Lynne Wong's PhD thesis

Lynne Wong's PhD thesis Lynne Wong's PhD thesis

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5.6.4.2 Kelly’s type of two-equilibria isotherms When the ln of EMC results obtained in Tables 5.8 – 5.16 were plotted against ln of vapour pressure (Table 5.3), as previously described for Kelly’s work (1957) in Section 5.4.1, twoequilibria isotherms were obtained for all nine cane components of R 570 aged 52 weeks (Fig 5.6) and 36 weeks (Fig 5.7). The transition point of the primary and secondary equilibria occurred at ln (EMC/% db) = 2.5, i.e. at EMC/% db = 12.5, compared to the value of 14.5 found by Kelly. The regression coefficient R 2 and the Freundlich constants s and k are compiled for 52 weeks samples (Table 5.17) and for 36 weeks samples (Table 5.18). All the slopes s of the primary equilibria for 30, 45, 55 and 60 °C isotherms are different for all cane components, the same applied to the slopes of the secondary equilibria for 30, 45, 55 and 60 °C isotherms. Therefore, it was not possible to calculate the heat of adsorption involved in the primary and secondary equilibria as did Kelly, since his calculations were based on the identical slope of 1.14 for the primary equilibria of both 27.2 °C and 51 °C isotherms, and 5.55 for their secondary equilibria. When Kelly’s EMC data (1957) were plotted similarly, the gradients of the primary equilibria at 27.2 °C and 51 °C were found respectively: 0.854 and 1.137, and of the secondary equilibria at 27.2 °C and 51 °C were respectively 3.305 and 4.551. 5.6.4.3 Adsorption isotherms The adsorption isotherms for the nine sugar cane component parts aged 52 weeks are shown in Fig 5.8. Typical S-shape curves referred to as type II isotherms were found. According to Van den Berg and Bruin (1981), type II isotherms can be divided into three different regions: in the first region at low water activity, there is monolayer adsorption of water held by strong hydrophilic bonds on polar sites by Van der Waal forces. In the second region, called the multilayer region, water is more loosely held by hydrogen bonds and is under transition to the natural properties of free water. The least firmly bound water occurs when a w is above 0.6. In the third region, the isotherm rises steeply as practically free water becomes mechanically entrapped in the void spaces of the material, mainly as a result of capillary condensation. Water uptake in the first region is normally rapid, slows down in the second region and is accelerated in the third region. The adsorbed water can be classified as monolayer, multilayer or condensed capillary water. The enthalpy of 203

vaporisation generally decreases from the first to the third region. The nine sugar cane components aged 36 weeks also exhibit type II isotherms (Fig 5.9). Stalk fibre Stalk pith Rind fibre 4 4 4 ln(EMC/% db) 3 2 1 3 2 1 3 2 1 0 0 2 4 6 0 0 2 4 6 0 0 2 4 6 Rind fines Top fibre Dry leaf fibre 4 4 4 ln(EMC/% db) 3 2 1 3 2 1 3 2 1 0 0 2 4 6 0 0 2 4 6 0 0 2 4 6 Dry leaf fines Green leaf fibre Green leaf fines 4 4 4 ln(EMC/% db) 3 2 1 3 2 1 3 2 1 0 0 2 4 6 0 0 2 4 6 0 0 2 4 6 ln (water vapour pressure/mm Hg) 30°C 45°C 55°C 60°C Figure 5.6. Adsorption isotherms of nine cane components aged 52 weeks (as per Kelly’s method, 1957). Note the similar behaviour of all the nine cane components. 204

vaporisation generally decreases from the first to the third region. The nine sugar cane<br />

components aged 36 weeks also exhibit type II isotherms (Fig 5.9).<br />

Stalk fibre Stalk pith Rind fibre<br />

4<br />

4<br />

4<br />

ln(EMC/% db)<br />

3<br />

2<br />

1<br />

3<br />

2<br />

1<br />

3<br />

2<br />

1<br />

0<br />

0 2 4 6<br />

0<br />

0 2 4 6<br />

0<br />

0 2 4 6<br />

Rind fines Top fibre Dry leaf fibre<br />

4<br />

4<br />

4<br />

ln(EMC/% db)<br />

3<br />

2<br />

1<br />

3<br />

2<br />

1<br />

3<br />

2<br />

1<br />

0<br />

0 2 4 6<br />

0<br />

0 2 4 6<br />

0<br />

0 2 4 6<br />

Dry leaf fines Green leaf fibre Green leaf fines<br />

4<br />

4<br />

4<br />

ln(EMC/% db)<br />

3<br />

2<br />

1<br />

3<br />

2<br />

1<br />

3<br />

2<br />

1<br />

0<br />

0 2 4 6<br />

0<br />

0 2 4 6<br />

0<br />

0 2 4 6<br />

ln (water vapour pressure/mm Hg)<br />

30°C<br />

45°C<br />

55°C<br />

60°C<br />

Figure 5.6. Adsorption isotherms of nine cane components aged 52 weeks (as per Kelly’s<br />

method, 1957).<br />

Note the similar behaviour of all the nine cane components.<br />

204

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