FIELD OF THE ART
[0001] The present invention relates to a polymer material preferably used for electric
insulation and other applications.
RELATED ART
[0002] Electric devices and power cables have recently been miniaturized and thus electric
field applied to their insulating materials has been increased, so that local discharge,
that is partial discharge, is generated in contact with the interior or surface of
the insulating materials. Particularly, the interior of the insulating materials has
many small voids (air spaces), and partial discharge is generated at the voids. Part
of the insulating materials is oxidized or burnt by the partial discharge, and the
properties of the insulating materials are thereby lowered. If the partial discharge
continues, it enlarges the voids and is transferred to tree-like discharge, which
lowers the insulation life of the devices and the cables and eventually causes dielectric
breakdown.
[0003] Particularly, in alternating current devices, partial discharge generates synchronously
and stationarily corresponding to the cycles of alternating voltage and presents serious
problem as compared with direct current devices.
[0004] As the mechanism for generating the partial discharge, the interior of the voids
is filled with gas, of which capacitance is small, and the voltage applied to the
gas is divided in inverse proportion to the large capacitance of the insulating materials
around the voids. Thus, the electric field strength of the voids becomes extremely
large and discharges easily.
[0005] Pulse-like or pulsating current is generated by the discharge of electric charge
accumulated in the voids.
[0006] After the pulsating voids discharges have taken place, they are charged again upon
the increase in the instantaneous value of the voltage applied. When the voltage applied
is raised, second pulse discharge is caused. Thus, sequential pulse discharges are
followed according to the increase of the electric voltage applied. When the instantaneous
value of the electric voltage applied passes through the peak value, voltage applied
to the voids turns and discharge pulse in the reverse direction is generated. The
discharge pulse is generated in the range wherein applied voltages to time vary largely,
and it forms pulses in the opposite direction every half cycle. Insulating materials
have a large number of voids, and thus electric current passing through the insulating
materials is an alternating current containing a number of pulses (as shown in Fig.
9(a) which will hereinbelow be described in more detail).
[0007] As the method for controlling partial discharge from insulating materials of devices,
there are mentioned methods of filling up voids by impregnation of the voids with
an oil having low viscosity, a voltage stabilizer or the like or by addition of a
variety of inorganic materials. The addition of inorganic materials has been conventionally
conducted and is to control discharge thanks to the semiconductive inorganic materials
deposited on the surface of the voids whereby the surface resistance of the voids
are lowered (see, Japanese Patent Laid-Open Publication No. 253711/1986).
[0008] However, the aforementioned methods of filling up voids by impregnation thereof with
an oil having low viscosity, a voltage stabilizer or the like or by addition of semiconductive
inorganic materials may not always give satisfactory results, since these methods
do not work for removing voids themselves.
[0009] The present invention has been accomplished on the basis of these backgrounds, and
the object of the present invention is to provide a polymer material which works for
removing the generation of voids affecting on insulating materials by the selection
of inorganic materials to be added and is suited preferably for electric insulation
or the like.
SUMMARY OF THE INVENTION
[0010] The present invention accomplished for solving the aforementioned problem has a feature
which comprises addition of, e.g., 0.1 - 3%, preferably 0.5 - 2.5%, more preferably
about 1% of lithium carbonate in a subdivided form, equivalent to, for example, 300
mesh or lower, to a molten polyethylene resin, percentage being by weight of lithium
carbonate + polyethylene resin, and cooling the admixture, or contact of a mass of
lithium carbonate with a molten polyethylene resin and cooling the admixture.
[0011] That is, the present inventor has found during a series of investigations for preventing
the aforementioned generation of the voids that the growth of spherulites causing
the generation of voids is inhibited by the addition of lithium carbonate, reached
the present invention. The inhibition of the growth of the spherulites with lithium
carbonate in the polyethylene resin containing lithium carbonate is also recognized
even when the lithium carbonate added is removed therefrom.
