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építôanyag
§ Journal of Silicate Based and Composite Materials
Effect of firing temperature on
triaxial electrical porcelain properties
made from Tanzania locally
sourced ceramic raw materials
blaSiuS NGAYAKAMO § The Nelson Mandela African Institution of Science and Technology,
Department of Materials Energy Science and Engineering § henryblasius@gmail.com
S. eugene PARK § The Nelson Mandela African Institution of Science and Technology,
Department of Materials Energy Science and Engineering
Érkezett: 2018. 02. 16. § Received: 16. 02. 2018. § https://doi.org/10.14382/epitoanyag-jsbcm.2018.19
Abstract
The study has investigated the effect of firing temperature during the production of technical
triaxial electrical porcelain, for electrical insulation applications using Tanzania locally sourced
ceramic raw materials. The green triaxial porcelain samples containing 50 wt% of Pugu kaolin,
35 wt% of Same clay and 15 wt% of feldspar were produced and fired at 1200°C-1300°C with
a heating rate of 10°C/min (dwell time of 1.5h) and cooled at 100C/min to a room temperature.
X-ray diffraction technique was used to investigate phases developed in the triaxial electrical
porcelain after firing process. The main crystalline phases revealed were mullite and quartz. The
technological properties of the triaxial electrical porcelain such as water absorption, apparent
porosity, bulk density, bending and dielectric strength were determined for each porcelain sample
fired at high temperature. The optimum physical-mechanical and electrical properties were found
at 12500C. However, the triaxial electrical porcelain properties were found to decrease with the
increase in firing temperature.
Keywords: Firing temperature, triaxial electrical porcelain, physical-mechanical and dielectric
properties
Kulcsszavak: Égetési hőmérséklet, triaxiális szigetelő porcelán, fiziko-kémiai és dielektromos
jellemzők
Blasius NGAYAKAMO
MSc Materials Scientist and Engineer
at NM-AIST. Department of Materials Energy
Science and Engineering. Fields of interest:
ceramic raw materials, flux materials and high
voltage porcelain insulators.
S. Eugene PARK
Associate Professor and chair, Materials and
Energy Science and Engineering at NM-
AIST Department of Materials Science and
Engineering, Fields of interest: Ceramic and
sustainable Energy Engineering.
1. Introduction
Triaxial electrical porcelain is composed of clay, feldspar which
are locally sourced ceramic raw materials and other ller materials
such as quartz and alumina. e raw materials play specic
roles in inuencing the properties and performance of the nal
products. Clay [Al2Si2O5 (OH)4] provides plasticity, quartz (SiO2)
maintains the shape of the porcelain structure during ring, and
feldspar [KxNa1-x (AlSi3) O8] promotes vitrication. e three
ceramic raw materials place electrical porcelain in the phase
system [(K, Na)2O-Al2O3-SiO2)] in terms of oxide hence referred
as triaxial porcelain [1, 2]. Traditional ceramic raw materials are
the potential candidate materials for the production of triaxial
electrical porcelains. e use of traditional ceramics as raw
materials instead of industrial chemicals is highly preferred due
to the lower price of the raw materials [3].
e properties of triaxial electrical porcelain are contributed
to the variations in the composition of the raw materials, the
method of production, and the ring temperature adopted
[1]. e sintered triaxial porcelain product contains mullite
(Al6Si2O13) and undissolved quartz (SiO2) crystals embedded
in glassy phase which result from the liquid phase formed by
the melting of feldspar in the raw materials [4].
