Embodiments of the present invention relate to a driving circuit of a plasma display panel (PDP) and a driving method thereof, more particularly to a driving circuit of a PDP and a driving method thereof, which can ensure simplification of the driving circuit and a stable sustain discharge waveform.
An alternating current plasma display panel (AC-PDP) has a structure including three electrodes, i.e., a scan electrode Y, a sustain electrode X and an address electrode A, and controls brightness by inducing stable discharge of cell using voltages applied to the respective electrodes. Such an AC-PDP is time-divisionally driven by dividing one frame into several subfields having different light-emitting times so as to realize a gray scale of an image.
Each of the subfields is divided into three periods, i.e., a reset period, an address period and a sustain period. The reset period is a period for controlling the state of a uniform wall charge suitable for discharge conditions of all cells in the panel to be maintained with respect to a voltage applied from the outside of the panel so as to induce stable address discharge in the address period. The address period is a period for selecting cells to be discharged and cells not to be discharged in the sustain period by sequentially applying a scan pulse to all scan electrodes and simultaneously applying a data pulse of a data voltage Vd to address electrodes. At this time, the discharge cells experience a large change in wall charge, and the discharge condition is formed so that sustain discharge can be sustained in the sustain period. The sustain period is a period for allowing the sustain discharge to be sustained in only the cells selected as discharge cells in the address period by alternately applying a high sustain discharge voltage Vsus between the scan and sustain electrodes.
Meanwhile, as shown in
A PDP driving circuit that realizes the driving waveform of
As described above, the conventional PDP driving circuit has a very complicated configuration, including a plurality of control switches. Therefore, it requires high manufacturing cost.
Therefore, the present invention has been made in view of the above problems, and provides a driving circuit of a PDP, which can ensure simplification of the driving circuit and a stable sustain discharge waveform.
In an aspect, the present invention provides a driving method of a plasma display panel (PDP) including a first electrode applying a ramp-up voltage, a ramp-down voltage, a scan pulse voltage, level voltage and a sustain discharge voltage; a second electrode; and a third electrode applying a data voltage for selecting discharge cells in an address period, the driving method using a driving waveform divided into a reset period, an address period and a sustain period, wherein, in the sustain period, positive and negative sustain discharge voltages are alternately applied to the first electrode and a ground voltage GND is applied to the second electrode.
In the reset period of the driving waveform, the maximum amplitude of the ramp voltage applied to the first electrode in the ramp-up period may be set differently for each subfield. The maximum amplitude of a ramp voltage of the first electrode in a ramp-up period is identical to or smaller than the sum of the positive sustain discharge voltage and the level voltage of the first electrode
In the ramp-up period, the voltage applied to the first electrode may not contain a level voltage component but may contain only a waveform with a slope using the positive sustain discharge voltage. Before the ramp-up period starts, a negative sustain discharge voltage may be applied to the first electrode.
In the ramp-up period, the ramp voltage rising with a slope applied to the first electrode may have two different slopes. Generally, a first slope may be steeper than a second slope. Alternatively, the second slope may be steeper than the first slope.
A voltage Vyd at the end time of the reset period may be identical to or higher than the negative sustain discharge voltage −Vsus. In a ramp-down period of the reset period, the ramp voltage falling with a slope may have two different slopes. Generally, a first slope may be steeper than a second slope.
The absolute values of the positive and negative sustain discharge voltages applied to the first electrode may be identical to each other. Alternatively, the absolute values of the positive and negative sustain discharge voltages applied to the first electrode may be different from each other.
In the ramp-down period, a level voltage may be applied to the second electrode. In some cases, the level voltage may be 0 V. As occasion demands, the level voltage applied to the second electrode may be a ground voltage GND (0 V) in the address period.