BRIEF DESCRIPTION OF THE DRAWINGS
[0012]
Figs. 1a, 1b and 1c show spatial configurations that the polymer chain of a polyethylene
resin can take;
Figs. 2a and 2b show crystal structures of a polyethylene resin;
Fig. 3 is a perspective view showing how a polymer chain of polyethylene is folded;
Fig. 4 is a photomicrograph showing a crystal structure of lamella microcrystals;
Fig. 5 is a polarization photomicrograph showing a crystal structure of spherulites
of a polyethylene resin;
Figs. 6a and 6g are polarization photomicrographs showing crystal structures of spherulites
of polyethylene having no or various powder materials added;
Fig. 7 shows absorbance characteristics of the gauche chains of polyethylenes having
no or various powder materials added;
Fig. 8 shows a side view of an electrode designed for partial discharge determination;
Figs. 9a and 9b are time charts showing wave forms of discharge currents;
Fig. 10 is a chart showing frequency of generation of discharge pulses on polyethylenes
having no or various powder materials added;
Fig. 11 is a chart showing absorbance characteristics of ketonic organics generated
upon partial discharge of polyethylenes having no or various powder materials added;
Figs. 12a to 12c are polarization photomicrographs of crystal structures of spherulites
of polyethylene resins; and
Figs. 13a to 13c are polarization photomicrographs showing crystal structures of spherulites
of various polyethylene resins after the treatment with xylene under heating into
solution.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0013] The present invention is characterized by,
inter alia, polyethylene resins having no or reduced content of spherulites by the contact of
the resin with lithium carbonate.
Polyethylene resins to be treated
[0014] Polyethylene resins which produce the polyethylene resins having no or reduced quantity
of spherulites in accordance with the present invention can be any of such resins
solely or predominantly comprising ethylene, non-crosslinked or crosslinked, produced
by any suitable process which may be polymerization of ethylene.
[0015] Polyethylene resins (e.g. a low density polyethylene resin having a density of 0.91
- 0.93 g/cm³ and medium and high density polyethylene resins having a density of 0.94
- 0.97 g/cm³ such as ASAHI DOW 6545 polyethylene resin pellets) is a mass of many
linear polymer chains

Polyethylenes having many side chains such as CH₃, C₂H₅ or C₄H₉ on the linear polymer
chain is referred to as low density polyethylene resins, and the ones having few such
side chains are referred to as medium or high density polyethylene resins.
[0016] The polymer chains of a polyethylene resin can take the spatial configurations represented
in Figs. 1a, 1b and 1c. In the figures, solid dots represent carbon atoms, and Fig.
1 shows the most stable configuration wherein the carbon atoms 1 and 4 are arranged
in the opposite directions to each other with reference to the chain of the bond between
carbon atoms 2 and 3. Such a configuration is called a trans bond, and all of polyethylene
resins at ordinary temperature take this bond. However, when the polyethylene resin
is heated to an elevated temperature, part of the resin takes a metastable configuration
which is called a gauche bond as shown in Figs. 1b and 1c. Such a bond indicates a
state that carbon atoms 1 and 4 are twisted at ±120° with reference to the chain of
the bond between carbon atoms 2 and 3. In Figs. 1a, 1b and 1c, vacant dots represent
the other configurations that the carbon atoms of solid dots can take.
[0017] The polymer chain which takes the gauche bond, viz. gauche chain, can be easily identified
from the absorbance of infrared absorption at 1078 cm⁻¹ and 1352 cm⁻¹. The present
inventor has found that when lithium carbonate is added to a polyethylene resin, strong
absorptions attributed to the gauche bond appears and indicates the twisting of a
part of the main chain of the polyethylene, which inhibits the growth of spherulites
described below.
[0018] Polyethylene resins have a zigzag plain structure wherein the main chain has a trans
bond without twisting, and the polymer chain is regularly arranged to form crystal
structures shown in Figs. 2a and 2b, wherein a large circle represents a carbon atom
and a small circle represents a hydrogen atom.
[0019] In this connection, a, b and c are lattice constants which represent the three axes
of a unit lattice, and a = 7.40 Å, b = 4.93 Å and c = 2.53 Å in the case of a polyethylene
resin.
[0020] The parallel main chain is folded at a length of ℓ = 100 - 150 Å as shown in Fig.
3 and takes a lamella microcrystal as shown in Fig. 4. The crystals are those deposited
from a dilute xylene solution of the polyethylene which contain the polyethylene resin
in a proportion of about 0.1% by weight to xylene. On the other hand, in a solid prepared
from a molten state at an elevated temperature of at least a melting point 105°C of
a low density polyethylene resin or of at least a melting point 125°C of a medium
or high density polyethylene resin or from a concentrated solution of a polyethylene
resin dissolved in a small amount of a solvent at the elevated temperature, the lamella
microcrystals comprise microcrystals piled up around a given nucleus in the radial
direction, and thus result in forming spherulites which is produced with spherical
symmetry as shown in Fig. 5. The spherulites are produced instantaneously.
[0021] In general, a polyethylene resin prepared from the molten state is such that ca.
80% by weight of it is crystallized in a state of spherulites. Such resins are called
a crystalline polymer. The low density polyethylene resin used in the present invention
has a crystallinity of 86.6%, provided that the crystals in the state of spherulites
are limited to the case that the main chain of the polymer has a trans bond.
