ie is reduced and the temperature independent current Ir is increased, the temperature coefficient is reduced.
The emitter current of npn bipolar transistor 42 is indicated by the dotted lines Ie0 and Ie in the graph
In both
Referring to
The resistance values of the resistors 43, 83, 91, and 92 in
Resistors 91, 92 and pnp bipolar transistors 93, 94 constitute a current mirror circuit that operates similarly to the current mirror in
If these resistance values R21 and R22 are mutually equal and are sufficiently large, currents Ie and Iy become substantially identical, even if there is some difference between the characteristics of the pnp bipolar transistors 93 and 94. This is particularly advantageous when the reference voltage generating circuit 70c is assembled by mounting discrete components such as transistors and resistors on a printed-wiring board, since precisely matched resistors can be obtained more easily than precisely matched transistors. The desired reference voltage can be obtained by selection of resistors 43, 83 with an appropriate resistance ratio, as in the reference voltage generating circuit 70a in
Referring to
The inverter 33 in
As indicated in
The NAND gate 34 has a power supply terminal 34a connected to the power source VDD and a ground terminal 34b connected to ground. When the output terminal 34c of the NAND gate 34 is at the high logic level, the NAND output potential is substantially equal to the potential Vdd of the power source VDD; when the output terminal 34c is at the low logic level, the NAND output potential is substantially equal to the ground potential. The output terminal 34c of the NAND gate 34 is connected to the gate terminal 125g of PMOS transistor 127. PMOS transistor 127 is accordingly switched off when the output terminal 34c of the NAND gate 34 is at the high logic level, and on when the output terminal 34c is at the low logic level. When PMOS transistor 127 is switched on, the amount of current Io determined by PMOS transistor 112 is supplied to the LED 113.
Since the gate lengths of PMOS transistors 112 and 122 are proportional, their source terminals 112s, 122s are at mutually identical potentials, and their gate terminals 112g, 122g are at mutually identical potentials, PMOS transistors 112 and 122 form a current mirror.
The regulated output voltage Vreg generated by the regulator circuit 41 shown in
In
Ir=(Vreg−Vbe)/R11 (30)
In the equation above, Vbe indicates the base-emitter voltage of npn bipolar transistor 125 and R11 indicates the resistance value of resistor 124. The regulator circuit output voltage Vreg is held at a prescribed value by the regulator circuit 41. The base-emitter voltage Vbe also has a prescribed value, typically about 0.6 V. Accordingly, the reference current Ir can be set to a desired value by selection of a resistor 124 with an appropriate resistance value R11.
PMOS transistors 112 and 122 have identical gate lengths, and their gate potentials are identically equal to the control voltage Vcont. PMOS transistors 112 and 122 both operate in their saturation region and thus constitute a current mirror circuit. As a result, the drive current Io supplied to the LED 113 is proportional to the reference current Ir. The reference current Ir is determined by the regulator circuit output voltage Vreg input to the VREG terminal, so all the LED drive currents supplied from one driver IC can be adjusted in unison by adjusting the regulator circuit output voltage Vreg. In addition, the npn bipolar transistor 125 in the control voltage generating circuit 36a in
Examples of the temperature coefficient will now be described. If the constant of proportionality between the LED drive current Io and the reference current Ir is K, the following relational expression (31) is true.
Io=K×Ir (31)
Since
Ir=(Vreg−Vbe)/R11
the following equation (32) is true.
Io=K×(Vreg−Vbe)/R11 (32)
The temperature coefficient Tc of the drive current Io is given by the following equation (33), in which T indicates temperature.
If the temperature dependency of the resistance value R11 of resistor 124 is negligibly small, the following equation (34) is obtained.
If, for simplification, the temperature coefficient of the output voltage of the regulator circuit 41 is zero, which is obtainable with the alternative regulator circuit configuration in
Given that the base-emitter voltage Vbe of the npn bipolar transistor 125 has a temperature dependency of approximately −2 mV/° C., the control voltage generating circuit 36a in
When Vreg is 1.2 V (Vreg=1.2 V) and Vbe is 0.6 V (Vbe=0.6 V), the temperature coefficient Tc of the LED drive current Io is expressed as follows.
The LED drive current Io can be set by selecting a proper resistance value R11 and mirror ratio K, and is adjustable separately from the temperature coefficient value.