erefore the desired properties of triaxial electrical
porcelains are achieved particularly during the ring process
since the technological properties of clay-based ceramics
products depend on ring conditions such as temperature
[5, 6]. However, other technological properties which are
evaluated to determine the performance of the ceramic product
aer ring are water absorption, ring shrinkage and bending
strength [6]. During the ring process, the triaxial porcelain
body undergoes several phase transitions, during which both
composition and structure change signicantly which inuence
triaxial porcelain properties at the end of the ring process
[5]. Hence, the properties of the triaxial porcelain are mainly
inuenced by sucient development of mullite during ring
process since the development of mullite in the porcelain is
highly associated with ring temperature of the porcelain which
should not be below 1150 to 1200 °C for the mullite forming
processes to be completed [5, 7]. erefore, the development of
the physical-mechanical and dielectric properties of porcelain
are contributed by each phase developed during ring which
depends on the concentration and microstructural attributes
which are inuenced by temperature and the chemical
composition of the raw materials which is an important factor
because of its eects on porcelain properties [8-11]. Since the
eect of ring temperature on the electrical porcelain properties
made from Tanzania locally sourced ceramic raw materials
is not reported. erefore, the work intends to evaluate the
eect of ring temperature on the triaxial electrical porcelains
made from Tanzania locally sourced ceramic raw materials.
However, the study focuses also on the phase changes, surface
morphology development as well as the physical-mechanical
and dielectric properties of the triaxial electrical porcelain
sample due to change in ring temperature.
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2. Experimental procedures
Pugu Kaolin was collected from the Pugu hills, 35 km west of
Dar es Salaam, Same clay and feldspar from Same, Kilimanjaro
region in the northern zone of Tanzania. e ceramic raw
materials were crushed and ball milled to reduce their size.
e particle size less than106 µm was achieved by using sieve
shaker Model RX-29-10 digit. e chemical composition of
the raw materials was analyzed by using X-Ray Fluorescence
(XRF) PANalytical, Model: Minipal4 (PW4030)-Rh X-Ray
Tube, 30kV, 0.002mA and the results are presented in Table 1.
e examination of the surface morphology of the porcelain
sample was carried out by Scanning Electron Microscope
(SEM) Model: JEOL JSM-6335F having a resolution of 10µm
at 2kV. e crystalline phase analysis of the porcelain insulator
was analyzed by X-ray diractometer Model: Bruker D2-
PHASER-40Kv/44mA. Six triaxial porcelain samples were
produced by varying the composition of the locally sourced
materials by 50%wt of Pugu kaolin, 35%wt of same clay and
15%wt of feldspar. e powder mixtures were uniaxially
compacted into rectangular shapes at 10 MPa. e porcelain
green body samples were seasoned at a room temperature for
5 days and they were oven dried at the temperature of 110 °C
for 24 hrs. e sintering of porcelain samples was done at 1200,
1250 and 1300 °C for 1.5 hrs at the ramp rate of 10 °C/min
in each ring process. e sintered porcelain bodies were le
to cool at 10 °C/min to room temperature and were subjected
to physical-mechanical properties and dielectric strength
analysis.
3. Results and discussion
3.1 Chemical composition of the raw materials
e chemical compositions of the raw materials in form of
their oxides are presented in Tabl e 1 . e study results reveal
that both clays have the higher content of silica and alumina.
However, feldspar and Pugu kaolin have a higher content
of Hematite (Fe2O3) compared to Same clay. e literature
reports that small amount of coloring oxides such as Fe2O3
and TiO2 less than 0.9% may be accepted for porcelain wares
production [12]. However, a considerable high amount of
Fe2O3 in Pugu kaolin and feldspar may not be accepted as
they may impart yellowish and reddish color in porcelain
wares unless beneciated. Feldspar has considerable higher
alkaline oxide K2O than Pugu kaolin and Same clay. During
the sintering process, the alkaline oxide K2O melts and
forms the liquid phase that contributes to densication at
higher temperatures due to the formation of the glassy phase.
Nevertheless, the quantities of the alkaline oxides depend on
the mineralogical nature of the clays and their reactivity during
melting of the clay minerals [13]. e alkaline oxides(K2O
and Na2O) play a signicant role towards vitrication,
phase transformation and mullite grain growth [14, 15].
