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| https://www.jeti.com/cms/index.php/general/radiant-intensity-calculation | |
| Application of JETI Spectroradiometers specbos 1211 | |
| Radiant Intensity Calculation Using Irradiance Measurement | |
| The Radiant intensity (I) of a (point like) source can be obtained by measuring the Irradiance (E) | |
| in a certain distance. Afterwards the inverse square law has to be used | |
| to convert the Irradiance into Radiant intensity. The distance d | |
| between the measuring plane and the source has to be measured before. | |
| The following figure shows the set up. | |
| Some conditions have to be matched to get a precise result: | |
| The distance between the light source and the measuring plane has to | |
| be at least 10 times the diameter (or largest illuminating dimension) | |
| of the light source to get a measuring error below 1 %. | |
| The Luxmeter has to be positioned exactly in line with the centre of | |
| the light source. If a specbos 1211 in Irradiance mode is used, the | |
| alignment can be done using the target laser in Radiance mode and | |
| attaching the diffusor after alignment. | |
| Stray light has to be avoided using appropriate apertures between source and measuring probe (see the figure above). | |
| The measurement of the distance has to be the more precise the | |
| smaller the distance d. It is measured from the top of the light source | |
| to the reference plane of the Luxmeter. If this plane is not known, the | |
| front plane of the diffusor can be used. | |
| [object]<-----------------d----------------->[diff][Luxmeter] | |
| The Inverse square law reads as follows: | |
| I : The Radiant intensity | |
| E : Irradiance | |
| d : The distance d between the measuring plane and the source has to be measured before | |
| I = E x d^2 | |
| It can be used for the radiometric (E,I), photometric (Eν,Iν) or spectral data (E(λ),I(λ)). | |
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