Tunable white lighting is one of the biggest trends in commercial and home lighting. A tunable-white luminaire is usually able to change its color and light output level along two independent axes.
An interface currents channeling circuit may be used to convert two current channels of a conventional two-channel driver into three driving currents for the three LED arrays. By doing so, the same two channel driver may be used for applications requiring just two LED arrays as well as three LED arrays.
A more detailed understanding may be had from the following description, given by way of example in conjunction with the accompanying drawings wherein:
In the following description, numerous specific details are set forth, such as particular structures, components, materials, dimensions, processing steps, and techniques, in order to provide a thorough understanding of the present embodiments. However, it will be appreciated by one of ordinary skill of the art that the embodiments may be practiced without these specific details. In other instances, well-known structures or processing steps have not been described in detail in order to avoid obscuring the embodiments. It will be understood that when an element such as a layer, region, or substrate is referred to as being “on” or “over” another element, it can be directly on the other element or intervening elements may also be present. In contrast, when an element is referred to as being “directly on” or “directly” over another element, there are no intervening elements present. It will also be understood that when an element is referred to as being “beneath,” “below,” or “under” another element, it can be directly beneath or under the other element, or intervening elements may be present. In contrast, when an element is referred to as being “directly beneath” or “directly under” another element, there are no intervening elements present.
In the interest of not obscuring the presentation of embodiments in the following detailed description, some processing steps or operations that are known in the art may have been combined together for presentation and for illustration purposes and in some instances may have not been described in detail. In other instances, some processing steps or operations that are known in the art may not be described at all. It should be understood that the following description is rather focused on the distinctive features or elements of various embodiments described herein.
Referring to
A chromaticity diagram is a color projected into a two-dimensional space that ignores brightness. For example, the standard CIE XYZ color space projects directly to the corresponding chromaticity space specified by the two chromaticity coordinates known as x and y, as shown in
Chromaticity is an objective specification of the quality of a color regardless of its luminance. Chromaticity consists of two independent parameters, often specified as hue and colorfulness, where the latter is alternatively called saturation, chroma, intensity, or excitation purity. The chromaticity diagram may include all the colors perceivable by the human eye. The chromaticity diagram may provide high precision because the parameters are based on the spectral power distribution (SPD) of the light emitted from a colored object and are factored by sensitivity curves which have been measured for the human eye. Any color may be expressed precisely in terms of the two color coordinates x and y.
All colors within a certain region, known as a MacAdam ellipse (MAE) 102, may be indistinguishable to the average human eye from the color at the center 104 of the ellipse. The chromaticity diagram may have multiple MAEs. Standard Deviation Color Matching in LED lighting uses deviations relative to MAEs to describe color precision of a light source.
The chromaticity diagram includes the Planckian locus, or the black body line (BBL) 106. The BBL 106 is the path or locus that the color of an incandescent black body would take in a particular chromaticity space as the blackbody temperature changes. It goes from deep red at low temperatures through orange, yellowish white, white, and finally bluish white at very high temperatures. Generally speaking, human eyes prefer white color points not too far away from the BBL 106. Color points above the black body line would appear too green while those below would appear too pink.
One method of creating white light using light emitting diodes (LEDs) may be to additively mix red, green and blue colored lights. However, this method may require precise calculation of mixing ratios so that the resulting color point is on or close to the BBL 106. Another method may be to mix two or more phosphor converted white LEDs of different correlated color temperatures (CCTs). This method is described in additional detail below.
To create a tunable white light engine, LEDs having two different CCTs on each end of a desired tuning range may be used. For example, a first LED may have a CCT of 2700 K, which is a warm white, and a second LED may have a color temperature of 4000 K, which is a neutral white. White colors having a temperature between 2700 K and 4000 K may be obtained by simply varying the mixing ratio of power provided to the first LED through a first channel of a driver and power provided to the second LED through a second channel of the driver.
Referring now to
However, in practice, it may be desirable to offer a wider tuning range of color temperatures between, for example, 2700 K and 6500 K, which may be cool white or day light. If only 2700 K LEDs and 6500 K LEDs are used in the mixing, the first straight line 202 between the two colors may be far below the BBL 106. As shown in
To remedy this, a third channel of neutral white LEDs (4000 K) may be added between the two LEDs and a 2-step tuning process may be performed. For example, a first step line 204 may be between 2700 K and 4000 K and a second step line 206 may be between 4000 K and 6500 K. This may provide 3 step MAE BBL color temperature tunability over a wide range of CCTs. A first LED array having a warm white (WW) CCT, a second LED array having a neutral white (NW) CCT, and a third LED array having a cool white (CW) CCT and a two-step tuning process may be used to achieve three-step MAE BBL CCT tunability over a wide range of CCTs.
