Manufacturing Metrology Team

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Manufacturing Metrology Team ComparaƟve study of cost effecƟve laser and DLP projectors for fringe projecƟon Amrozia Shaheen 1 , Petros Stavroulakis 1 , Richard Leach 1 1 Manufacturing Metrology Team, Faculty of Engineering University of Noƫngham, NG8 1BB, UK Email: amrozia.shaheen1@noƫngham.ac.uk Abstract Commercially available projectors are subject to gamma non‐linearity, lack of depth‐of‐focus (DOF), system vibraƟon and noise which distort the fringe paƩerns and introduce significant errors in the phase measurement. In this work, we will compare a low‐cost DLP and a laser projector in terms of gamma performance and DOF, and assess which projector type performs beƩer for fringe projecƟon applicaƟons. Our study finds that the focus‐free eye‐safe laser projector provides more con‐ sistent high‐quality sinusoidal paƩerns and has a much longer DOF and is, therefore, recommended for pracƟcal implementaƟon in fringe projecƟon systems. Results Methodology Gamma‐correcƟon: Laser (Laser Beam Pro, C‐200) projector DLP (ICODIS‐G1 Mini) projector Raspberry‐Pi camera SoŌware for data acquisiƟon DOF: A camera‐projector assembly Checkerboard paƩern Rail SoŌware for image processing Fig. 3 Comparison of gamma curves Fig. 2 SchemaƟc illustraƟon of DOF A lookup table is used to compensate for the non‐linear sinusoidal behaviour of the fringes. The gamma curve is ac‐ quired by projecƟng mulƟple grayscale values on an imaging target and capturing by a camera. The DOF is measured by determining the maximum of the Fourier transform of the region‐of‐interest. 3D Metrology Conference ‐ 3DMC, 16‐18 October 2018, Hamburg Germany Fig. 1 SchemaƟc diagram of the gamma‐correcƟon Fig. 5 AŌer gamma‐correcƟon (laser) Conclusions The laser projector has the following upsides, Eye‐safe class‐1 laser Focus free Longer DOF Requires less gamma correcƟon Outperforms a DLP projector Recommended in high‐speed 3D applicaƟons Future work IntegraƟng the a‐priori informaƟon and fusion of different opƟcal tech‐ niques Sources of error CalibraƟon Traceability UlƟmately, designing a high‐speed 3D opƟcal imaging system Fig. 7 Phase image before gamma‐correcƟon (DLP) Fig. 8 AŌer gamma‐correcƟon (DLP) Fig. 6 Comparison of DOF Acknowledgements The authors would like to acknowledge the support provided by the Marie‐ Skłodowska‐Curie InnovaƟve Training Network (ITN), funded by the European Union under Horizon 2020 programme, Grant Agreement N o 721383. Horizon‐2020 Grant Agreement No 721383 Fig. 4 Phase image of a flat plane before gamma‐correcƟon (laser)

Transcript of Manufacturing Metrology Team

Page 1: Manufacturing Metrology Team

Manufacturing Metrology

Team Compara ve study of cost effec ve laser and DLP projectors for fringe projec on

Amrozia Shaheen1, Petros Stavroulakis1, Richard Leach1

1Manufacturing Metrology Team, Faculty of Engineering

University of No ngham, NG8 1BB, UK

Email: amrozia.shaheen1@no ngham.ac.uk

Abstract Commercially available projectors are subject to gamma non‐linearity, lack of depth‐of‐focus (DOF), system vibra on and noise which distort the fringe pa erns and introduce significant errors in the phase measurement. In this work, we will compare a low‐cost DLP and a laser projector in terms of gamma performance and DOF, and assess which projector type performs be er for fringe projec on applica ons. Our study finds that the focus‐free eye‐safe laser projector provides more con‐sistent high‐quality sinusoidal pa erns and has a much longer DOF and is, therefore, recommended for prac cal implementa on in fringe projec on systems.

Results 

Methodology  Gamma‐correc on:

Laser (Laser Beam Pro, C‐200) projector

DLP (ICODIS‐G1 Mini) projector

Raspberry‐Pi camera

So ware for data acquisi on

DOF:

A camera‐projector assembly

Checkerboard pa ern

Rail

So ware for image processing

Fig. 3 Comparison of gamma curves

Fig. 2 Schema c illustra on of DOF

A lookup table is used to compensate for the non‐linear sinusoidal behaviour of the fringes. The gamma curve is ac‐quired by projec ng mul ple grayscale values on an imaging target and capturing by a camera. The DOF is measured by determining the maximum of the Fourier transform of the region‐of‐interest.

3D Metrology Conference ‐ 3DMC, 16‐18 October 2018,

Hamburg Germany

Fig. 1 Schema c diagram of the gamma‐correc on

Fig. 5 A er gamma‐correc on (laser)

Conclusions The laser projector has the following upsides,

Eye‐safe class‐1 laser

Focus free

Longer DOF

Requires less gamma correc on

Outperforms a DLP projector

Recommended in high‐speed 3D

applica ons

Future work  Integra ng the a‐priori informa on

and fusion of different op cal tech‐niques

Sources of error

Calibra on

Traceability

Ul mately, designing a high‐speed 3D op cal imaging system

Fig. 7 Phase image before gamma‐correc on (DLP)

Fig. 8 A er gamma‐correc on (DLP) Fig. 6 Comparison of DOF

Acknowledgements The authors would like to acknowledge the support provided by the Marie‐Skłodowska‐Curie Innova ve Training Network (ITN), funded by the European Union under Horizon 2020 programme, Grant Agreement No 721383.

Horizon‐2020 Grant Agreement No 721383

Fig. 4 Phase image of a flat plane before gamma‐correc on (laser)