The present application relates to the generation of optical energy using light-emitting diodes (LEDs). More particularly, the application relates to LED systems having outputs with a stabilized intensity, and methods for providing optical energy of stable intensity from an LED.
Many electronic devices, such as analog optical sensors, require a stable source optical energy. Thermoelectrically-cooled lasers have typically been used as sources of stabilized optical energy. Recent developments in the field of low-cost, high-intensity, super-luminescent LEDs, however, have made it desirable to use these types of devices in lieu of lasers in some applications.
The intensity of the optical energy generated by an LED, however, typically varies with the temperature of the LED. LEDs can be required to operate over temperature ranges as great as, or greater than −40° C. to +70° C. For example, the output intensity of certain types of surface-mount LEDs can fluctuate by as much as ten percent when the temperature decreases from ambient to about −40° C., or increases from ambient to about +70° C. Moreover, the output intensity usually varies as the LED ages. For example, the output intensity of certain types of LEDs can decrease over the operational life of the LED by as much as 27 percent.
Optical signals, in general, are usually monitored by tapping a relatively small, predetermined fraction of optical energy from the optical fiber carrying the signal. For example, a tapping fiber may be wrapped around and fused with the optical fiber carrying the signal. Alternatively, the optical fiber carrying the signal may be sharply bent so that a fraction of the optical energy escapes from the optical fiber. It is believed that the ratio of the tapped optical energy to the optical signal can vary by ten percent or more using each of these techniques. Stabilizing the intensity of the optical output of an LED, it is believed, requires measurement of the intensity with an accuracy of about one percent or better.
Consequently, an ongoing need exists for a system and method for providing optical energy of stabilized intensity using an LED.
Systems for providing optical energy comprise an LED, a detector of optical energy, such as a photodiode, that measures the intensity of optical energy emitted by the light-emitting diode, and a controller. The controller adjusts the intensity of the optical energy emitted by the LED based on the intensity measurement provide by the photodiode, to maintain the intensity of the emitted optical energy at a desired level.
Embodiments of systems comprise a light-emitting diode, a detector of optical energy in optical communication with the light-emitting diode, and a controller communicatively coupled to the light-emitting diode. The controller adjusts an output of the light-emitting diode in response to an output of the detector of optical energy.
Methods comprise generating optical energy using a light-emitting diode, measuring an intensity of the optical energy, and changing the intensity of the optical energy in response to the measured intensity of the optical energy.
Other embodiments of systems comprise a light-emitting diode, a detector of optical energy, and a closed loop controller operatively coupled to the light-emitting diode and the detector of optical energy.
Other methods comprise energizing a light-emitting diode, monitoring an intensity of optical energy emitted by the light-emitting diode, and changing an operating parameter of the light-emitting diode based on the intensity of the optical energy emitted by the light-emitting diode.
The foregoing summary, as well as the following detailed description of embodiments, are better understood when read in conjunction with the appended diagrammatic drawings. For the purpose of illustrating the embodiments, the drawings diagrammatically depict specific embodiments. The appended claims are not limited, however, to the specific embodiments disclosed in the drawings. In the drawings:
The figures depict an embodiment of a system 10 for generating optical energy. The system 10 comprises an LED 12, and a detector of optical energy in the form of a photodiode 14.
The LED 12 and the photodiode 14 can be mounted on a substrate by a suitable technique such as soldering. The substrate can be, for example, a printed circuit board (PCB) 18 shown in
The LED 12 can be mounted on the first surface 20, and the photodiode 14 can be mounted the second surface 22. The first and second surfaces 20, 22 are depicted in
The LED 12 emits optical energy in omni-directional manner, i.e., in all directions, although the primary direction of emission is upward. An optical connector 24 is mounted is mounted on the upper portion of the LED 12. The optical connector 24 can be, for example, a SMA connector. The optical connector 24 transmits the upwardly-directed optical energy from the LED 12 to a fiber optic cable 25. The fiber optic cable 25, in turn, transmits the optical energy to a device, such as an analog optical sensor package (not shown), that requires the use of optical energy.
Directional terms such as “upward,” “downward,” “above,” “below,” etc., are used with reference to the component orientations depicted in
The LED 12 should be chosen so that the LED 12 can be safely driven at levels sufficient to maintain a desired output intensity as the LED 12 ages, or as the temperature of LED 12 fluctuates during operation.
