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                      IR LED LEARNING LAB!

 

 

 

                                                                      

 

 

 

                                                                      

                                                                         LED Size  8mm 5mm 3mm

 


An IR-illuminator is a device that emits infrared light, or low frequency electromagnetic radiation that’s outside the visible spectrum. In other words, it gives off light that a camera can use, but a person cannot see so while it’s still dark to the human eye, the camera can see just fine.

 

IR light is measured in a unit called nanometers (abbreviated nm).  IR illuminators are typically used when ambient light is not present.  Sometimes an IR camera's IR array is too narrowly focused, or not strong enough, in that case an external IR illuminator can provide an extra source of invisible infrared light.

 

 

 

   

 

 

The verticle line A represents intensity of the illumination, and the horizontal line B represents the distance away from the illuminator. 

 

At distance "a" the illumination is at a miminum, and the video image is too dark.

 

At distance "b" the illumination is at the maximum, and the video is to bright.

 

At distance "H" we are at the optimum distance away from the illuminator where it is not to bright, or too dark.

 

 

Measure from where your illuminator will be mounted to the area that it will light up.  Double this distance, and this should give you an idea of the IR rating that you will need for your night time video.

 

 

Most illuminators will use the 850nm.  850nm is semi covert, and the LEDs will have a slight reddish glow.  There are some illuminators that use the 940nm.  They are completely covert, and cannot be seen, but it is more expensive therefore they are not used that much.

 

 

Most camera with built in IR will have a photo cell that turns the IR illumination on, and it will switch the color camera to a black, and white camera.

 


When setting up IR illumination for security cameras then you will need to know what your shot is going to look like, and you need to put some thought in to how you setup the illuminators.

 

You will need to think just like a photographer setting up for a photo shoot.  Photographers will set up a flash inside of an umbrella, and they will hold one in their hand to side of the camera pointed at the subject.  Think how a photographer would set up lighting in order to get a prize winning photograph.  Do they use back lighting?  Do they use down lighting?  Down lighting is used to create highlights in the hair recreating in outdoor effect from the light from the sun.  The umbrella diffuses the light, and makes it less harsh by bouncing the light in many directions.

 

 

 

 

 

 

 

 

If you are setting up a surveillance camera then you need to keep the camera close to where the subject may stand, or you will need to get a zoom lense to get up on the area.  You will need to get an IR illuminator that matches your lens.  If you are using a wide angle camera then you will want a short throw, but wide throw illuminator.

 

If you are using a zoom lens then you will need an illuminator that is narrow, but has a long throw.

 

Try different setups with you IR illumination.  You direct lighting, and use side lighting.

 


 

Machine Vision Optical Filters

http://en.wikipedia.org/wiki/Machine_vision_optical_filters

 

Wiki LED

http://en.wikipedia.org/wiki/Light-emitting_diode
 

Wiki Infrared
http://en.wikipedia.org/wiki/Infrared

 

Wiki Infrared Data Association

http://en.wikipedia.org/wiki/Infrared_Data_Association

 

 

LED STRUCTURE

http://hyperphysics.phy-astr.gsu.edu/Hbase/electronic/led.html

 

LIGHT SOURCES IN ELECTRONICS

http://hyperphysics.phy-astr.gsu.edu/Hbase/electronic/leds.html#c5

 

 


The International Commision on Illumination (CIE) recommended the division of optical radiation into the following three bands:
 
IR-A: 700 nm–1400 nm
IR-B: 1400 nm–3000 nm
IR-C: 3000 nm–1 mm 
 

Wiki CIE

http://en.wikipedia.org/wiki/International_Commission_on_Illumination


LED Safety Standards

 

The United States applies different emission limits than other countries so care should be taken to apply the proper Standard and emission limit.


In the United States, ANSI Z136.1-2000, American National Standard for Safe Use of Lasers, is the standard used to define emission limits for Lasers.

 

Appendix H of this Standard refers manufacturers to ANSI RP27.1 and RP27.3 to apply Safety Standards for LED’s.


Western Europe, and other Countries, apply IEC 60825-1, Safety of Laser Products as the standard for LED’s and Lasers. This document does not make a distinction or apply different emission limits between LED’s and lasers.


Reflector cups, multiple LED’s, external lenses and/or other optical components applied by the equipment manufacturer may significantly alter the emission level. It is the responsibility of the equipment manufacturer to test and verify the actual emission in the system. Opto Diode will be available to provide values at the component level as requested.

 

 


Beam Angle

Generally specified as the off-axis angle where the output power drops to 50% of the peak value. Can be specified from 50% to 50% point, or peak to 50%. Generally speaking if the value is referred to as Half Intensity Beam Angle or FWHM, the value is from 50% to 50% points.

