Thermo- physical characterization of paraffin and beeswax on cotton fabric

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Research Article
*Correspondence : susumeme1983@yahoo.com
Thermo- physical characterization of
paraffin and beeswax on cotton fabric
Mahamasuhaimi Masae*and Pichya Pitsuwan
Department of Industrial Engineering, Rajamangala University of Technology Srivijaya,
Songkhla Campus, Boyang Sub-district, Muang District, Songkhla 90000, Thailand
Lek Sikong , Kalayanee Kooptarnond
, Peerawas Kongsong and
Phatcharee Phoempoon
Department of Mining and Materials Engineering, Prince of Songkla University,
Hat Yai Campus, Songkhla 90110, Thailand.
Abstract
Cotton fabric (CF) has been widely used as a batik clothing material due to its suitable
physical characteristics. Cotton woven fabrics were treated with droplets of different types of
waxes including paraffin and beeswax. The physical and thermal properties of the waxes were
characterized. This article presents an experimental study of the deposition of small droplets of
molten waxes on CF surfaces. The method is based on an evaluation of the chemical functional
groups of the waxes that were characterized by using fourier transform infrared spectroscopy
(FTIR). The thermal properties of the waxes were analyzed by using a differential scanning
calorimeter (DSC). The viscosity of the molten waxes was measured with a viscometer. The
spread of the molten waxes was determined in terms of the contact angles of the droplets on the
CF surface. It was indicated that the contact angle of beeswax droplets on the CF surface is higher
than that of paraffin. It should be noted that the contact angle correlates to the viscosity of the
molten wax samples.
Keywords: Cotton fabric (CF);Paraffin; Beeswax; waxes.
1. Introduction
Batik is a type of cloth that is traditionally
made by hand with wax resistant a
and dyeing technique. In southern Thailand,
batik is easily found in the form of resort
uniforms and decorations in many places. It is
also used for local casual wear in the forms of
sarongs, shirts and blouses. Batik is usually
made from cotton fabric.
Wax, such as paraffin, beeswax, and
turpentine, is introduced to the cotton fabric
surface, followed by heating in the range of
80-100 °C prior to the color painting process.
In the wax drop process, the molten wax
droplets are introduced to the cotton fabric
surface at a certain drop rate. After wax
removal, the cotton fabrics are immersed in
boiling water. In this paper, paraffin and
beeswax droplets have been applied to cotton
fabrics for batik utilization. The prepared
molten wax drop can improve the contact
angle and viscosity properties.
Chemically, waxes are mixtures of
organic substances, which are usually long
chain molec ules. Th ey are c o mp osed
of hydrocarbons [1], tri- di-or mono-esters of
Thammasat International Journal of Science and Technology Vol.19, No.4, October-December 2014
70
medium length fatty acids, long chain
alcohols, free long chain alcohols, aldehydes,
ketones,
-diketones, sterols, triterpenols and
triterpenic acids [1-2]. Their chemical
compositions depend on their animal, vegetal
or mineral origin [1,3].
In this work, cotton fabrics were
treated with droplets of paraffin and beeswax
in an attempt to develop molten wax droplets
that exhibit a low contact angle spread on
cotton fabric and a low thickness. Good
wettability of a surface is a prerequisite for
ensuring good adhesive bonding. The
characterization of the molten waxes was
studied through a variety of techniques.
2. Materials and methods
2.1. Materials
Cotton fabric (CF) was purchased from
Krisna Store Thai Silk Co., Ltd., Thailand.
Paraffin and beeswax were purchased from
Saiburi herbal Co., Ltd., Thailand. The FTIR
transmittance spectra of the waxes were also
analyzed in order to confirm chemical
functional groups of the wax mixture.
2.2. Differential scanning calorimetric
(DSC) analysis
The thermal characteristics of paraffin
and beeswax were analyzed with a differential
scanning calorimeter (DSC), specifically a
PerkinElmer DSC7. The sample weight was
about 5 mg. All analyses were performed in
the scanning mode from 20 to 200 °C at the
heating rate of 10 C/min. Dry nitrogen gas
was introduced into the DSC cell as the
purging gas.
2.3. Viscosity measurement
A Rheometer (RVDV-II, Brookfield,
USA) was used to measure the viscosity in
our experiment. The device is an advanced
controlled stress, direct strain and controlled
rate rheometer with a magnetic-levitation
thrust bearing and a drag cup motor to allow
torque control. A wide range of cones and
plates, often called geometry, is available for
use with a Peltier setup or an oven.
Temperature control can be achieved using a
heated plate setup, a fluid bath or an oven,
allowing temperatures from 25°C to 150°C
with the temperature resolution of 0.02°C.
The device is controlled by a rheology
advantage software. Before the
measurements, the rheometer was carefully
calibrated with pure base fluid.
