Electric lamp and discharge devices: systems – Current and/or voltage regulation
Reexamination Certificate
2001-02-06
2003-01-07
Wong, Don (Department: 2821)
Electric lamp and discharge devices: systems
Current and/or voltage regulation
Reexamination Certificate
active
06504321
ABSTRACT:
TECHNICAL FIELD
This invention relates generally to a method and apparatus for providing closed loop feedback control for a circuit. This invention has particular application in the feedback control of high-frequency switching mode power converters used in lighting applications.
BACKGROUND OF THE INVENTION
Future intelligent power management systems for lighting applications will require electronic ballasts with network control and communications capabilities. As well, the emerging electronic ballast must be universal. It must be able to drive different lamp types as well as operate globally, i.e., be interoperable with differing AC line voltages.
An electronic ballast drives a lamp with a nearly sinusoidal wave of a particular frequency. The driving pulse output by the ballast is generally a combination of one or more outputs of a switching-mode power converter, such as, e.g., a half-bridge power converter. These power-converter outputs are generally square waveforms, but before being applied to the lamp, are passed through an LC tank, resulting in near sinusoidal waveforms applied to the lamp.
The output signals of switching-mode power converters used in lamp driving circuits are periodic waveforms whose frequencies are equal to the switching frequency of the converters. The width and frequency of these output signals govern the intensity, and therefore the power, delivered to the lamp. In order to properly regulate the output signals of these switching-mode power converters a closed feedback loop is required. The feedback loop is used to continually communicate back to the electronic ballast the voltage across and current through the lamp so that the output voltage wave from the ballast can be continually controlled.
In a universal ballast, the control should be flexible and programmable. A ballast should be able to calculate, for example, at least real lamp power, average rectified lamp current or rectified lamp voltage. Accordingly, the ideal ballast should be programmable so as to implement various control mechanisms, such as lamp current regulation, lamp voltage regulation, real-power regulation, or a combination of these control methods. Such flexibility supports driving various lamp types, a feature which is more and more an important functionality in the ballast marketplace.
Unfortunately, current ballast control systems are either inflexible and non-universal, or programmable, but unable to provide real time control. Current feedback loops in power converters are mostly implemented in analog hardware. They therefore comprise numerous discrete components such as resistors, capacitors, operational amplifiers, comparators, and analog integrated circuit controllers. Such feedback loop implementations are necessarily hardwired, and thus not at all programmable.
The other approach taken in existing feedback power converter control for electronic ballasts is the use of a low-cost microcontroller based integrated circuit which includes a low speed analog to digital converter for digitizing the analog input signals. Such a system is depicted in
FIG. 1
, operating on two feedback signals A
101
and B
102
. These analog input signals A
101
and B
102
are generally the voltage and current signals coming from the lamp. The sampling speed of these analog lamp signals must be kept low in such an approach, due to the limited processing speed of the standard micro-controller. As a result, in order to send low speed digitized signals to the microcontroller to be operated upon by a micro-processor implemented control algorithm, the bandwidth of the feedback signals must be significantly reduced. In order to achieve this reduction of bandwidth, the high frequency analog signals coming from the lamp must first be processed by analog low pass filters prior to their being digitized by a low speed analog to digital converter. Such low pass filters are depicted as LPF
105
and LPF
106
, respectively. Once the bandwidth has been limited by the analog filters, the low frequency signals
107
and
108
, respectively, can be converted to the digital domain by the analog to digital converters
110
and
111
, respectively. Once digitized at the low sampling speed, the signals are fed into a micro-controller
115
, which operates upon them and generates thereby control signals which are sent to the pulse width modulator
120
which drives the lamp.
There are significant problems inherent in each of the two above-described approaches. The feedback implementation in analog hardware includes several discrete components. The more components there are, the greater the cost; both in terms of actual components as well as in terms of manufacture, design, compatibility, and testing considerations. Furthermore, a pure hardware analog feedback implementation will be limited to a particular application to insure stable operation. Since the processing of the analog signals that can be done is in no way programmable when using discrete analog components, the optimal feedback loop for a given application will only optimally work for that one application. Flexibility is lost. This simply does not work for applications such as universal ballasts where the power converter needs to operate with different input voltages and must be able to drive a wide range of possible loads.
Additionally, the complexity of signal processing that can be done with discrete analog components is limited. As well, in truth, analog signal processing in control systems is fast becoming obsolete.
On the other hand, because the output signals of switching-mode power converters are periodic waveforms of frequency equal to the switching frequency of the converters, it is desirable in any optimal feedback control loop to preserve the high frequency information that is contained in these output signals. Lamp signals generally have a basic frequency equal to the switching frequency of the power converter that drives them, as well as numerous higher order harmonic frequencies contained in them. The harmonics present affect the lamp's power. The effects of higher order harmonics increase in proportion to the lamp dimming level. In other words, the lower the power level of the lamp, the more significant the contribution of higher order harmonics. This is generally the case because at low dim levels the pulse-width of the square waveform at the half-bridge output is reduced, resulting in increased harmonic content of the signal fed to the low pass filter. Furthermore, the lamp impedance increases at low dimming levels, thus affecting the roll-off of the filter, which in turn results in increased harmonic content of the of the signal directly driving the lamp.
To preserve the information contained in the higher order harmonics, a high sampling rate is necessitated. The well known Nyquist Sampling Theorem determines the sampling frequency that must be used to fully characterize continuous time signals by a sequence of discrete samples. The Nyquist theorem states that the sampling frequency must be at least twice as high as the maximum signal frequency.
If a microcontroller based integrated circuit feedback loop control implementation is desired to be used, then it is necessary to sample the output of the lamp circuit at twice the highest relevant harmonic of the maximum switching frequency. As an example, if the maximum switching frequency of the lamp is 100 KHz, and due to the required accuracy the effects of the first through fifth harmonics cannot be ignored, the following equation is operative: f
s
≧2*5*f
HB
, i.e., the sampling frequency f
s
must equal or exceed twice the fifth harmonic (or 10X) of the base frequency f
HB
, which is the half-bridge switching frequency. In the above described example, where the maximum frequency of the lamp is 100 KHz, the sampling frequency must therefore be higher than 1 MHz.
On the other hand, if the maximum switching frequency is 100 KHz, and the information contained in the 16
th
order harmonic cannot be ignored based upon the accuracy requirements of the control algorithm, then the sampli
Giannopoulos Demetri
Wacyk Ihor
Wang Shenghong
A Minh D
Biren Steven R.
Koninklijke Philips Electronics , N.V.
Wong Don
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