 

Candela
A measurement of luminous intensity. Visible LED’s are usually specified in Candela (cd) or millicandela (mcd). Angle of measurement is critical when comparing lensed (narrow beam) products from different vendors. Value is pegged to the human eye response, making the peak wavelength a critical factor in the final value. Infrared LED’s have a value of nearly zero, because they do not emit appreciable levels of visible light.

 

Centroid Wavelength
The wavelength value where half of the light energy is at shorter and half the energy is at longer wavelengths. Value is stated in nanometers (nm) or microns (µ). This value is of interest to people in the test and measurement industries. Not commonly specified for standard LED products of any wavelength.

 

Dark Current
Usually abbreviated as ID. The current flowing through a reverse biased photodiode when light is not incident upon a photodiode. Higher reverse bias voltages result in higher dark currents. Dark current is not present in zero photodiode bias circuits (see shunt resistance).

 

Dominant Wavelength
The color, or perceived wavelength of a light source by the human eye. Also called the hue wavelength. Most visible LED’s are specified by the dominant wavelength.

 

Full-Width-Half-Max
Usually abbreviated as FWHM. Used most commonly when discussing beam angle or spectral bandwidth. In both cases it refers to the distance from 50% to 50% point, or –3db to –3db point. Beam angle value is specified in degrees and spectral bandwidth values are specified in nanometers.

 

Junction Capacitance
P-N junctions have an inherent capacitance similar to a parallel plate capacitor. The junction capacitance is proportional to the active area of the semiconductor. In the case of photodiodes, the junction capacitance can be reduced by reverse biasing it. The junction capacitance in conjunction with the inherent series resistance of the diode is not the limiting factor for response time of the device (see response time).

 

Light Emitting Diodes
Commonly abbreviated as LED, LED’s, or IRLED’s in the case of infrared light emitting diodes. Refers to any diode which when forward biased converts electrons (electrical current) to photons (light) in a non-coherent waveform.

 

Lumens
A measurement of total visible energy emitted from a point source. Output is measured in an integrating sphere with a detector whose spectral sensitivity approximates the human eye. This value is not commonly specified for LED’s.

 

Peak Wavelength
The wavelength value with the highest amount of energy radiating from the source. Most commonly specified for non visible (infrared) LED’s.

 

Photoconductive Detector
Common name given to a photodiode operated in a reverse bias mode. This mode decreases junction capacitance, increases speed and linearity. It also increases noise current by introducing dark current to the circuit.

 

Photodiode
Generic name given to any diode used as a light detector. Device has no internal gain like a photodiode or photodarlington. Directly converts photons (light) into electrons (current). It is linear over at least 6 decades of light input. Average saturation point is 10mW/cm2. Used extensively where light must be accurately measured or higher speeds (greater than 30KHz) is required. Response is measured in Amps/Watt (A/W).

 

Photovoltaic Detector
Common name given to a photodiode operated in a zero bias mode. This mode is commonly used in lower speed applications where rise time and junction capacitance are less important than minimizing dark current and thus reducing noise current.

 

Power Output
Value is expressed in Watts or milliwatts. A radiometric measurement of the total light energy radiating from an emitter regardless of wavelength. Measurement is made with an integrating sphere. This figure of merit is most commonly used with IRLED’s. It is the optical output measurement that is most easily correlated from one measurement facility to another.

 

Radiant Intensity
Radiant measurement of on axis intensity. This value must be known to calculate optical power incident on a detector that is greater than 6 inches from the LED. The angle of measurement is a critical component when comparing data sheets from one vendor to the next.

 

Response Time
Also known as rise or fall time. The period of time it takes an emitter or detector to go from the 10%-90% point, emitting and detecting respectively, or the 90%-10% point. RC time constant of the device is almost never the limiting factor. The speed of the device is almost always due to the transit time of the semiconductor material and the distance from the depletion region to edge of device.

 

Short Circuit Current
Operation of photodiode in a condition where a voltage bias is not allowed to generate across the diode. Usually accomplished by using a transimpedence amplifier circuit.

 

Shunt Resistance
The zero bias resistance of a photodiode. In practical measurements, most manufacturers put a 10mV reverse bias on the photodiode and measure current. The ratio between the bias voltage and current determine the shunt resistance value. This value must be known to determine noise current generated by the photodiode in a photovoltaic, short circuit current mode circuit.

 

Spectral Response
The conventional method for determining the sensitivity of photodiodes. The term is expressed in Amps/Watt (A/W). The monochromatic wavelength the measurement is done at must be specified as well.

