1. Field of the Invention
The present invention relates to a power supply circuit for supplying power to an electronic device such as an image forming apparatus.
2. Description of the Related Art
A developing device in an electrophotographic or electrostatic printing image forming apparatus efficiently develops an electrostatic latent image with toner by applying, to a developing sleeve, a voltage in which DC (Direct Current) and AC (Alternating Current) voltages are superposed. In particular, an AC voltage having a rectangular waveform increases the charging efficiency of toner with respect to a latent image (ratio at which toner charges couple with latent image charges).
A voltage applied to the developing sleeve needs to have a target value. This is because various problems arise if an applied voltage greatly exceeds a target voltage to generate an overshoot. For example, a current flows through an unintended conductor via the surface of an insulator or an air layer. Also, aerial discharge occurs in a conductive impurity mixed in a developing agent, damaging a latent image. As one solution to relieve these problems, a damping resistor having a sufficiently large resistance value is adopted.
However, the use of the damping resistor also has disadvantages. For example, the rise and fall responses become slower than those of an ideal rectangular wave, resulting in a blunt rectangular wave. The blunt rectangular wave is poorer in charging efficiency than the ideal rectangular wave. The power loss across the damping resistor accounts for half the input power to an AC voltage generation circuit, increasing the space for permitting the energy loss and raising the component cost.
In Japanese Patent Laid-Open No. 2002-354831, an AC voltage generation circuit is formed from a full bridge circuit made up of four switching elements. A predetermined OFF period is set in part of a period during which each switching element is turned on. This arrangement relieves an overshoot without depending on a damping resistor.
The invention disclosed in Japanese Patent Laid-Open No. 2002-354831 can correct an output waveform distortion by LC resonance satisfactorily for a developing unit, photosensitive member, developing high-voltage power supply, and developing agent under a given condition. However, a problem arises when the conventional technique is applied to a so-called blank pulse waveform having a pulse period during which a rectangular wave is output and a blank period during which output of a rectangular wave stops.
It is a feature of the present invention to achieve stable development while decreasing dependence on a damping resistor by suppressing a shape distortion of a blank pulse waveform.
The present invention provides an image forming apparatus comprising the following elements. A developing unit develops a latent image with a developing agent. A supply unit supplies, to the developing unit, a developing alternating current bias voltage with a waveform having a pulse period during which a rectangular wave is output and a blank period during which no rectangular wave is output. An input signal generation unit generates, as an input signal be supplied to a primary side of a transforming unit that forms the developing alternating current bias voltage, an input signal obtained by adding an additional pulse smaller in width than the rectangular wave in the pulse period at a timing to transit from the pulse period to the blank period.
Further features of the present invention will become apparent from the following description of exemplary embodiments (with reference to the attached drawings).
An image forming apparatus 100 shown in
When a host controller (not shown in
The AC voltage generation circuit 201 functions as an AC voltage generation unit which outputs a blank pulse waveform having a pulse period during which a rectangular wave is output and an idle period (blank period) during which no rectangular wave is output. The AC voltage generation circuit 201 and transformer T1 generate and output an AC voltage (rectangular wave) to be superposed on a DC voltage. The AC voltage generation circuit 201 includes a full bridge circuit made up of four semiconductor switching elements Q1, Q2, Q3, and Q4. The semiconductor switching elements Q1, Q2, Q3, and Q4 correspond to the first, second, third, and fourth switching units, respectively. The semiconductor switching element Q1 has one end coupled to a +24 V voltage source, and the other end coupled to a primary-side (primary winding-side) first terminal Ta of the transformer T1 and one end of the semiconductor switching element Q2. The other end of the semiconductor switching element Q2 is coupled to ground (that is, grounded). The semiconductor switching element Q3 has one end coupled to the +24 V voltage source, and the other end coupled to a primary-side second terminal Tb of the transformer T1 and one end of the semiconductor switching element Q4. The other end of the semiconductor switching element Q4 is coupled to ground. The transformer T1 is an example of a transforming unit which has the primary-side first terminal Ta coupled to the other end of the first switching unit and one end of the second switching unit, and the primary-side second terminal Tb coupled to the other end of the third switching unit and one end of the fourth switching unit, and receives a blank pulse waveform generated by the AC voltage generation unit.
