The invention relates to an LED driver circuit comprising at least one string of LEDs connected in series, and a power supply for converting a mains voltage into an output voltage to be applied to said at least one string of LEDs.
More particularly, the invention relates to high power lighting applications such as industrial lamps, sport field lamps, street lamps and the like, wherein an array of a plurality of LEDs is powered by a common power supply.
Since the forward voltage of a single LED, typically in the order of magnitude of 1 to 5 V, is significantly smaller than the mains voltage of, e.g., 400 VAC, 230 VAC or 110 VAC, it is necessary to convert the mains voltage into a output voltage that is suitable for the LEDs. When a plurality of LEDs are connected in series, the output voltage should correspond to the sum of the forward voltages of the LEDs in the string.
Most conventional LED driver circuits comprise a plurality of strings which each have only a relatively small number of LEDs, so that the output voltage will be lower than the mains voltage. However, when a plurality of strings are connected in parallel to a common power supply, the output current must be relatively high, which leads into increased system losses, and additional measures must be taken to assure a correct current balance between the parallel LED strings. In general for each LED string a separate converter operated in a current mode is applied to regulate the LED current. In addition, these systems require numerous connections and interconnection wires, so that the costs for the electronic components and their installation are relatively high.
EP 2 315 497 A1 and EP 2 458 940 A1 describe LED driver circuits which have a two-stage power supply. The first stage is a converter with a power factor correction function which converts the AC mains voltage into a DC voltage and assures compliance with the AC grid regulations. The second stage is a driver that regulates the current in the LED string or strings.
It is an object of the invention to provide an LED driver circuit with increased system efficiency and reduced system costs.
In order to achieve this object, according to the invention, the power supply includes a single-stage boost converter adapted to directly convert the mains voltage into the output voltage.
Since the mains voltage is boosted to a higher voltage level, the efficiency is improved and system losses are reduced. Moreover, the output current is relatively low, so that the electronic components on the output side of the power supply need only be designed for low currents. Preferably, the output voltage will exceed even the peak value of the applied mains voltage. This implies that sufficient insulation of the entire system is necessary. As a consequence, however, the conventional galvanic insulation of the LED driver (or transformer) may be dispensed with.
More specific optional features of the invention are indicated in the dependent claims.
In a preferred embodiment, the boost converter is a multi-level converter, e.g. of a type as generally described in an article by J. Rodrigues, J. S. Lai, F. Zheng, “Multilevel Inverters: A Survey of Topologies, Controls and Applications”, IEEE Trans. Industrial Electronics, vol. 49, 2002, pages 724-738, and in an article by M. T. Zhang, J. Yiming, F. C. Lee, M. M. Jovanovic, “Single-Phase Three-Level Boost Power Factor Correction Converter”, IEEE APEC 10th annual, 1995, pages 434-439. This topology permits to raise the output voltage level without using expensive high voltage rated semiconductor devices. For example, the output voltage may be raised to at least 1.5 times the peak value of the mains voltage. Preferably, the output voltage is evenly divided over a series connection of LED strings.
In order to increase the efficiency, it is preferable to operate the converter in the critical discontinuous mode, as has been described by J. Zhang, J. Shao, P. Xu, F. C. Lee, “Evaluation of Input Current in the Critical Mode Boost PFC Converter for Distributed Power Systems”, IEEE, APEC 16th annual, 2001, pages 130-136, and L. Huber, B. T. Irving, M. M. Jovanovic, “Effect of valley switching and switching-frequency limitations on a line-current distortions of DCM/CCM boundary boost PFC converters”, IEEE Trans. Power Electronics, vol. 24, 2009, pages 339-347. Additionally the cycle-by-cycle control can be simplified by applying a constant ON time of the electronic switches over the sine wave period of the mains voltage.
The multi-level topology has the further advantage that it enables a LED current balance control, whereby the efficiency can be raised even further. (J. R. Pinhiero, D. L. R. Vidor, H. A. Gründling, “Dual Output Three-Level Boost Power Factor Correction Converter with Unbalanced Loads”, IEEE PESC, 27th annual, 1996, pages 733-739).
In a preferred embodiment, the converter is protected against excessive inrush currents and transient voltages.
Embodiment examples of the invention will now be described in conjunction with the drawings, wherein:
FIGS. 3(A)-(E) are time diagrams illustrating different modes of operation of the converter shown in
As is shown in
Although, for simplicity, only two LEDs 12 have been shown in the string 10 in
The converter 14 comprises a diode bridge formed by diodes D1-D4, and a series connection of an inductor L, a diode D5 and a capacitor C connected between the output terminals of the diode bridge. An electronic switch S (e.g. a MOSFET) which is controlled by an electronic controller Q is connected in parallel to the diode D5 and the capacitor C. The string 10 of LEDs is connected in parallel to the capacitor C.
The diode bridge D1-D4 rectifies the mains voltage AC into a pulsating DC voltage Uin. When the switch S is ON (closed), the voltage Uin drops across the inductor L, so that a current through the inductor L increases (positive slope). The diode D5 prevents the capacitor C from being discharged via the switch S. As long as the switch S is on, an increasing amount of energy is stored in the inductor L while the capacitor C discharges via the LED string 10.