2.4. Fabrication of wax-droplet cotton
fabrics
Before the introduction of the wax
droplets, the fabrics were immersed in 1 M.
NaOH solution 24 h. and leached with water.
Then, wax was melted in the oven at 100ºC.
Cotton fabric (3×8 cm.) was stretched on a
glass slide. The melted wax was immediately
dropped onto the CF and left it dry at room
temperature. The formation of the wax
droplet in terms of contact angles was
investigated at room temperature using a
contact angle meter (OCA15EC). The gap
distance between eject head and cotton fabric
surface was 1 mm., and the wax volume was
at 14 µL. The wax droplet thickness was
measured using a micrometer specifically the
Mitoyo series 103.
3. Results and discussion
3.1. FTIR analysis
The band frequencies of the spectra
obtained with their assignment [4-6] are given
in Table 1. The FTIR spectra of the waxes
covering paraffin and beeswax consisted of
five main groups of absorption bands in the
wavelength range of 400 3900 cm (Fig. 1).
-1
The bands in the region of 719-730 were
Vol.19, No.4, October-December 2014 Thammasat International Journal of Science and Technology
Table 1.
FTIR analysis of paraffin and beeswax with major peak frequency (cm ) and assignment.
-1
Range/cm
-1
Assignment
Vibrating group
Intensity
Samples
Beeswax
719
ρ(CH
2
)
(CH
2
)
n
, n>3
w-m
1162
v(ring)
Heterocyclics and their aromatically
w-m
1260
v(ring)
Ethers, aliphatic (Epoxides)
m-s
1268
v
as
(O-CO-O)
Carbonates aliphatic
vs
1367
v(ring)
Heterocyclics and their aromatically
m-s
δ
s
(CH
3
)
Aliphatic hydrocarbons
m-s
1463
δ(CH
2
)
Aliphatic hydrocarbons
m
1691
v(C=O)
Aromatic-COOH
vs
1733
v(C=O)
Esters of aromatic carboxylic acids
with alcohols
vs
2846
v
s
(CH
2
)
3
Aliphatic hydrocarbons
m
2910
v
as
(CH
2
)
Aliphatic hydrocarbons
m-s
Note: s:strong, m:medium, w:weak, v:very, v:stretching vibration, γ : out of plane
deformation vibration, ρ: rocking vibration, δ: in plane
deformation vibration, s
(as subscript)
:
symmetric, as : antisymmetric.
(as subscript)
Fig.1. FTIR spectra of: (a) paraffin and (b) beeswax.
assigned to the deformation vibrations of a
long-chain hydrocarbon.
The bands in the region of 1366-1382
cm
-1
δ
s
(CH
3
) and 1458-1475 cm
-1
δ(CH
2
) can
be assigned to the wax aliphatichydrocarbons.
Bands appearing in the region of 1689-1691
cm
-1
ν(C=O) and 2848-3000 cm ) were
-1
ν(CH
2
assigned to the wax aromatic and aliphatic
hydrocarbons respectively. The predominant
components of the wax samples were
aliphatic hydrocarbons. Long-chain esters
and acids have also been found.
This phenomenon maybe caused by the fact
that beeswax has wetting hydrophobic more
effective than paraffin due to a higher wax
aromatic hydrocarbon structure. Beeswax was
adsorbed by the cotton fabric with the
hydrophobic spreading. This behavior also
confirms that the beeswax has a higher wax
aromatic hydrocarbon structure than paraffin
does.
(b)
(a)
71
Thammasat International Journal of Science and Technology Vol.19, No.4, October-December 2014
72
Fig.2. DSC curves of (a) paraffin and (b) beeswax.
0
1
2
3
4
5
6
7
8
20 40 60 80 100
Temperature (C)
DSC (W/g)
0
1
2
3
4
5
6
7
8
20 40 60 80 100
Temperature (C)
DSC (W/g)
3.2. DSC curves of waxes samples
There were 1 to 2 heat absorbing peaks
or heat releasing peaks clearly seen in the
melting or crystallizing curves of DSC
diagrams according to different samples. DSC
analysis is designed such that different peaks
occur with different chemical compositions,
so it was inferred from the curves that waxes
were not single chemicals. For its high
sensitivity, a slight change of heat could be
measured by DSC. Thus, the small amounts of
the chemical constituents of the waxes were
also shown in the diagram, and the DSC was
able to identify the wax purity.