A drive signal generation circuit 202 outputs gate signals to the gates (driving terminals) of the respective semiconductor switching elements to turn on Q1, off Q2, off Q3, and on Q4. As a result, a voltage is applied so that the potential at the first terminal Ta of the transformer winding becomes higher than that at Tb, generating a voltage with a positive amplitude in the secondary winding. Similarly, in accordance with an output instruction, the drive signal generation circuit 202 outputs gate signals to turn off Q1, on Q2, on Q3, and off Q4. Then, a voltage is applied between Ta and Tb so that the potential at the second terminal Tb of the transformer winding becomes higher than that at Ta, generating a voltage with a negative amplitude in the secondary winding.
Referring to
Referring to
In the period T4 serving as the first ON period, the drive signal generation circuit 202 enables gate signals to Q2 and Q3. Then, the transformer T1 starts outputting a negative output voltage. In the period T5 serving as the OFF period, the drive signal generation circuit 202 disables the gate signals to Q2 and Q3 to suppress the resonant waveform. In the period T6 serving as the second ON period, the drive signal generation circuit 202 enables the gate signals to Q2 and Q3. Accordingly, the output voltage becomes a rectangular wave which falls from Vtar+ to a negative target value Vtar− in the periods T4 to T6. Note that even the sum of the periods T4 to T6 corresponds to the half cycle of the rectangular wave. This half cycle will be called Th−. In the first embodiment, the periods Th+ and Th− are equal to each other because the ratio of the absolute value of the positive target value Vtar+ and that of the negative target value Vtar− in the rectangular wave is 1:1. More specifically, the drive signal generation circuit 202 outputs the first and second drive signals so that the ratio of the duration Th+ of the first drive signal and the duration Th− of the second drive signal becomes equal to that of the maximum amplitude Vtar− of a half-wave output in correspondence with the second drive signal and the maximum amplitude Vtar+ of a half-wave output in correspondence with the first drive signal.
The first ON period, OFF period, and second ON period of the respective half-waves (half cycles) always satisfy T1≠T4, T2≠T5, and T3≠T6, and T1<T4. That is, the length of the first ON period T1 of the first drive signal differs from that of the first ON period T4 of the second drive signal. The length of the OFF period T2 of the first drive signal differs from that of the OFF period T5 of the second drive signal. The length of the second ON period T3 of the first drive signal differs from that of the second ON period T6 of the second drive signal. Further, the first ON period T4 of the second drive signal is longer than the first ON period T1 of the first drive signal. These conditions aim at reducing a distortion at the start of outputting a blank pulse waveform. In this fashion, the drive signal generation circuit 202 functions as a drive signal generation unit which outputs the second drive signal to the second and third switching units out of the four switching units to cause the AC voltage generation unit to output a rectangular wave of the second half cycle in the blank pulse waveform.
In the period T4′ serving as the first ON period, the drive signal generation circuit 202 enables the gate signals to Q1 and Q4. Then, the transformer T1 starts outputting a positive output voltage. In the period T5′ serving as the OFF period, the drive signal generation circuit 202 disables the gate signals to Q1 and Q4 to suppress the resonant waveform. In the period T6′ serving as the second ON period, the drive signal generation circuit 202 turns on Q1 and Q4. As a result, a rectangular wave which changes from the negative target voltage Vtar− to the positive target value Vtar+ in the periods T4′ to T6′ is obtained. In this case, T4=T4′, T5=T5′, and T6=T6′ suffice. This is partly because the potential difference between an initial value (0) and the negative target value Vtar− and that between the initial value and the target value Vtar+ have peak-to-peak symmetry. Also, a voltage applied across the primary side of the transformer T1 has peak-to-peak symmetry between a case in which Q1 and Q4 of the AC voltage generation circuit 201 are ON and a case in which Q2 and Q3 are ON.
