Lynne Wong's PhD thesis
Lynne Wong's PhD thesis Lynne Wong's PhD thesis
Table 6.4. The GAB model maximum net isosteric heat of sorption, q st , and entropy of sorption, S d , and the corresponding EMC/% db for the nine cane components aged 52 and 36 weeks. Sample Maximum q st/kJ mol -1 Maximum S d/kJ mol -1 52 weeks EMC/% db 36 weeks EMC/% db 52 weeks EMC/% db 36 weeks EMC/% db Stalk fibre 27.27 3 40.88 0 -69.77 3 -93.87 1 Stalk pith 130.77 0.01 14.08 5 -363.07 1 -33.51 5 Rind fibre 31.30 3 64.28 0.1 -83.93 3 -173.40 2 Rind fines 15.89 4 20.92 2 -38.49 4 -46.95 3 Top fibre 40.81 3 25.17 4 -109.80 4 -66.96 4 Dry leaf fibre 43.24 3 64.82 2 -117.87 3 -182.59 2 Dry leaf fines 23.59 5 41.95 0.01 -63.55 5 -98.93 2 Green leaf fibre 9.75 5 53.92 2 -22.97 6 -146.76 2 Green leaf fines 24.70 3 49.67 2 .62.47 4 -136.16 3 6.6 ENTHALPY-ENTROPY COMPENSATION A promising theory that has been widely considered to investigate the physical and chemical phenomena involved in water sorption (Aguerre et al., 1986, Madamba et al., 1996) is the enthalpy-entropy compensation theory, or isokinetic relationship, as originally applied by Bell (1937). This theory states that compensation arises from changes in the nature of the interaction between the solute and the solvent causing the reaction, and that the relationship between enthalpy and entropy for a specific reaction is linear. When this theory is applied to a sorption process, the enthalpy corresponds to the net isosteric heat of sorption. For a linear enthalpy and entropy relation, the isokinetic temperature (T β ) can be determined from the slope of the line and, if the theory is valid, should be constant at any point (Heyrovsky, 1970). It represents the temperature at which all the reactions in the series proceed at the same rate (Heyrovsky, 1970), and the free energy at T β , ΔG, provides a criterion to evaluate whether the water sorption is a spontaneous (-ΔG) or a nonspontaneous process (+ΔG). To test the validity of the compensation theory, the isokinetic temperature is compared with the harmonic mean temperature (T hm ), and T β ≠ T hm . T hm is defined as: T hm = ni ∑ = n i i 1 1/ T where n i is the total number of isotherms and, T is the Kelvin temperature (K). 257
Moreover, if T β > T hm the process is enthalpy-driven, and if T β < T hm , the process is considered to be entropy-controlled (Telis et al., 2000). If the net isosteric heat of sorption q st is plotted as ordinate against the entropy of sorption S d as abscissa, the slope of the plot gives the isokinetic temperature T β and the intercept gives the free energy ΔG at the isokinetic temperature. The harmonic mean temperature for this study can be calculated to be 320.23 K, since the isotherm was investigated at four different temperatures of 30, 45, 55 and 60 °C. 4 T hm = − 1 − 1 − 1 − 1 (303.15) + (318.15) + (328.15) + (333.15) = 320.23 K The plots of the net heat of sorption q st (kJ mol -1 ) against the entropy of sorption S d (kJ mol - 1 K -1 ) for the nine cane components of R 570 aged 52 and 36 weeks are shown in Fig 6.10, the coefficient of determination R 2 , the slope and the intercept for the enthalpy-entropy relationship are shown in Table 6.5. The slope corresponds to the isokinetic temperature T β, and the intercept, ΔG. It can be seen from Table 6.5 that T β for all cane components aged 52 and 36 weeks is greater than the harmonic mean temperature T hm of 320.23 K except in the case of stalk pith aged 36 weeks, hence, all processes except stalk pith aged 36 weeks are enthalpycontrolled. Hence the driving force for the adsorption of moisture on these fibres is the strength of binding of water molecules to the surface of the fibre. The positive sign of ΔG (except for the case of rind fines aged 36 weeks) indicates that the water sorption process in the cane components is non-spontaneous, and that the enthalpy-entropy compensation theory was satisfied. Beristain et al. (1996) applied the enthalpy-entropy compensation theory to water adsorption in starchy materials. Two isokinetic temperatures were observed, suggesting that during the initial stages (at low water activity) the isotherm process was entropycontrolled, whereas in the later stage, the process was controlled by changes in the enthalpy of water. They also reported a spontaneous sorption isotherm for starch materials. 258
- Page 259 and 260: 30 o C isotherm 45 o C isotherm 55
- Page 261 and 262: 4 0 Stalk fibre 5 0 Stalk pith 5 0
- Page 263 and 264: 5.6.4.4 Fitting of sorption models
- Page 265 and 266: Table 5.19. Parameters of the sorpt
- Page 267 and 268: Table 5.21. Parameters of the sorpt
- Page 269 and 270: Table 5.23. Parameters of the sorpt
