Known in the industry are a few drivers for light emitting diodes (“LEDs”), like charge pumps with the multi-output current mirror from National Semiconductor. These drivers cannot economically boost input voltage more than 1.5 to 2 times and therefore call for parallel circuits for identical driving of multiple LEDs. That makes these drivers large and expensive. Also desired in this case is a linear current regulator in each channel which compromises the efficiency of an LED driver.
Also known is an inductor based boost converter, like LT 1932 from Linear Technology™ or NTC5006 from On-Semiconductor™. The most frequently used topology is a current mode regulator with the ramp compensation of PWM circuit. Such a current mode regulator needs relatively many functional circuits and still exhibit stability problems when it is used in the continuous current mode with the duty ratio over 50%. As an attempt to solve these problems, the designers introduced constant off time boost converter or hysteric pulse train booster. While they addressed the problem of stability, hysteretic pulse train converters exhibit difficulties with meeting EMC and high efficiency requirements.
U.S. Pat. Nos. 6,515,434 and 6,747,420 provide some solutions outside original power converter stages, focusing on additional feedbacks and circuits, which eventually make the driver even larger.
To overcome the problems listed above, a process and system is disclosed for controlling a switching power converter, constructed and arranged for supplying power to one or a plurality of LEDs to reduce the size and cost of LED driver. Also disclosed is a controller which is stable regardless of the current through the LED. Further disclosed is a high efficiency LED driver with a reliable protection of driver components and input battery from discharging at the damaged output.
An LED, having a diode-type volt amp characteristic, presents a very difficult load for voltage type regulators. That is why all up to date LED drivers are constructed as a regulated current source, including the referenced prior art in
The teachings of the present disclosure can be readily understood by considering the following detailed description in conjunction with the accompanying drawings.
The embodiments of the present disclosure will be described below with reference to the accompanying drawings. Like reference numerals are used for like elements in the accompanying drawings.
The power converter in
Assuming ideal components, the relationship between input voltage and other parameters can be defined by the following equation:
V
IN
=L(IP1−IP2)/TON, (1)
VIN=DC input voltage,
IP1=peak current in the inductor at the end of charging,
IP2=peak current in the inductor at the beginning of the inductor charging,
TON=on time, and
L=inductance.
When the power switch 8 is open, the inductor 7 discharges energy into the output load. The output voltage is defined by the following equation:
−VIN+VOUT=L(IP1−IP2)/TOFF, (2)
VOUT=DC output voltage, and
TOFF=off time.
Assuming average LEDs current:
I
AVG
−V
OUT
/R
D (3)
RD=equivalent DC resistance of the LEDs is assumed to be known.
I
AVG=(IP1+IP2)TOFF/2(TON+TOFF) (4)
and assuming a steady process,
V
IN
*T
ON=(−VIN+IAVG*RD)*TOFF (5)
The on time can be determined by the following equation:
T
ON=(−VIN+IAVG*RD)*TOFF/VIN (6)
The frequency of the output is equivalent to:
f=1/(TON+TOFF) (7)
Solving equations (1) through (6),
I
P1=(VOUT−VIN)TOFF/2L+IAVG(VOUT/VIN) (8)
I
P2=(VOUT−VIN)TOFF/2L−IAVG(VOUT/VIN) (9)
According to the waveform for LEDs 4 in
Comparing Iavg in equation (11) and integral (10) we can make a conclusion that the integral (10) would be (a) proportional to the average LEDs current if cycle time T is constant and (b) equal to the average LEDs current if the integrated value is divided by cycle time T. In one embodiment of the present disclosure, the process of driving LEDs with the constant switching frequency is based on steps of storing energy in the inductor during on time of the power switch, discharging it into LEDs during off time of the power switch, measuring ampseconds of said inductive element at off time and adjusting peak current through the said switch to keep said off time ampseconds in the inductor during off time constant and proportional to the set average current through LEDs. Thus, the disclosure is using generation of the off time ampseconds signal in the inductor as one switching cycle feedback. The ampseconds are measured by integrating discharging inductor 7 current during off time, sampling the integrator 14 at the end of off time, and resetting the integrator 14 during on time.
