1. Field of the Invention
The present invention relates to a plasma display device and a method of driving the same.
2. Discussion of Related Art
A plasma display device is a flat panel display device that can display characters or images using a gas discharge plasma wherein, according to the size of the display panel, more than several hundreds of thousands to several millions of pixels are arranged in a matrix format.
A conventional plasma display device is driven by dividing one image frame into a plurality of subfields, and gray levels are displayed by the combination of the subfields. Each subfield includes a reset period, an address period, and a sustain period.
As the number of subfields in the image frame is increased, a false contour, which is an important problem with the image quality of a PDP, can be reduced. Accordingly, studies continue to search for a method for increasing the number of subfields in order to reduce a false contour, as do other various studies for securing an operation margin in driving of a plasma display device. Among others, one is a method using a ramp reset waveform.
When using a ramp reset waveform, a falling ramp reset waveform is applied in a state where plenty of wall charges are accumulated on the whole panel using a weak discharge according to the application of a rising ramp reset waveform, so that only wall charges that are proper for an address operation in a subsequent address period are retained, and the remaining wall charges are erased, making it possible to perform a low voltage address operation.
Among driving signals for driving a plasma display panel, in particular, a scan electrode driving signal has a very complicated waveform including an erase waveform in an erase period, a reset waveform in a reset period, an address waveform in an address period, and a sustain waveform in a sustain period. In the case of the reset waveform, its voltage falls from a very high electric potential to a ground electric potential or an electric potential close to ground, so the difference between the starting electric potential and the ending electric potential of the scan electrode during the time its voltage falls is very large, causing a problem in that its current can stress the driving circuit.
Accordingly, there is a need for an improved plasma display device capable of reducing or preventing deterioration due to current stress. It is an aspect of an exemplary embodiment of the present invention to provide an improved plasma display device and a driving method thereof by reducing or preventing the deterioration of components such as a switching device, and relieving current stress from a driving circuit.
In particular, it is a further aspect of an exemplary embodiment of the present invention to provide an improved plasma display device and a driving method thereof, capable of relieving current stress applied to a driving circuit when a large reduction in voltage occurs during a falling ramp reset waveform of a scan electrode.
Also, it is a further aspect of an exemplary embodiment of the present invention to provide a plasma display device and a driving method thereof, capable of reducing or preventing stress due to the overcurrent right after the plasma display device powers on.
In order to accomplish the above and other aspects, according to a first exemplary embodiment of the present invention, a plasma display device comprises a plasma display panel with a plurality of discharge cells corresponding to an electrode. A panel electrode driver drives the electrode with a low level power source, a switch controller, and falling ramp switch coupled between the electrode and the low level power source. The switch controller generates a switching pulse that causes the falling ramp switch to repeatedly couple and de-couple the electrode to the low level power source. This achieves a ramping reduction in the voltage of the electrode from a first voltage to a second voltage.
Herein, the respective turn-on period of the switching pulse (i.e., when the falling ramp switch couples the electrode to the low level power source) follows the equations below:
T=4a×C2/(Ipeak)2
According to a second embodiment, a plasma display device comprises a plasma display panel with a plurality of discharge cells corresponding to an electrode. A panel electrode driver drives the electrode with a low level power source, a switch controller, and falling ramp switch coupled between the electrode and the low level power source. The switch controller generates a switching pulse that causes the falling ramp switch to repeatedly couple and de-couple the electrode to the low level power source. This achieves a ramping reduction in the voltage of the electrode from a first voltage to a second voltage. In this second embodiment, the turn-on time of the switching pulse for an initial ramping reduction following a power-on of the plasma display device is shorter than the turn-on time of the switching pulse for other ramping reductions.
In the plasma display device according the first and second embodiments of the present invention, the electrode is a scan electrode that applies a reset waveform for resetting the discharge cells.
Also, the driving signals for the electrode include a reset period, an address period, and a sustain period. The first voltage may be a ground voltage, and the second voltage may be the lowest level voltage of the electrode during the reset period.
Also, the panel electrode driver can further include a sustain switch for generating a sustain waveform during the sustain period, and a rising switch for generating a rising ramp waveform during the reset period.