For instance, the waxes shown in Fig. 2
consisted of have at least two composed
chemicals, were one in a small amount with a
low melting peak at 40 to 60 °C, and another
in a larger amount with an orderly significant
peak at 60 to 70°C. It was known with wax
composition that the change in the slope in
the chart between 40 and 60°C was due to the
heat absorbed from the free acids and the
hydrocarbons [7]. From the DSC curves
shown in Fig.2, the values of the melting
point, the softening point, the melting peak,
melting and crystallization enthalpies were
obtained as shown in Table 2.
a
b
Vol.19, No.4, October-December 2014 Thammasat International Journal of Science and Technology
73
Table 2. . The starting, ending and summit temperatures of the melting peak of the waxes
sample
sample
weight
(mg)
T
0l
(Cº)
T
m1
(Cº)
T
f1
(Cº)
T
02
(Cº)
T
m2
(Cº)
T
f2
(Cº)
Melting
enthalpy
(J/g)
Crystallization
enthalpy (J/g)
Paraffin
5.37
51.49
58.00
61.80
54.76
52.30
45.30
132.58
114.63
Beeswax
5.78
42.26
67.83
69.89
59.42
57.30
47.63
176.00
162.42
Note:1) T : softening point 2) T : melting peak temperature 3) T : melting point (ending
01 m1 f1
temperature of melting) 4) T :starting temperature of crystallizing 5) T : peak temperature
o2 m2
of crystallizing 6) T ending temperature of crystallizing.
f2
:
Fig.3. Viscosity for different waxes
0
2
4
6
8
10
12
60 80 100
Temperature (C)
Viscosity (cP)
Paraffin
Beeswax
According to the DSC curves in Fig.
2 and the data in Table 2, from the starting to
the ending temperatures, the summit
temperature of the melting or crystallization
peak of the waxes varied due to their
different compositions. The melting point of
the beeswax was higher than that of the
paraffin. In Table 2, the melting points of the
paraffin were lower than those of the
beeswax because the structure of paraffin was
simples with some chain alkanes and because
its molecular weight was smaller than that of
beeswax, which is composed of mix esters in
high molecular weights and complicated
structures. From Table 2, it was inferred that
there were great variances among melting
enthalpy of the waxes. The enthalpy of the
beeswax was higher than that of the paraffin.
It was known from the above that there were
some relations between the enthalpies and the
melting points of the waxes.
3.2. Viscosity tests
The experiments to analyze the changes
of the viscosity curve were performed on the
fluid samples with different waxes (Paraffin
and Beeswax). The viscosity measurements
indicated that the melted waxes change the
fluid’s viscosity significantly at different
temperatures as shown in Fig. 3.It was found
that the viscosity of the molten beeswax is
higher than that of paraffin. Since the melted
waxes were expected to change the
precipitated wax crystal’s size distribution [8-
9], it is understandable that this also affects
the fluid viscosity [10].
Thammasat International Journal of Science and Technology Vol.19, No.4, October-December 2014
74
thicknesses to be much lower, with thickness
values reduced to only approx. 0.99 mm.
3.3. Wax droplet contact angle
When a droplet of molten sample impacts
the cotton fabric surface, which is at a lower
temperature than the molten sample, it
spreads out and may retract, producing a
sample bump (or sample dot) sticking to the
cotton fabric surface.
The process of impact can be divided into
two stages: the spreading, driven by inertial
forces, and the subsequent oscillation, driven
by surface tension forces [11]. Both stages
involve viscous dissipation and solidification.
For a liquid droplet impacting a solid surface
without a phase change, the final shape of the
droplet is determined by its equilibrium state
depending on the properties of the liquid, the
substrate materials and the temperature [12-
13].The deposition, including the
solidification, of small molten droplets on
cotto n fab ric s urf aces is a c omplex
fluid/thermal problem. The final shape of the
droplets is not determined by the fluid flow
alone, but depends on the thermal histories of
the droplets during the impact since they may
freeze before reaching their equilibrium
shape.
The coupling between solidification and
fluid dynamics can lead to a variety of
solidified shapes and textures of deposited
droplets. There are no simple models to
predict what these will be. The final shape
can be characterized the contact angles of the
bases of the droplet and their thickness.
Contact angle measurements of molten the
samples carried out in ambient air
environments are shown in Fig. 4.
It was found that paraffin has a significant
effect on lowering the contact angle of sample
droplets due to their enhancement of the
molten samples, in turn lowering the viscosity
of the compared to beeswax samples. The
contact angle of the sample droplets on the
cotton fabric surface not only depends on the
type of sample but also on the temperature
and the viscosity. It should be noted that
contact angle correlates with the viscosity of
the molten samples. The smaller contact angle
corresponded to the low viscosity. The
paraffin samples displayed smaller contact
angles than the beeswax sample did. The
paraffin sample droplets with a contact angle
of 39° were observed at 100 °C (Figs. 4 and
5).The contact angle images of the molten
sample droplets on sample that have been
treated at different temperatures and their
contact angles, are shown in Figs 5 and 4,
respectively. It was observed that the contact
angles of paraffin were smaller than those of
the beeswax samples due to the fluid viscosity
effect of the sample mixture. It was found that
beeswax has the structure of aromatic
hydrocarbon which is not found in paraffin
wax, so the paraffin wax has a better spread
than beeswax does.
