Transmission Efficiency of plastic Films Part 1
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TRANSMISSION EFFICIENCY OF PLASTIC FILMS<br />
dependent on the equilibrium relative humidity <strong>of</strong> the base film (35%), the relative<br />
humidity <strong>of</strong> the dry side (10%) and the water vapour transmission rate <strong>of</strong> the barrier<br />
layer separating them. After some time, the base film reaches equilibrium and the<br />
water vapour moving from the 100% relative humidity side equals that arriving on the<br />
dry side. As the two barrier materials are identical and have a much lower<br />
transmission rate than the base film, this will reach equilibrium at a relative humidity<br />
about midway between the wet and dry conditions, i.e. 55%. Under these conditions<br />
the transmission <strong>of</strong> water vapour will have increased above that in the initial<br />
conditions because the vapour pressure difference is due to a relative humidity<br />
differential <strong>of</strong> 45% (= 55% — 10%), compared with the initial value <strong>of</strong> 25% (= 35% —<br />
10%). The transmission rate will, therefore, rise by a factor <strong>of</strong> about 1.8.<br />
Similarly, a specimen where the base film is initially in equilibrium with a relative<br />
humidity greater than the final value will have a high apparent water transmission rate<br />
initially, and this will fall as the specimen approaches equilibrium. Hence, although<br />
rapid test instruments can measure transmission rates in a short time, the results<br />
may differ significantly from those obtained after dynamic equilibrium has been<br />
reached within the test cell. With non hygroscopic arrivers results agreeing closely<br />
with the dish method can be obtained.<br />
2. GAS PERMEABILITY<br />
Measurement <strong>of</strong> gas permeability is carried out under controlled conditions <strong>of</strong><br />
pressure, as well as <strong>of</strong> temperature and relative humidity. In essence the usual tests<br />
consist in making a partition between a test cell and an evacuated manometer.)The<br />
pressure across the film is usually one atmosphere. As the gas passes through the<br />
film sample the mercury in the capillary leg <strong>of</strong> the manometer is depressed. After a<br />
constant transmission rate is achieved, a plot <strong>of</strong> mercury height against time gives a<br />
straight line. The slope <strong>of</strong> this line can be used to calculate the gas transmission. Gas<br />
permeability measurements are described in ASTM D. 1434 and BS.2782: <strong>Part</strong> 5:<br />
1970.<br />
The foregoing method is known as the pressure increase method. Another common<br />
method is that <strong>of</strong> concentration increase. Two gases are used, a reference gas and<br />
the test gas. A partial pressure difference across the barrier material with respect to<br />
the test gas is created, without a difference in total pressure. Because the method <strong>of</strong><br />
measuring the concentration <strong>of</strong> the test gas can be specific 10 that gas even in the<br />
presence <strong>of</strong> other gases or vapors, equipment can be developed in which the relative<br />
humidity <strong>of</strong> both the test and the reference gases can be controlled. This is not<br />
possible where equipment has to be evacuated and is very important when<br />
Determinations are carried out on barrier materials having a hygroscopic base.<br />
Various methods <strong>of</strong> measuring the concentration change are used, including<br />
chemical analysis, gas chromatography and radioactive tracer techniques.<br />
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