- Page 271 and 272: Table 5.25. Parameters of the sorpt
- Page 273 and 274: Table 5.27. Parameters of the sorpt
- Page 275 and 276: Modified GAB Kuhn Iglesias - Chirif
- Page 277 and 278: Table 5.28. Classification of resid
- Page 279 and 280: Stalk fibre Stalk pith Rind fibre 4
- Page 281 and 282: 5.6.4.5 Calculated EMC values of re
- Page 283 and 284: Table 5.30. Calculated equilibrium
- Page 285 and 286: m/m of 96% Table 5.32. Calculated e
- Page 287 and 288: Table 5.33. Parameters of the Hailw
- Page 289 and 290: CHAPTER 6. PROPERTIES OF THE SORBED
- Page 291 and 292: where m is the equilibrium moisture
- Page 293 and 294: Stalk fibre Stalk pith Rind fibre 8
- Page 295 and 296: Stalk fibre Stalk pith Rind fibre 4
- Page 297 and 298: 6.2 THE NUMBER OF ADSORBED MONOLAYE
- Page 299 and 300: 6.3 TOTAL SOLID SURFACE AREA AVAILA
- Page 301 and 302: Thus, for each cane component of ea
- Page 303 and 304: abscissa. For each moisture level (
- Page 305 and 306: Stalk fibre Stalk pith Rind fibre 1
- Page 307 and 308: A similar procedure was followed to
- Page 309: 10 0 Stalk fibre Stalk pith Rind fi
- Page 313 and 314: Table 6.5. Characteristic parameter
- Page 315 and 316: Binding energy/kJ (kg mol) -1 2 0 0
- Page 317 and 318: 6.8 CALCULATION OF BOUND WATER AND
- Page 319 and 320: The values of K 1 , K 2 and W were
- Page 321 and 322: Table 6.7. Separation of the total
- Page 323 and 324: Table 6.7. (Contd.) Sample 30 o C 4
- Page 325 and 326: 3 0 S talk fibre 4 0 Stalk pith 3 0
- Page 327 and 328: 3 0 Reconstituted cane at 30 o C 3
- Page 329 and 330: when water is added to dry wood, wh
- Page 331 and 332: It is evident that in some cases ma
- Page 333 and 334: The number of adsorbed monolayers,
- Page 335 and 336: Data in Tables 2.9 and 2.11 show th
- Page 337 and 338: particular fibre is systematically
- Page 339 and 340: Anon. (1985b). Laboratory manual fo
- Page 341 and 342: Blanchi R.H. and A.G. Keller (1952)
- Page 343 and 344: Day D.L. and G.L. Nelson (1965). De
- Page 345 and 346: Heyrovsky J. (1970). Determination
- Page 347 and 348: Kuhn I.J. (1964). A new theoretical
- Page 349 and 350: Madamba P.S., R.H. Driscoll and K.A
- Page 351 and 352: Prinsen Geerligs, H.C. (1897). Stud
- Page 353 and 354: Sing K.S.W., D.H. Everett, R.A.W. H
- Page 355 and 356: Van der Pol C., C.M. Young and K. D
Moreover, if T β > T hm the process is enthalpy-driven, and if T β < T hm , the process is<br />
considered to be entropy-controlled (Telis et al., 2000).<br />
If the net isosteric heat of sorption q st is plotted as ordinate against the entropy of sorption<br />
S d as abscissa, the slope of the plot gives the isokinetic temperature T β and the intercept<br />
gives the free energy ΔG at the isokinetic temperature. The harmonic mean temperature<br />
for this study can be calculated to be 320.23 K, since the isotherm was investigated at four<br />
different temperatures of 30, 45, 55 and 60 °C.<br />
4<br />
T hm = − 1<br />
− 1<br />
− 1<br />
− 1<br />
(303.15) + (318.15) + (328.15) + (333.15)<br />
= 320.23 K<br />
The plots of the net heat of sorption q st (kJ mol -1 ) against the entropy of sorption S d (kJ mol -<br />
1<br />
K -1 ) for the nine cane components of R 570 aged 52 and 36 weeks are shown in Fig 6.10,<br />
the coefficient of determination R 2 , the slope and the intercept for the enthalpy-entropy<br />
relationship are shown in Table 6.5. The slope corresponds to the isokinetic temperature T<br />
β, and the intercept, ΔG.<br />
It can be seen from Table 6.5 that T β for all cane components aged 52 and 36 weeks is<br />
greater than the harmonic mean temperature T hm of 320.23 K except in the case of stalk<br />
pith aged 36 weeks, hence, all processes except stalk pith aged 36 weeks are enthalpycontrolled.<br />
Hence the driving force for the adsorption of moisture on these fibres is the<br />
strength of binding of water molecules to the surface of the fibre. The positive sign of ΔG<br />
(except for the case of rind fines aged 36 weeks) indicates that the water sorption process<br />
in the cane components is non-spontaneous, and that the enthalpy-entropy compensation<br />
theory was satisfied.<br />
Beristain et al. (1996) applied the enthalpy-entropy compensation theory to water<br />
adsorption in starchy materials. Two isokinetic temperatures were observed, suggesting<br />
that during the initial stages (at low water activity) the isotherm process was entropycontrolled,<br />
whereas in the later stage, the process was controlled by changes in the<br />
enthalpy of water. They also reported a spontaneous sorption isotherm for starch<br />
materials.<br />
258