PAPERmaking! Vol8 Nr2 2022

Polymers 2021 , 13 , 2485

14of 16

of the different components are (assuming bulk phase dominates the volume for both components when the moisture content is high).

M i ρ i

(A3)

V i =

For cellulose, we obtain the volume

( 1 − c l ) M f ρ c

(A4)

V c =

where M f is dry fibre mass and ρ c is cellulose density. The water mass in terms of moisture content mc and dry fibre mass M f becomes

mcM f 100 − mc

(A5)

M w =

leading to the water volume

mcM f ( 100 − mc ) ρ W

(A6)

V w =

where ρ w is water density. The total volume of the water-cellulose gel can be approximated as V T ≈ V c + V w =  1 − c l ρ c + mc ( 100 − mc ) ρ w  M f = ( 1 − c l )( 100 − mc ) ρ w + mc ρ c ρ c ( 100 − mc ) ρ w M f (A7) Thus, we can write volume fractions as

V w V T ≈ V c V T ≈

mc ρ c ( 1 − c l )( 100 − mc ) ρ w + mc ρ c ( 1 − c l )( 100 − mc ) ρ w ( 1 − c l )( 100 − mc ) ρ w + mc ρ c

(A8)

φ w =

(A9)

φ c =

In Figure A1 we show the behaviour of vapour pressure for varied temperatures and solids contents. The used values of the parameters are presented in Table A1.

( a ) ( b ) FigureA1. ( a ) Vapour pressure as a function of temperature for three different levels of solids content, 90%, 70%, and 50%. ( b ) Vapour pressure as a function of solids content for three different temperature levels, 20 ◦ C, 190 ◦ C, and270 ◦ C.

Made with FlippingBook - Online magazine maker