In accordance with another aspect of the present invention, there is provided a PDP driving circuit controlling a driving waveform divided into a reset period, an address period and a sustain period, the driving circuit controlling a ramp-up voltage, a ramp-down voltage, a scan pulse and a sustain discharge voltage applied to a first electrode; a level voltage applied to a second electrode; and a data voltage applied to a third electrode, wherein the driving circuit has a combination of a first electrode board controlling the voltage applied to the first electrode and a second electrode board controlling the voltage applied to the second electrode, and the first electrode board includes: a control switch SW3 supplying a positive sustain discharge voltage +Vsus; a control switch SW4 supplying a negative sustain discharge voltage −Vsus; a control switch SW5 connected to the positive sustain discharge voltage to generate a ramp-up waveform rising with a slope; and a control switch SW6 connected to the negative sustain discharge voltage to generate a ramp-down waveform falling with a slope.
The first electrode board may further include a control switch device for energy recovery having first and second control switches SW1 and SW2; and a capacitor CR storing energy recovered by the first and second control switches. A negative terminal of the capacitor CR storing the recovered energy may be connected to the negative sustain discharge voltage −Vsus, or a positive terminal of the capacitor CR may be connected to the ground voltage GND of 0 V.
The first electrode board may further include a scan device having control switches SW9 and SW10, and a positive terminal of the control switch SW9 may be connected to a level voltage Vyl of the first electrode. Alternatively, a positive terminal of the level voltage Vyl may be connected to a diode D3 restricting reverse current and a capacitor C1 stabilizing the level voltage Vyl, and a negative terminal of the level voltage Vyl may be connected to the negative sustain discharge voltage −Vsus.
The second electrode board may include a control switch SW7 applying a level voltage Vxl to the second electrode; and a control switch SW8 applying a ground voltage. Particularly, when the level voltage Vxl of the second electrode is 0 V, the second electrode of the PDP may be directly connected to the ground voltage GND. In this case, no control switch may be used in the second electrode board.
Although it has been described in the driving waveform and the driving circuit that a voltage of 0 V is not used in the first electrode, the voltage of 0 V may be used. In this case, the voltage of 0 V may be applied to the first electrode in a period preceding the ramp-up period, a period preceding the sustain period, or the like. The PDP driving circuit may further include a control switch SW11 applying a voltage of 0 V and a diode D4 connected in series to the control switch SW11, and the diode D4 may be connected to the ground voltage. Alternatively, the PDP driving circuit may further include control switches SW12 and SW13 connected in series, and the control switch SW12 may be connected to the ground voltage.
A PDP driving circuit and a driving method thereof according to the present invention have advantages as follows.
The PDP driving circuit according to the present invention has a simpler circuit configuration than the conventional PDP driving circuit. In the PDP driving circuit according to the present invention, a sustain discharge voltage can be more stably supplied to a panel than in the conventional PDP driving circuit. In the conventional PDP driving circuit of
Hereinafter, a driving circuit of a plasma display panel (PDP) and a driving method thereof according to embodiments of the present invention will be described in detail with reference to the accompanying drawings.
First of all, the PDP driving waveform shown in
The PDP driving waveforms of
First, the period T1 corresponds to a ramp-up period of a reset period. A ramp-up process functions to reduce a difference of wall charges between discharge and non-discharge cells in a previous subfield. In case of a discharge cell, due to sustain discharge, negative (−) charges are accumulated on the cell wall positioned at a second electrode of the discharge cell, and positive (+) charges are accumulated on the cell wall positioned at a first electrode of the discharge cell. The discharge cell is in the state that the sustain discharge can be operated when a sustain discharge voltage is applied. On the other hand, in case of a non-discharge cell, the state of wall charges that have been formed during a ramp-down period of a reset period in the previous subfield is still maintained at cell walls respectively positioned at first and second electrodes of the non-discharge cell. That is, at the final time of the previous subfield or the start time of a current subfield, the state of wall charges in the discharge cell selected to operate the sustain discharge is different from that of wall charges in the non-discharge cell that was not selected. For this reason, it is required to readjust the states of wall charges to be uniform. In each of the cells that were discharge cells in the previous subfield, positive (+) charges are accumulated on a dielectric positioned at a first electrode and negative (−) charges are accumulated on a dielectric positioned at a second electrode by a negative sustain discharge voltage pulse which is a sustain discharge voltage pulse for final discharge. Here, instead of a positive square type sustain discharge voltage pulse, a ramp-up type reset driving wave is applied to generate a weak discharge, thereby preventing a rapid change in wall charge. In the case of the non-discharge cell, although a weak discharge is not generated even though a voltage increases up to a positive sustain discharge voltage Vsus. However, if a voltage higher than the positive sustain discharge voltage is applied to the non-discharge cell, a weak discharge is generated alike the discharge cell which was discharged in the previous subfield. The weak discharge is generated by applying a high ramp voltage in the initial subfield of subfields for displaying an image.