Referring now to
A three-channel driver may be used to control the three LED arrays in a similar manner. However, a three-channel driver may be more complex and expensive than a conventional two channel driver. It may be desirable to multiply the output of a driver to power a greater number of LED arrays than channels, such that there is more than a 1:1 ratio of driver channels to LED arrays.
Referring now to
In an embodiment, the interface currents channeling circuit may be mounted on a converter printed circuit board (PCB) 404 between the two channel driver 402 and a LED board 406. The two channel driver 302 may be a conventional LED driver known in the art. The interface currents channeling circuit may allow the two channel driver 402 to be used for applications requiring two LED arrays as well as applications with three LED arrays. Because the same two channel driver 402 may be used in both cases, circuit complexity, size, and expense may be reduced.
It should be noted that although
As described in more detail below, the interface currents channeling circuit mounted on the converter PCB 404 may enable the two channel driver 402 to power two LED arrays at the ends of a desired tunable range as well as an additional LED array in approximately the middle of the desired tunable range. A first LED array 408 having a first CCT, a second LED array 410 having a second CCT, and a third LED array 412 having a third CCT may be mounted on the LED board 318. A first channel 412 of the two channel driver 402 and a second channel 414 may be connected to the PCB 404 by a first set of connections 416, such as wires or direct board to board connections. The first channel 412 and the second channel 414 may each have a positive and a negative output.
The converter PCB 404 may provide three driving currents to the LED board 406 over a second set of electrical connections 418, such as wires or direct board to board connections. The second set of electrical connections 418 may be connected to one or more solder points 420 on the LED board 406. The second set of electrical connections 418 may include three separate negative outputs for the first LED array 408, the second LED array 410, and the third LED array 412. A LED+ output from the converter PCB 404 may be connected to a positive output of the two channel driver 402. The LED+ output may be connected to anode ends of the first LED array 408, the second LED array 410, and the third LED array 412.
The mathematical relationship between the inputs and outputs of the interface currents channeling circuit are described herein. In the following equations, a first input current may be I1 and a second input current may be I2. The output currents may be IWW for warm white (WW) LEDs, INW for neutral white (NW) LEDs, and ICW for cool white (CW) LEDs. The relationship may be defined as follows:
If I1≥I2 then
I
WW
=I1−I2, INW=2×I2, ICW=0 (1)
I
WW=0, INW=2×I1, ICW=I2−I1 (2)
In the case of I1>I2, the WW channel may receive a current equal to the difference between I1 and I2, while the NW channel may receive twice the amount of current of I2. The sum of IWW and INW may still be I1+I2. It should be noted that the actual sum may be slightly less than I1+I2 as part of the total current is used to power the interface currents channeling circuit.
If the current in I1 is 0 and I1 corresponds to the WW LEDs, all the current in I2 will go to the CW LEDs and no current will go to the WW LEDs or the NW LEDs. Likewise, if the current in I2 is 0 and I2 corresponds to the CW LEDs, all the current in I1 will go to the WW LEDs and no current will go to the CW LEDs or the NW LEDs.
Referring now to
The first input current I1 may be connected to a first sense resistor (Rs) 502. The second input current I2 may be connected to a second Rs 504. The first Rs 502 and the second Rs 504 may have the same resistance value. A first diode D1506 may prevent the first input current I1 from injecting into the second input current I2. A second diode D2508 may prevent the second input current I2 from injecting into the first input current I1. The first Rs 502 and the second Rs 504 may share one common terminal Vc, which may be connected to the anodes of a first LED string 510 that includes WW LEDs, a second LED string 512 that includes NW LEDs, and a third LED string 514 that includes CW LEDs. The voltages at Va and Vb are representative of the currents flowing through the first Rs 502 and the second Rs 504 with a common-mode component, which is the voltage at Vc.