As described in detail above, the drive circuit in the third embodiment enables the LED drive current Io and its temperature coefficient Tc to be set independently to desired values. Accordingly, the temperature coefficient Tc can be set to a value that provides correct temperature compensation for the type of LEDs used, while the reference voltage Vreg that controls the LED drive current can have a value large enough to make the effects of noise voltage negligible.
The drive circuit in the third embodiment is low in cost because it includes no operational amplifier or other large components.
The electrophotographic print heads described in the preceding embodiments can be used in, for example, the tandem color printer illustrated in
Process unit 603 includes a photosensitive drum 603a that turns in the direction indicated by the arrow. Disposed around the photosensitive drum 603a are a charger 603b for charging the surface of the photosensitive drum 603a by supplying electrical charge, an exposure unit 603c for forming a latent image by selectively illuminating the surface of the charged photosensitive drum 603a, a developing unit 603d for forming a toner image by applying magenta toner to the surface of the photosensitive drum 603a on which a latent image is formed, and a cleaning unit 603e for removing toner left after the toner image is transferred from the photosensitive drum 603a. The LED head described in any one of the three preceding embodiments is used as the exposure unit 603c. The drums and rollers used in the process units are driven by a motor such as the develop/transfer process motor 14 in
The printer 600 has at its bottom a paper cassette 606 for holding a stack of paper or other recording media 605. Disposed above the paper cassette 606 is a hopping roller 607 for taking sheets of the recording medium 605 separately from the paper cassette 606. Disposed downstream of the hopping roller 607 in the transport direction of the recording medium 605 are a pair of pinch rollers 608, 609, a transport roller 610 for transporting the recording medium 605 past pinch roller 608, and a registration roller 611 for transporting the recording medium 605 past pinch roller 609. The hopping roller 607, transport roller 610, and registration roller 611 are driven by a motor such as the paper transport motor 16 in
Each of the process units 601 to 604 also includes a transfer roller 612, made of a semiconductive rubber or similar material, facing the photosensitive drum. A voltage applied to the transfer roller 612 creates an electrical potential difference between the surfaces of the photosensitive drum and the transfer roller 612. This potential difference transfers the toner image formed on the photosensitive drum onto the recording medium 605.
A fuser 613, which includes a heating roller and a backup roller, fuses the toner image onto the recording medium 605 by pressure and heat. A pair of delivery rollers 614 and 615 and a pair of pinch rollers 616 and 617 disposed downstream of the fuser 613 transport the recording medium 605 from the fuser 613 to a recording medium stacker 618. The delivery rollers are also driven by a motor and gears (not shown).
The operation of the tandem color printer 600 will be described briefly. The hopping roller 607 picks up the sheet at the top of the stack of recording medium 605 in the paper cassette 606. The recording medium 605 is carried between the transport roller 610 and pinch roller 608, aligned against the registration roller 611 and pinch roller 609, and then carried between the registration roller 611 and pinch roller 609 into the black process unit 601. As the recording medium 605 is transported between the photosensitive drum and transfer roller of process unit 601 by the rotation of its photosensitive drum, a toner image is transferred onto the recording surface of the recording medium 605.
The recording medium 605 then passes through the other process units 602 to 604, which transfer toner images of other colors onto its recording surface. The toner images of all four colors are fused onto the recording medium 605 by the fuser 613 to form a full-color image, and the recording medium 605 is ejected by the delivery rollers 614 and 615 and their pinch rollers 616 and 617 onto the recording medium stacker 618 outside the printer 600.
A printer, copier, or similar image forming apparatus using any of the LED heads in the embodiments described can produce images of consistently high quality.
Similar effects can be obtained not only in full-color image forming apparatus as described above but also in monochrome and multiple-color image forming apparatus, but greatest advantages can be obtained in full-color image forming apparatus with many optical printing heads.
Applications of the invention are also envisioned in the driving of light-emitting thyristors, light-emitting transistors, organic light-emitting diodes (OLEDs), and resistive heating elements. For example, the invention can be used in electrophotographic printers having OLED heads with arrays of OLEDs, light-emitting thyristor heads with arrays of three-terminal or four-terminal light-emitting thyristors, or thermal printers having arrays of resistive heating elements.
The present invention can be also applied to the driving of an array of display elements arranged in a row or matrix, by control of the voltage applied to the display elements. For example, the invention can be employed with an array of thyristors used as switching elements for driving arrays or matrices of display elements.
Those skilled in the art will recognize that further variations are possible within the scope of the invention, which is defined in the appended claims.
Number | Date | Country | Kind |
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2010-027905 | Feb 2010 | JP | national |