 


 

ICNIRP STATEMENT

 

ICNIRP STATEMENT ON LIGHT-EMITTING DIODES (LEDS)

AND LASER DIODES: IMPLICATIONS FOR HAZARD

ASSESSMENT

http://www.icnirp.de/documents/led.pdf

 

 

ICNIRP GUIDELINES

 

Guidelines On Limits of Exposure To Broad Band Incoherent Optical Radiation  0.38 - 3uM

http://www.icnirp.de/documents/broadband.pdf

 


 

The Potential Ocular Hazards of LED Emitters



Cut and Paste in to Browser

http://www.cie.co.at/div2/meetings/LED Sympo 2001/Abstracts/David_Sliney.pdf

 

Questions have arisen as to whether laser or incoherent radiation exposure limits ( ELs) should

be applied to LED emitters. Based upon current exposure limits from the International

Commission on Non-Ionizing Radiation Protection (ICNIRP), most LEDs - particularly surfaceemitting

LEDs — pose no clear hazard to the eye. Current surface-emitting LEDs produce

exposure levels at the retina which are less than 1% of the levels that are known to cause retinal

injury even when the LEDs are viewed at extremely close distances (e.g., at 10 cm) (Sliney and

Wolbarsht 1980). At typical viewing distances of 0.5 to 2 m, the levels are less than 0.1% of

retinal injury levels. Even lengthy exposures of the cornea and lens of the eye pose no hazards

whatsoever. From a safety standpoint, LEDs have been treated both as lasers (e.g., in IEC

standard 60825-1-2001 and in ANSI Z-136.2-1997, and as lamps (CIE 1998; ANSI/IESNA 1996).

Because of some confusion relating to the actual risk, ICNIRP organized a panel of experts to

review the potential hazards of current diode emitters and they reported their findings in 1999

(ICNIRP, 1999). This tastk group noted that laser diodes are constructed with miniature resonant

cavities with gain, produce a very narrow spectral bandwidth, can generally achieve shorter pulse

durations, are not limited in radiance, and can emit much higher radiant powers than LEDs.

Light-emitting diodes of low to moderate brightness (luminance) are used in many types of visual

displays, as indicator lights and many related products. Higher power LEDs and IREDs are used

as signal lamps and in a wide variety of domestic and industrial products, and can compete with

laser diodes in limited optical communications systems, i.e., in local-area networks (LANs). They

are generally not competitive with laser diodes because of their radiance limitations. These

differences in output characteristics define both their uses and their potential eye hazards. Most

current LEDs--and all surface emitting LEDs--have very limited radiance and do not pose any

realistic eye hazard, despite the fact that they have been included in some laser safety standards

in the past few years (IEC, 2001).

After a careful review of all possible emission characteristics of surface-emitting LEDs and

IREDs, the ICNIRP concluded that these would be judged safe by applying the ICNIRP Exposure

Limits (ELs) for incoherent radiation. This conclusion applies as well if one follows the

recommendations of CIE TC 6-38 (Lamp Safety) for realistic viewing conditions. This conclusion

applies to any LED device which does not have optical gain. Only as a result of applying

extraordinarily "worst-case" assumptions and simplifications that are built into some current

product safety standards, can anyone arrive at the conclusion that an LED or IRED poses a

retinal hazard. On the other hand, the use of laser ELs and IEC 60825-1 measurement

techniques to evaluate LEDs could result in an understatement of the lenticular risk if the source

is very large and the lens becomes overheated. Thus, the ICNIRP recommended that safety

evaluations and related measurement procedures for LEDs follow the guidelines for incoherent

sources (ICNIRP 1997). This approach provides the most accurate assessment of incoherent

sources without problems originating from certain underlying assumptions about lasers that

remain incorporated into the limits developed for collimated laser beams. They also conclused

that diode lasers and VCSELs be treated in all safety evaluations and safety standards as lasers.

 

 


Ocular effects of GaAs lasers and near infrared radiation

 

http://www.opticsinfobase.org/abstract.cfm?&uri=ao-23-13-2181

 

Fiber optic communication systems present a possible or potential hazard to the eyes of engineers and technicians who work with or maintain these systems. To investigate this hypothesis, the retinas of macaque monkeys were exposed to near infrared cw radiation and to GaAs lasers modulated at 22 MHz and 1600 Hz. Trained animals (two) were exposed monocularly under normal physiological conditions to modulated GaAs lasers for several months, on a 5 day/week basis, 1000 sec/day. No loss of visual function or funduscopically visible damage was detected. One of these animals was sacrificed and examined histologically for damage. No differences were detected between the foveae of the exposed and control eyes in this monkey. The radiant exposure in J . cm-2 required to produce minimal lesions was determined on anesthetized animals for cw radiation at three wavelengths (820, 860, 910 nm) and for radiation at 830 nm from a GaAs laser modulated at a digital rate of 44 Mbit/sec. It required from 6 to 8.4 mW of GaAs radiation entering the eye for periods ranging from 400 to 3000 sec to produce a detectable lesion. Since the spot size on the retina was <50 µm in diameter, it is difficult if not impossible to imagine how the human eye could remain focused on such a source for an appreciable time, even if 8 mW were entering the pupil. Extrapolation to man is always dangerous, but these experiments do not suggest that engineers and technicians operating and maintaining fiber optic communication systems are subject to an ocular risk unless they use magnification optics.