The final thicknesses of droplets ejected
at different temperatures and landing on the
cotton fabric surface were measured. The
average thickness values on the cotton fabric
surface region of these molten samples are
shown in Table 3. The effect of the contact
angles can be seen through a comparison of
the thicknesses in Table 3. Smaller spread
diameters and larger contact angles are
formed on the cotton surface. Earlier studies
showed that the dynamic contact angle
increases with the equilibrium contact angle
[14] and that the maximum spread of a
droplet decreases as the dynamic contact
angle increases [15-17]. Very low thickness
molten dropletsare formed from high molten
temperatures (100°C) and a increased
thickness molten droplet at low molten
temperatures (70, 80 and 90 °C) as shown in
Table 3. The use of paraffin rendered the
Vol.19, No.4, October-December 2014 Thammasat International Journal of Science and Technology
75
Fig.4. Molten sample contact angles vs. temperature of paraffin and beeswax sample.
Samples
70 °C
80 °C
90 °C
100 °C
Paraffin
Beeswax
Fig.5. Images of molten waxes droplets on cotton fabric surface compared with those of
different temperature during 70 100 °C.
Table 3. Thickness values of wax droplets on cotton fabric surface at different
temperature conditions.
Samples
Thickness (mm)
70 ºC
80 ºC
90 ºC
100 ºC
Paraffin
2.41
1.99
1.53
0.99
Beeswax
2.50
2.25
1.61
1.12
20
40
60
80
100
120
140
70 80 90 100
Temperature (C)
Contact angle (Degree)
Paraffin
Beeswax
Thammasat International Journal of Science and Technology Vol.19, No.4, October-December 2014
76
4. Conclusions
Paraffin exhibited lower contact angles
than beeswax did. It should be noted that
contact angles correlate with the viscosity of
the molten samples. was found that molten It
samples could decrease the contact angle
(hydrophilicity) on the cotton fabric surface.
Molten paraffin was excellent and spread on
the cotton fabric surface. The utilization of
beeswax only increased the droplet contact
angles and the thicknesses of the droplets.
In summary, DSC was available for
thermal characteristic determination of
paraffin and beeswax qualitatively and
quantitatively, with better accuracy than than
traditional mercury surface measurement.
FTIR is a convenient way to preliminary
evaluate the wax chemical composition.
5. Acknowledgements
We would like to thank the Office of the
Higher Education Commission, Thailand for
granting the fund. We would also like to
acknowledge the Department of Industrial
En gine ering, Fa cult y of En gi n eeri n g,
Rajamangala University of Technology
Srivijaya, Songkhla, Thailand and Materials
Engineering Research Center (MERC),
Faculty of Engineering, Prince of Songkla
University for their facility supp orts.
6. References
[1] Mills, J.S. and White, R., The Organic
Chemistry of Museum Objects, second
ed., Butterworth, Oxford, 1994.
[2] Planeta, J., Novotn´a, P., Pac´akov´a, V.,
Stulik, K., Mikesov´a, M., and Vejrosta,
J. Application of Supercritical Fluid
Chromatography to the Analysis of
Waxes in Objects of Art, J High Res
Chromatog., Vol. 23, pp.393-396, 2000.
[3] Asperger, A., Engewald, W., and Fabian,
G. Analytical characterization of natural
waxes employing pyrolysis-gas
chromatography-mass spectrometer, J
Anal ApplPyrol., Vol.50, pp.103-115,
1999.
[4] Birshtein, V., and YaTul'chinskii, V. M.
Determination of bees wax and some
impurities by IR spectroscopy, Chem
Nat Compd., Vol. 13, pp. 232-235, 1997.
[5] Fallahi, E., Barmar, M., and Haghighat
Kish, M. Preparation of phase-change
material microcapsules with paraffin or
camel fat cores: application to fabrics,
Iran polym J., Vol 19, pp. 277-286,
2010.
[6] Hummel D. O., Atlas of plastics additives,
Analysis by spectrometric methods,
Springer-Verlag Berlin Heidelberg, New
York, 2002.
[7] Ruguo, Z., Hua, Z., Hong, Z., Ying, F.,
Kun, L., and Wenwen, Z., Thermal
analysis of four insect waxes based on
differential scanning calorimetry (DSC),
P Eng., Vol. 18, pp. 18:101 106, 2011.
[8] Hoffmann, R., and Amundsen, L. Single-
phase wax deposition experiments, J
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[9] Kuzmić, A. E., Radošević, M., Bogdanić,
G., Srića, V., and Vuković, R. Studies on
the influence of long chain acrylic esters
polymers with polar monomers as crude
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87, pp.2943-2950, 2008.
[10] Pedersen, K. S., and Rønningsen, H. P.
Influence of wax inhibitors on wax
appearance temperature, pour point and
viscosity of waxy crude oils, Energ
Fuel., Vol. 17, pp.321-328, 2003.