Expression (10) is a theoretical interpretation of the method: to keep LED brightness constant at constant frequency, the input voltage changes are compensated in such a manner that the inductor off time ampseconds and average current of the LED remains constant (or regulated). The method is illustrated on
Iset=V14 Vc(n+1)=Vcn
Iset>V14 Vc(n+1)=Vcn−ΔVc
Iset<V14 Vc(n+1)=VcnT+ΔVc
Thus regulator 6 in
In yet another embodiment of the present disclosure, the control voltage ΔVc is adjusted based on function presented in
In yet another embodiment of the present disclosure, shown in
Different combinations of the circuits may be used to drive one or multiple of LEDs according to said method. A digital implementation of the same regulator 6 is shown on
Traditionally, in peak current mode control regulation, a user specifies a reference current, and then the power switch switches off when the inductor current rises to this reference current (minus an appropriate slope compensation to maintain global stability). However, in pulsed current averaging, we propose to regulate differently: we propose to directly regulate the length of power switch on time (Ton) in order to create the desired peak value Ip. We then relate this peak value to the load output current's average value. Hence, load current regulation becomes possible. Since LEDs call for current regulation instead of voltage regulation, this makes pulsed current averaging a prime candidate for its application. Our goal is now to relate the control variable Ton to the output current through the load. Peak current in the inductor, assuming discontinuous operation:
Ip=Peak current in the inductor 7, and
Vin=Input voltage.
Average current in the load:
Volt second balance of the inductor:
Vin*Ton=(Vout−Vin)Toff, (14)
Vout=Output average voltage.
Combining equations (12) to (14) and solving it to Ton will get dependence of average current from the variable Ton:
The conclusion of this simplified analysis is that the on time of the power switch is proportional to the output current. Thus, by adjusting Ton, the output current through the load will be changed in a linear relation. Notice, also, that the output current is inversely proportional to the output voltage in this relation. Therefore, in systems in which output voltage may quickly deviate from a desired value, this method may need to utilize advanced nonlinear controllers for regulation. This has compelled researchers to utilize multiplications in controllers to adjust Ton. That is, an inner current loop in power factor correction circuits often makes Ton∝kVOUT(IRef−IL). This is obviously a more complicated and nonlinear controller because it uses digital multiplication, as well as an additional outer voltage loop (usually PI controller) to help regulate the voltage.
Instead of a complicated approach to control, we propose to use the relation of Ton to Iav in a hysteretic/sliding mode scheme that simplifies implementations and may not use external A/D converters. The idea is to increase or decrease Ton by discrete pulses in order to control the average current being delivered to a load: hence, the terminology pulse average current control. Conventional methods for controlling the current output of commercially available integrated circuits for LEDs drivers uses a combination of analog operational amplifiers and compensation ramp generators. We have come up with a digital control approach to controlling output currents that does not use these additional parts. This is not a DSP engine with software overhead; this is an optimized digital core that uses a sliding control algorithm to determine the amount of power to transfer to the output using a boundary/sliding mode control criteria.
To demonstrate the proposed regulation approach according to one embodiment of the disclosure and show its potential, we describe the pulsed average current regulation using a simple hysteretic controller. The pulse average current regulation comprises the following steps, see
Inductor 7 starts to discharge (it is assumed that the conversion process is discontinuous);
LED current is sensed and integrated by integrator 14 for a period of off time Toff;
the integrated value is sampled by digital logic 25 at the end of cycle time and integrator 14 is reset by switch 15;
sampled integrated value is divided in divider 14A by cycle time T and it is compared with the set value of the LED current Iset
on time in the Time register 25A is adjusted by +Δton or −Δton; and
new cycle starts.
If the system detects more than two consecutive cycles with the same sign of Δton increment, the system may use look-up tables to adjust these increments to accelerate convergence of measured Is signal and reference Iset.
A simplified sliding mode regulator is presented in
In another embodiment of the present disclosure (
the digital logic 25 starts Iset timer (not shown separately from digital logic 25) and keeps power switch 8 off;
power switch 8 is off and Iset timer is counting time Tt until LED current comparator 16 detects Is transition below Iset level by sending a signal (low) to the digital logic 25; and
the digital logic stops Iset timer, reads its content and divides it by off time to define new Ton time as Toni+1=Toni−Δton((Tt/Toff)−1).
We call the described process as asymmetrical hysteretic algorithm of adjusting on time Ton, the purpose of which is to improve the dynamic response of the regulator and limit the ripple of LED current. Asymmetrical hysteretic algorithms include two LED comparators (not shown) each set slightly apart to form a window for current ripple and otherwise working independently and similar to the above-described process.
