molecular diffusion in liquids - ksu

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MOLECULAR DIFFUSION IN LIQUIDS For gases, ≠ () For liquid, = () 1. Equimolar Counter Diffusion in Liquids For this case, = − Therefore, the following equation, = − ( ) + ( + ) leads to, = − ( ) +0 = ( 1 2 ) ( 2 1 ) = ( 1 2 ) ( 2 1 ) where, =( ) =( 1 1 + 2 2 )2 2. Diffusion of A through non-diffusing B in liquid phase = ( 2 1 ) 1 2 can be rewritten as,

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Page 1: MOLECULAR DIFFUSION IN LIQUIDS - KSU

MOLECULAR DIFFUSION IN LIQUIDS

For gases, 𝐷𝐴𝐵 ≠ 𝑓(𝑐)

For liquid, 𝐷𝐴𝐵 = 𝑓(𝑐)

1. Equimolar Counter Diffusion in Liquids

For this case,

𝑁𝐴 = −𝑁𝐵

Therefore, the following equation,

𝑁𝐴 = −𝑐𝐷𝐴𝐵

𝑑(𝑥𝐴)

𝑑𝑧+

𝑐𝐴

𝑐(𝑁𝐴 + 𝑁𝐵)

leads to,

𝑁𝐴 = −𝑐𝐷𝐴𝐵

𝑑(𝑥𝐴)

𝑑𝑧+ 0

𝑁𝐴 =𝐷𝐴𝐵𝑐𝑎𝑣(𝑥𝐴1 − 𝑥𝐴2)

(𝑧2 − 𝑧1)=

𝐷𝐴𝐵(𝑐𝐴1 − 𝑐𝐴2)

(𝑧2 − 𝑧1)

where,

𝑐𝑎𝑣 = (𝜌

𝑀)

𝑎𝑣= (

𝜌1

𝑀1+

𝜌2

𝑀2) 2⁄

2. Diffusion of A through non-diffusing B in liquid phase

𝑁𝐴 =𝐷𝐴𝐵

(𝑧2 − 𝑧1)

𝑃

𝑅𝑇

𝑝𝐴1 − 𝑝𝐴2

𝑝𝐵𝑀

can be rewritten as,

Page 2: MOLECULAR DIFFUSION IN LIQUIDS - KSU

𝑁𝐴 =𝐷𝐴𝐵

(𝑧2 − 𝑧1)𝑐𝑎𝑣

𝑥𝐴1 − 𝑥𝐴2

𝑥𝐵𝑀

𝑥𝐵𝑀 =𝑥𝐵2 − 𝑥𝐵1

𝑙𝑛𝑥𝐵2

𝑥𝐵1

For dilute solutions (small concentration of A), 𝑥𝐵𝑀 ≅ 1. Therefore,

𝑁𝐴 =𝐷𝐴𝐵

(𝑧2 − 𝑧1)(𝑐𝐴1 − 𝑐𝐴2)

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Diffusion Coefficients for Liquids

1. Experimental determination of liquid diffusivities

𝐷𝐴𝐵 = 𝑓(𝑐) 𝐷𝐴𝐵 ≠ 𝐷𝐵𝐴

Dilute solution and relatively concentrated solution are placed in chambers on opposite sides of a porous membrane of sintered glass.

Diffusion length = 𝐾1𝛿, 𝐾1 > 1

Another solute with known diffusivity is used to determine the diffusion length. Then,

𝑁𝐴 =휀𝐷𝐴𝐵

𝐾1𝛿(𝑐 − 𝑐′)

휀 is the fraction of the open area for diffusion across the membrane. For V=V’,

ln(𝑐0 − 𝑐0

′ )

(𝑐 − 𝑐′)= (

2휀𝐴

𝐾1𝛿𝑉) 𝐷𝐴𝐵𝑡

where, 𝑐0 is the initial concentration. Another solute (e.g. KCl) with known diffusivity

is used to determine the cell constant (2 𝐴

𝐾1𝛿𝑉)

Page 4: MOLECULAR DIFFUSION IN LIQUIDS - KSU

2. Experimental liquid diffusivity data

Range 0.5 × 10−9– 5 × 10−9 𝑚2

𝑠

Page 5: MOLECULAR DIFFUSION IN LIQUIDS - KSU

3. Prediction of Diffusivities in Liquids

For dilute solutes in liquids (Eq. 6.3-8 in C. J. Geankoplis):

𝐷𝐴𝐵 = 9.96 × 10−16

𝑉𝐴1 3⁄

(𝑇) (1

𝜇)

where, A is solute molecule present in low concentration in solvent B, 𝐷𝐴𝐵is the

diffusivity (m2/s), T is the absolute temperature (K), 𝜇 is the viscosity (Pa·s or

kg/(m·s) ) and VA is the solute molar volume at its normal boiling point

(𝑚3 𝑘𝑔 𝑚𝑜𝑙⁄ ). This equation give good predictions for very large un-hydrated and

spherical-like solute molecules of molecular weight more than 1000 or where VA>

0.5 𝑚3 𝑘𝑔 𝑚𝑜𝑙⁄ in aqueous solution.

For smaller solute molar volume, the Wilke-Chang correlation can be used (Eq. 6.3-

9 in C. J. Geankoplis):

𝐷𝐴𝐵 = 1.173 × 10−16(𝜑𝑀𝐵)1 2⁄ (𝑇

𝜇𝐵𝑉𝐴0.6)

where, A is solute molecule present in low concentration

in solvent B, 𝐷𝐴𝐵is the diffusivity (m2/s), T is the absolute

temperature (K), 𝜇 is the viscosity (Pa·s or kg/(m·s) ) and

VA (see Table 6.3-2) is the solute molar volume at its

normal boiling point (𝑚3 𝑘𝑔 𝑚𝑜𝑙⁄ ). 𝜑 is an association

parameter of the solvent.

Solvent 𝝋

Water 2.6

Methanol 1.9

Ethanol 1.5

Benzene 1.0

Ether 1.0

Heptane 1.0

Unassociated 1.0

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