[11] Li, R., Ashgriz, N., Chandra, S., and
Andrews, J. R. Shape and surface texture
of molten droplets deposited on cold
surfaces, Surf coat., Vol. 202, pp.3960-
3966, 2008.
[12] Kim, H.Y., and Chun, J.H. The recoiling
of liquid droplets upon collision with
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pp.643-659, 2001.
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[13] Chandra, S., and Avedisian, C.T. On the
collision of a droplet with a solid surface,
P Roy SocLond A Mat., Vol. 432, pp.
13-41. 1991.
[14]Hoffman, R.L. Single-phase wax
deposition experiments, J CollidInterf
Sci., Vol. 50, pp.228-241, 1975.
[15] Amada, A., Haruyama, M., Ohyagi, T.,
and Tomoyasu, K. Wettability effect on
the flattening ratio of molten metal
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pp.211-219, 2001.
[16] Bennett, T. and Poulikakos, D. Splat-
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Preview text:

Research Article
Thermo- physical characterization of
paraffin and beeswax on cotton fabric
Mahamasuhaimi Masae*and Pichya Pitsuwan
Department of Industrial Engineering, Rajamangala University of Technology Srivijaya,
Songkhla Campus, Boyang Sub-district, Muang District, Songkhla 90000, Thailand
Lek Sikong , Kalayanee Kooptarnond , Peerawas Kongsong and Phatcharee Phoempoon
Department of Mining and Materials Engineering, Prince of Songkla University,
Hat Yai Campus, Songkhla 90110, Thailand. Abstract
Cotton fabric (CF) has been widely used as a batik clothing material due to its suitable
physical characteristics. Cotton woven fabrics were treated with droplets of different types of
waxes including paraffin and beeswax. The physical and thermal properties of the waxes were
characterized. This article presents an experimental study of the deposition of small droplets of
molten waxes on CF surfaces. The method is based on an evaluation of the chemical functional
groups of the waxes that were characterized by using fourier transform infrared spectroscopy
(FTIR). The thermal properties of the waxes were analyzed by using a differential scanning
calorimeter (DSC). The viscosity of the molten waxes was measured with a viscometer. The
spread of the molten waxes was determined in terms of the contact angles of the droplets on the
CF surface. It was indicated that the contact angle of beeswax droplets on the CF surface is higher
than that of paraffin. It should be noted that the contact angle correlates to the viscosity of the molten wax samples.
Keywords: Cotton fabric (CF);Paraffin; Beeswax; waxes. 1. Introduction
In the wax drop process, the molten wax
Batik is a type of cloth that is traditionally
droplets are introduced to the cotton fabric made by hand with a wax resistant
surface at a certain drop rate. After wax
and dyeing technique. In southern Thailand,
removal, the cotton fabrics are immersed in
batik is easily found in the form of resort
boiling water. In this paper, paraffin and
uniforms and decorations in many places. It is
beeswax droplets have been applied to cotton
also used for local casual wear in the forms of
fabrics for batik utilization. The prepared
sarongs, shirts and blouses. Batik is usually
molten wax drop can improve the contact made from cotton fabric.
angle and viscosity properties.
Wax, such as paraffin, beeswax, and
Chemically, waxes are mixtures of
turpentine, is introduced to the cotton fabric
organic substances, which are usually long
surface, followed by heating in the range of
chain mol ec ul es. Th ey are c o mp os ed
80-100 °C prior to the color painting process.
of hydrocarbons [1], tri- di-or mono-esters of
*Correspondence : susumeme1983@yahoo.com
Thammasat International Journal of Science and Technology Vol.19, No.4, October-December 2014
medium length fatty acids, long chain
rate rheometer with a magnetic-levitation
alcohols, free long chain alcohols, aldehydes,
thrust bearing and a drag cup motor to allow  ketones,
-diketones, sterols, triterpenols and
torque control. A wide range of cones and
triterpenic acids [1-2]. Their chemical
plates, often called geometry, is available for
compositions depend on their animal, vegetal
use with a Peltier setup or an oven. or mineral origin [1,3].
Temperature control can be achieved using a
In this work, cotton fabrics were
heated plate setup, a fluid bath or an oven,
treated with droplets of paraffin and beeswax
allowing temperatures from 25°C to 150°C
in an attempt to develop molten wax droplets
with the temperature resolution of 0.02°C.
that exhibit a low contact angle spread on
The device is controlled by a rheology
cotton fabric and a low thickness. Good advantage software. Before the
wettability of a surface is a prerequisite for
measurements, the rheometer was carefully
ensuring good adhesive bonding. The
calibrated with pure base fluid.
characterization of the molten waxes was
2.4. Fabrication of wax-droplet cotton
studied through a variety of techniques. fabrics
2. Materials and methods
Before the introduction of the wax 2.1. Materials
droplets, the fabrics were immersed in 1 M.