In the period T4″, the drive signal generation circuit 202 enables the gate signals to Q2 and Q3. Then, the transformer T1 starts outputting a negative output voltage. In the period T5″, the drive signal generation circuit 202 disables the gate signals to Q2 and Q3 to suppress the resonant waveform. In the period T6″, the drive signal generation circuit 202 enables the gate signals to Q2 and Q3. Then, a rectangular wave which changes from the positive target value Vtar+ to the negative target value Vtar− in the periods T4″ to T6″ is obtained. The initial value in this period is Vtar+, which is different only in sign from the target value Vtar− in this period. Hence, T4=T4″, T5=T5″, and T6=T6″.
In the period T7, the drive signal generation circuit 202 disables all the gate signals to be supplied to Q1, Q2, Q3, and Q4 to transit from the pulse period to the blank period. In the period T8, the drive signal generation circuit 202 enables the gate signals to be supplied to Q2 and Q3 to suppress the resonant waveform. After that, the drive signal generation circuit 202 disables the gate signal to Q2. By controlling the gate signals in this manner, the output voltage transits from Vtar− to the target control value of 0 V in the periods T7 and T8. Thus, the drive signal generation circuit 202 functions as a drive signal generation unit which outputs the third drive signal to the second and third switching units to transit the blank pulse waveform from the pulse period to the blank period.
Note that the operation in the period T7 during which all the gate signals to be supplied to Q1, Q2, Q3, and Q4 are disabled is different from those in the periods T1 and T4 during which a voltage is applied to the primary terminal of the transformer T1. This is because the former operation is an operation of transiting to the blank period while the latter operation is an operation of generating a rectangular wave. Thus, T7≠T1≠T4, and T8≠T2≠T5. That is, the length of the first ON period T1 of the first drive signal, that of the first ON period T4 of the second drive signal, and that of the OFF period T7 of the third drive signal are different from each other. Further, the length of the OFF period T2 of the first drive signal, that of the OFF period T5 of the second drive signal, and that of the ON period T8 of the third drive signal are different from each other. These conditions aim at reducing the distortion which may occur when transiting from the pulse period to the blank period.
The use of the above driving sequence can provide a rectangular wave of two pulses in which a resonant distortion is suppressed. Thereafter, the drive signal generation circuit 202 ensures a period of a desired length during which Q1 and Q3 are turned on and Q2 and Q4 are turned off. This length is large enough to achieve a blank period (including the periods T7 and T8) determined at the design stage of the image forming apparatus. A waveform whose one cycle is defined by the start of the period T1 and the end of the blank period serves as a blank pulse waveform of two pulses and two blanks.
According to the first embodiment, the period T1 and period T4 (T4′ and T4″) each serving as the first ON period have different lengths, and the periods T2 and period T5 (T5′ and T5″) each serving as the OFF period have different lengths. In addition, the periods T7 and T8 during which output of the rectangular wave ends are added to the gate signal driving pattern. As is apparent from
As is apparent from
As described above, the embodiment can basically omit the damping resistor R1. However, the damping resistor R1 may be employed for another reason, for example, to adjust the response speed of the blank pulse waveform. The damping resistor R1 may also be used in a case in which no resonant waveform can be fully suppressed by only adjusting the length of each period. Even in this case, a small resistor can be adopted as the damping resistor R1, which is superior to the conventional technique.
In
The capacitance value of the added capacitor C3 is set to a value large enough not to change the voltage across the capacitor C3 from a potential difference of 6 V between the two power supply voltages of 18 V and 12 V, in order to suppress a change of the voltage across the capacitor C3 caused by a switching operation by semiconductor switching elements Q1, Q2, Q3, and Q4.