In a subsequent subfield, the high ramp voltage used in the first subfield is not used, but a ramp voltage lower than the high ramp voltage is usually used to decrease background light luminance. The state of wall charges in the non-discharge cells is the same as that at the end time of the period T2 in which the reset is finished. For this reason, in case of some subfields, the maximum ramp-up voltage may be smaller than that in the first subfield, or the period T1, in which a ramp-up type reset driving waveform is applied, may not be included, if required so. Further, a level voltage Vyl of the first electrode may not be used in the ramp-up period.
At the end time of the period T1, the state of wall charges in the discharge cell is not completely identical to that of wall charges in the non-discharge cell. However, the state of wall charges in the discharge cell becomes identical to that of wall charges in the non-discharge cell because of the period T2 which is a ramp-down period. The ramp-down period is a period in which the voltage of the first electrode decreases down to a voltage Vyd. Here, the voltage may be decreased to have two slopes when the voltage decreases down to the voltage Vyd as shown in
In the period T2, the cells that were discharge cells in the previous subfield have more wall charges than those of the non-discharge cells during the reset period having the ramp-up type reset driving waveform. For this reason, a relatively large number of weak discharges are generated. Accordingly, the sate of wall charges in the discharge cells is identical to that of wall charges in the non-discharge cells, and the reset discharge process is finished. Then, it is ready to start an address discharge.
After the reset periods T1 and T2 are finished, the address period T3 starts. In the period T3, a scan pulse is sequentially applied to respective scan lines of first electrodes that are scan electrodes. First, the level voltage Vyl of the first electrodes is applied to all the first electrodes based on the voltage Vsc. Here, the level voltage Vyl is applied to the positive high-voltage input terminal of the scan device, and the voltage Vsc is applied to the negative high-voltage input terminal of the scan device. While the voltage Vyl is connected as an output of each of the scan lines and applied to cells, the voltage Vsc is sequentially connected as an output of each of the scan lines, so that the respective scan lines are sequentially selected. Simultaneously, address discharge is generated by applying a data voltage Vd to a third electrode that is an address electrode A. At this time, the data voltage is controlled to be applied only to data lines of cells to be discharged in all the cells of the selected scan lines. In a cell in which the address discharge is generated, positive (+) charges are accumulated on the wall of the first electrode in the cell, and negative (−) charges are accumulated on the wall of the second electrode in the cell. Like in the period T2, the level voltage of the second electrode may be set as 0 V in the period T3, depending on the state of the PDP.
In the cells selected as discharge cells through the address discharge, a continuous sustain discharge is generated as a sustain discharge voltage is applied in the period T4. The continuous sustain discharge is generated by alternately applying positive and negative sustain discharge voltage +Vsus and −Vsus to a Y electrode. On the other hand, in the non-discharge cell, wall charges are not accumulated sufficiently to induce discharge with the sustain discharge voltage only. For this reason, discharge is not generated there. The number of pulses of the sustain discharge is controlled to express luminance, and may be varied depending on the subfields.
PDP driving waveforms according to the embodiments of the present invention have been described. Hereinafter, a PDP driving circuit for realizing the PDP driving waveforms according the embodiments of the present invention will be described.
