PRACTICAL 4 : DETERMINATION OF DIFFUSION COEFFICIENT
Date of experiment:
22 May 2014
Objectives:
To study the
diffusion of molecules in an agar medium.
To determine the
diffusion coefficient of crystal violet and bromothymol blue at different
temperature.
Introduction:
Theory
Diffusion, which
is the spontaneous movement of solutes from an area of high concentration
to an area of low concentration can be explained by Fick's law which states that
the flux of material (amount dm in time dt) across a given plane (area A) is proportional to the
concentration gradient dc/dx.
dc
dm = -DA ---- dt ---------------------------------- (i)
dx
D is the diffusion coefficient or diffusivity for the solute, in unit m2s-1
.
If a solution containing neutral particles with the concentration M0, is
placed within a cylindrical tube next to a water column, diffusion can
be stated as
M = M0 exp (-x2/4Dt) ------------------------------------------------------ (ii)
where M is the
concentration at distance x from the intersection between water and solution
that is measured at time t.
By changing equation (ii) to its logarithmic form, we get
ln M =1n M0 - x2 /4Dt
or 2.303
x 4D (log10 M0 – log10 M) t= x2 ---------------------------------------------------- (iii)
Thus a plot of x2 against t can produce a straight line that passes through the origin
with the slope 2.303 x 4D (log10 M0
– log10 M). From here D can be calculated.
If the particles in the solution are assumed to be spherical, their size
and molecular weight can be calculated by
the Stokes-Einstein equation.
D = kT/6πηa
where k is the Boltzmann constant
1.38 x 1023 Jk-1,
T temperature in Kelvin, π the viscosity of the solvent in Nm-2s and a
the radius of particle in M. The volume of a spherical particle is 4/3 πa3, thus its weight M is equivalent to
4/3 πa3Nρ (ρ =
density).
It is known
that molecular weight M=mN (N is Avogadro’s number 6.023 x 1023 mol-1).
∴
M = 4/3 πa3Nρ
---------------------------- (v)
Diffusion for charged particles, equation
(iii) needs to be modified to include potential gradient effect that
exists between the solution and solvent. However, this can be overcome by adding a
little sodium chloride into the solvent to prevent the formation of this potential gradient.
Agar gels contain a partially strong network
of molecules that is penetrated by water. The water molecules form a continuous
phase around the gel. Thus, the molecules of solutes can diffuse
freely in the water if chemical interactions and adsorption effects do not exist entirely.
Therefore, the gel forms an appropriate support system to be used in diffusion studies for molecules in a medium
of water.
Apparatus:
10ml, 50ml, 100ml and 250ml measuring cylinders,
1000ml beaker, 14 test tubes with stoppers, weighing boat, spatula, glass rod,
electronic balance, hot plate and stirrer, test tube rack, dropper, filter
funnel,marker and water bath.
Materials:
Jelly Powder, Ringlet’s solution, 1 : 200 crystal
violet indicator, 1 : 400 crystal violet indicator, 1 : 600 crystal violet
indicator, 1 : 500 000 crystal violet indicator, 1 : 200 bromothymol blue
solution, 1 : 400 bromothymol blue solution, 1 : 600 bromothymol blue solution,
1 : 500 000 bromothymol blue solution, and distilled water.
Procedures:
1. Agar in Ringer’s
solution was prepared as four tablets were crushed by using pestle and mortar.
2. Then, the crushed
tablets were transfered into the 1000ml beaker and 500ml of distilled water was
added into the beaker to dissolve the tablets.
3. 7g of agar powders
were weighed on electronic balance and 425ml Ringer’s solution was measured in
a suitable measuring cylinders.
4. Agar powders
and Ringer’s solution were mixed in the beaker. The mixed solution was heated
until the solution completely dissolved and boiled.
5. The solution
was continuously stirred during the heating process to prevent the jelly powder
from embed in the mixture.
6. During
the heating process, 14 test tubes were labelled according to the
concentrations and types of the solutes, which are bromotyhmol blue and crystal
violet. The heating process was stopped when the mixture become clear dissolved
solution.