Chemistry of polyethylene resins contacted with Li₂CO₃
[0022] When lithium carbonate (Li₂CO₃) is added to a molten polyethylene resin, about 3
- 4% by weight of the main polymer chain may be transformed into one comprising non-crystalline
gauche bonds as judged from the gel fraction of the resin described later, whereby
the production of spherulites is suppressed due to formation of the gauche bonds.
As a result, sharp infrared absorptions attributed to the gauche bond are observed
in the samples having lithium carbonate added.
[0023] The present invention is now explained with reference to Figs. 6 - 12. Some detailed
explanation of each figure is as follows:
Among Figs. 6a, 6b, 6c, 6d, 6e, 6f and 6g, Figs. 6a to 6e are polarization photomicrographs
showing crystal structures of spherulites of low density polyethylene resins having
no or various additives added, wherein Fig. 6a shows the case of the resin having
no additive, Fig. 6b shows the case of the resin having 1% by weight of lithium carbonate
added, Fig. 6c shows the case of the resin having 1% by weight of cobalt carbonate
added, Fig. 6d shows the case of the resin having 1% by weight of quartz added and
Fig. 6e shows the case of the resin having 1% by weight of calcium carbonate added;
Figs. 6f and 6g are polarization photomicrographs showing crystal structures of spherulites
of high density polyethylene resins having no additive and lithium carbonate added,
respectively, wherein Fig. 6f shows the case of the resin having no additive and Fig.
6g shows the case of the resin having 1% by weight of lithium carbonate added;
Fig. 7 shows absorbance characteristics of the gauche chains of polyethylenes having
no additive or lithium carbonate, calcium carbonate, cobalt carbonate or quartz added;
Fig. 8 shows a side view of an electrode designed for partial discharge determination;
Figs. 9a and 9b are time charts showing waveforms of discharge currents, wherein
Fig. 9a is a waveform chart of alternating current and Fig. 9b is a pulse waveform
chart after filtration treatment;
Fig. 10 is a chart showing frequency of generation of discharge pulses on polyethylenes
having no additive or lithium carbonate, calcium carbonate, cobalt carbonate or quartz
added;
Fig. 11 is a chart showing absorbance characteristics of ketonic organics generated
upon partial discharge on partial discharge of polyethylenes having no additive or
lithium carbonate, calcium carbonate, cobalt carbonate or quartz added;
Figs. 12a, 12b and 12c are polarization photomicrographs of crystal structures
of spherulites of polyethylene resins, wherein Fig. 12a pertains the case where the
polyethylene resin having lithium carbonate and paraffin for lowering the viscosity
added both in 10% by weight, respectively, was heated and the lithium carbonate added
was removed by filtration, Fig. 12b pertains to the case where the polyethylene resin
in which one lithium carbonate particle of diameter of 100 µm had been added was heated
to be molten, the lithium carbonate added was then removed and the resin was melted
again by heating, and Fig. 12c pertains to the same case as shown in Fig. 12b except
for the fact that the left part adjacent to the part shown in Fig. 12b is shown; and
Figs. 13a, 13b and 13c are polarization photomicrographs showing crystal structures
of spherulites of various polyethylene resins after the treatment with xylene under
heating into solution, wherein Fig. 13a pertains to the case where the crystal structure
of the spherulite that the sample of the polyethylene resin which had undergone the
treatment with xylene at 100°C under heating into solution for 10 minutes was dried
and then melted by heating, Fig. 13b pertains to the case where the sample of the
polyethylene resin having 1% by weight of lithium carbonate added and treated was
subjected to the treatment such that the resin was heated at 100°C for 10 min. in
the presence of xylene and products insoluble in xylene including lithium carbonate
was removed by a filter paper and the sample after being dried was heated; and Fig.
13c pertains to the case where the sample treated according to the method described
in Fig. 13b was crosslinked chemically with a crosslinking agent of dicumyl peroxide.
- 1, 2, 3, 4
- carbon atoms,
- ℓ
- length of the folded parallel main polymer chain of the polyethylene resin in Angstrom:
Å,
- a, b, c
- lattice constants showing the lengths of the three axes constituting the unit lattice.
[0024] The spherulites are observed in a polarization photomicroscope as a substance having
black cross dark lines, and the micrographs of the spherulites of the low density
polyethylene resins having a density of 0.91 g/cm³ are shown in Figs. 6a, 6b, 6c,
6d and 6e. Fig. 6a shows the spherulites of the polyethylene resin having a diameter
in the range of about 20 - 30 µm. Fig. 6b shows the sample of the polyethylene resin
having 1% by weight of lithium carbonate added, in which white parts is lithium carbonate
and large spherulites have disappeared while spherulites having a diameter of about
5 µm are dimly seen.