As shown in
In the first electrode board, the control switches SW1 and SW2 are control devices for energy recovery, and a capacitor CR connected between the control switches SW1 and SW2 is a capacitor for energy recovery, in which recovered energy is charged. A negative terminal of the capacitor CR for energy recovery is connected to a negative sustain discharge voltage source. In some cases, the capacitor for energy recovery may not be used, but a middle node connected between a drain terminal of the first control switch SW1 and a source terminal of the second control switch SW2 may be connected to a ground GND. The control switch SW3 supplies a positive sustain discharge voltage +Vsus to the panel and is connected to the positive sustain discharge voltage +Vsus. The control switch SW4 supplies the negative sustain discharge voltage −Vsus to the panel and is connected to the negative sustain discharge voltage −Vsus. The control switch SW5 is used to generate a ramp-up waveform that rises with a predetermined slope. The control switch is connected to the positive sustain discharge voltage +Vsus and is designed to supply a voltage as high as the positive sustain discharge voltage +Vsus. The control switch SW6 is used to generate a ramp-down waveform that falls with a predetermined slope, and connected to the negative sustain discharge voltage −Vsus. The control switch SW4 applying the negative sustain discharge voltage −Vsus is commonly used as a control switch that supplies a negative high voltage to the scan device in an address period.
Meanwhile, the driving circuit is designed so that the level voltage Vyl of a first electrode has a predetermined voltage level based on a negative high-voltage input terminal of the scan device and is applied to a positive high-voltage input terminal of the scan device. As shown in
The second electrode board includes control switches SW7 and SW8. Here, the control switch SW7 applies the level voltage Vxl of a second electrode to the second electrode board, and the control switch SW8 applies a ground voltage GND of 0 V to the second electrode board. In some cases, the level voltage Vxl of the voltages applied to the second electrode board may be applied as 0 V throughout the entire region. In this case, the control switches SW7 and SW8 may be omitted as shown in
Hereinafter, the operation of the PDP driving circuit configured as described above will be described with reference to a timing diagram.
As shown in
First, the period T1 is shown in
In the period T2, the rising output voltage of the first electrode falls down to the voltage Vyd, and uniformity of wall charges can be stably achieved without causing any strong discharge. To this end, the ramp voltage Vramp that rises above than the positive sustain discharge voltage is decreased down to the positive sustain discharge voltage. In the first electrode board, while the control switch SW9 of the scan device is off, the control switch SW10 of the scan device is on, and the control switch SW3 supplying the positive sustain discharge voltage Vsus is on. In the second electrode board, the control switch SW8 remains in an on state. As shown in
Thereafter, in a ramp-down period, a control switch operation is performed, in which the rising output voltage of the first electrode falls with a slope down to the voltage Vyd that is the final voltage of the ramp-down waveform. Specifically, in the first electrode board, the control switch generating a slope of the ramp-down waveform is on. In the second electrode board, the control switch SW7 is on and the control switch SW8 is off so as to apply the level voltage Vxl of the second electrode. Here, the level voltage Vxl of the second electrode may be applied from the period T3 that is an address period. In this case, a control switch conversion operation is not performed in the second electrode board. As the output voltage of the first electrode board decreases continuously with a slope, it may decrease to have two slopes like in the PDP driving waveforms shown in
As shown in
Subsequently, the period T3 is a period in which address discharge is induced to distinguish discharge cells from non-discharge cells. In the period T3, two voltages are applied each of the scan electrodes through the scan device of the first electrode board. The scan device has the same number of control switches SW9 and SW10 as the number of scan lines. For reference, only a pair of control switches SW9 and SW10 are shown in the drawings of the present invention, for the convenience of simplicity.