7. 20ml of agar
solution was prepared in 14 labelled test tubes.
8. 5ml
of 1:500 000 crystal violet solution was added into a test tube containing hot
agar solution labelled with 1:500 000 crystal violet at 28°C whereas 5ml of
1:500 000 bromothymol blue solution was added into test tube containing the hot
gel solution labelled with 1:500 00 bromothymol blue at 37°C. These two test
tubes will be used as the standard to measure the colour distance resulting
from the solute diffusion.
9. The agar solution in
the rest of test tubes were allowed to cool at room temperature until they
become solid agar.
10. 5ml of each crystal violet solution was
added into the gels that were prepared in 6 test tubes according to their
concentration.
11. This step was repeated by using bromothymol
blue as an indicator. All test tubes were closed to prevent evaporation and
stored at temperature 28°C and 37°C.
12. The distance of crystal violet and
bromothymol blue solution diffused in the agar were measured and recorded for
seven days.
Results
a) Crystal Violet
System
|
Time (seconds)
|
x, cm
|
x2, cm2
|
Slope of graph
|
D, cm2s-1
|
Temp., o C
|
Average Diffusion Coefficient, D cm2s-1
|
1:200
|
0
|
0
|
0
|
3.057 X 10-5
|
9.7662 x 10-7
|
28
|
2.8652 x 10-7
|
86400
|
1.3
|
1.69
|
172800
|
2.1
|
4.41
|
259200
|
2.8
|
7.84
|
345600
|
3.3
|
10.89
|
432000
|
3.7
|
13.69
|
518400
|
4.1
|
16.81
|
604800
|
4.3
|
18.49
|
|
|
|
1:400
|
0
|
0
|
0
|
1.911 X 10-5
|
6.6986 x
10-7
|
28
|
86400
|
1.2
|
1.44
|
172800
|
1.8
|
3.24
|
259200
|
2.4
|
5.76
|
345600
|
2.7
|
7.29
|
432000
|
3.0
|
9.00
|
518400
|
3.3
|
10.89
|
604800
|
3.4
|
11.56
|
|
|
|
1:600
|
0
|
0
|
0
|
1.488X 10-5
|
5.5281 x
10-7
|
28
|
86400
|
0.75
|
0.56
|
172800
|
1.6
|
2.56
|
259200
|
2
|
4.0
|
345600
|
2.3
|
5.29
|
432000
|
2.5
|
6.25
|
518400
|
2.8
|
7.84
|
604800
|
3.0
|
9.0
|
|
|
|
1:200
|
0
|
0
|
0
|
3.652 X 10-5
|
1.16669 x10-6
|
37
|
9.2097 x 10-7
|
86400
|
1.6
|
2.56
|
172800
|
2.4
|
5.76
|
259200
|
3.0
|
9.00
|
345600
|
3.6
|
12.96
|
432000
|
4.0
|
16.00
|
518400
|
4.4
|
19.36
|
604800
|
4.7
|
22.09
|
|
|
|
1:400
|
0
|
0
|
0
|
2.646 X 10-5
|
9.27497 x 10-7
|
37
|
86400
|
1.4
|
1.96
|
172800
|
2.0
|
4.00
|
259200
|
2.6
|
6.76
|
345600
|
3.0
|
9.00
|
432000
|
3.4
|
11.56
|
518400
|
3.8
|
14.44
|
604800
|
4.0
|
16.00
|
|
|
|
1:600
|
0
|
0
|
0
|
