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LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak and J Horak: CIE Conference Vienna, 2010

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Page 1: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

LED photobiology János Schanda

University of Pannonia

Virtual Environment and Imaging Technologies Laboratory

based on the paper by

W. Halbbritter, W Horak and J Horak:

CIE Conference Vienna, 2010

Page 2: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Overview

Introduction Optical radiation

LED emission spectra Human eye transmission

Optical hazards

Conclusions and summary

Page 3: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Optical radiaton - photobiology

UltraViolet radiation: actinic radiation UV-A: 315 m – 400 nm UV-B: 280 nm – 315 nm UV-C: 100 nm – 280 nm

Visible radiation: 380 nm – 780 nm Infrared radiation

IR-A: 780 nm – 1400 nm IR-B: 1.4 mm – 3 mm IR-C: 3 mm – 1 mm

Page 4: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

LED emission LEDs now available from 245 nm Visible wavelengths + white Near infrared – optical communication LED spectrum bandwidth: 20 nm – 40 nm

Page 5: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Penetration of UV radiation into the eye

After Sliney DH, Wolbarsht ML. Safety with Lasers and Other Optical Sources. (New York: Plenum Publishing Corp); 1980.

Page 6: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Ocular hazards

Photokeratitis, photo-conjuntivitis Redening of the

eye, disapers within 24 – 48 hours

Page 7: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Optical hazards

Chemical – biochemical hazards Photon energy in the range of energy of

chemical bonds Skin damages Ocular damages

Thermal hazards Skin damages Ocular damages

Page 8: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Eye hazard spectra after CIE TC 6-55 draft report

Page 9: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Lamp risk cathegories- acceptance angles

exempt low risk moderate risk

Unit

Blue light 0.1 0.011 0.0017 rad

Thermal 0.011 0.011 0.0017 rad

Thermal weak visual stimulus

0.011 0.011 0.011 rad

Eye movement, time dependent smear effect takeninto consideration

Page 10: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Lamp safety measurement conditionsof

Measurement distance: Minimum viewing distance: 200 mm GSL lamps: 500 mm

Measurement aperture: Maximum human pupil size: 7 mm Source size and angular subtense:

Thermal retinal hazard depends on irradiated surface (heat flow)

380nm-1400nm: eye focuses- minimum angular subtense: amin=1.7mrad

Maximal angular subtense: amax=100mrad

Page 11: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

„Physiological” radiance/irradiance and time

average Radiance weighted according tothe action

spectum of the given hazard Thermal effects: important the heat conduction of

the tissue away from the irradiation site, the irradiated tissue volume and the irradiance – local burn. Size of irradiation importan!, irradiance

dependent, W/m2. Photochemical effects: strong wavelength

dependence, follows Bunsen-Roscow law. Radiant exposure, J/m2, dependence.

Page 12: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Ocular hazards Radiation between 380 nm and 1400 nm reaches the retina.

Light source focused on retina Retinal irradiance: Er = p Ls t de

2/(4f 2)

where: Er: retinal irradiance L s: source radiance f: : effective focal length of eye De : pupil diameter : t transmittance of ocular media

A worst-case assumption is: Er= 0.12 L s

This linear dependence of retinal irradiance of source radiance breaks down for small sources, lasers.

Thus retinal safety limits for 300/380 nm – 1400 nm are given in W/m2 or J/m2

Page 13: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Lamp safety regulation measurements

Physiological (time integrated) radiance:Radiant power passing through a defined aperture stop (pupil) at a defined distance Aperture area defines solid collection angle W (sr) and

measurement area: field of view:FOV (m2), measured by the acceptance angle: g

Page 14: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Time dependence of acceptance angle to be

used Due to eye movents for short durations small acceptance angles have to be chosen FOV can be over- or under-filled

Page 15: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Product safety standard conditions Measurement distance

200 mm meas.distance (GSLs: 500 lx distance) Measurement aperture: maximum pupil size, 7 mm

diameter Source size & angular subtense

Thermal hazard source image size dependent:a = 2 arctan(apparent source size/2 sourcedistance)a But amin=1.7mrad, amax=100 mrada Apparent source position

Page 16: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Product safety issues CIE S 009/IEC 62471: Photobiological Safety of Lamps and

Lamp Systems Lamp and lamp system manufacturer requirements

If applicable FOV<source area (overfilled)-> ->LED radiance data hold for luminaire

If underfilled, multiple small sources can fall into the FOV area and averaged radiance will sum up!

For such applications the tru weighted radiance of the source is needed, acceptance angle should not be smallerthan 1.7 mrad.

But LED assembieswith beam shapingoptics have tobe measured according to the standard.

P-LEDs(and blue LEDs) might exceed the low-risk group

Page 17: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Example: p-LED, individual LED

Page 18: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

LED-lamp based on LED component evaluation

Page 19: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

CIE S009/IEC62471 requirements, 1

Page 20: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

CIE S009/IEC62471 requirements, 2

Page 21: LED photobiology János Schanda University of Pannonia Virtual Environment and Imaging Technologies Laboratory based on the paper by W. Halbbritter, W Horak

Thanks for your kind attention!