Also, the plasma display panel can further include a sustain electrode for generating a gas discharge together with the scan electrode, and an address electrode crossing the scan electrode and the sustain electrode.
Also, the panel electrode driver may be a scan electrode driver.
Also, the plasma display device may further include a sustain electrode driver for generating driving signals for the sustain electrode; and an address electrode driver for generating driving signals for the address electrode.
Also, the respective turn-on times of the switching pulse for the initial ramping reduction in the voltage of the electrode following a power-on of the plasma display device may be shorter than the respective turn-on times of the switching pulse for ramping reductions after the initial ramping reduction.
A third embodiment of the present invention includes a method of driving a plasma display device including a first electrode, a second electrode, and a third electrode crossing the first and second electrodes at a discharge cell, wherein an image frame comprises a plurality of subfields, the subfields including a reset period, an address period, and a sustain period. The method includes: (a) setting the first electrode to a first voltage; and (b) repeatedly coupling and de-coupling the first electrode to a low level power source in order to achieve a ramping reduction in a voltage of the first electrode from the first voltage to a second voltage, wherein the a time during which the first electrode is coupled to the low level power source follows the equations below:
T=4a×C2/(Ipeak)2
A fourth embodiment of the present invention includes a method of driving a plasma display device including a first electrode, a second electrode, and a third electrode crossing the first and second electrodes at a discharge cell, wherein an image frame comprises a plurality of subfields, the subfields including a reset period, an address period, and a sustain period. The method comprises (a) setting the first electrode to a first voltage; and (b) repeatedly coupling and de-coupling the first electrodes to a low level power source in order to achieve a ramping reduction in a voltage of the first electrode from the first voltage to a second voltage, wherein the ramping reduction during an initial subfield following a power-on of the plasma display device comprises a longer ramping time than the ramping reduction in another subfield.
In the method of driving the plasma display device according to the third and fourth embodiments of the present invention, the first electrode can have ground voltage following the power-on of the plasma display panel.
Also, the coupling and de-coupling can be done by applying a switching pulse to a falling ramp switch, wherein the falling ramp switch is coupled at one side to the first electrode, and coupled at a second side to the low level power source.
Also, the address period may include applying an addressing pulse to the first and third electrode, and the sustain period may include alternately applying a sustain discharge pulse to the first electrode and the second electrode.
Also, the first electrode may be a scan electrode for applying a reset waveform removing the wall charges of the discharge cell, the second electrode may be a sustain electrode for generating a sustain discharge together with the scan electrode, and the third electrode may be an address electrode for determining whether the discharge cell is turned on depending on display data.
These and/or other aspects and features of the invention will become apparent and more readily appreciated from the following description of certain exemplary embodiments, taken in conjunction with the accompanying drawings of which:
Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings so that those skilled in the art to which the present invention pertains can easily carry out the present invention. However, the present invention may be modified in many different forms and it should not be limited to the embodiments set forth herein. Also, in the context of the present application, when an element is referred to as being “coupled to” another element, it can be directly coupled to the another element or be indirectly coupled to the another element with one or more intervening elements interposed therebetween. Like reference numerals designate like elements throughout the specification.
In order to reduce or prevent a current stress associated with the ramping voltage, the present applicant has previously proposed the improved technique of Korean Patent Application No. 10-2004-0095008. However, although the improved technique disclosed there has proposed a useful solution controllably driving a switch in order to prevent the current stress, it fails to discuss the numeral value to concretely regulate the switch.
Immediately following the power-on of a plasma display device, it is in a state where energy storage elements of a capacitor are empty, and a buffer operation by means of an overcurrent is not sufficient to create a reset waveform. However, the prior art has not presented a solution to this problem.
As shown in
The controller 200 receives image signals from an external circuit to output address driving control signals, sustain electrode driving control signals, and scan electrode driving control signals. The controller is driven by dividing one frame into a plurality of subfields, wherein the respective subfields include a reset period, an address period, and a sustain period, over time during the operation.
The address electrode driver 300 receives the address driving control signals from the controller 200 and generates display data signals for selecting discharge cells to be transmitted through the respective address electrodes. The sustain electrode driver 400 receives the sustain electrode driving control signals from the controller 200 and generates a driving voltage to be transmitted through the sustain electrodes X. The scan electrode driver 500 receives the scan electrode driving control signals from the controller 200 and generates a driving voltage to be transmitted through the scan electrodes Y.