1.800 X 10-5
|
6.6871 x 10-7
|
37
|
86400
|
1.0
|
1.00
|
172800
|
1.7
|
2.89
|
259200
|
2.2
|
4.84
|
345600
|
2.5
|
6.25
|
432000
|
2.8
|
7.84
|
518400
|
3.1
|
9.61
|
604800
|
3.3
|
10.89
|
b) Bromothymol
Blue
System
|
Time (seconds)
|
x, cm
|
x2, cm2
|
Slope of graph
|
D, cm2S-1
|
Temp, o C
|
Average Diffusion Coefficient, D cm2S-1
|
A (1:200)
|
0
|
0
|
0
|
2.917 X 10-5
|
9.31886 x 10-7
|
28
|
1.25302 x10-6
|
86400
|
1.5
|
2.25
|
172800
|
2.3
|
5.29
|
259200
|
2.7
|
7.29
|
345600
|
3.2
|
10.24
|
432000
|
3.6
|
12.96
|
518400
|
3.9
|
15.21
|
604800
|
4.2
|
17.64
|
|
|
|
B (1:400)
|
0
|
0
|
0
|
2.388 X
10-5
|
8.3703 x 10-7
|
28
|
86400
|
1.3
|
1.69
|
172800
|
1.9
|
3.61
|
259200
|
2.5
|
6.25
|
345600
|
2.9
|
8.41
|
432000
|
3.2
|
10.24
|
518400
|
3.6
|
12.96
|
604800
|
3.8
|
14.44
|
|
|
|
C (1:600)
|
0
|
0
|
0
|
5.357 X 10-6
|
1.99017 x 10-6
|
28
|
86400
|
0.4
|
0.16
|
172800
|
0.8
|
0.64
|
259200
|
1.1
|
1.21
|
345600
|
1.3
|
1.69
|
432000
|
1.4
|
1.96
|
518400
|
1.6
|
2.56
|
604800
|
1.8
|
3.24
|
|
|
|
D (1:200)
|
0
|
0
|
0
|
3.652 X 10-5
|
1.16669 x 10-6
|
37
|
1.3313 x 10-6
|
86400
|
1.7
|
2.89
|
172800
|
2.5
|
6.25
|
259200
|
3.1
|
9.61
|
345600
|
3.6
|
12.96
|
432000
|
4
|
16
|
518400
|
4.4
|
19.36
|
604800
|
4.7
|
22.09
|
|
|
|
E (1:400)
|
0
|
0
|
0
|
2.388 X
10-5
|
8.3703 x
10-7
|
37
|
86400
|
1.3
|
1.69
|
172800
|
2.0
|
4.00
|
259200
|
2.5
|
6.25
|
345600
|
2.9
|
8.41
|
432000
|
3.2
|
10.24
|
518400
|
3.5
|
12.25
|
604800
|
3.8
|
14.44
|
|
|
|
F (1:600)
|
0
|
0
|
0
|
8.003 X
10-6
|
1.9901 x 10-6
|
37
|
86400
|
0.7
|
0.49
|
172800
|
1.1
|
1.21
|
259200
|
1.4
|
1.96
|
345600
|
1.6
|
2.56
|
432000
|
1.9
|
3.61
|
518400
|
2.1
|
4.41
|
604800
|
2.2
|
4.84
|
|
|
______ |
Graph
Calculations:
From equation:
2.303 x 4D (log 10 Mo – log 10 M) t = X²
Hence the slope
of the graph = 2.303 x 4D (log 10 Mo - log 10 M)
1. Crystal violet system with dilution
1:200 (28 0C)
Slope= 3.057 x 10-5cm2/sec
M =
1:500000
M0 = 1:200
= 1 /
500000 = 1 / 200
= 2 x 10-6 = 5 x 10-3
2.303x4D [log 10
(5x10-3)-log 10 (2x10-6)] = 3.057×10-5
cm2/sec
D = 9.7662×10-7
cm2/sec
2. Crystal violet system with dilution
1:400 (28ºC)
Slope = 1.911×10-5 cm2/sec
M =
1:500000
Mo = 1:400
= 1 / 500000 = 1 / 400
= 2 x 10-6
=
2.5 x 10-3
2.303x4D [log 10
(2.5x10-3)-log 10 (2x10-6)] = 1.911×10-5
cm2/sec
D = 6.6986×10-7
cm2/sec
3.
