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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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160 Christian Wohlfarth<br />

There is a broad variety <strong>of</strong> experimental equipment that is based on this procedure (see<br />

below). This isopiestic technique is the recommended method for most polymer solutions<br />

since it is advantageous in nearly all aspects <strong>of</strong> measurement: It covers the broadest concentration<br />

range. Only very small amounts <strong>of</strong> polymer are needed (about 30-50 mg with the<br />

classical quartz spring balance, about 100 μg with piezoelectric sorption detector or<br />

microbalance techniques - see below). It is much more rapid than all other methods explained<br />

above, because equilibrium time decreases drastically with such small amounts <strong>of</strong><br />

polymer and polymer solution (about 12-24 hours for the quartz spring balance, about 3-4<br />

hours for piezoelectric or microbalance techniques). The complete isotherm can be measured<br />

using a single loading <strong>of</strong> the apparatus. Equilibrium is easier to obtain since comparatively<br />

small amounts <strong>of</strong> solvent have to diffuse into the bulk sample solution. Equilibrium<br />

can better be tested by measuring sorption and desorption runs which must lead to equal results<br />

for thermodynamic absorption equilibrium. Supercritical solvents can be investigated<br />

if the piezoelectric detector is used (otherwise buoyancy in dense fluids may cause serious<br />

problems). Much broader pressure and temperature ranges can be covered with relatively<br />

simple equipment, what may again be limited by the weighing system. Isopiestic sorption<br />

measurements can be automated and will allow also kinetic experiments. There are two disadvantages:<br />

First, isopiestic sorption measurements below about 30 wt% polymer are subject<br />

to increasing error because very small temperature differences (vapor pressure<br />

changes) are connected with large changes in concentration. Second, problems may arise<br />

with precise thermostating <strong>of</strong> both the solvent and the solution at different constant temperatures<br />

over a longer period <strong>of</strong> time.<br />

Because <strong>of</strong> their importance, several technical solutions will now be presented in<br />

some detail. The classical concept is the sorption method using a quartz spring balance.<br />

Refs. 81-90 provide some examples, where the concentration (mass) <strong>of</strong> the solution is measured<br />

by the extension <strong>of</strong> the quartz spring according to Hook’s law (linear relationship, no<br />

hysteresis). It was not originally developed for polymer solutions but for gas-solid adsorption<br />

measurements by McBain. 91 The principle was introduced into the investigation <strong>of</strong><br />

polymer solutions by van der Waals and Hermans 84 and became popular after the work <strong>of</strong><br />

Bonner and Prausnitz. 85 In this method, a weighed quantity <strong>of</strong> the (non-volatile) polymer is<br />

placed on the pan <strong>of</strong> the quartz spring balance within a measuring cell. The determination <strong>of</strong><br />

spring extension vs. mass has to be made in advance as a calibration procedure. Reading <strong>of</strong><br />

the spring extension is usually made by means <strong>of</strong> a cathetometer. The cell is sealed, evacuated<br />

and thermostated to the measuring temperature (T 2), and the solvent is then introduced<br />

into the measuring cell as solvent vapor. The solvent vapor is absorbed by the polymer sample<br />

to form the polymer solution until thermodynamic equilibrium is reached. The solvent<br />

vapor is provided from a reservoir either <strong>of</strong> pure liquid solvent thermostated at a lower temperature<br />

(T 1) or <strong>of</strong> a reference liquid solution <strong>of</strong> known concentration/solvent partial pressure<br />

like in the case <strong>of</strong> the isothermal distillation procedure as described above. A compact<br />

version <strong>of</strong> such an apparatus was developed by Illig 82 and widely used within the author’s<br />

own work (see Appendix 4.4A for the corresponding references). Figure 4.4.7a shows the<br />

details <strong>of</strong> the equilibrium cell, which has a vacuum double-walled jacket.<br />

The following problems have to be solved during the experiment: The equilibrium cell<br />

has to be sealed carefully to avoid any air leakage over the complete duration <strong>of</strong> the measurements<br />

(to measure one isotherm lasts about 14 days). Specially developed thin Teflon<br />

sealing rings were preferred to grease. The polymer sample has to withstand the tempera-

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