The plasma display panel 100 of
The reset period is when the wall charges formed in the previous sustain period are removed. During the reset period of a first subfield, a main reset waveform accumulates wall charges in the whole discharge cells and then removes them. During an auxiliary reset waveform, which occurs in subfields subsequent to the first subfield, the wall charges in the discharge cells discharged in the previous subfield are removed, without the process accumulating the wall charges in the discharge cells. The address period is the period during which the discharge cells to be displayed are selected, and the sustain period is the period during which a gas discharge occurs in the discharge cells selected in the address period.
First, during the reset period of the first subfield (a first subfield for each frame), i.e., when a main reset waveform is applied, a ramp voltage gradually rising in voltage from Vs to Vset to exceed a discharge initiating voltage, is applied to the scan electrode Y. While the ramp voltage is applied, weak discharges occur between the scan electrode Y and the address electrode A and the sustain electrode X. Owing to such a discharge, the negative (−) wall charges are accumulated on the scan electrode Y, and the positive (+) wall charges are accumulated on the address electrode A and the sustain electrode X.
Next, a ramp signal gradually falling in voltage from Vs to Vnf is applied to the scan electrode Y. At this time, the reference voltage (assumed to be 0V in
Generally, in the discharge cell, if the voltage exceeds the discharge initiating voltage Vfay between the scan electrode and the address electrode, or between the scan electrode and the sustain electrode, a gas discharge occurs between the scan electrode and the address electrode, or between the scan electrode and the sustain electrode. In particular, when the discharge occurs during the slowly falling ramp voltage, the wall voltage in the inside of the discharge cells is reduced at the same speed as the falling ramp voltage. Such a principle is described in detail in U.S. Pat. No. 5,745,086 and thus, the detailed description thereof will be omitted.
The node N2 between a sustain switch Ys and a ground switch Yg can be coupled to a power recovery circuit including a capacitor (e.g., energy recovery capacitor Cerc) and/or an inductor, and can use the LC resonance between the panel capacitance and the inductor to improve the efficiency of power consumption.
In
A scan driver IC is coupled to the high level and low level scan signal suppliers 530 and 540, making it possible to drive a scan electrode used for the display.
Also, the sustain driver 520 is coupled to the node N1 via a main path, wherein a rising ramp switch Yset generating a ramp waveform rising in the reset period and a falling ramp switch Yfr generating a ramp waveform falling therein is coupled to the main path.
The sustain driver 520 generates an AC sustain discharge pulse using a sustain switch Ys coupled to a high level power source Vs and a ground switch Yg coupled to a low level power source 0V.
The high level scan signal supplier 530 includes a scan capacitor Csc of which one end is coupled to a high level scan power source VscH, and the other end is coupled to the scan electrode Y of the plasma display panel through the scan driver IC. The low level scan signal supplier 540 includes a scan switch Ysc of which one end is coupled to a low level scan power source VscL, and the other end is coupled to the scan electrode Y of the plasma display panel through the scan driver IC.
Also, the high level scan signal supplier 530 can further include a diode Dsc for blocking the current path in the reverse direction between the high level scan power source VscH and the scan capacitor Csc. When the scan switch Ysc is turned on, the scan capacitor Csc has a voltage of VscH-VscL.
Next, the principle used to apply the rising ramp waveform and the falling ramp waveform using the rising/falling ramp switches will be described. In the following description, some of the details about the waveforms applied to the sustain electrode and the address electrode are omitted.
First, the rising ramp switch Yset of a rising reset unit 560 is turned on during the reset period to maintain an on-state during the rising period in the reset period. Then, the waveform gradually increases to the Vset voltage while the rising ramp switch Yset maintains the on-state. Next, the falling ramp switch Yfr of a falling reset unit 570 is turned on to likewise maintain an on-state during the falling period in the reset period. Then, the waveform gradually reduces to a VscL voltage (=Vnf voltage) while the Yfr switch maintains the on-state.
Hereinafter, the process to obtain ramp waveforms having a slope, which may be predetermined, using the ramp switches will be described in detail. In particular, the method using a falling ramp switch will be described.
