Transmission Efficiency of plastic Films Part 1
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TRANSMISSION EFFICIENCY OF PLASTIC FILMS<br />
1.98 m (78 in) and the lens is placed midway between them. When a test sample <strong>of</strong><br />
film is placed behind the lens, as shown, only light which is transmitted by the film<br />
with a deviation <strong>of</strong> less than 4 mm will enter the photocell. The photocell reading,<br />
expressed as a percentage <strong>of</strong> the intensity <strong>of</strong> the incident beam, is the ‘see-through’<br />
clarity. This figure is, <strong>of</strong> course, a measure not only <strong>of</strong> the distortion but also <strong>of</strong> the<br />
light transmission, and the see-through’ clarity and the light transmission (determined<br />
as in the previous paragraph) must be compared in order to assess the effect <strong>of</strong><br />
deviation alone.<br />
3. HAZE:<br />
Haze can be taken as a measure <strong>of</strong> the ‘silkiness’ <strong>of</strong> the film and is usually <strong>of</strong> greater<br />
importance than ‘see-through’ clarity in the case <strong>of</strong> packaging films since these are<br />
usually closer to the contents <strong>of</strong> the pack. One cause <strong>of</strong> haze is surface imperfections<br />
<strong>of</strong> the film so that the amount <strong>of</strong> haze is not necessarily proportional to film thickness<br />
the appearance <strong>of</strong> haze is caused by light being scattered by the face imperfections<br />
or by in homogeneities in the film. These latter can be caused by voids, large<br />
crystallites, incompletely dissolved additives or cross-linked material.<br />
PHYSICAL AND CHEMICAL PROPERTIES<br />
Haze is measured by a technique specified in ASTM D1003 and in BS.2782: <strong>Part</strong> 5:<br />
1970. It is defined in these standards as the percentage <strong>of</strong> transmitted light which, in<br />
passing through a specimen, deviates by more than 24° on average, from an incident<br />
parallel beam by forward scattering from both surfaces, and from within the<br />
specimen.<br />
A beam <strong>of</strong> light is passed through the film sample and on to the highly reflecting<br />
internal surface <strong>of</strong> an integrating sphere in such a manner that all the transmitted light<br />
is collected into a photo electric cell. Next, the sphere is moved through a small angle<br />
so that the path <strong>of</strong> the light beam now falls on an extension <strong>of</strong> the sphere comprising<br />
a matt black surface that absorbs the entire light transmitted straight forward along<br />
the path <strong>of</strong> the beam. Any light that is appreciably scattered in a forward direction is<br />
still gathered by the highly reflective internal surface <strong>of</strong> the sphere and into the<br />
photocell. The ratio <strong>of</strong> the second photocell reading to the first is a measure <strong>of</strong> the<br />
haze. The apparatus for tile measurement <strong>of</strong> haze is shown diagrammatically in<br />
Figure.<br />
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