[0025] Figs. 6c, 6d and 6e are the photomicrographs of the samples for comparison having
1% of cobalt carbonate (black part), quartz or calcium carbonate, respectively, added,
in which a number of spherulites having got out of shape are present. Furthermore,
it has been confirmed that the spherulites are observed also in the cases of the polyethylene
resins having a lithium salt compound such as lithium oxalate or lithium fluoride
added.
[0026] Moreover, Figs. 6f and 6g are photomicrographs of a low-pressure, high density polyethylene
resin having a density of 0.955 g/cm³. Fig. 6f shows the spherulites, which have a
diameter of 90 µm and are large and clear. Fig. 6g shows the sample which underwent
the addition of lithium carbonate and heating, in which the spherulites have disappeared.
[0027] As is apparent from the above description, lithium carbonate is most effective for
the inhibition of the growth of the spherulites.
[0028] Fig. 7 shows absorbance characteristics at 1078 cm⁻¹ in the infrared absorption of
the gauche bonds of low density polyethylenes having 0.5 - 5% of various inorganic
materials added and indicates that the larger the absorbance, the more the gauche
chain. The polyethylene resin having quartz added has the largest absorbance, which
is due to the wide strong absorption at 1080 cm⁻¹ including also 1078 cm⁻¹ which is
not attributed to the gauche bonds, and no particular inhibition of the growth of
the spherulites are thus observed.
[0029] Particularly, when lithium carbonate is added, a larger absorption appears as compared
with the addition of calcium carbonate or cobalt carbonate. In this connection, it
is only lithium carbonate that shows an infrared absorption at 1078 cm⁻¹ corresponding
to the infrared absorption of the gauche bond in these inorganic materials, and lithium
carbonate exhibits an absorbance of about 0.05 when it is compacted into a tablet.
It is the inventor's assumption that the molecular vibration of lithium carbonate
as an inorganic material added in a small amount into a polyethylene resin induces
the molecular vibration of the gauche bond of the polyethylene resin as an organic
material, the trans chain of the polyethylene main polymer chain is transformed into
the gauche chain, the adjacent main polymer chain due to the folding is then transformed
into the gauche chain by the induction effect, and the sequential propagation of the
induction effect produces a number of molecular chain of the gauche bond.
[0030] In the case of the polyethylene resin in which the gauche chain is formed by the
addition of lithium carbonate, part of the non-crystallized portion is transformed
into the gauche chain, and the production of large spherulites is thereby suppressed.
Electrical aspect of polyethylene resins contacted with Li₂CO₃
[0031] The measurement of the anti-partial discharge characteristics of samples having various
inorganic materials added are explained below.
[0032] A molten material having an inorganic material added is formed into a film sample
having a thickness of 0.1 mm by a heating roll stretcher at 190°C, arranged between
electrodes shown in Fig. 8 and dipped into an oil such as silicon oil in order to
prevent discharge from the ends of the electrodes. An electric field having an electric
field strength of 50 KV/mm is applied, and the frequency of the generation of pulses
at an electric charge of 10 pc (pc: 10⁻¹² coulomb) or more in proportion to the amount
of the inorganic material added is measured by a corona measuring apparatus. The "frequency
of the generation of pulses" indicates, as shown in, for example Fig. 9b, the frequency
of the generation of only a pulse component obtained by the filtration treatment of
an alternating current containing a number of pulses, having a unit of counts per
second referred to as cps. The results are shown in Fig. 10.
[0033] As Fig. 10 shows, when each of the inorganic materials except cobalt carbonate is
added in an amount of 1%, the frequency of generation exhibits the minimum and decreases
to one fourth of the case of the polyethylene resin having no additive, which indicates
the improvement of the anti-partial discharge characteristics.
[0034] While the sample having quartz added has a minimal frequency of the generation of
discharge pulse, such a minimal frequency is due to the lowering of the void surface
resistance. The sample having quartz added has a very distinguished defect of the
oxidative deterioration due to the partial discharge described below.
[0035] The electrodes for homogeneously denaturating and oxidatively deteriorating the film
sample by partial discharge are desirably those comprising a pair of parallel plates
having a gap therebetween of a 1 mm. When a sample is arranged within the gap and
an alternating voltage of 50 Hz and 6 KVrms is applied, a large amount of ozone is
generated within the gap by the strong partial discharge, and the sample generates
a large amount of organic acids, particularly ketonic acids, by ozone oxidation. Thus,
the sample is deteriorated due to the lowering of the insulating properties.
[0036] It is possible to observe the extent of the deterioration due to the partial discharge
by the infrared absorbance of the ketone at 1715 cm⁻¹.
