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KIT – The Research University in the Helmholtz Association
Light Technology Institute (LTI), Department of Electrical Engineering and Information Technology
www.kit.edu
Calculation Methods of Luminous Intensity Distributions from Ray Files by using Different Solid Angles
Markus Katona, Ingo Rotscholl, Klaus Trampert, Cornelius Neumann
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
2
Motivation
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
Luminous Intensity DistributionRay file
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
3
Motivation
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
Far field:
Luminous Intensity Distribution
Near field:
Luminance
http://www.ilumetrix.de/de/photometrie
𝐼 𝜑, 𝜗𝐿 𝑥, 𝑦, 𝑧, 𝜑, 𝜗
𝐼/𝐼𝑚𝑎𝑥
𝜗 [°]𝜑 = 𝑐𝑜𝑛𝑠𝑡.
𝜗
𝜑
𝐿 =d2Φ
cos 𝜀′ d𝐴 ∙ dΩ𝐼 =
dΦ
dΩ
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
4
LID calculation of near field data
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
𝜗[°]
𝐿 =d2Φ
cos 𝜀′ d𝐴 ∙ dΩ𝐼 =
dΦ
dΩ
𝐼 𝜑, 𝜗𝐿 𝑥, 𝑦, 𝑧, 𝜑, 𝜗
ϑ
φdA
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
5
LID calculation of near field data
Influence parameters:
Number of rays 𝑀 (stochastic uncertainty)
Shape of the solid angle
Resolution/size of the solid angle
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
𝜗[°]
𝐿 =d2Φ
cos 𝜀′ d𝐴 ∙ dΩ𝐼 =
dΦ
dΩ
𝐼 𝜑, 𝜗𝐿 𝑥, 𝑦, 𝑧, 𝜑, 𝜗
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
6
Cartesian polar coordinates Canonical solid angle Triangulated solid angle
Angle constant Solid angle constant
Cartesian polar coordinates Canonical solid angle Triangulated solid angle
Angle constant
• Resolution (𝑑𝜑, 𝑑𝜗)
• Standard
• dΩ ≠ const
Cartesian polar coordinates Canonical solid angle Triangulated solid angle
Angle constant Solid angle constant
• Resolution (𝑑𝜑, 𝑑𝜗)
• Standard
• dΩ ≠ const
• Number of solid
angles 𝑁
• Almost dΩ = const
Cartesian polar coordinates Canonical solid angle Triangulated solid angle
Angle constant Solid angle constant
• Resolution (𝑑𝜑, 𝑑𝜗)
• Standard
• dΩ ≠ const
• Number of solid
angles 𝑁
• Almost dΩ = const
• Opening angle ω
• Perfect shape
• dΩ = const
• Overlapping/incom-
plete space cover
x
y
zϑ
Cartesian polar coordinates Canonical solid angle Triangulated solid angle
Angle constant Solid angle constant
• Resolution (𝑑𝜑, 𝑑𝜗)
• Standard
• dΩ ≠ const
• Number of solid
angles 𝑁
• Almost dΩ = const
• Opening angle ω
• Perfect shape
• dΩ = const
• Overlapping/incom-
plete space cover
• Number of solid
angles 𝑁
• Dynamic solid angle
LID calculation of near field data
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
Different types of solid angles
𝜔
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
7
Calculation results
Point light source, 𝑀 ≈ 25 million, 𝑁 ≈ 1000
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
x
y
zϑ
Deviation𝐼𝑛𝑢𝑚𝐼𝑎𝑛𝑎 = 𝐼0 cos 𝜗 𝜖 =𝐼𝑎𝑛𝑎 − 𝐼𝑛𝑢𝑚
𝐼𝑎𝑛𝑎
Τ𝐼 𝐼𝑚𝑎𝑥 Τ𝐼 𝐼𝑚𝑎𝑥 𝜖 [%]
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
8
Calculation results
Point light source, 𝑀 ≈ 25 million
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
Τ𝐼 𝐼𝑚𝑎𝑥 𝜖 [%] Τ𝐼 𝐼𝑚𝑎𝑥 𝜖 [%]
𝐼∕𝐼_𝑚𝑎𝑥 𝜖 [%] Τ𝐼 𝐼𝑚𝑎𝑥 𝜖 [%]
x
y
zϑ
𝑁:𝜑 × 𝜗
2=30 × 60
2= 900 𝑁 = 1000
𝑁 = 943𝑁: 𝜔 = 6.36°
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
9
Calculation results
Real lambertian light source, 𝑀 ≈ 25 million
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
𝐼 [𝑐𝑑]
𝐼[𝑐𝑑]
𝜗[°]0°
𝑁𝑎:𝜑 × 𝜗
2=65 × 60
2= 1950
𝑁𝑏 = 2000
𝑁𝑐: 𝜔 = 4.55°
𝑁𝑑 = 2058
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
10
Calculation results
Real narrow beam flash light, 𝑀 ≈ 25 million
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
𝐼[𝑐𝑑]
𝐼[𝑐𝑑]
𝜗[°]
𝑁𝑎:𝜑 × 𝜗
2=50 × 720
2= 18000
𝑁𝑏 = 200 000
𝑁𝑐: 𝜔 = 0.455°
𝑁𝑑 = 2668
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
11
Comparison
a b c D
Calculation speed + + - o
Uniform solid angle size - + + o
Dynamic solid angle disposition o o o +
Unique space cover + + - +
Pseudo-LID calculation + + + -
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
12
Conclusion
LID calculation possible with all types of solid angle
Every solid angle types has their own advantages and limitations
Fastest very unshaped
Fast & good solid angle shape bad for narrow beam LID
Perfect solid angle shape slow & space cover
Dynamic no Pseudo-LID calculation
Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
Light Technology Institute (LTI), Department of
Electrical Engineering and Information Technology
13 Markus Katona - Calculation Methods of Luminous Intensity Distributions from Ray
Files by using Different Solid Angles
27.09.2017
Thank you for your
attention