A through hole 28 is formed in the PCB 18, as shown in
The photodiode 14 generates an electrical output proportional to the intensity of the optical energy incident thereupon. The use of the photodiode 14 as the detector of optical energy in the system 10 is disclosed for exemplary purposes only. Other types of detectors can be used in the alternative.
The system 10 further comprises an LED driver circuit 30 and a computing device 40, as shown in
The driver circuit 30 also comprises a current to voltage converter 34 communicatively coupled to the computing device 40 and the photodiode 14. The current to voltage converter 34 converts the output current of the photodiode 14 into an analog voltage that is input to the computing device 40.
The LED driver circuit 30 is depicted schematically in
The current to voltage converter 34 comprises a second operational amplifier U2, a third resistor R3, and fourth capacitor C4. The third resistor R3 and the fourth capacitor C4 are used to set the respective gain and bandwidth of the operational amplifier U2.
The LED driver circuit 30 also includes second and third capacitors C2, C3 that function as bypass capacitors that help to maintain the stability of the power supply (not shown) of the LED driver circuit 30.
Specific details of the LED driver circuit 30 are presented for exemplary purposes only. Alternative embodiments can include circuitry configured in other manners to effectuate the noted current and voltage conversions.
The system 10 further comprises a computing device 40. The computing device 40 comprises a processor such as a microprocessor 42, as shown in
The computing device 40 functions as a closed loop controller that regulates the optical output of the LED 12 to maintain the intensity of the output at a substantially constant level. In particular, the computing device 40 is programmed with a proportional-integral-differential (PID) control algorithm. The PID control algorithm can be expressed as follows:
where u(t) is the system output, e is the error signal, Ti is the integration time, and Td is the differentiation time. The error signal e is a result of the difference between the set point for the operation and the process variable.
The transfer function of the PID control algorithm expressed in Laplace form is as follows:
where G(s) is the PID control algorithm transfer function, Kd is the differential gain, Kp is the proportional gain, and Ki is the integral gain.
The error signal is sent to the controller depicted in
The output of the controller is fed as an input to the process depicted in
The control loop effectuated by the system 10 is depicted in
The computing device 40 functions as a closed-loop controller. In particular, the computing device 40 is programmed with the PID transfer function represented by equation (2). The computing device 40 thus generates an output voltage based on the sum of a proportion, an integral, and a derivative of the error signal. The output voltage of the computing device 40 is input to the voltage to current converter 32, which converts the output voltage to a current. The current is input to, and energizes the LED 12.
Changes in the output of the photodiode 14 cause a corresponding change in the output voltage of the current to voltage converter 34, which in turn results in a change in the error signal. The computing device 40 increases or decreases its voltage output in response to the error signal, based on the PID algorithm. The computing device 40 thereby causes the intensity of the optical energy generated by the LED 12 to vary in a manner that drives the process variable toward the set point. The intensity of the output of the LED 12 is stabilized when the process reaches a steady-state condition, i.e., when the process variable and the set point are approximately equal.
An LED system having an output whose intensity is stabilized in the above-noted manner was constructed by the Applicants. The output of the system was evaluated under changing temperatures, and at different set points. The system is depicted in part in
The prototype system included a surface-mount LED. A Nichia Corporation NSFG036BT LED was used as the LED. The LED was soldered to a printed circuit board as depicted in
An SMA connector was mounted on the upwardly-facing side of the LED, i.e., on the side of the LED opposite the PCB. A three-meter long fiber optic cable (not shown in
The fiber optic cable of the prototype system was connected to an optical power meter capable of measuring the intensity of the optical energy emitted by the LED. An Oz Optics Limited 23700 POM-300-VIS hand held optical power meter was used as the optical power meter. The optical energy emitted by the LED in the upward direction, i.e., in a direction away from the PCB, was measured using the optical power meter.
The photodiode of the prototype system was mounted on an underside of the printed circuit board, and was in optical communication with the LED by way of a through hole (not shown) formed in the circuit board. A Hamamatsu S1336-5BQ photodiode was used as the photodiode.