[0037] Fig. 11 thus shows the absorbance characteristics of ketonic organic acids generated
from samples having various inorganic materials added in an amount of 1%, respectively,
plotted against the discharge time. As the figure shows, the samples having cobalt
carbonate or quartz added are deteriorated more seriously than the sample having no
additive. The least deterioration is observed in the sample having lithium carbonate
added, which has a deterioration resistant properties against partial discharge.
[0038] As described above, it has been found to be optimal to add about 0.8 - 1.4% by weight,
particularly about 1% by weight, of fine powder of lithium carbonate of, for example,
300 mesh or 46 µm in average diameter or smaller improve polyethylene resins by reducing
the generation of the partial discharge of the polyethylene resin and minimizing the
oxidation or deterioration due to the partial discharge thereby improve anti-partial
discharge properties of the polyethylene resins. Thus, the production of the spherulites
of polyethylene can be inhibited and the generation of the partial discharge can be
suppressed by the disappearance of voids between one spherulites and the other. Moreover,
the possibility of the polyethylene main polymer chain to take the configuration of
the gauche bond indicates the "filling" effect of voids produced during the molding
of the resin, and thus the voids will disappear.
Li₂CO₃-free compositions
[0039] Lithium carbonate which has, as shown above, an effect to diminish the voids between
one spherulite and the other in the mass of polyethylene resins and voids produced
during the molding scarcely affect the electric insulating property of the polyethylene
resin even when it remains in the resin if its content is about 1%. It is, however,
desirable to remove the added lithium carbonate after the transformation of the polyethylene
main polymer chains into the gauche chain has taken place in consideration that the
mechanical strength or the like of the polyethylene resin be maintained at the highest
level possible. When experiments were conducted on the basis of the viewpoint, it
has been found that the gauche chain of the polyethylene resin which has been once
transformed by the addition thereto of lithium carbonate may not revert to the original
trans chain even after the removal of the lithium carbonate added and thus a new polyethylene
resin containing the gauche chain and having functions excellent in thermal, electric
or chemical properties is thereby formed. In this case, the lithium carbonate added
can be considered to act as a catalyst on the polyethylene resin.
[0040] Fig. 12a shows the polarization photomicrograph of the sample that to a molten polyethylene
resin was added 10% by weight of lithium carbonate having a particle size of 65 mesh
(210 µm) or more, a part of the polyethylene main polymer chain was thereby transformed
into the gauche chain, 10% of paraffin (melting point: 60 - 62°C) was then added for
lowering the viscosity to convert it into a fluid, and lithium carbonate was removed
from the fluid composition by a filter having 300 mesh. No spherulites are observed
in this microphotograph, and lithium carbonate is not contained in the sample and
has thus acted only as a catalyst on the polyethylene resin.
[0041] Fig. 12b shows the polarization microphotograph of the sample of a polyethylene resin
that one particle of lithium carbonate having a particle diameter of 100 µm is placed
in a polyethylene resin and the polyethylene resin undergoes the heat treatment at
190°C, the lithium carbonate added is removed, and another heat treatment is again
conducted to the polyethylene resin. The dark area at the right hand side of the figure
shows the trace that the lithium carbonate has been removed.
[0042] In this case, it is observed that within 200 µm in the radial direction from the
lithium carbonate placed the spherulites are inhibited from growth and will not be
reproduced easily even by the further heat treatment after the removal of the lithium
carbonate added. The spherulites in the center and the left hand side of Fig. 12c
which shows the portion adjacent to the left side of the microphotograph shown in
Fig. 12b are found in the region which is too remote from the lithium carbonate placed
to produce the gauche chain and to which the influence of placement of the lithium
carbonate has not reached.
[0043] It has thus been confirmed from the above description that the gauche chain once
produced by the addition of lithium carbonate is thermally stable even if the lithium
carbonate has been removed and is not dissolved easily by heating whereby the effect
of the lithium carbonate on inhibiting the growth of the spherulites is maintained.
[0044] It is believed in the art that the gauche chain of a polymer has a higher energy
by about 500 - 600 Cal/mole as compared with the trans chain and thus is stable thermally
(see Physical Property and Molecular Structure of Polymers, in Japanese: KAGAKU DOJIN;
page 64; published on May, 1973). As a test method of the resistance to thermal decomposition
of high molecular resins, there is a way in which the half-life temperature determined
by the reduction in the weight by the thermal decomposition of a sample is used as
a thermal decomposition temperature (Durability of Plastics, in Japanese: KOGYO CHOSAKAI;
page 65; published on May, 1975).