Cotton fabric (CF) was purchased from
NaOH solution 24 h. and leached with water.
Krisna Store Thai Silk Co., Ltd., Thailand.
Then, wax was melted in the oven at 100ºC.
Paraffin and beeswax were purchased from
Cotton fabric (3×8 cm.) was stretched on a
Saiburi herbal Co., Ltd., Thailand. The FTIR
glass slide. The melted wax was immediately
transmittance spectra of the waxes were also
dropped onto the CF and left it dry at room
analyzed in order to confirm chemical
temperature. The formation of the wax
functional groups of the wax mixture.
droplet in terms of contact angles was
investigated at room temperature using a
2.2. Differential scanning calorimetric
contact angle meter (OCA15EC). The gap (DSC) analysis
distance between eject head and cotton fabric
The thermal characteristics of paraffin
surface was 1 mm., and the wax volume was
and beeswax were analyzed with a differential
at 14 µL. The wax droplet thickness was
scanning calorimeter (DSC), specifically a
measured using a micrometer specifically the
PerkinElmer DSC7. The sample weight was Mitoyo series 103.
about 5 mg. All analyses were performed in
the scanning mode from 20 to 200 °C at the
3. Results and discussion
heating rate of 10◦C/min. Dry nitrogen gas 3.1. FTIR analysis
was introduced into the DSC cell as the
The band frequencies of the spectra purging gas.
obtained with their assignment [4-6] are given
2.3. Viscosity measurement
in Table 1. The FTIR spectra of the waxes
A Rheometer (RVDV-II, Brookfield,
covering paraffin and beeswax consisted of
USA) was used to measure the viscosity in
five main groups of absorption bands in the
our experiment. The device is an advanced
wavelength range of 400–3900 cm-1(Fig. 1).
controlled stress, direct strain and controlled
The bands in the region of 719-730 were 70
Vol.19, No.4, October-December 2014 Thammasat International Journal of Science and Technology
assigned to the deformation vibrations of a
long-chain hydrocarbon.
Table 1. FTIR analysis of paraffin and beeswax with major peak frequency (cm-1) and assignment. Range/cm-1 Assignment Vibrating group Intensity Samples Paraffin Beeswax 720 719 ρ(CH2) (CH2)n, n>3 w-m 1162 v(ring)
Heterocyclics and their aromatically w-m 1260 v(ring) Ethers, aliphatic (Epoxides) m-s 1268 vas(O-CO-O) Carbonates aliphatic vs 1367 v(ring)
Heterocyclics and their aromatically m-s 1371 δs(CH3) Aliphatic hydrocarbons m-s 1463 1463 δ(CH2) Aliphatic hydrocarbons m 1691 v(C=O) Aromatic-COOH vs 1733 v(C=O)
Esters of aromatic carboxylic acids vs with alcohols 2846 2846 vs(CH2)3 Aliphatic hydrocarbons m 2910 2910 vas(CH2) Aliphatic hydrocarbons m-s
Note: s:strong, m:medium, w:weak, v:very, v:stretching vibration, γ : out of plane
deformation vibration, ρ: rocking vibration, δ: in plane deformation vibration, s(as subscript):
symmetric, as(as subscript): antisymmetric.
The bands in the region of 1366-1382
This phenomenon maybe caused by the fact cm-1 δs(CH
3) and 1458-1475 cm-1 δ(CH2) can
that beeswax has wetting hydrophobic more
be assigned to the wax aliphatichydrocarbons.
effective than paraffin due to a higher wax
Bands appearing in the region of 1689-1691
aromatic hydrocarbon structure. Beeswax was
cm-1 ν(C=O) and 2848-3000 cm-1 ν(CH2) were
adsorbed by the cotton fabric with the
assigned to the wax aromatic and aliphatic
hydrophobic spreading. This behavior also
hydrocarbons respectively. The predominant
confirms that the beeswax has a higher wax
components of the wax samples were
aromatic hydrocarbon structure than paraffin
aliphatic hydrocarbons. Long-chain esters does.