Oxides Pugu kaolin Same clay Feldspar
SiO260.0 60.4 57.1
Al2O330.3 13.9 14.0
Fe2O33.95 1.40 3.08
MnO 0.021 0.00 0.32
CaO 0.39 0.00 1.0
Na2O0.00 0.04 0.20
K2O2.14 2.6 12.09
Table 1. Chemical composition of raw materials
1. táblázat Alapanyagok kémiai összetétele
3.2 Mineralogical composition of the raw materials
e X-ray diraction patterns of the ceramic raw materials
before and aer ring are presented in Fig. 1 as reported by
[16]. e result shows phase compositions of both Pugu kaolin
and Same clay are kaolinite, however, Pugu kaolin showed the
development of crystalline phases of mullite and quartz at a
temperature of 1400 °C. In addition, Same clay was observed
to form cristobalite and sillimanite above 1200 °C. Feldspar
contains albite, and microcline, tridymite, and quartz. Since
the major components of interests are potassium feldspar
(K2OAl2O3O6SiO2) sodium feldspar (Na2O Al2O3O6SiO2);
and lime feldspar (CaOAl2O3O6SiO2). However, the results
indicate that feldspar deposit contains a high content of potash
feldspar compared to soda feldspar which is also supported by
the chemical composition by XRF that is K2O is 12.09% while
Fig. 1. X-ray diraction patterns of Pugu kaolin, Same clay and feldspar [16]
1. ábra Pugu kaolin, Same agyag és földpát röntgendiraktogramjai [16]
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Na2O is only 0.20%.So feldspar deposit is, therefore, a potash
feldspar. Feldspar promotes vitrication of the porcelain
insulator at the end of the sintering process.
3.2 Characterization of red triaxial porcelain samples
Fig. 2 presents the results of water absorption, apparent
porosity, and bulk density respectively for the porcelain
samples versus ring temperature. e gure shows that
the best values for physical properties for triaxial electrical
porcelain are achieved at the ring temperature of 1250 °C.
is might be due to the formation of the liquid phase and
densication at this ring range. However, the values of water
absorption, apparent porosity, and bulk density were observed
to decrease at higher ring temperature. is might be due to
the expansion of trapped water bubbles inside the porcelain
matrix and change in the composition of the glassy phase [1,
3]. e results of the study are in agreement with the works
of [1, 3, 13]. e authors reported that water absorption and
bulk density increased due to vitrication and densication of
the porcelain samples. However, the physical properties were
observed to vary due to the decrease of vitrication range
and an increase of ring temperature due to the expansion
of trapped water bubbles inside the porcelain sample at high
ring temperatures. Generally, the variation of the physical
properties of the triaxial electrical porcelain might have
been caused by the method of production, chemical and
mineralogical properties of the raw materials.
Fig. 2. Physical properties of triaxial electrical porcelain sample versus ring
temperature
Fig. 2. Triaxiális szigetelő porcelán zikai jellemzői az égetési hőmérséklet
függvényében
Fig. 3 shows changes in the mechanical strength of triaxial
electrical porcelain with ring temperature. e trend shows
that the increase of mechanical strength of porcelain sample may
be due to increased densication, vitrication and in absence of
microcracks. e best mechanical strengths (both bending and
compressive strengths) were obtained at 1250 °C. However, the
mechanical strengths began to decrease above 1250 °C due to
closed pores development and a considerable amount of cracks
on the surface of the porcelain samples. e results of the current
study are in agreement with the previous studies as reported
in the works of Kitouni et al.,[13] and Olupot et al., [1]. e
authors have reported that the mechanical strength increases
due to increased densication with temperature and tends to
decrease due to development of pores at high ring temperature.
However, the mechanical strength was found to decrease with
the increase of the ring temperature due expansion of closed
pores and microcracks [1]. Hence the mechanical strength of a
porcelain sample is strongly dependent on the defects such as
pores and cracks [13].
