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Laboratory Glass-Working for Scientists - Sciencemadness Dot Org

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©ENERAL PHYSICAL PROPERTIES OF GLASS<br />

Transmission of Light<br />

A 1-mm thick sheet of Phoenix glass will transmit 90 per cent or more<br />

Of the light incident on it, <strong>for</strong> wavelengths of 350 millimicrons to<br />

Almost 2 microns. In the infra-red region a strong absorption occurs<br />

at 3 microns and little transmission beyond 4 microns. In the ultraviolet<br />

region increasing absorption occurs as the wavelength falls<br />

below 350 millimicrons and very little transmission occurs below 270<br />

millimicrons. The transparent variety of vitreous silica (fused quartz)<br />

has very superior optical properties, and is widely used in photochemical<br />

and optical researches. In the ultra-violet region it transmits<br />

at high efficiency down to 1850 Angstrom units (185 millimicrons).<br />

'Quality O.H. VitreosiV of The Thermal Syndicate Ltd is<br />

A special optical quality in which the absorption band at 2400<br />

Angstrdrns has been eliminated. A special quality of fused quartz is<br />

also available which transmits infra-red up to 3*5 microns approximately<br />

('I.R. quality VitreosiV of The Thermal Syndicate Ltd). In this<br />

Vitreosil the absorption band at 2*7 microns has been much reduced.<br />

The Stress-Optical Coefficient<br />

It IS not usual to take quantitative measurements of the strain in glass<br />

apparatus made <strong>for</strong> research; when a strain-viewer is used (p. 43)<br />

qualitative observations are normally made. Quantitative measure-<br />

Kits can be made when the stress-optical coefficient is known. The<br />

M -- i<br />

j^'t<br />

involved requires a knowledge of the optical behaviour of<br />

doubly refracting materials and depends on the fact that a ray of<br />

p!ane»polarized light entering strained glass is broken into two rays—<br />

the 'ordinary ray' and the 'extraordinary ray'—vibrating at right<br />

•llgles to each other. For glass subject to simple axial tension or<br />

Compression, the extraordinary ray vibrates in the plane which<br />

includes the axis of the stress. The birefringence of strained glass is<br />

proportional to the strain, and thus to the stress. The stress-optical<br />

OOefficient is the maximum double refraction or birefringence obgerved<br />

in polarized sodium light <strong>for</strong> 1 cm path length when there is a<br />

Uni<strong>for</strong>m stress of 1 kg/cm 2 . It is expressed either in wavelengths of<br />

•Odium light or in millimicrons. This coefficient varies from one<br />

glass to another; it is around 3*5 millimicrons, or 0*006 wavelengths<br />

of sodium light A. JOHANNSEN (1918) has given an account of<br />

methods <strong>for</strong> determining double refraction, and very valuable data<br />

<strong>for</strong> practical work are given by J. H. PARTRIDGE (1949).<br />

Resistance to Chemical Actions<br />

General Chemical Properties of <strong>Glass</strong><br />

Vittoous silica is the most chemically inert glass <strong>for</strong> most purposes.<br />

15

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