Presentation of the Secondary Image Measuring Instrument Dr. B. - - PowerPoint PPT Presentation

presentation of the secondary image measuring instrument
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Presentation of the Secondary Image Measuring Instrument Dr. B. - - PowerPoint PPT Presentation

Presentation of the Secondary Image Measuring Instrument Dr. B. Grubert 7.th International CTI-Forum Automotive Glazing October, 8th 2013 Overview 1 Introduction to M OLLER-WEDEL OPTICAL GmbH 2 Causes and properties of the secondary


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SLIDE 1

Presentation of the Secondary Image Measuring Instrument

  • Dr. B. Grubert

7.th International CTI-Forum ”Automotive Glazing“

October, 8th 2013

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SLIDE 2

Overview

1 Introduction to M ¨

OLLER-WEDEL OPTICAL GmbH

2 Causes and properties of the secondary image 3 Presentation of the laser-based measurement method 4 Comparison with the method according to ECE R43

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SLIDE 3

Introduction to M ¨ OLLER-WEDEL OPTICAL GmbH

Established 2000 as independent subsidiary of M ¨ OLLER-WEDEL GmbH Located: Wedel near Hamburg Mid-size company Member of the Swiss based HAAG-STREIT Holding AG Main products: Optical measuring and testing instruments

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Appearance of the Secondary Image

Double image with 6 arcmin secondary image angle separation.

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SLIDE 5

Limits for Secondary Image Angle Separation

Investigations showed that a separation below 10 arcsec are not recognised as annoying. According to the regulation ECE R43 the largest permissible value is 15 arcmin for area A and 25 arcmin for area B.

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Secondary Images in Windshields Caused by Wedge

The secondary images are caused by internal reflections in the windshield.

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SLIDE 7

Secondary Images in Windshields Caused by Wedge

The secondary image angle is the angle between primary and secondary image beam.

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SLIDE 8

Calculation of the Secondary Image Angle Separation for Wedges

ǫ ≈ 2 α

  • n2 − sin θ2

cos θ The amount of secondary image angle ǫ

increases with increasing internal wedge angle α of the windshield, increases with increasing tilting angle θ of the windshield, increases with increasing refractive index n of the windshield material.

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SLIDE 9

Secondary Images in Windshields Caused by Curvature

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SLIDE 10

Calculation of the Secondary Image Angle Separation for Curvature

ǫ ≈ 2 t tan arcsin sin θ

n

R 3438 arcmin The amount of secondary image angle ǫ

decreases with increasing radius of curvature R of the windshield, increases with increasing angle of incidence θ on the windshield, increases with increasing thickness t of the windshield, decreases with increasing refractive index n of the windshield material.

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SLIDE 11

Measurement Principle of the Secondary Image Angle Measuring Instrument

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SLIDE 12

Image of Camera with Linear Sensitivity

Secondary image not visible.

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Brightness Ratio Primary to Secondary Image

The primary image is usually 50 ∼ 100 times brighter than the secondary for incidence angles 50◦ ∼70◦. → for a camera with 8-bit resolution depth the brightness of the secondary image is only 3 to 5, when the primary image has maximum brightness (255).

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SLIDE 14

Image of Camera with Linear Sensitivity (Overmodulated)

Primary image is strongly overmodulated in order to make secondary image visible

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SLIDE 15

Image of Camera with Logarithmic Sensitivity

Primary and secondary image are visible.

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SLIDE 16

Polarisation of the Secondary Image

The secondary image is predominantly linearly polarised in the perpendicular plane for incidence angles ∼60◦ (∼Brewster angle). → The contrast between primary and secondary image can be improved by a factor of 2 when using linearly polarised illumination instead of non-polarised.

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Illumination with linearly polarised light — parallel direction

Secondary image not visible.

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SLIDE 18

Secondary Image Angle Measuring Instrument

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Features of the Secondary Image Angle Measurement (SIAM)-Instrument

Instrument is based on a proven set-up used at VW. No disturbance by local refractive index and power variations due to small diameter of the test beam. Easy and fast set-up of the instrument. Laser is eyesafe (laser safety class 2). Measurement value is independent of the distance between laser, windshield and telescope. Measuring range: 68 arcmin × 50 arcmin. Measurement uncertainty: better than 0.5 arcmin Objective measurement results due to PC-based image evaluation software.

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SLIDE 20

Features of the Evaluation Software

Real-time evaluation with 25 Hz frame rate. Automatic brightness control. Evaluation according to ECE R43. Display of the double image angle with magnitude (ǫ) and direction (ϕ). Use of predefined customisable measurement templates. Generation of protocol (PDF or ODT). Export of measurement results to spreadsheet software (CSV-format).

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SLIDE 21

Windshield View of the Software

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Live-Image View of the Software

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Protocol View of the Software

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Sketch of the Set-Up for Conformity Check According to ECE R43

Double3Collimator Telescope3with3Camera Telescope3with3Camera Folding3Mirror Laser

120° 1 5 ° 2 1 ° 240° 300° 3 3 ° 3 ° 60°

10´ 10´ 20´ 20´ 30´ 30´ 10´ 10´ 20´ 20´ 30´ 30´

12,6S33330°

Beam- Splitter Cube Beam- Splitter Cube Test Wedge

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Photograph of the Set-Up for Conformity Check According to ECE R43

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Camera Image from the Set-Up According to ECE R43

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SLIDE 27

Results for Magnitude of Secondary Image Angle

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SLIDE 28

Results for Direction of Secondary Image Angle

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Summary

1 The secondary image is predominantly linearly polarised. 2 By using a camera with logarithmic sensitivity and linear

polarised illumination the visibility of the secondary image is strongly improved.

3 Automatic real-time evaluation allows objective

measurement of the secondary image angle separation.

4 Evaluation is according to ECE R43.