[0045] For example, this method comprises heating about 10 mg of a sample isothermally for
5 minutes for each of the temperatures of room temperature and the temperatures of
100°C, 200°C, 300°C and so on so that the temperature is raised by 100°C until the
reduction of the weight by the pyrolysis of the sample reaches 0 mg, obtaining the
reduction characteristics of the sample weight at the respective temperatures and
thus determining the temperature corresponding to the level at which the weight reduction
rate is 50% to be the half-life temperature which is finally used as a thermal decomposition
temperature.
[0046] The thermal decomposition temperature obtained by this method is 357°C for the low
density polyethylene resin; 430°C for the sample of the low density polyethylene resin
which has undergone the heat treatment in the presence of 0.5% by weight of lithium
carbonate of 300 mesh added; 460°C for the sample of the low density polyethylene
which has undergone the heat treatment in the presence of 1.0%, 10% and 20% by weight
of lithium carbonate added; and 430°C for the sample of the low density polyethylene
which has undergone the heat treatment in the presence of lithium carbonate and of
10% by weight of paraffin shown in Fig. 12a followed by removal of the lithium carbonate
by filtration. It has thus been found that the thermal decomposition temperatures
are raised by 73 to 103°C by the heat treatment in the presence of lithium carbonate
whereby the heat resistance is extensively improved.
[0047] It is also known in the art that polymer resins are crosslinked by crosslinking agents
or due to hydrogen bonding to form a gel which is insoluble in a solvent. The extent
of the cross-linking or gelling can be represented by a gel fraction determined on,
for example, a low density polyethylene resin by dissolving the polyethylene with
xylene in 10 times by weight of the sample at 100°C for 10 minutes, separating the
insoluble resin component by a filter, weighing it, and indicating the weight in %
by weight.
[0048] While the gel fraction of the low density polyethylene resin after the aforementioned
xylene treatment is 0%, it is 3.5% in the sample which has undergone the heat treatment
in the presence of 1% by weight of lithium carbonate. In this case, it is believed
that the gauche chains produced by lithium carbonate added produces the gel.
[0049] Fig. 13a shows the polarization photomicrograph of the sample that the xylene solution
having 0% of the aforementioned gel fraction was dried and then heated to be molten.
The spherulites have a diameter as small as about 10 µm and is out of shape. In this
case, the molecular chains of the polyethylene resin are swollen by the xylene, and
small spherulites are produced.
[0050] Fig. 13b shows the polarization photomicrograph of the sample produced by dissolving
by xylene the aforementioned polyethylene resin having lithium carbonate added and
having 3.5% of the gel fraction, filtering the solution, drying the solution and then
heating to be molten, wherein no spherulites are observed contrary to the case shown
in Fig. 13a.
[0051] Thus, it has thus been found that even if the lithium carbonate once added to a polyethylene
resin is removed by filtration from the solution of the polyethylene resin in xylene,
the gauche chain produced is not decomposed by the solvent and retaining its function
to inhibit the production of spherulites.
[0052] Fig. 13c shows the polarization photomicrograph of the sample shown in Fig. 13b having
been chemically cross-linked with a cross-linking agent which is dicumyl peroxide.
No production of the spherulites are observed also in this case.
[0053] When a high electrical insulating property is expected of polyethylene resins, the
resins should desirably be of a single species and pure, and thus lithium carbonate
used for the production of the gauche chain is desirably removed. Even when lithium
carbonate once added to polyethylene resins is removed therefrom when the resins are
"fluid" upon dissolution or melting by filtration or centrifugation, gauche chain
once produced will not be transformed into the trans chain and a homogeneous polyethylene
resin free of a compounding additive can be obtained with maintenance of a pulse discharge
suppressing effect due to the disappearance of voids between one spherulite from the
other. For making the polyethylene resin "fluid", use can be made, at 60°C or higher,
of 5% by weight or less of a solvent such as a paraffinic hydrocarbon, an aromatic
hydrocarbon or a chlorinated hydrocarbon, for example paraffin, tetralin, xylene,
carbon tetrachloride or perchloroethylene. Therefore, a resin having electric and
mechanical properties superior to those of the polyethylene resin having lithium carbonate
added in an amount, for example, of about 1% by weight (when the lithium carbonate
is in the powder of around 300 mesh) can be prepared.
[0054] Moreover, instead of transforming a part of the polyethylene main polymer chain into
the gauche chain by addition of lithium carbonate, which acts as a catalyst as described
above, and then removing the lithium carbonate, the polyethylene resin in the molten
state may alternatively be agitated with the lithium carbonate which has been molded
into a rod with a bonding agent as an alternate application of lithium carbonate as
catalyst. In this case, the lithium carbonate and the polyethylene resin are generally
contacted with each other less sufficiently, it may thus be necessary to conduct a
long period of treatment.