As shown in a first computational circuit 560, the voltage at Vb may be attenuated by a resistive divider that includes a first resistor (R1) 516 and a second resistor (R2) 518. The resulting signal may be sent through a first low-pass filter (LPF) 520 to generate Vbb in a low voltage domain. Vbb may be defined as:
V
bb
=LPF(Vb×α), (3)
where α is an attenuation factor, which may be defined as:
As shown in a second computational circuit 562, the voltage at Va may be attenuated by a resistive divider that includes a first resistor (R1) 522 and a second resistor (R2) 524. In an embodiment, the first resistor (R1) 522 may be the same value as the first resistor (R1) 516 and the second resistor (R2) may be the same value as the second resistor (R2) 518. The resulting signal may be sent through a second LPF 526 to generate Vaa in a low voltage domain. In an embodiment, the second LPF 526 may perform the same operations as the first LPF 520. Vaa may be defined as:
V
aa
=LPF(Vaα) (5)
where α is the attenuation factor defined above in Equation (4).
Vbb may be fed to a first operational amplifier (opamp) 528 that is configured to perform subtraction between Vbb and Vaa. The outputs of the first opamp 528 may be VWW. VWW may be defined as:
V
WW=(Vaa−Vbb)×β, (6)
where
β=R4/R3. (7)
VWW may also be defined as:
V
WW=(I1−I2)×RS×α×β (8)
The current IWW may therefore be defined as:
I
WW
=V
WW
/R=(I1−I2)×α×β×RS/R (9)
When α*β/R equals the value of 1/Rs, the current IWW will equal I1−I2.
Vaa may be fed to a second opamp 530 that is configured to perform subtraction between Vaa and Vbb. The output of the second opamp 530 may be VCW. VCW may be defined as:
V
CW=(Vbb−Vaa)×β (10)
where β is defined above in Equation (7). In an embodiment, R3 and R4 may have the same values in the first computational circuit 560 and the second computational circuit 562.
VCW may also be defined as:
V
CW=(I2−I1)×RS×α×β. (11)
The current IWW may therefore be defined as:
I
CW
=V
CW
/R=(I2−I1)×α×β×RS/R (12)
When α*β/R equals the value of 1/Rs, the current ICW will equal I2−I1.
The VWW may be fed to a voltage controlled current source, which may be implemented with a first amplifier (amp) 536. The first amp 536 may output a voltage Vg1. The voltage Vg1 may be input to a first transistor M1 that is used to provide a driving current for the first LED string 510. The first transistor M1 may be a conventional metal oxide semiconductor field effect transistor (MOSFET). The first transistor M1 may be an n-channel MOSFET.
The first amp 536 may regulate the voltage Vg1 in a closed loop such that current flowing through the first transistor M1 is equal to VWW/Rs. The inputs to the first amp 536 may be very close to each other in a closed loop regulation. The first amp 306 may compare the value of VWW to the sensed voltage across Rs 564 at the source of the first transistor M1. The Rs 564 may have the same resistance value as the first Rs 502 and/or the second Rs 504. If the sensed voltage is lower than VWW, the first amp 306 may raise Vg1 to increase the current in the first transistor M1 until the sensed voltage is approximately equal to VWW. Likewise, if the sensed voltage is higher than VWW, the first amp 306 may reduce Vg1, which may reduce the current in the first transistor M1.
The VCW may be fed to the voltage controlled current source, which may be implemented with a second amp 538. The second amp 538 may output a voltage Vg2. The voltage Vg2 may be input to a third transistor M3 that is used to provide a driving current for the third LED string 514. The third transistor M3 may be a conventional metal oxide semiconductor field effect transistor (MOSFET). The third transistor M3 may be an n-channel MOSFET.
The second amp 538 may regulate the voltage Vg2 in a closed loop such that current flowing through the third transistor M3 is equal to VCW/Rs. The inputs to the second amp 538 may be very close to each other in a closed loop regulation. The second amp 538 may compare the value of VCW to the sensed voltage across Rs 566 at the source of the third transistor M3. The Rs 566 may have the same resistance value as the first Rs 502 and/or the second Rs 504. If the sensed voltage is lower than VCW, the second amp 538 may raise Vg2 to increase the current in the third transistor M3 until the sensed voltage is approximate equal to VCW. Likewise, if the sensed voltage is higher than VCW, the second amp 538 may reduce Vg2, which may reduce the current in the third transistor M3.
The output of the first amp 536 and the output of the second amp 538 may be clamped to zero when the difference between its inputs is negative.