Crystal violet system with dilution 1:600 (28 0C)
Slope=1.488×10-5 cm2/sec
M =
1:500000
Mo = 1:600
= 1 /
500000 = 1 / 600
= 2 x 10-6 = 1.67 x 10-3
2.303x4D [log 10 (1.67x10-3)-log
10 (2x10-6 )] = 1.488×10-5 cm2/sec
D = 5.5281×10-7
cm2/sec
Average of Diffusion Coefficient, m²/sec for Crystal violet system at
28ºC
= (9.7662×10-7
cm2/sec+6.6986×10-7 cm2/sec+5.5281×10-7
cm2/sec) / 3
= 2.8652×10-7 cm2/sec
4. Crystal violet system with dilution
1:200 (37ºC)
Slope =3.652×10-5 cm2/sec
M =
1:500000
M0 = 1:200
= 1 /
500000 = 1 / 200
= 2 x 10-6 = 5 x 10-3
2.303x4D [log 10 (5x10-3)-log 10 (2x10-6
)] = 3.652×10-5 cm2/sec
D=1.16669×10-6
cm2/sec
5.
Crystal violet system with dilution 1:400 (37ºC)
Slope =2.646×10-5 cm2/sec
M =
1:500000
Mo = 1:400
= 1 / 500000 = 1 / 400
= 2 x 10-6
=
2.5 x 10-3
2.303x4D [log 10 (2.5x10-3)-log
10 (2x10-6)] = 2.646×10-5 cm2/sec
D =
9.267497×10-7 cm2/sec
6. Crystal violet system with dilution 1:600 (37ºC)
Slope = 1.8×10-5 cm2/sec
M =
1:500000
Mo = 1:600
= 1 /
500000 = 1 / 600
= 2 x 10-6 = 1.67 x 10-3
2.303x4D [log 10 (1.67x10-3)-log
10 (2x10-6 )] = 1.8×10-5 cm2/sec
D = 6.871×10-7
cm2/sec
Average of Diffusion Coefficient, m²/sec for Crystal violet system at 37ºC
= (1.16669×10-6 cm2/sec + 9.267497×10-7 cm2/sec
+6.871×10-7 cm2/sec) / 3
= 9.2097×10-7 cm2/sec
# Value of D37°C for crystal violet using the equation
D28°C/D37°C = T28°C/T37°C
2.8652×10-7/D37°C
= (28°C + 273.15K)/(37°C + 273.15K)
D 37°C = 2.9508×10-7
cm2/sec
7.
Bromotymol blue system with dilution 1:200 (28ºC)
Slope = 2.917×10-5 cm2/sec
M = 1:500000
Mo = 1:200
= 1 /
500000
= 1 / 200
= 2 x 10-6 = 5 x 10-3
2.303x4D [log 10
(5x10-3)-log 10 (2x10-6)] = 2.917×10-5 cm2/sec
D = 9.1886×10-7
cm2/sec
8. Bromotymol blue system with
dilution 1:400 (28ºC)
Slope = 2.388×10-5 cm2/sec
M =
1:500000
Mo = 1:400
= 1 /
500000
= 1 / 400
= 2 x 10-6 = 2.5 x 10-3
2.303x4D [log 10
(2.5x10-3)-log 10 (2x10-6 )] = 2.388×10-5
cm2/sec
D= 8.3703×10-7 cm2/sec
9. Bromotymol blue system with dilution 1:600 (28ºC)
Slope =5.357×10-6
cm2/sec
M =
1:500000
Mo = 1:600
= 1 /
500000 = 1 / 600
= 2 x 10-6 = 1.67 x 10-3
2.303x4D [log 10 (1.67x10-3)-log 10 (2x10-6
)] = 5.357×10-6 cm2/sec
D = 1.9907×10-7
cm2/sec
Average of Diffusion Coefficient, m²/sec for Bromothymol blue system at
28ºC
= (9.1886×10-7 cm2/sec + 8.3703×10-7
cm2/sec +11.9907×10-7 cm2/sec) / 3
= 1.253×10-6 cm2/sec
10. Bromotymol blue system with dilution 1:200 (37ºC)
Slope = 3.625×10-5 cm2/sec
M =
1:500000
Mo = 1:200
= 1 /
500000 = 1 / 200
= 2 x 10-6
= 5 x 10-3
2.303x4D [log 10
(5x10-3)-log 10 (2x10-6 )] = 3.625×10-5
cm2/sec
D = 1.1669×10-6
cm2/sec
11. Bromotymol blue system with dilution 1:400 (37ºC)
Slope =2.388×10-5 cm2/sec
M =
1:500000
Mo = 1:400
= 1 / 500000 = 1 / 400
= 2 x 10-6
=
2.5 x 10-3
2.303x4D [log 10 (2.5x10-3)-log 10 (2x10-6)]
= 2.3888×10-5 cm2/sec
D = 8.3703×10-7
cm2/sec
12. Bromotymol blue system with dilution 1:600 (37ºC)
Slope =8.003×10-6 cm2/sec
M =