Fig. 3. Variation of mechanical strength of triaxial electrical porcelain sample versus
ring temperature
Fig. 3. Triaxiális szigetelő porcelán mechanikai jellemzői az égetési hőmérséklet
függvényében
Fig. 4 shows the variation of the dielectric strength of
porcelain samples red at 1200, 1250 and 1300 °C. e trend
shows that the dielectric strength increases with an increase
in ring temperature and began to decrease with further
temperature rise at 1300 °C. e increase of the dielectric
strength of electrical porcelains is due to increased vitrication
range of the electrical porcelains samples. e results of the
current study are also reported by Olupot et al, [1]. e authors
evaluated ceramic raw materials from Uganda for electrical
porcelain production. e authors obtained the highest
dielectric strength of 19kV/mm at 1250 °C. However, above
1250 °C, the samples became more porous due to change in
the composition of the glassy phase. e dielectric strength
was found to decrease with the increase of ring temperature
which aected vitrication range and the dielectric properties
of the triaxial electrical porcelain.
Fig. 4. Variation of dielectric strength of triaxial electrical porcelain sample versus
the ring temperature
Fig. 4. Triaxiális szigetelő porcelán dielektromos jellemzői az égetési hőmérséklet
függvényében
In Fig. 5 the X-diraction pattern of triaxial electrical
porcelain is presented. e diractogram conrms that the
mullite and quartz phases are present in the porcelain insulator.
Both phases promote the mechanical and dielectric properties
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of the porcelain insulator. However, high peaks of quartz
may lead to high amount of glassy phase which may lower
the dielectric strength of the porcelain insulators but not the
mechanical strength of a porcelain insulator which is aected
by microcracks. e high amount glassy phase provides free
movement of mobile ions such as Na+, K+, and Al3+ which
increases the conductivity [17].
Fig. 5. X-ray diraction pattern of a porcelain insulator red at 1250 °C
Fig. 5. 1250 °C hőmérsékleten égetett szigetelő porcelán röntgendiraktogramja
Fig. 6 shows the examination of the surface morphology using
the Scanning Electron Microscope (SEM) Model: JEOL JSM-
6335F having a resolution of 10nm at 2kV. It was evidenced the
densication on the surface of the triaxial electrical porcelain
sample aer the ring process was completed.
Fig. 6. SEM micrographs showing densication of triaxial electrical porcelain sample
at 1250 °C
Fig. 6. 1250 °C hőmérsékleten égetett triaxiális szigetelő porcelán
elektronmikroszkópos felvétele
4. Conclusions
In this research work, the eect of ring temperature on
triaxial porcelain samples properties was investigated. At the
optimum ring temperature of 1250 °C, the best physical-
mechanical and dielectric properties were achieved. However,
ring beyond 1250 °C resulted in progressive deterioration of
the physical-mechanical and the dielectric properties of the
electrical porcelain samples. is might have been caused by
the development of microcracks and high content of glassy
phase caused by high peaks of quartz. So it is imperative to
be aware that, the actual ring temperature and its inuence
on the triaxial electrical porcelain properties depend on the
chemical composition of the materials under study. erefore,
the locally sourced materials need to be evaluated from time to
time in order to avoid deviation of the desired triaxial electrical
porcelain properties during the ring process.
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Ref.:
Ngayakamo, Blasius – Park, S.Eugene: Eect of ring temperature on
triaxial electrical porcelain properties made from Tanzania locally
sourced ceramic raw materials
Építő anyag – Journal of Silicate Based and Composite Materials,
Vol. 70, No. 4 (2018), 106–109. p.
https://doi.org/10.14382/epitoanyag-jsbcm.2018.19
Az égetési hőmérséklet hatása tanzániai helyben
bányászott kerámia alapanyagokból készült triaxiális
porcelán szigetelők jellemzőire
xxxxxxx
Kulcsszavak: égetési hőmérséklet, triaxiális szigetelő porce-
lán, fiziko-kémiai és dielektromos jellemzők
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