and acids have also been found. (b) (a)
Fig.1. FTIR spectra of: (a) paraffin and (b) beeswax. 71
Thammasat International Journal of Science and Technology Vol.19, No.4, October-December 2014
3.2. DSC curves of waxes samples
For instance, the waxes shown in Fig. 2
There were 1 to 2 heat absorbing peaks
consisted of have at least two composed
or heat releasing peaks clearly seen in the
chemicals, were one in a small amount with a
melting or crystallizing curves of DSC
low melting peak at 40 to 60 °C, and another
diagrams according to different samples. DSC
in a larger amount with an orderly significant
analysis is designed such that different peaks
peak at 60 to 70°C. It was known with wax
occur with different chemical compositions,
composition that the change in the slope in
so it was inferred from the curves that waxes
the chart between 40 and 60°C was due to the
were not single chemicals. For its high
heat absorbed from the free acids and the
sensitivity, a slight change of heat could be
hydrocarbons [7]. From the DSC curves
measured by DSC. Thus, the small amounts of
shown in Fig.2, the values of the melting
the chemical constituents of the waxes were
point, the softening point, the melting peak,
also shown in the diagram, and the DSC was
melting and crystallization enthalpies were
able to identify the wax purity. obtained as shown in Table 2. 8 7 a 6 5 (W/g) 4 3 DSC 2 1 0 20 40 60 80 100 Temperature (C) 8 7 6 b ) /g 5 (W 4 C S 3 D 2 1 0 20 40 60 80 100 Temperature (C)
Fig.2. DSC curves of (a) paraffin and (b) beeswax. 72
Vol.19, No.4, October-December 2014 Thammasat International Journal of Science and Technology
According to the DSC curves in Fig.
its molecular weight was smaller than that of
2 and the data in Table 2, from the starting to
beeswax, which is composed of mix esters in the ending temperatures, the summit
high molecular weights and complicated
temperature of the melting or crystallization
structures. From Table 2, it was inferred that
peak of the waxes varied due to their
there were great variances among melting
different compositions. The melting point of
enthalpy of the waxes. The enthalpy of the
the beeswax was higher than that of the
beeswax was higher than that of the paraffin.
paraffin. In Table 2, the melting points of the
It was known from the above that there were
paraffin were lower than those of the
some relations between the enthalpies and the
beeswax because the structure of paraffin was melting points of the waxes.
simples with some chain alkanes and because
Table 2. The starting, ending and summit temperatures of the melting peak of the waxes. sample sample T Crystallization 0l Tm1 Tf1 T02 Tm2 Tf2 Melting weight (Cº) (Cº) (Cº) (Cº) (Cº) (Cº)
enthalpy enthalpy (J/g) (mg) (J/g) Paraffin 5.37
51.49 58.00 61.80 54.76 52.30 45.30 132.58 114.63 Beeswax 5.78
42.26 67.83 69.89 59.42 57.30 47.63 176.00 162.42
Note:1) T01: softening point 2) Tm :
1 melting peak temperature 3) Tf : 1 melting point (ending
temperature of melting) 4) To :
2 starting temperature of crystallizing 5) Tm : 2 peak temperature
of crystallizing 6) Tf2: ending temperature of crystallizing. 3.2. Viscosity tests
temperatures as shown in Fig. 3.It was found
The experiments to analyze the changes
that the viscosity of the molten beeswax is
of the viscosity curve were performed on the
higher than that of paraffin. Since the melted
fluid samples with different waxes (Paraffin waxes were expected to change the
and Beeswax). The viscosity measurements
precipitated wax crystal’s size distribution [8-
indicated that the melted waxes change the
9], it is understandable that this also affects
fluid’s viscosity significantly at different the fluid viscosity [10]. 12 Paraffin 10 Beeswax ) 8 (cP y 6 sit co is V 4 2 0 60 80 100 Temperature (C)
Fig.3. Viscosity for different waxes 73
Thammasat International Journal of Science and Technology Vol.19, No.4, October-December 2014
3.3. Wax droplet contact angle
contact angle correlates with the viscosity of
When a droplet of molten sample impacts
the molten samples. The smaller contact angle
the cotton fabric surface, which is at a lower
corresponded to the low viscosity. The
temperature than the molten sample, it
spreads out and may retract, producing a
paraffin samples displayed smaller contact
sample bump (or sample dot) sticking to the
angles than the beeswax sample did. The cotton fabric surface.
paraffin sample droplets with a contact angle
The process of impact can be divided into
of 39° were observed at 100 °C (Figs. 4 and
two stages: the spreading, driven by inertial
5).The contact angle images of the molten
forces, and the subsequent oscillation, driven
sample droplets on sample that have been
by surface tension forces [11]. Both stages
treated at different temperatures and their
involve viscous dissipation and solidification.
For a liquid droplet impacting a solid surface
contact angles, are shown in Figs 5 and 4,
without a phase change, the final shape of the
respectively. It was observed that the contact
droplet is determined by its equilibrium state
angles of paraffin were smaller than those of
depending on the properties of the liquid, the
the beeswax samples due to the fluid viscosity
substrate materials and the temperature [12-
effect of the sample mixture. It was found that
13].The deposition, including the
beeswax has the structure of aromatic
solidification, of small molten droplets on
hydrocarbon which is not found in paraffin
cot to n f ab ri c s urf ac es is a c om ple x
fluid/thermal problem. The final shape of the
wax, so the paraffin wax has a better spread
droplets is not determined by the fluid flow than beeswax does.
alone, but depends on the thermal histories of
The final thicknesses of droplets ejected
the droplets during the impact since they may
at different temperatures and landing on the
freeze before reaching their equilibrium
cotton fabric surface were measured. The shape.