In the period T11 serving as the first ON period shown in
In the period T14, the drive signal generation circuit 202 enables gate signals to Q2 and Q3. Then, output of an output voltage with a negative amplitude starts. In the period T15, the drive signal generation circuit 202 disables the gate signals to Q2 and Q3 to suppress the resonant waveform. In the period T16, the drive signal generation circuit 202 enables again the gate signals to Q2 and Q3. In the periods T14 to T16, the amplitude of the output voltage changes from Vtar+ to Vtar−. As described above, Th+:Th−=3:2. The first ON periods, OFF periods, and second ON periods of the respective half-waves have relations of T11≠T14, T12≠T15, and T13≠T16. This is because the potential difference between the initial and target values of the amplitude differs between the respective half-waves. That is, the periods T11 to T16 have lengths corresponding to respective potential differences.
In the period T17, the drive signal generation circuit 202 enables the gate signals to Q1 and Q4. In response to this, an output voltage with a positive amplitude is output. In the period T18, the drive signal generation circuit 202 disables the gate signals to Q1 and Q4 to suppress the resonant waveform. In the period T19, the drive signal generation circuit 202 enables the gate signals to Q1 and Q4. In the periods T17 to T19, a rectangular wave whose amplitude changes from Vtar− to Vtar+ is obtained. The potential difference from the initial value to target value of the amplitude in the periods T14 to T16 is equal to that in the periods T17 to T19 except for the sign. However, a voltage applied across the primary side of the transformer T1 differs between a case in which Q1 and Q4 are ON and a case in which Q2 and Q3 are ON. More specifically, the voltage across the transformer T1 in transition from the initial value Vtar+ to the target value Vtar− is −18 V, whereas the voltage in transition from the initial value Vtar− to the target value Vtar+ is 12 V. From this, conditions which should be satisfied by the first ON period, OFF period, and second ON period are T14≠T17, T15≠T18, and T16≠T19.
In the period T14′, the drive signal generation circuit 202 enables the gate signals to Q2 and Q3. Then, output of an output voltage with a negative amplitude starts. In the period T15′, the drive signal generation circuit 202 disables the gate signals to Q2 and Q3 to suppress the resonant waveform. In the period T16′, the drive signal generation circuit 202 enables again the gate signals to Q2 and Q3. In the periods T14′ to T16′, a rectangular wave whose amplitude changes from Vtar+ to Vtar− is obtained. In the periods T14′ to T16′, conditions regarding the initial value Vtar+ and target value Vtar− are the same as those in the periods T14 to T16. Hence, T14=T14′, T15=T15′, and T16=T16′.
In the period T20, the drive signal generation circuit 202 disables all the gate signals to Q1, Q2, Q3, and Q4 to transit to the blank period. In the period T21, the drive signal generation circuit 202 enables the gate signals to Q2 and Q3 to suppress the resonant waveform. The operation in the period T20 during which all the gate signals to Q1, Q2, Q3, and Q4 are disabled is different from those in the periods T11 and T14 during which a voltage is applied to the transformer T1. Hence, T20≠T11≠T14, and T21≠T12≠T15 are established.
Finally, the drive signal generation circuit 202 enables the gate signals to Q1 and Q3, and disables those to Q2 and Q4. The amplitude of the output voltage then changes from Vtar− to 0 V.
By the above driving sequence, a rectangular wave of two pulses almost free from a resonant distortion can be obtained. Thereafter, the drive signal generation circuit 202 ensures a blank period by enabling the gate signals to Q1 and Q3 and disabling those to Q2 and Q4. The periods T20 and T21 are also part of the blank period.
The conditions imposed on the respective periods in the first and second embodiments have been explained. The practical lengths of the respective periods depend on conditions necessary for the developing bias. It suffices to determine the lengths of the respective periods by experiment or simulation to meet the above-described conditions.
While the present invention has been described with reference to exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.
This application claims the benefit of Japanese Patent Application No. 2010-212706, filed Sep. 22, 2010 which is hereby incorporated by reference herein in its entirety.
Number | Date | Country | Kind |
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