A Dell INSPIRON 9300 notebook computer was used as the computing device. The notebook computer was programmed with the PID transfer function represented by equation (2). The parameters listed in the table presented as
The values for the parameters listed in the table of
The prototype system included an LED driver substantially identical to the LED driver 30 depicted in
The LED of the prototype system was operated at a constant set point of about 8.067 volts, while the temperature of the LED was varied between about −30° C. and about +70° C. The set point was chosen to correspond to an output intensity for the LED of about 172 μW measured at the end of the three-meter fiber optic cable. The LED was operated on a continuous basis, i.e., without pulsing. The temperature of the LED was varied by placing the LED, the substrate, and the photodiode in a temperature chamber, and increasing temperature incrementally. The output of the LED was measured using the optical meter.
The feedback loop was deactivated at each temperature setting after an initial intensity reading was obtained at the setting. An intensity reading was then obtained with the feedback control loop inactive. The feedback control loop was subsequently activated, and the temperature of the LED was increased to the next incremental setting. Back to back intensity readings were thus obtained with the system operated in closed loop and open loop control modes.
The results of the above procedure are depicted in
The measured intensity of the LED of the prototype system varied by about 16.1 μW over the above-noted temperature range when the feedback control loop was inactive. The closed loop control effectuated by the prototype system thus substantially reduced variations in the intensity of the output of the LED as a function of temperature.
The prototype system was subsequently operated while varying the set points between 8.067, 7.779, and 7.900 volts while the feedback control loop was active, and then deactivating the closed control loop. Readings of the output intensity of the LED were obtained at each set point with the feedback control loop activated. The intensity was also measured with the control loop deactivated. This procedure was performed at a series of discrete temperatures spanning a range of about −30° C. to about +70° C. The results of this exercise are depicted in
The response of the photodiode used in the prototype system had a specification temperature coefficient of 0.05 percent at the wavelength at which the photodiode was operated. It is believed that the output intensity of the LED of the prototype system can be further stabilized through the use of a photodiode or other detector of optical energy having a response which is less sensitive, or flat with respect to temperature variations. Moreover, a temperature sensor can be added to the prototype system to permit the system to compensate for temperature-induced variations in the response of the detector.
The foregoing description is provided for the purpose of explanation and is not to be construed as limiting. While the embodiments have been described with reference to specific embodiments or methods, it is understood that the words which have been used herein are words of description and illustration, rather than words of limitation. Furthermore, although particular embodiments and methods have been described herein, the appended claims are not intended to be limited to the particulars disclosed herein. Those skilled in the relevant art, having the benefit of the teachings of this specification, may effect numerous modifications to the embodiments and methods as described herein, and changes may be made without departing from the scope of the appended claims.
Alternative embodiments can be based on a closed-loop control methodology other than proportional-integral-derivative control. Moreover, closed loop control of the system 11 can be effectuated by hardware, as opposed to the use of software described above. For example,
Alternative embodiments of the system 10 can include an LED, and a photodiode or other detector of optical energy packaged as single unit. For example, alternative embodiments can include an integrated circuit comprising an LED, and a photodiode or other detector of optical energy.
This application claims priority under 35 U.S.C. §119(e) to U.S. provisional application No. 60/859,324, filed Nov. 16, 2006, the contents of which is incorporated by reference herein in its entirety.
Number | Name | Date | Kind |
---|---|---|---|
4032817 | Richmond | Jun 1977 | A |
4234820 | Widmayer | Nov 1980 | A |
4284884 | Dyment et al. | Aug 1981 | A |
4998043 | Unami et al. | Mar 1991 | A |
5229596 | Ujihara | Jul 1993 | A |
5345167 | Hasegawa et al. | Sep 1994 | A |
6097159 | Mogi et al. | Aug 2000 | A |
6303916 | Gladnick | Oct 2001 | B1 |
6441558 | Muthu et al. | Aug 2002 | B1 |
6624892 | Johnston | Sep 2003 | B1 |
6649896 | Birrer et al. | Nov 2003 | B2 |
6720544 | Barna et al. | Apr 2004 | B2 |
6831290 | Mentzer | Dec 2004 | B2 |
6891142 | Ogawa | May 2005 | B2 |
7157681 | Tetzlaff | Jan 2007 | B1 |
7276863 | Lee et al. | Oct 2007 | B2 |
20030076056 | Schuurmans | Apr 2003 | A1 |
20050040773 | Lebens et al. | Feb 2005 | A1 |
Number | Date | Country | |
---|---|---|---|
60859324 | Nov 2006 | US |