principle of rt ok, but too slow !

1
Principle of RT OK, but too slow ! Towards a 3D light model for growth chambers using an experiment-assisted design Michaël Chelle 1 , Mustafa Demirel 1 , Christophe Renaud 2 Yes, but what in the real world ? What next? What next? The next steps are: implementing in Java or C++ this new algorithm testing for contrasted growth chamber types and cultures. Conclusion Conclusion Simple experiments have enabled us to quickly proposed a new light model, well adapted to the growth chamber case. 1 INRA -UMR Environnement et Grandes Cultures 78850 Thiverval-Grignon - France chelle @ grignon . inra . fr 2 Laboratoire d'Informatique du Littoral (LIL) BP 719 - 62228 Calais cedex - France renaud @ lil . univ -littoral. fr FSPM modeling Plant organ response law to physical environment Fine scale analysis of plant growth and development Genomic studies Analysis of various genotypes in the same environment Isolating a gene for a given function without environment bias. Comparing plants grown in the same chamber Comparing experiments in different growth chambers Need of spatially homogenous growth conditions Needs of “standardized” conditions between chambers Growth chamber experiments Spatial variability of irradiance (Strader chamber, France) What a diversity for growth chamber models How to bypass a “growth chamber” effect in ecophysiology due to spatial heterogeneity Modeling the incident or absorbed light for each plant (or organ) But there is two main difficulties: Complexity of light sources High level of multiple scattering Case of an empty Strader growth chamber Measurement the spatial distribution of light by distinguishing using black occultations the 0, 1 and (2 to ∞) orders of scattering E=E0(75%) + E1(18%) + Ex(7%) Results for PAR worktable irradiance Ray-tracing on simple geometry of perfect mirror Angular radiance distribution measured simulated ctionality of light sources + glossy materials => choice of the light model radiosity photon mapping (Ray Tracing) Step 2 Follow the photon path within the room until having bounced a wall n times or hitting the foliage bounding box Step 1 Trace a photon within a light source Step 3 Follow the photon within the plant bounding box A future OO photon mapping for growth chamber lighting Test with Radiance (G. Ward) rradiance distribution in an empty room

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Towards a 3D light model for growth chambers using an experiment-assisted design Michaël Chelle 1 , Mustafa Demirel 1 , Christophe Renaud 2. radiosity photon mapping (Ray Tracing). Test with Radiance (G. Ward) Irradiance distribution in an empty room. A future OO photon mapping - PowerPoint PPT Presentation

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Page 1: Principle of RT OK,  but too slow !

Principle of RT

OK, but too slow!

Towards a 3D light model for growth chambers using an experiment-assisted design

Michaël Chelle1, Mustafa Demirel1, Christophe Renaud2

Yes, but what in the real world ?

What next? What next? The next steps are: implementing in Java or C++ this new algorithm testing for contrasted growth chamber types and cultures.

Conclusion Conclusion Simple experiments have enabled us to quickly proposed a new light model, well adapted to the growth chamber case.

1INRA -UMR Environnement et Grandes Cultures78850 Thiverval-Grignon - France

[email protected]

2 Laboratoire d'Informatique du Littoral (LIL) BP 719 - 62228 Calais cedex - France

[email protected]

FSPM modelingPlant organ response law to physical environment

Fine scale analysis of plant growth and development

Genomic studiesAnalysis of various genotypes in the same environment

Isolating a gene for a given function without environment bias.

Comparing plants grown in the same chamberComparing experiments in different growth chambers

Need of spatially homogenous growth conditions Needs of “standardized” conditions between chambers

Growth chamber experiments

Spatial variability of irradiance (Strader chamber, France)

What a diversity for growth chamber models

How to bypass a “growth chamber” effect in ecophysiology due to spatial heterogeneityModeling the incident or absorbed light for each plant (or organ)

But there is two main difficulties:Complexity of light sources High level of multiple scattering

Case of an empty Strader growth chamber

Measurement the spatial distribution of light

by distinguishing using black occultations

the 0, 1 and (2 to ∞) orders of scattering

E=E0(75%) + E1(18%) + Ex(7%)Results for PAR worktable irradiance

≈Ray-tracing

on simple geometry of perfect mirror

Angular radiance distribution measured simulated

Directionality of light sources + glossy materials => choice of the light modelradiosity

photon mapping (Ray Tracing)

Step 2Follow the photon path within the roomuntil having bounced a wall n times or

hitting the foliage bounding box

Step 1Trace a photon

within a light source

Step 3Follow the photon within the plant bounding box

A future OO photon mapping for growth chamber lighting

Test with Radiance (G. Ward) Irradiance distribution in an empty room