The above-presented sliding mode regulator 6 will be stable in the discontinuous mode of operation. Another embodiment of the present disclosure in
As ramp generator 28 starts the ramp, both comparators 24 and 31 are in the same state, low or high. Example of
(a) measuring off time ampseconds of said inductor or directly average LED current;
(b) generating a periodical ramp signal at a constant frequency, generally smaller than switching frequency of said power converter, wherein said ramp signal is equal, generally at the middle of the ramp to LEDs current set reference signal;
(c) comparing once per a cycle of said ramp frequency said ampseconds signal with said ramp signal and generating a first signal at the instance when said ramp signal starts exceeding said ampseconds signal;
(d) comparing once per a cycle of said ramp frequency said set reference signal with said ramp signal and generating a second signal at the instance when said ramp signal starts exceeding said set reference signal;
(e) starting an error time counter by said first signal or by said second signal whichever comes first;
(f) stopping said error time counter by said first signal or by said second signal whichever comes last;
(g) reading said error time counter as a digital error and assigning a sign to said error positive if said first signal comes last and negative if said second signal comes last; and
(h) resetting all registers and start new cycle of error estimation.
Digital logic 26 is using the generated error to process it in a digital PI or PID regulator (not shown separately) with desired stability gains of proportional and integrated/differential parts. The output of the PI/PID regulator may generate in digital form either on time Ton for keeping the switch 8 closed (
The design of such compensation can be a routine task. The PID controller has the transfer function:
where:
s=complex variable of Laplace transform,
Gc(s)=compensator,
K1=proportional gain coefficient,
K2=differential coefficient, and
K3=Integral coefficient.
The PID controller has a robust performance and a simplicity that allows for digital implementation to be very straight forward.
The Z domain transfer function of a PID controller is:
where:
z=complex variable of Z transform,
Gc(z)=compensator,
K1=proportional gain coefficient,
K2=differential coefficient, and
K3=integral coefficient.
The differential equation algorithm that provides a PID controller is obtained by adding three terms
u(k)=[K1+K2T+(K3/T]x(k)+K3Tx(k−1)+K2u(k−1)
where:
u(k)=the control variable, this signal is used to add or subtract to control pulse,
x(k)=current error sample,
x(k−1)=previous error sample,
T=sampling period,
K1=proportional Gain coefficient,
K2=differential coefficient, and
K3=integral coefficient.
This is a useful control function to create a PI or PID controller simply by setting the appropriate gain to zero. The ramp function will determine a digital value that will serve as the x(k) value in a given control loop. By adjusting gain and delay, precise digital control can be obtained over a variety of systems.
The system 1 for driving LED in
The protection circuit 32-38 provides adequate current protection to the input battery of the system, however it may overstress the isolation switch 35 at the time capacitor 36 is discharging into low impedance. The circuit in
Open circuits are one of the common failures of an LED. At this failure an overvoltage is developing very quickly, potentially dangerous to all components of the system.
If regulator 6 gets a signal from the application system to shut down the system 1, it is an advantage of such a system to isolate the battery 2 from driving circuits to save its power. It is a function of another embodiment of the disclosure implemented by a signal of regulator 6 at the AND gate 33. When the signal from the regulator 6 goes low, the switch 35 is open and the battery 2 is disconnected from driving circuits and load.
Although the present disclosure has been described above with respect to several embodiments, various modifications can be made within the scope of disclosure. The various circuits described in
This application is a division of U.S. patent application Ser. No. 13/558,237, filed Jul. 25, 2012, which is a division of U.S. patent application Ser. No. 12/497,682, filed Jul. 5, 2009 (now U.S. Pat. No. 8,232,735), which is a division of U.S. patent application Ser. No. 11/838,186, filed Aug. 13, 2007 (now U.S. Pat. No. 7,583,035), which is a division of U.S. patent application Ser. No. 11/142,859, filed May 31, 2005 (now U.S. Pat. No. 7,276,861), which claims the benefit of U.S. Provisional Application No. 60/611,539, filed Sep. 21, 2004. U.S. patent application Ser. No. 12/497,682, filed Jul. 5, 2009 (now U.S. Pat. No. 8,232,735), is also a division of U.S. patent application Ser. No. 11/838,208, filed Aug. 13, 2007 (now U.S. Pat. No. 7,710,047), which is a continuation of U.S. patent application Ser. No. 11/142,859, filed May 31, 2005 (now U.S. Pat. No. 7,276,861), which claims the benefit of U.S. Provisional Application No. 60/611,539, filed Sep. 21, 2004. Each of the disclosures of said applications are incorporated by reference herein in their entirety.
Number | Date | Country | |
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60611539 | Sep 2004 | US |
Number | Date | Country | |
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Parent | 13558237 | Jul 2012 | US |
Child | 13942664 | US | |
Parent | 12497682 | Jul 2009 | US |
Child | 13558237 | US | |
Parent | 11838208 | Aug 2007 | US |
Child | 12497682 | US | |
Parent | 11838186 | Aug 2007 | US |
Child | 11838208 | US |
Number | Date | Country | |
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Parent | 11142859 | May 2005 | US |
Child | 11838208 | US |