[0055] In this case, the lithium carbonate used functions as a catalyst, and thus its function
is accelerated by increasing the reaction surface of and the reaction time with the
lithium carbonate bar regardless of the particle size or the added amount of the lithium
carbonate when lithium carbonate is powder. In this embodiment wherein no residual
lithium carbonate is contained in the so-treated polyethylene resins, the deterioration
of the frequency property of the pulse generation which could presumably be due to
the residual lithium carbonate when the lithium carbonate added is not removed is
not observed.
[0056] Moreover, while examples of applying the lithium carbonate to the ordinary polyethylene
resin has been described, it is needless to say that the lithium carbonate can also
be applied to the heat resistant cross-linked polyethylene resins.
Use of the polyethylene resins
[0057] The polymer materials suitable for electrical insulation which is obtained by adding
about 1% by weight of lithium carbonate fine powder (of, e.g. 300 mesh) as "a filler"
to a molten polyethylene resin which is then molded into a certain form, or alternatively
by transforming a part of the polyethylene main polymer chains into the gauche chains
by lithium carbonate used as a catalyst to a molten polyethylene resin which is then
molded into a certain form as described above has an excellent partial discharge resistant
property which can suppress the generation of the partial discharge due to the disappearance
of the voids between one spherulite and the other and the voids generated during the
molding, and it is possible to suppress the decrease of the insulation life in power
cables such that a conductor is covered and insulated with a polyethylene resin in
accordance with the present invention.
[0058] In this connection, it is needless to say that the aforementioned polymer material
in accordance with the present invention suitable for electric insulation or the like
can be used not only for the power cable but also for insulating materials of electric
devices or the others such as a variety of containers, packings, liners, packaging
films or fibers.
[0059] Furthermore, as the polyethylene resins, there can be used as described above not
only the high-pressure low density polyethylene resins but also medium- or low-pressure
high density polyethylene resins.
Examples of practice
[0060] The present invention is now explained with reference to the Examples and Comparative
Examples of the preparation of samples.
[0061] Low density and medium or high density polyethylene resins are thermoplastic resins,
which can be formed or molded into any shapes by heating and produce a large number
of molded articles. There are mentioned for example a film by a heating roll stretcher,
a cover for insulating an electric wire by an extruder, a casting for insulating a
power cable by heating impregnation or the like.
[0062] The forms of these resins for molding are generally prepared in the form of pellets
(particles) to ensure that molding by heating can be easily conducted.
[0063] Various samples for the illustration of the present invention have been obtained
by first preparing the aforementioned resin in the form of pellets or blocks and then
molding it into a certain shape as a sample for test.
[0064] As the samples for measuring the infrared absorbance characteristics (Fig. 7), the
frequency properties of pulse generation by partial discharge (Fig. 10) and the oxidation
and deterioration properties by the discharge with parallel plate electrodes (Fig.
11), respectively, low density polyethylene resin having a gravity of 0.91 g/cm³ (ASAHI-DOW
M6545) was used as a polyethylene resin for the test, and samples were prepared from
the resin, when the resin with no additive was tested, by heating pellets of the resin
by means of a pair of molding rolls heated at 190°C into a film sample of 0.1 mm thickness;
and, when the resin with an additive was tested, by placing pellets of the resin (in
a hard glass beaker) in a desiccator, heating the pellets to 190°C by an electric
heater in an atmosphere of nitrogen to be molten, to which a variety of fine powders
as additives such as lithium carbonate having a particle size smaller than 300 mesh
(46 µm) were added, agitating the mixture for about 5 minutes until it appeared to
be mixed well to naked eyes, and transferring the melt to a teflon beaker to form
pellets which were upon being cooled gradually to room temperature subjected to the
same rolling operation used for the resin with no additive.
[0065] As the samples for polarization photomicrographs (Figs. 6a, 6b, 6c, 6d, 6e, 6f and
6g, Figs. 12a, 12b and 12c, and Figs. 13a, 13b and 13c) for the illustration of the
present invention, small amounts (several milligrams) of the various resins in the
form of pellets were taken on cover glasses for a microscope and heated at 190°C for
about 10 seconds to form photomicrographic samples, respectively.
[0066] Moreover, a sample in an amount of 10 mg for measuring the temperature of pyrolysis
was also taken from the aforementioned resins in the form of pellets.
[0067] As the raw materials for the resins in the form of pellets, there were used a low
density polyethylene resin pellet (ASAHI-DOW M6545) and a high density polyethylene
resin (MITSUI POLYCHEMICAL HZ7000F).
[0068] Examples for the preparation of various resins in the form of pellet according to
the present invention are described below.