average thickness values on the cotton fabric
The coupling between solidification and
fluid dynamics can lead to a variety of
surface region of these molten samples are
solidified shapes and textures of deposited
shown in Table 3. The effect of the contact
droplets. There are no simple models to
angles can be seen through a comparison of
predict what these will be. The final shape
the thicknesses in Table 3. Smaller spread
can be characterized the contact angles of the
diameters and larger contact angles are
bases of the droplet and their thickness.
formed on the cotton surface. Earlier studies
Contact angle measurements of molten the
showed that the dynamic contact angle samples carried out in ambient air
environments are shown in Fig. 4.
increases with the equilibrium contact angle
It was found that paraffin has a significant
[14] and that the maximum spread of a
effect on lowering the contact angle of sample
droplet decreases as the dynamic contact
droplets due to their enhancement of the
angle increases [15-17]. Very low thickness
molten samples, in turn lowering the viscosity
molten dropletsare formed from high molten
of the compared to beeswax samples. The
temperatures (100°C) and a increased
contact angle of the sample droplets on the
thickness molten droplet at low molten
cotton fabric surface not only depends on the
temperatures (70, 80 and 90 °C) as shown in
type of sample but also on the temperature
Table 3. The use of paraffin rendered the
t hicknesses to be much lower, with thickness
and the viscosity. It should be noted that v
alues reduced to only approx. 0.99 mm. 74
Vol.19, No.4, October-December 2014 Thammasat International Journal of Science and Technology 140 120 ree) g 100 le (De Paraffin g 80 n Beeswax ct a 60 ta n Co 40 20 70 80 90 100 Temperature (C)
Fig.4. Molten sample contact angles vs. temperature of paraffin and beeswax sample. Samples 70 °C 80 °C 90 °C 100 °C Paraffin Beeswax
Fig.5. Images of molten waxes droplets on cotton fabric surface compared with those of
different temperature during 70–100 °C.
Table 3. Thickness values of wax droplets on cotton fabric surface at different temperature conditions. Samples Thickness (mm) 70 º C 80 ºC 90 ºC 100 ºC Paraffin 2.41 1.99 1.53 0.99 Beeswax 2.50 2.25 1.61 1.12 75
Thammasat International Journal of Science and Technology Vol.19, No.4, October-December 2014 4. Conclusions
[4] Birshtein, V., and YaTul'chinskii, V. M.
Paraffin exhibited lower contact angles
Determination of bees wax and some
than beeswax did. It should be noted that
impurities by IR spectroscopy, Chem
contact angles correlate with the viscosity of
Nat Compd., Vol. 13, pp. 232-235, 1997.
the molten samples. It was found that molten
[5] Fallahi, E., Barmar, M., and Haghighat
samples could decrease the contact angle
Kish, M. Preparation of phase-change
(hydrophilicity) on the cotton fabric surface.
material microcapsules with paraffin or
Molten paraffin was excellent and spread on
camel fat cores: application to fabrics,
the cotton fabric surface. The utilization of
Iran polym J., Vol 19, pp. 277-286,
beeswax only increased the droplet contact 2010.
angles and the thicknesses of the droplets.
[6] Hummel D. O., Atlas of plastics additives,
In summary, DSC was available for
Analysis by spectrometric methods,
thermal characteristic determination of
Springer-Verlag Berlin Heidelberg, New
paraffin and beeswax qualitatively and York, 2002.
quantitatively, with better accuracy than than
[7] Ruguo, Z., Hua, Z., Hong, Z., Ying, F.,
traditional mercury surface measurement.
Kun, L., and Wenwen, Z., Thermal
FTIR is a convenient way to preliminary
analysis of four insect waxes based on
evaluate the wax chemical composition.
differential scanning calorimetry (DSC),
P Eng., Vol. 18, pp. 18:101 – 106, 2011. 5. Acknowledgements
[8] Hoffmann, R., and Amundsen, L. Single-
We would like to thank the Office of the
phase wax deposition experiments, J
Higher Education Commission, Thailand for
Petrol Sci Eng., Vol. 107, pp. 12-17,
granting the fund. We would also like to 2013.
acknowledge the Department of Industrial
[9] Kuzmić, A. E., Radošević, M., Bogdanić,
En gi ne er i n g, Fa cu lt y of En gi n ee ri n g,
G., Srića, V., and Vuković, R. Studies on
Rajamangala University of Technology
the influence of long chain acrylic esters
Srivijaya, Songkhla, Thailand and Materials
polymers with polar monomers as crude
Engineering Research Center (MERC),
oil flow improver additives, Fuel., Vol.
Faculty of Engineering, Prince of Songkla 87, pp.2943-2950, 2008.
Uni ve rsi ty for their fac ili ty supp orts .
[10] Pedersen, K. S., and Rønningsen, H. P. 6. References
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