Application of JETI Spectroradiometers specbos serie

Optical Characterization of LED and LED based Illuminaires

Currently LEDs and LED illumination products can be classified into three categories:
  1. Low power LEDs – classical plastic housed or SMD types
  2. High power LEDs – modern high intensity types with heat dissipation means
  3. Solid State Lighting products (SSL) – Light sources based on high power LEDs

lowhighpower led differenttypes

Examples of low and high power LEDs

ssl led differenttypes 300

Examples of SSL products
 
 
 
Different set ups are used to characterize the optical parameters of such sources:
The detector for all these measurements can be a photometric detector, a tristimulus instrument, a spectroradiometer or a Video photometer. The application of spectral resolving technique allows to get more information about the DUT and reduces the measuring uncertainty because the Color Matching functions are used directly. Therefore this technique becomes more and more important and is now the prefered one for LED measurement.
The currently relevant publications for the measurements are CIE 127:2007 for Low Power LEDs and IES LM-79 for High Power LEDs and SSL products.
Angular resolved Luminous flux measurement based on a Goniometer
Goniometer and nearfield goniometer are used to measure the angular distribution of LEDs (Light distribution curve – angular distribution of Luminous intensity). This measurement is time consuming, but delivers the most extensive data set of a light source. The integral values like Luminous and Radiant flux will be calculated as summation of the light distribution data. “Color quantities shall be measured as values that are spacially averaged over the entire solid angle …” (from: IES LM-79)
Commonly photometric or tristimulus detectors are used for such measurements. If the distribution of the spectral characteristics is of interest in addition, a spectroradiometer as specbos 1211 can be applied as detector of the goniometer. Due to its high sensitivity the measuring time for each step becomes acceptably short. The instrument can be equipped with a remote diffusor (Diffusor with fiber optic extension) so that the installation will be very flexible.
The integral values like Luminous and Radiant flux will be calculated as summation of the light distribution data.
 
olino1 300 olino2 new

Goniometer mit specbos 1211     Source:  http://www.olino.org/us

Total Luminous flux measurement based on an Integrating sphere
If a goniometric scan is too slow and only integral values are of interest (e.g. in production), the measurements can be done with an Integrating sphere. This sphere contains at least two ports – one for the sample and one for the probe. A baffle is needed to avoid direct incidence of the sample light to the probe. The probe is calibrated for Radiant flux, but basically measures the Illuminance in the plane of the inner sphere surface. The sphere needs to fulfil the following requirements to guarantee an almost equal illuminance on all surface parts (that the illuminance at the measuring location is representative for the whole sphere):
  • Ratio of port diameter to sphere diameter max. 1:3
  • Neglectable self absorption of sample and sample holder or useage of an auxiliary lamp
  • Homogenious, high reflective and diffuse coating of the inner surface (BaSO4)
The CIE publication 127:2007 as well as IES LM-79 define the conditions for such Luminous Flux measurements.
There exist three different sphere measuring set ups according to this publication:
  • 2π set up : Sample is arranged in the plane of the inner sphere surface – can be applied for LEDs with no backwards emission, often used for single LEDs and LED arrays
  • 4π set up: Sample is arranged inside the sphere using a holder – often used  for SSL illuminaires, an auxiliary lamp is definitely needed to compensate the absorption effect of the sample
  • Partial flux measuring set up: Sample is arranged in a distance to the sample port – a precise aperture in front of the port defines a solid angle

led_measurement_skizze_300

Measurement geometry for LEDs with no backward emission (2π geometry)
 
 
specbos 1311/500 is the combination of specbos 1211 with a hinged 500 mm sphere with an auxiliary lamp. It can be used for 2 π and 4π measurements. The correction of self absorption is especially necessary for the 4π geometry where the full sample is inserted into the sphere and thus may drastically disturb the conditions in the sphere.
 
  Sphere_opened
 
 specbos 1311 (500 mm hinged sphere with auxiliary lamp)
Luminous intensity measurement based on reverse square law

The detector for the measurements can be a photometric detector, a tristimulus instrument, a spectroradiometer or a videophotometer.
The Luminous Intensity (cd) measurement is normally carried out as an Illuminance measurement. It can be done with the set up described in the CIE publication 127:2007. The main idea of this set up is that the adjustment of the sample is done according to mechanical conditions – the measuring distance is measured from the tip of the LED and the angular adjustment is done with regard to its mechanical axis.

 
 conditiona
Condition A

 

The measuring result is called Averaged LED Intensity rather than Luminous intensity because it is not necessarily the maximum value of the LED.
specbos 1411 uses the basic modell specbos 1211 and combines it with the measuring tubes and the measuring integrating sphere according to CIE 127:2007. Two measuring distances (cond. A – 316 mm and cond. B – 100 mm) can be used.
 

specbos_1401_300

specbos 1401 condition B
 
 

If a CIE 127 measuring set up for Luminous Intensity is not available, the measurement can be done with a Luxmeter on an optical bench (see: Radiant Intensity Calculation using Irradiance Measurement).