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Lynne Wong's PhD thesis

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50<br />

40<br />

30<br />

20<br />

% adsorbed water/dry fibre<br />

10<br />

8<br />

6<br />

5<br />

4<br />

3<br />

2<br />

5 6 8 10 20 40 60 80 100<br />

Water vapour pressure/mm Hg<br />

Figure 5.2. Adsorption isotherms of cane fibre (Kelly, 1957).<br />

According to Kelly (1957), below the transition point, a primary monolayer adsorption<br />

process represented by the first part of the curve took place, and above the transition point,<br />

a secondary process involving the condensation of moisture on top of the primary adsorbed<br />

layer (multilayer adsorption) represented by the second part of the curve, occurred. For the<br />

isotherms at 27.2 °C and 51 °C, he found a similar slope (1.14) for the isotherms below the<br />

transition point and a similar, but much steeper, slope (5.55) above the transition point.<br />

Based on these similar slopes, he calculated that the heat of adsorption involved in the<br />

primary process to be 43 cal g -1 (i.e. 180 J g -1 ) or 775 cal mol -1 (i.e. 3240 J mol -1 ), and in the<br />

secondary process to be 19 cal g -1 (i.e. 80 J g -1 ) or 342 cal mol -1 (i.e. 1430 J mol -1 ).<br />

Kelly concluded that the adsorbed water is firmly attached to the sugar cane fibre, and part<br />

of this water represents the so-called ‘hygroscopic water’ of Behne (1937), which is also<br />

known as Brix-free water.<br />

Foster (1962) conducted vapour sorption experiments on pre-dried cane fibre of variety<br />

Q 50 at 20 °C for 35 – 95% relative humidity. He subsequently extrapolated his results to<br />

100% relative humidity and quoted a value of 25% for Brix-free water.<br />

181

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