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TRANSPORT OF IONS IN SOLUTION

Jaslin Ikhsan, Ph.D.

Chemistry Ed. Department State University of Yogyakarta 

Conductivity of electrolyte

solutions

Strong and weak electrolyte

Ion Mobility

Ion mobility and conductivity,

Transport number

(2)

Conductivity of Electrolyte Solution

 Ions in solution can be set in motion by applying a potential difference between two electrodes.

 The conductance (G) of a solution is defined as the inverse of the resistance (R):

 For parallel plate electrodes with area A, it

follows:

G

R

in units of

1

1

,

G

A

L

Where,

: the conductivity,

L : the distance separating the plates Units:

G → S (siemens) R →

(3)

Conductivity of Electrolyte Solution

 The conductivity of a solution depends on the number of ions present. Consequently, the molar conductivity m is used

C is molar concentration of electrolyte and unit of Λm is S m2 mol-1

m

C

In real solutions, m depends on the concentration of the electrolyte. This could be due to:

 Ion-ion interactions  γ  1

 The concentration dependence of conductance indicates that there are 2 classes of electrolyte

Strong electrolyte: molar conductivity depends slightly on the molar concentration

(4)

Conductivity of Electrolyte Solution

In real solutions, m depends on the concentration of the electrolyte. This could be due to:

1. Ion-ion interactions  γ  1

2. Incomplete dissociation of electrolyte

strong electrolyte,

weak dependence of m on C

weak electrolyte,

(5)

Strong Electrolyte

 Fully ionized in solution  Kohlrausch’s law

 0

m is the limiting molar conductivity

K is a constant which typically depends on the stoichiometry of the electrolyte

 C1/2 arises from ion-ion interactions as estimated by the

Debye-Hückel theory.

(6)

Strong Electrolyte

Law of the independent migration of ions: limiting molar conductivity can be expressed as a sum of ions contribution

ions migrate independently in the zero concentration limi

0
(7)

Weak Electrolyte

 Not fully ionized in solution

HA aq

H O l

H O

aq

A aq

c

c

c

(

)

( )

(

)

(

)

(

)

  2 3

1

K

a

c

2

1

,

2 2 2 2

0

4

2

2

4

2

c K

K

c

K

K

K

K

K c

c

K

c

K

K c

c

a a

a a

a a a

a a a

K

c

K

c

c

K

K

c

c

K

a a a a a

2

2

1

4

2

1

4

1

1 2 1 2 / / 1 1  

  c

(8)

Weak Electrolyte

 The molar Conductivity (at higher concentrations) can be expressed as:

 At infinite dilution, the weak acid is fully

dissociated (α = 100%)  It can be proven by the

Ostwald dilution law which allows estimating limiting molar conductance:

m

0m

m m m m m m

m m a

m m a m

m m

x

x

c

K

c

K

x

0 0 0 0

0 0 0

1

1

1

1

1

1

1

1

1

1

1

1

0 0 2

(9)

Weak Electrolyte

 The limiting molar conductance:

1

1

0 0 2

m m

m

a m

c

K

(

)

(10)

The Mobility of Ions

 Ion movement in solution is random. However, a migrating flow can be onset upon applying an electric field ,

E

L

 

  is the potential difference between 2 electrodes separated by a distance L

 F accelerates cations to the negatively charged electrode and anions in the opposite direction. Through this motion, ions experience a frictional force in the opposite direction.

Taking the expression derived by Stoke relating friction and the viscosity of the solvent (), it follows:

F zeE ze

L

  

(11)

The Mobility of Ions

 When the accelerating and retarding forces balance each other, s is defined by:

u is mobility of ions, and r is hydrodynamic radius, that might be different from the ionic radius, small ions are more solvated than the bulk ones.

s zeE

r E where

ze r

  

6  ,  6

(12)

The Mobility of Ions and Conductivity

 Finally, it can be shown that:

 Fully dissociated electrolyte:

z F

,

where F

N e

A

J ions s tA vcN

A t svcN

J ch e zervcN zrvcF z EvcF

I J A z EvcFA z vcFA

L

I

R G L

A

A

A

( ) .

( arg )

(13)

 

 

z F

z

v

z

v

F

m

0

(

)

 In solution:

The Mobility of Ions and Conductivity

Example:

1. if =5x10-8 m2/Vs and z=1, =10mS m2 mol-1.

2. From the mobility of Cl- in aqueous solution, calculate the molar ionic conductivity.

 = 7.91 x 10-8 m2 s-1V-1 x 96485 Cmol-1 = 7.63x10-3 sm2 mol-1

(14)

The Mobility of Ions and Conductivity

• Taking a conductimetre cell with electrodes separated by 1 cm and an applied voltage of 1 V, calculate the drift speed in water at 298 K. rCs = 170 pm

H2O = 0.891x10-3 kg m-1 s-1

                             ze r x C

x x x kgm s x x m

x m V s

E

L

V

m Vm

s E x m V s x Vm x ms

6

1 602 10

6 31416 0 891 10 170 10

5 10

1

0 01 100

5 10 100 5 10

19

3 1 1 12

8 2 1 1

1

8 2 1 1 1 6 1

.

. .

.

 It will take a Cs+ ion 2000 s to go from one electrode to another.

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Summary

 Migration: Transport of ions induced by an electric field. The concentration dependence of the molar conductivity strongly differs for strong and weak electrolytes.

 Diffusion: Mass transport generated by a gradient of concentration.

m

0m

KC

1 2/

0

2

m

z v D

z v D

F

RT

(

 

 

)

D

RT

zF

D

k T

r

B

(27)

Referensi

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