The operation of the PDP driving circuit in the period T3 will be described. A voltage −Vsc is applied to the negative high-voltage input terminal of the scan device. Here, the voltage −Vsc is a voltage identical to the negative sustain discharge voltage −Vsus. Simultaneously, a voltage Vyl-Vsc higher by the voltage Vyl than the voltage −Vsc is applied to the positive high-voltage input terminal. In this case, the control switch SW4 remains in an on state, and the control switches SW9 and SW10 of the scan device apply a scan pulse by operating in such a manner that the control switch SW10 is sequentially on for each of the scan lines. Here, the level voltage Vyl of the first electrode board is not greater than the maximum allowance voltage applied to the scan device. As a corresponding scan line is selected while the voltage Vyl-Vsc is applied to each of the scan electrodes by allowing the control switches SW9 and SW10 to be on and off, respectively, the control switch W9 is off and the control switch SW10 is on only in the corresponding scan line. Accordingly, the voltage −Vsc is applied as the scan pulse. At this time, in the second electrode board, the control switch SW8 is off and the control switch SW7 is on so as to apply the level voltage Vxl of the second electrode.
Current flow in the period T3 will be described with reference to
Finally, the period T4 will be described. The period T4 that is a sustain discharge period is complicated as compared with the periods T1, T2 and T3. First, after the period T3 that is an address period is finished, the control switch SW1 is on and the control switch SW4 is off in the energy recovery circuit. In the scan device, the control switch SW9 is off and the control switch SW10 is on. As such, if the control switch SW1 is on, the voltage applied to the negative high-voltage terminal of the scan device increases smoothly by means of the LC resonance induced by an inductor LR of the energy recovery circuit and a capacitor component of the panel CP. Subsequently, when the control switch SW3 is on to apply the positive discharge voltage Vsus, discharge is performed in the discharge cell. At this time, the control switch SW1 may be off or on. Then, after a certain time is maintained to generate a sufficient discharge, the control switches SW1 and SW3 are off, and the control switch SW2 is on so as to recover energy supplied to the panel. Therefore, the voltage is changed into the negative sustain discharge voltage −Vsus by means of the LC resonance induced by the inductor LR and recovery capacitor CR of the energy recovery circuit. Thereafter, if the control switch SW4 applying the negative sustain discharge voltage is on, discharge is performed in the discharge cell so that the first electrode of the discharge cell has negative charge. In this case, the control switch SW2 may also be off or on. In all the periods where the switching of the first electrode board is performed to apply a sustain discharge voltage, the control switch SW9 of the second electrode board remains on so as to apply a voltage of 0 V.
The current flow in the period T4 will be described with reference to
The operation of the PDP driving circuit in the periods T1 to T4 has been described. After the period T4 is finished, the voltage waveform of the second electrode is connected to a reset waveform of the next subfield. Two methods may be used as a method for raising the switching driving voltage described in the period T1. A first method is a method in which a voltage is increased up to a predetermined level by allowing the control switch SW1 of the energy recovery circuit to be on, and the control switch SW is then off. A second method is a method in which a driving circuit having two slopes is implemented using the control switches SW5 as described above.
The PDP driving circuit according to the embodiment of the present invention has a simpler circuit configuration than that of the conventional PDP driving circuit. In
Meanwhile, an application of a ground voltage GND to the second electrode waveform will be described as another embodiment of the present invention.
At the time when a ramp-up period starts after a negative sustain discharge voltage −Vsus is applied, a control method is not used, in which the ramp-up control switch is immediately on, or the ramp-up voltage has two slopes using the control switch SW1 of the energy recovery circuit. However, as shown in
The driving circuit for realizing the PDP driving waveform of the
The invention has been described in detail with reference to exapmle embodiments thereof. However, it will be appreciated by those skilled in the art that changes may be made in these embodiments without departing from the principles and spirit of the invention, the scope of which is defined in the accompanying claims and their equivalents.
A PDP driving circuit and a driving method thereof according to the present invention have advantages as follows.
The PDP driving circuit according to the present invention has a simpler circuit configuration than the conventional PDP driving circuit. In the PDP driving circuit according to the present invention, a sustain discharge voltage can be more stably supplied to a panel than in the conventional PDP driving circuit. In the conventional PDP driving circuit of
Number | Date | Country | Kind |
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10-2007-0095785 | Sep 2007 | KR | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/KR2008/005560 | 9/19/2008 | WO | 00 | 3/16/2010 |