As shown in
When the plasma display panel is powered on, it is in a state where the capacitor Csc in the driving circuit is not sufficiently filled with energy storage elements (charge and electric field), so it is difficult to expect a sufficient reaction to provide instantaneous high current using the capacitor Csc.
Therefore, the voltage potential between the ground voltage and the lowest scan voltage VscL is converted into the overcurrent flowing through the falling ramp switch so that it directly applies stress to the falling ramp switch. The stress by means of the overcurrent may also seriously affect a Zener diode, etc., coupled to the falling ramp switch Yfr.
To the contrary, although the driving method as shown has a disadvantage that the falling time of the falling ramp of the Y electrode driving signal is extended, in the first Y electrode driving signal after the plasma display panel is powered on, a waveform for erasing is not used and the falling ramp is directly generated from the ground electric potential so that a sufficient time for offsetting the falling time of the extended falling ramp is available.
Now, when the turn-on time of the falling ramp switch Yfr is limited as shown in
If the current flowing to the falling ramp switch from the turn-on thereof to the turn-off thereof is approximated as a continuous, linearly increasing sawtooth wave, the relation between time t and current I can be represented by Equation 1, the linear function having a fixed slope c:
I=ct. Equation 1
Meanwhile, if the plasma display panel is viewed as one capacitor, the amount of charge Q to be discharged from the plasma display panel when falling from a first voltage to a second voltage, can be expressed by Equation 2:
Q=CΔV Equation 2
where C is the panel capacitance, and ΔV=first voltage−second voltage.
Assuming that the amount of charge Q discharged from the plasma display panel is divided into n turn-on periods, the amount of unit charge Qu discharged at one turn-on period can be expressed by Equation 3:
Q
u
=CΔV/n Equation 3
Herein, the amount of charge in the unit charge Qu is discharged during the unit turn-on time of the switching pulse applied to the falling ramp switch Yfr, wherein if the current has a triangular shape, such as the sawtooth waveform of
Q
u=(½)Tu×Ipu Equation 4
where Ipu is the peak current generated during the unit turn-on time, and Tu is the unit turn-on time.
Substituting equation 3 into equation 4 results in Equation 5:
(½)Tu×Ipu=CΔV/n, and therefore, Equation 5
I
pu=2CΔV/(Tu×n).
Herein, in order to disclose the relationship between n and Tu and discharge the same amount of charge Q, the relation between the time required for the path having the fixed linear slope and turn-on times is graphically shown in
The charge, which is the area under the current-time curve, can be appreciated in
T
1
=n
2
·T
u, and therefore, Equation 6
n=(T1/Tu)1/2.
If Equation 6 is substituted into Equation 5 and solved for Tu, it can be expressed by Equation 7:
I
pu=2CΔV/[Tu×(T1/Tu)1/2 Equation 7
T
u=(4/T1)×(CΔV/Ipu)2.
Herein, if ΔV and T1 are considered to be fixed values according to the characteristics of the plasma display panel and the driving circuit, and thus are substituted by a constant “a,” the relationship only between Tu, Ipu and C can be expressed by Equation 8:
T
u=4a×(C/Ipu)2 Equation 8
Therefore, in one embodiment of the present invention, each turn-on time of the switching pulses applied to the falling ramp switch Yfr of
T=4a×C2/(Ipeak)2 Equation 9
With the plasma display device and the driving method thereof according to the present invention, the current stress of the driving circuit can be relieved.
In particular, one aspect of an exemplary embodiment of the present invention is the relief of the current stress of the driving circuit when a falling voltage with a large deviation occurs in the reset waveform of the scan electrode.
While the present invention has been described in connection with certain exemplary embodiments, it is to be understood that the invention is not limited to the disclosed embodiments, but, on the contrary, is intended to cover various modifications and equivalent arrangements included within the spirit and scope of the appended claims, and equivalents thereof.
Number | Date | Country | Kind |
---|---|---|---|
10-2007-0049621 | May 2007 | KR | national |
This application claims priority to and the benefit of Korean Patent Application No. 10-2007-0049621, filed on May 22, 2007, in the Korean Intellectual Property Office, the entire content of which is incorporated herein by reference.