A second transistor M2 may control power to the second LED string 512. The second transistor M2 may be a conventional metal oxide semiconductor field effect transistor (MOSFET). The second transistor M2 may be an n-channel MOSFET. The second transistor M2 may only be switched on when both the first input current I1 and the second input current I2 are in regulation. The second transistor M2 may have a pull up resistor (R7) 544 tied to Vc. The pull up resistor (R7) 544 may be tied to the node Vc because, at startup, the low voltage supply VDD may not be available. As a result, the first transistor M1 and the third transistor M3 would be in an off state. If the second transistor M2, which provides a driving current for the second LED string 512, is also off, the whole circuit would appear as open-circuit to the current sources. This may trigger open-circuit protection and lead to a non-startup condition. By tying the gate of M2 to the node Vc, it may provide a current path available at startup.
The current produced by the voltage controlled current sources for the first LED string 510 and the third LED string 514 may be slightly larger than the absolute value of (I1−I2). This may ensure that the second LED string 512 is off when either I1 or I2 carries zero current. In other words, only one string of LEDs at either endpoint of the desired tuning range may be on at a time.
The AND logic of the switching transistor may be realized by the gate control block 532. The gate control block 532 makes use of the fact that the output of the first amp 536 (Vg1) and the output of the second amp 538 (Vg2) in a voltage controlled current source may swing to its supply rail (VDD) if it is unable to maintain regulation. The VDD may be chosen in such a way that the voltages Vg1 and Vg2 are significantly lower than VDD when the first amp 536 and the second amp 538 are in regulation under all operating conditions.
The Vg1 may be attenuated by resistive dividers that include a first resistor (R5) 540 and a second resistor (R6) 542, and then fed to a REF input of a first shunt regulator 570. The Vg2 may be attenuated by resistive dividers that include a first resistor (R5) 574 and a second resistor (R6) 576, and then fed to a REF input of a second shunt regulator 572. In an embodiment, the first resistor (R5) 540 and the second resistor (R6) 542 may be the same value as the first resistor (R5) 574 and the second resistor (R6) 576 Vg2. The first shunt regulator 570 and the second shunt regulator 572 may have an internal reference voltage of 2.5V. When the voltage applied at their REF nodes is higher than 2.5V, the first shunt regulator 570 and the second shunt regulator 572 may sink a large current. When the voltage applied at their REF nodes is lower than 2.5V, the first shunt regulator 570 and the second shunt regulator 572 may sink a very small quiescent current.
The large sinking current may pull the gate voltage of the second transistor M2 down to a level below its threshold, which may switch off the second transistor M2. The first shunt regulator 570 and the second shunt regulator 572 may not be able to pull their cathodes more than the Vf of a diode below their REF nodes. Accordingly, the second transistor M2 may have a threshold voltage that is higher than 2V. Alternatively, a shunt regulator with a lower internal reference voltage, such as 1.5V, may be used.
If Vg1 and Vg2 would be maximum around 3V, the VDD may be set to be 5V and the attenuation factor a may be set to 0.6. When the first amp 536 and the second amp 538 are in regulation, the voltage appearing at the REF node of the shunt regulator would be a maximum of 1.8V, the shunt regulator may draw a minimum current and the gate of the second transistor M2 may be pulled high towards the VDD. If either the first amp 536 or the second amp 538 is out of regulation, the shunt regulator may switch off the NMOS.
It should be noted that well-known structures shown in
Referring now to
The method shown in
Although features and elements are described above in particular combinations, one of ordinary skill in the art will appreciate that each feature or element can be used alone or in any combination with the other features and elements. In addition, the methods described herein may be implemented in a computer program, software, or firmware incorporated in a computer-readable medium for execution by a computer or processor. Examples of computer-readable media include electronic signals (transmitted over wired or wireless connections) and computer-readable storage media. Examples of computer-readable storage media include, but are not limited to, a read only memory (ROM), a random access memory (RAM), a register, cache memory, semiconductor memory devices, magnetic media such as internal hard disks and removable disks, magneto-optical media, and optical media such as CD-ROM disks, and digital versatile disks (DVDs).
This application is a continuation of U.S. application Ser. No. 15/640,549, filed Jul. 2, 2017, which is hereby incorporated by reference in its entirety.
Number | Date | Country | |
---|---|---|---|
Parent | 15640549 | Jul 2017 | US |
Child | 16895780 | US |