The present invention relates to driver circuits and more specifically to an apparatus and method for monitoring forward LED voltages to enable optimal energy efficiency in LED driver circuits.
Portable battery power devices are increasingly common in modern life, e.g., mobile telephones, MP3 players, personal digital assistants (PDAs), notebook computers, DVD players, CD players, radios, televisions, and the like. However, the relatively short span of time before a fully charged battery becomes discharged and needs to be either recharged or replaced is a common problem in the operation of most battery powered devices To extend the “lifetime” of a battery's effective use, energy efficient circuitry is often included in battery powered devices.
Many battery powered devices include displays that provide information regarding the operation of the devices. Often, these displays are backlit to enable their use in low light environments. However, since backlit displays can consume a relatively large percentage of the available energy in the battery, relatively efficient LED driver solutions are preferred.
In the past, current regulated switch capacitor LED drivers have been employed to achieve a relatively optimized energy efficiency by switching between different gains. These different gains are switched to follow the voltage drop across the battery as it discharges. For example, when the battery is fully charged a gain of 1 is often selected because the battery's voltage is high enough to efficiently drive the LEDs. However, as the battery discharges and its voltage drops, a gain greater than 1 is then selected (1.5X for example) to boost the output of the LED driver above the battery's voltage. Previously, it has been difficult to determine the optimal point for this gain transition. Thus, it is with respect to these considerations and others that the present invention has been made.
Non-limiting and non-exhaustive embodiments of the present invention are described with reference to the following drawings. In the drawings, like reference numerals refer to like parts throughout the various figures unless otherwise specified.
For a better understanding of the present invention, reference will be made to the following Detailed Description of the Invention, which is to be read in association with the accompanying drawings, wherein:
The present invention is described fully hereinafter with reference to the accompanying drawings, which form a part hereof, and which show, by way of illustration, specific exemplary embodiments by which the invention may be practiced. This invention may, however, be embodied in many different forms and should not be construed as limited to the embodiments set forth herein; rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the scope of the invention to those skilled in the art. Among other things, the present invention may be embodied as methods or devices. Accordingly, the present invention may take the form of an entirely hardware embodiment or an embodiment combining software and hardware aspects. The following detailed description is, therefore, not to be taken in a limiting sense.
Briefly stated, the present invention is directed to an apparatus and method for monitoring the forward voltage for a plurality of LEDs in a battery powered device so that the gain in the LED driver circuit can be switched at a point that optimizes the energy provided by the battery to illuminate the LEDs. The invention provides for sensing each LED's voltage, VLED, and determining the maximum forward voltage, VLEDmax, between the plurality of LEDs. The invention uses the knowledge of VLEDmax in conjunction with VIN, converter output resistance and LED current, and current source/sink minimum headroom to switch from an initial gain to some final gain (higher than initial gain) just before the current sinks/sources would drop out. Similarly, the invention provides for switching from the higher gain back to the initial gain in the event that the battery voltage rises back to its initial voltage after being momentarily pulled down by a heavy load or other factors.
In part, because of differences in the gain selection circuitry when implemented for a high side LED driver versus a low side LED driver, the invention provides for two complementary embodiments that enable gain selection on the high side and low side. The conditions for gain switching that account for the above mentioned factors are developed in the implementation section below.
As discussed above, after discharging for some period of time, the battery's voltage drops. For example, the cell voltage of a lithium ion battery (typical battery for mobile phones) usually ranges from 4.2 Volts at full charge down to 2.5 Volts at deep discharge. Since this lower voltage is often less than the desired power supply voltage for a battery powered device, a boost converter is employed to extend the period of time that the battery can be a useful energy source for the device.
Although the invention can be implemented with both high side and low side LED drivers,
Additionally, as shown in
The efficiency of the LED driver depends on the gain that the LED driver is operating in:
The quiescent current IQ is negligible for moderate to high output current applications. This equation highlights that the efficiency is optimal when the LED driver operates in the lowest possible gain that can still provide a VOUT voltage to enable the operation of the battery powered electronic device.
For the case where the LED driver is operating with a gain of one, the following second equation applies:
For the case where the LED driver is operating with a 1.5 times gain (1.5X boost mode), the following third equation applies:
The LED current sources that are connected between VOUT and the diodes need enough headroom, VHR, across them to provide the desired current in the LED. The headroom is the voltage across each current source VHR=VOUT−VLED. The current sources require a sufficient amount of headroom voltage to be present across them in order to regulate properly. The minimum headroom voltage VHRmin is proportional to the current flowing through the current source as described by the equation: VHRmin=RHR*ILED, then RHR represents the ON resistance of the current source.
For LED drivers, the optimal efficiency is achieved by switching gains based on the value of VIN and the forward LED voltage VLED as Equations 2 and 3 highlight it. This optimal efficiency can be achieved by enabling its DC-DC converter to stay in a gain of one (unity) over the largest input voltage range possible, while at the same time preventing the headroom of the current sources from dropping below VHRmin. The input voltage at which the converter switches gains depends on the forward voltage of the LEDs that are being driven.
The invention provides for initially sensing each LED voltage, VLED, and determining the maximum forward voltage, VLEDmax, between several LEDs. The invention employs the knowledge of VLEDmax in conjunction with what is known about VIN, converter output resistance and LED current, and current source/sink minimum headroom to switch from an initial gain to some higher gain just before the current sinks/sources drop out or from a higher gain to a lower gain in the event of the battery voltage going back to its initial value after being momentarily pulled down by a heavy load.
