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Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

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Page 1: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Properties of cell walls prepared using supercritical fluids

Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Page 2: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Presentation overview:

•Wood cell wallspolymerswater

•Fibre-saturation point

•Supercritical CO2

•Water extraction

•Wood material properties

•Summary

Page 3: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Structure of wood cell wall

H2O ?

Page 4: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Fibre-saturation point

Stamm et al, 1935-1971: cell water as gas, liquid, ‘solid solution’ phases

Cells from green wood –full lumens & fully-water-swollencell walls – xylem sap

FSP –empty lumens & fully-water-swollencell walls

-a chemical phenomenon at molecular/supramolecular scales

•FSP- independent of scale –log/fibres•Discrete water binding sites - OH•Exothermic wood cell wall hydration – a molecular chemical interaction

Page 5: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Partial specific volume of water at %mc below FSP

Stamm & Seborg, 1935; Stamm, 1967

‘Compression’ of water molecules at binding sites

200 bar

1000 bar

Page 6: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Wood material dynamics

Wood at variable moisture content – dimensional, conformational & MoE change

Water an integral part of the cell wall supramolecular cellulose-hemicellulose-lignin nanocomposite dynamics-

- ‘Velcro’ mechanics

Where is water located and how structured?

Difficulty in preparing wood specimens for study of FSP &material dynamics – heating, solvents, azeotropes, critical-point, high-pressure

Page 7: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Supercritical CO2 water extraction

Theory: Physical-chemical interaction of cell water and carbon dioxide according to Henry’s Law, the Le Chatelier Principle and the Phase Rule.

Variables:P, T, phase (gas, liquid, supercritical)

[CO2] P, 1/T

CO2 + H2O H2CO3 H+ + HCO3- H+ + CO3

2-

F = C – P + 2

Page 8: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

The reactant’s properties

80.36 ε0 at 20 °C

40.68

108.9

1.85

Rel static permittivity

Dipole moment D

Enthalpy evap kJ/mol

Entropy evap J/(mol·K)

1.60 ε0 at 0 °C, 50 B

0

15.33 at –57.5°C

70.8

Page 9: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Supercritical Fluids

Phase-changedriving chemicalchange

Page 10: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Supercritical CO2 wood dewatering

Fibre SaturationPoint

Comparison of oven-dried (105C) and

SCCO2 dewatered radiata pine wood

Page 11: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Dewatering & air-drying

0

50

100

150

200

250

1 3 5 7 9 11 13 15 17 19 21 23 25

y = -33.837x + 233.2

y = -1.4143x + 36.781

FSP=28%

Dewatering & drying sequence

Wo

od

sp

ecim

en m

c (%

)

SCCO2 chemi-mechanical dewatering

Diffusion-evaporation drying

Page 12: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Practical specimen preparation

Wo

od

sp

ecim

en m

c (%

)

Preparation time (min)

0

50

100

150

200

250

0 2 4 6 8 10 12

5 SCCO2 – gaseous CO2 sequences

Page 13: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

1H NMR imaging of SCCO2 dewatering

Page 14: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Cycle

105% 96% 94% 91% 91% mean0 168% 216% 221% 231% 223% 159%

192% 199% 207% 218% 208%165% 173% 167% 172% 123%116% 117% 117% 123% 144%

107% 146% 151% 161% 165% mean1 103% 101% 99% 91% 89% 142%

155% 167% 165% 162% 157%185% 200% 207% 209% 199%105% 116% 113% 103% 94%

91% 96% 94% 86% 83% mean2 143% 151% 157% 152% 138% 113%

82% 86% 103% 122% 84%161% 111% 75% 73% 89%124% 142% 141% 131% 105%

44% 43% 43% 43% 48% mean3 69% 72% 75% 81% 70% 59%

72% 81% 91% 95% 76%46% 50% 52% 54% 48%43% 42% 43% 44% 49%

45% 38% 36% 40% 46% mean4 50% 46% 37% 36% 38% 43%

44% 53% 56% 40% 38%39% 39% 47% 54% 48%45% 38% 38% 40% 46%

39% 39% 39% 39% 41% mean5 43% 41% 40% 40% 42% 40%

41% 45% 43% 40% 41%37% 37% 36% 37% 37%39% 39% 38% 38% 40%

SCCO2 dewatering

Preparation of woodspecimen with uniform mc distributionapproaching FSP

Re-wetting?

Further drying?

15968

402

Page 15: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Solid State 13C NMR Spectrum

O

HO

HO

OH

OH

OH

C1

C2

C3

C4

C5

C6

Pinus radiata wood at 12% mc

180 160 140 120 100 80 60 40 20 ppm

acetyl acetyl

methoxylignin

C1c

C1h

C4i/sC6i/s

C3,5

C2

Cellulose LigninHemicellulose

Page 16: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

T1(H) Nutation-Diffusion NMR

Lignin

Cellulose

Hemicellulose

Lignin

T1

(H)

(ms)

Page 17: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Water in cell wall at FSP

NMR evidence of a water layer between the cellulose aggregate -phase and the matrix

in the supramolecular nanocomposite of green wood.

Stamm’s ‘solid-solution’ ?Cellulose

Hemicellulose

Lignin

Water layer

Page 18: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

SCCO2 dewatering process - summary

Reaction of lumen water with SCCO2

with reversal of chemistry in gas phase

Bound water bond strength higher than enthalpy of SCCO2 reaction – no change

Wood material derived approaching FSP from green

Material suitable for wood-water dynamics & cell wall studies – Green to FSP & below

Page 19: Properties of cell walls prepared using supercritical fluids Paul Callaghan (VUW), Robert Franich, Stefan J. Hill, and Roger Newman (Scion)

Acknowledgements

Hank Kroese, Suzanne Gallagher,

Bernard Dawson & Meeta Patel

FRST – ‘Wood Products for the Future’

Contract C04X0205