1:500000
Ma = 1:600
= 1 /
500000 = 1 / 600
= 2 x 10-6 = 1.67 x 10-3
2.303x4D [log 10
(1.67x10-3)-log 10 (2x10-6 )] = 8.003×10-6
cm2/sec
D = 1.9901×10-6
cm2/sec
Average
of Diffusion Coefficient, m²/sec for Bromotymol blue system at 37ºC
= (1.1669×10-6 cm2/sec +8.3703×10-7cm2/sec
+1.9901×10-6 cm2/sec) / 3
= 1.3313×10-6 cm2/sec
# Value of D37°C for bromothymol blue using the equation
D28°C/D37°C = T28°C/T37°C
1.253×10-6
/D37°C = (28°C + 273.15K)/(37°C + 273.15K)
D 37°C = 1.2904×10-6
cm2/sec
Discussion: :
Diffusion is
the movement of solute particles in a solid from a high concentration area to a
low concentration area, resulting in the uniform distribution of the substance.
Diffusion is a process which is not due to the force action but due to the
random movements of atoms. In each diffusion reaction the flux of matter is
equal to the conductivity multiplied by a driving force. Conductivity is the
mobility of the diffusing species or known as diffusivity. The presence of
concentration gradient acts as the driving force for the solute particles to
move.
Fick’s First Law states that the flux, dm, across a membrane of unit area, A,
is proportional to the concentration gradient, dc/dx, and is expressed by
dm = -DA(dc/dx)dt
D is the diffusion coefficient or diffusivity for the
solute. The value of diffusivity describes the rate of diffusion and therefore
its unit is m2s-1. Diffusion coefficient depends on
several factors such as temperature, pressure, composition, physical state,
structure of the phase, and oxygen fugacity. The higher the value of diffusion
coefficient, the easier for that solute to penetrate through the continuous
phase.
The negative sign indicates that the direction of the
diffusive flux is down the concentration gradient. Diffusive flux goes from
high concentration region to low concentration region with the gradient going
the opposite direction, from low to high concentration. Fick’s First Law only
applies to steady state flux where the concentration gradient is uniform.
In this practical, a solution containing neutral molecules with the
concentration M0 is placed within a cylindrical tube. The diffusion
can be expressed as
M = Mo exp (x²/4Dt)
The equation is derived into logarithmic form and
produce new equation,
ln M = ln Mo – (x²/4Dt)
or 2.303 x 4D (log
10 Mo- log 10 M) t = x²
Therefore, a graph of x2 against time
produces a straight line that passes through origin with the slope of 2.303 x
4D (log 10 Mo- log 10 M). D can be calculated from the
gradient obtained.
The results show that the diffusion coefficient, D, for both crystal violet and
bromothymol blue is increasing from 1:600<1:400<1:200 which mean that
1:200 concentration is the easiest to diffuse as 1:200 concentration is the
most concentrated solution. Therefore, the solute with high concentration is
easier to diffuse through the solid medium compared to the low concentration.