When the switch S is switched OFF (opened), the inductor L forces a current to flow through the diode D5 and through the LED string 10 while the capacitor C is being recharged. Because the output voltage Uout is always larger than the voltage Uin or, more precisely, the instantaneous value of the time-dependent voltage Uin, the current flow through the inductor L decreases (negative slope) until the switch S is closed again.
A current shunt is provided for measuring the current ILED flowing through the LED string 10. The controller Q receives measured values of the current ILED, input voltage Uin and of the current flowing through the inductor L (and optionally, for protection purposes, of the output voltage Uout) and may be configured to feedback control the ON time of the switch S on a time scale that is large compared to the mains sine wave period, whereas the OFF times are controlled such that the current flowing through the inductor L has just time enough to decay to zero. In other words, the converter is operated in the so-called critical mode on the border between a continuous conduction mode (CCM) in which a current would flow continuously through the inductor L and a discontinuous conduction mode (DCM) in which there would be periods with no current flowing through the inductor.
Thus, the difference between the instantaneous values of Uout and Uin will determine the duration of the off periods of the switch S and hence, in conjunction with the duration of the ON time of the switch, the switching frequency of the converter. In general, the ON times of the switch S (constant or not) will be selected such that the switching frequency is in the order of magnitude of several kHz, so that an efficient power conversion can be achieved with an inductor with relatively low inductivity.
As a more practical example,
The main difference between the converter 16 shown in
In the example shown, the inductor L has also been replaced by two inductors L1 and L2. Moreover, a mode selector switch Sm is connected between the mid-point of the diodes D2 and D4 and the mid-point between the switches S1 and S2.
When the mode selector switch Sm is open and the switches S1 and S2 are operated synchronously (by the controller Q which has not been shown in
The mode selector switch Sm may be used to switch the converter into a voltage doubling mode in which the same output voltage Uout with almost the same conversion efficiency can be achieved with a lower mains voltage of only 110 VAC, for example. In this mode, i.e. when the switch Sm is closed, the inductor L1, the switch S1 and the capacitor C1 form a first converter (with only half the total inductivity) powered via the diode D1 during the positive half wave of the mains voltage, and the inductor L2, the switch S2 and the capacitor C2 form a second converter powered via the diode D3 during the negative half wave of the mains voltage. Due to the reduced inductivity, each converter will convert the reduced mains voltage of 110V into a voltage ULED of 200 V-250 V, so that the total output voltage Uout (=2 ULED) will still be 400 V to 500 V.
In the normal mode (no voltage doubling), the two-level topology according to
However, when Uin is smaller than ULED, it is more efficient to use a switching pattern as shown in
Then, the switch S1 is switched OFF while switch S2 remains ON. Consequently, the current through L1 is forced to charge C1 and/or to flow through the upper string 10 and then through the switch S2 and inductor L2. The slope of the current through L1 is negative because ULED is larger than Uin.
When the current has dropped to zero (critical mode), S1 is switched ON again, so that the current will rise again. Then, when switch S2 is switched OFF, S1 remains ON, so that, now, the current flowing through L1 is forced to flow towards capacitor C2 and the lower string 10 before returning via L2. The slope will be negative again because the voltage ULED dropping across the capacitor C2 is also larger than Uin.
This switching pattern has the advantage that the overall losses, including switching losses, are reduced under conditions in which instantaneous value of Uin is smaller than ULED.
In the example shown in
The embodiments that have been described above may be modified in various ways, as will now exemplified in conjunction with
In
In this embodiment, the voltage drop across the inductors L1 and L2 may be modified step-wise by closing one, two, three or all four of the switches S1-S4. For control purposes, the LED currents ILED flowing through each LED string 10 may be measured individually (just as in
This topology has the advantage that the capacitance of the capacitors C1-C4 which is needed as energy buffer may be smaller, so that electrolytic capacitors may be replaced by film capacitors which have an increased lifetime and are advantageous in applications with a high ambient temperature. In principle, this topology can be extended to even more levels, e.g. 8 or 16 levels.
In all these embodiments, it will be preferable to provide additional measures for over-voltage protection and for limiting inrush currents. Examples are illustrated in
In order to limit inrush currents, a resistor R is interposed between the switch S and the rectifier diode bridge. A protector switch Sp is connected in parallel to the resistor R.
This protector switch Sp is switched on and off dependent upon the measured output voltage Uout. When the system is powered-on, and the capacitor 10 has to be charged, the switch Sp is off, so that the current will be limited by the resistor R. Only when the output voltage Uout has reached its operating level the switch Sp will be closed to short-circuit the resistor R, so that the converter may operate as has been described before.
Further, in order to prevent the inductor L from becoming saturated, a diode D11 is connected in parallel to the inductor L and the dial D5.
In addition,
Number | Date | Country | Kind |
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13158806.3 | Mar 2013 | EP | regional |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2014/054112 | 3/4/2014 | WO | 00 |