The conditions for gain switching that account for the above mentioned factors are developed in the implementation section below. Because of the uniqueness of the gain selection circuitry when implemented for a high side LED drive solution versus a low side LED drive solution, there are two subsections in the implementation. The first subsection describes the circuitry used for gain selection in a high side drive system and the second describes circuitry used for gain selection in a low side drive system.
Implementation of Gain Selectors for High Side and Low side Drivers
The forward voltage of different LEDs driven by the same amount of current may vary considerably. As shown in
The LED with the largest forward voltage forces a larger gate voltage onto the NMOS which is sampling the LED voltage. The NMOS with the maximum gate drive tends to take most of the current i1 and the voltage at its gate appears at its source minus its Vgs as illustrated in the fourth equation:
VA=VLEDmax−Vgs Equation 4
The maximum LED forward voltage is hence measured. Although this example is based on 4 LEDS, the invention can be implemented for any greater or lesser number of LEDs.
As shown in
Additionally, NPN transistors can be used instead of MOS transistors to reduce the impact of current density differences. In the case of a bipolar transistor, equation 4 is modified as follows: VA=VLEDmax−Vbe Equation 4b
One embodiment, of a final high side maximum forward LED voltage selector circuit is shown in
Gain Transitions
To improve efficiency, a gain of unity (one) is selected instead of 3/2 if VIN is high enough. For example, if Vin is greater than the required headroom across the current sources, the drop across the charge pump and the maximum LED voltage, then Vin can be passed to Vout. In one embodiment, to avoid gain chattering, a hysteresis voltage Vhys is added when switching gain from 3/2 to 1.
The equations for further implementing the invention are as follows:
G=1 if Vin>Vhr+VLEDmax+Rout1X* Iout+Vhys Equation 6
G=3/2 if Vin<Vhr+VLEDmax+Rout1X* Iout Equation 7
Equation 6 can be reworked as:
G=1 if VLED max<VIN−VHR−Rout1X* IOUT−Vhys Equation 8
In this case, the gain selection is based on a comparison between a headroom replica circuit that models the right part of the equation 8 and VLEDmax. The headroom replica circuit is yet another exemplary embodiment of the maximum selector circuit. Also, since the determination of VLEDmax introduces Vbe (or Vgs)—see equation 4b above—the headroom replica circuit also uses a source follower:
G=1 if VLEDmax−Vbe>VIN−VHR−Rout1X* IOUT−Vhys−Vbe Equation 9
An exemplary schematic that implements equation 9 is shown in
As shown in
Switching too early into a gain of 1 due to a too small headroom replica could be a real issue for the LED: the charge pump would not be able to deliver the right current lout and the LED light would be dimmed. Also, changes in headroom voltage from one current source to the next, which is possible with LED forward voltage mismatch can result in different output currents and LED brightness mismatch. However, if too much error compensation is added, it can negatively impact efficiency by causing switching between gains to occur too late.
To model the charge pump output impedance in gain of 1, Rout1X, a small PMOS M7 is chosen in
For this case, the ratio selected is 1:1000 as shown below:
Referring to
The charge pump should switch from gain of 1 to 3/2 as Vin falls below:
Vin
The charge pump should switch from gain of 3/2 to 1 as Vin rises above:
Vin
Where Vhyst is a hysteresis voltage needed so that gain chattering does not occur.
While a voltage mode type comparison can be used for the high side gain selector because a level shifted VLEDmax (relative to ground) can be directly measured using the maximum voltage selector circuit shown in
Referring to
The right most subcircuit in
The left most circuit composed of M1-M5, R, and CS1 is used to generate and route a current that is proportional to the voltage across a fully driven PMOS device that replicates the voltage drop in one possible implementation of a gain of one, which is a PMOS pass transistor from Vin to VO. Again, the current sink CS1 pulls a current that is proportional to the current being supplied by the charge pump so that the gain select circuit optimizes efficiency over LED current as well as input voltage. Care is taken to size M2 and M3 so that A is equal to the current density ratio between the devices.
Finally, the current mode comparator resolves the comparison between currents I1 and I2.
If I2>I1 then G=1 (high state=gain of 1 selected) or:
or after appropriate regrouping and cancellation of terms:
G=1 when: Vin>VLEDmax+VHRref+Vhyst+VDSM1 (Equation 13)
And,
G=0 when: Vin<VLEDmax+VHRref+VDSM1 (Equation 14)
The exemplary circuit as shown in
Next, the process advances to block 910 where these determined values and the input voltage are employed to switch from an initial gain to a final gain to drive the plurality of LEDS. The determined switching point enables the plurality of LEDs to be driven in an optimally energy efficient manner. Further, the process steps to a return block and returns to performing other actions. Additionally, although the actions of blocks 902, 904, 906, and 908 are shown performed in parallel, it is understood that in other embodiments, some or all of these actions could be performed serially without departing from the spirit and scope of the invention.
The above specification, examples and data provide a description of the manufacture and use of the composition of the invention. Since many embodiments of the invention can be made without departing from the spirit and scope of the invention, the invention also resides in the claims hereinafter appended.
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