This is because the concentration gradient is high for concentrated solute and
forces the solute particles to diffuse further through the medium.
If we compare the diffusion coefficient in the term of temperature between 28°C
and 37°C, the D for 37°C has the larger value than that of 28°C. The same
phenomena occurred for both crystal violet and bromothymol blue solution.
Temperature is one of the factors that affect the rate of diffusion. As the
temperature increases, the amount of energy available for diffusion is
increased. There would be increase in molecules' mobility (kinetic energy). The
molecules move faster and there will be more spontaneous spreading of the
material which means that diffusion occurs quicker. Thus, the diffusivity
increases as the temperature increases.
The value of D37°C can be determined
if we already know the value for D28°C by using the equation below
D28°C/D37°C = T28°C/T37°C
where T is the temperature in Kelvin.
However, there are the differences between the value
of D37°C that we get from the experiment and from the theoretical value. For
crystal violet, 9.2099×10-7 cm2s-1 is the
experimental value of D37°C whereas 7.5502×10-7 cm2s-1
is the theoretical value that obtained from the equation above. Meanwhile, for
bromothymol blue the D37°C from theoretical and experimental is 6.7559×10-7
cm2s-1 and 7.6703×10-7 cm2s-1
respectively. Generally, the experimental value for D37°C is higher than
theoretical value. This is maybe due to the some errors that occurred during
the experiment is carried out. The temperature may be set higher than 37°C that
cause the rate of diffusion to increase. Besides, the errors also due to the
room temperature at 28°C that is not constant throughout the experiment and the
viscosity of agar in the test tube that is not uniform. Misreading or parallax
error might occur.
According to the equation:
M = 4/3πa3 N Þ
a3 = 3M / 4πN Þ
a = 3√ 3M / 4πN
Þ --------------------------- (1)
Where M= molecular weight, a = radius of particle,
N=Avogadro's number (6.02x1023),
Þ =density.
Another
equation:
D = kT / 6 πηa --------------------------- (2)
Substituting (1) into the equation (2)
D = kT / 6 πηa
= kT / 6 πη 3√ 3M/4πNÞ
= kT 3√4πNÞ / 6 πη 3√
3M ------------------------- (3)
Where D=diffusion coefficient, η= viscosity,
T=temperature, k=Boltzmann
constant
(1.38 x1023 Jk-1)
According to equation (3), D is inversely proportional
to M. So, D increases when M decreases. Crystal violet with molecular formula C25N3H30Cl
has molecular weight of 407.979 g mol-1 while bromothymol blue
solution with molecular formula C27H28Br2O5S
has molecular weight of 624.38 g mol−1. Molecular weight is how much
mass each particle has or how heavy it is. The heavier the particle, the slower
it diffuses into solidified agar solution, assuming energy of the system
remains constant. Crystal violet solution diffuses faster than bromothymol blue
since the value of diffusion coefficient for crystal violet is higher than
bromothymol blue at both temperatures. Crystal violet solution diffuses easily
because its molecular weight is much smaller compared to that of bromothymol
blue and thus easy for them to penetrate through gel medium.
Conclusion
From the experiment, the diffusion coefficient of
crystal violet at 28°C is 7.3311×10-7 cm2s-1
and at 37°C is 9.2099×10-7 cm2s-1.
Meanwhile, for bromothymol blue solution the diffusion coefficient at 28°C is 6.5599×10-7
cm2s-1 and at 37°C is 7.6703×10-7 cm2s-1.
The diffusion coefficient of crystal violet is generally higher than
bromothymol blue because of the difference inmolecular weight. In term of
temperature, diffusivity at 37°C is much higher than diffusivity at 28°C. This
is due to the rapid movement of the solute particles as the temperature
increases.
References
- http://urila.tripod.com/mole.htm
- http://en.wikipedia.org/wiki/Molecular_mass
- http://www.pojman.com/mg_materials/Diffusion/Diffusion.html
Appendix
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Continuous stirring until a clear solution is formed which is shown below |
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The test tubes before being separated into water bath and left to room temperature |