Example 1
[0069] The low density polyethylene resin having a density of 0.91 g/cm³ in a hard glass
beaker was placed in a desiccator, heated to 190°C with an electric heater in an atmosphere
of nitrogen to form a melt, to which a fine powder of lithium carbonate having a particle
size smaller than 300 mesh (46 µm) was added in an amount of 1% by weight, and the
mixture was stirred for about 5 minutes until it was mixed well to naked eyes, then
transferred into a teflon beaker to form a pellet, which was cooled gradually to room
temperature to prepare a sample. The sample has the minimal values in both of the
frequency of pulse generation by the partial discharge shown in Fig. 10 and the oxidation
and deterioration by discharge with parallel plate electrodes shown in Fig. 11, and
particularly large spherulites as shown in Fig. 6b have disappeared. It is pliable
and thus suitable for the insulating materials of powder cables.
Example 2
[0070] The high density polyethylene resin having a density of 0.955 g/cm³ was heated to
210°C by the same heating method as in Example 1 to form a melt, to which lithium
carbonate having a particle size smaller than 300 mesh (46 µm) was added in an amount
of 1% by weight and treated in the same manner as in Example 1 to prepare a sample
in the form of pellets. In this sample, the spherulites have completely disappeared
as shown in Fig. 6g.
Example 3
[0071] The low density polyethylene resin having a density of 0.91 g/cm³ was heated to 190°C
by the same heating method as in Example 1 to form a melt, to which 10% by weight
of lithium carbonate having a particle size larger than 65 mesh (210 µm) was added
and 10% by weight of paraffin was further added for lowering the viscosity of the
melt, the mixture was stirred for about 20 minutes to form pellets, which were gradually
cooled to room temperature. The resin in the form of pellets was then heated into
a melt at 210°C for 25 minutes in an atmosphere of nitrogen, and the lithium carbonate
added was removed by a 300 mesh (46 µm) and the melt was processed into pellets, which
were gradually cooled to room temperature to form a sample. The sample is the one
on which lithium carbonate has acted as a catalyst, and large spherulites have disappeared
as shown in Fig. 12a.
Example 4
[0072] The resin in the form of pellets prepared in Example 1 and having 1% by weight of
lithium carbonate added was subjected to dissolution in pure xylene in a weight of
10 times of the sample resin at 100°C for 10 minutes, the xylene insoluble component
containing lithium carbonate was removed by a filter, and the filtrate was left standing
for drying to form a sample. When the sample was heated into a melt at 190°C for 1
minute, the production of the spherulites were not observed as shown in Fig. 13b.
Also, in this case, lithium carbonate has acted as a catalyst.
Example 5
[0073] The sample obtained in Example 4 was heated with 2% by weight of dicumyl peroxide
as a cross-linking agent at 130°C for 10 minutes to prepare a sample which was crosslinked
chemically. In the sample, no spherulites are not observed as shown in Fig. 13c.
Comparative Example 1
[0074] When no additive is added to the low density polyethylene resin having a density
of 0.91 g/cm³, spherulites having a diameter of 20 - 30 µm are observed as shown in
Fig. 6a.
Comparative Example 2
[0075] When no additive is added to the high density polyethylene resin having a density
of 0.955 g/cm³, large and clear spherulites having a diameter of about 90 µm are observed
as shown in Fig. 6f.
Comparative Example 3
[0076] The low density polyethylene resin having a density of 0.91 g/cm³ is heated to 190°C
into a molten state by the same heating method as in Example 1, cobalt carbonate having
a particle size smaller than 300 mesh (46 µm) was added in an amount of 1% by weight,
and a sample in the form of pellets was then prepared in the same way as in Example
1. The sample has, as shown in Fig. 6c, an extremely large number of spherulites observed,
although the spherulites are out of shape.
Comparative Example 4
[0077] The low density polyethylene resin having a density of 0.91 g/cm³ is heated to 190°C
into a molten state by the same heating method as in Example 1, quartz having a particle
size smaller than 300 mesh (46 µm) was added in an amount of 1% by weight, and a sample
in the form of pellets was then prepared in the same way as in Example 1. The sample
has, as shown in Fig. 6d, an extremely large number of spherulites observed, although
the spherulites are out of shape.
Comparative Example 5
[0078] The low density polyethylene resin having a density of 0.91 g/cm³ is heated to 190°C
into a molten state by the same heating method as in Example 1, calcium carbonate
having a particle size smaller than 300 mesh (46 µm) was added in an amount of 1%
by weight, and a sample in the form of pellets was then prepared in the same treatment
as in Example 1. The sample has, as shown in Fig. 6e, an extremely large number of
spherulites observed, although the spherulites are out of shape.