TECHNICAL FIELD
The present invention relates to a casing enclosed type
magnetic core, for example, a casing enclosed type magnetic
core which is used in a magnetic component for use in an
electronic circuit.
BACKGROUND ART
In a magnetic component constructed by forming a coil
produced by winding a wire round a magnetic core, a wire
coated with an insulating film is used as the coil to prevent
the coil from short-circuiting during the formation of the
coil.
Since the magnetic core is harder than the insulating
film formed on the wire, when the wire is wound round the
magnetic core directly, the insulating film of the wire may be
damaged and short-circuited during winding.
To prevent the insulating film from being damaged, the
magnetic core is enclosed in a resin casing and then a coil is
formed around the casing, or a coil is formed around a resin
bobbin and then the bobbin is attached to the magnetic core.
Which method among the above should be used to protect
the insulating film depends on the shape of the magnetic core
of interest.
For example, in the case of a magnetic core composed of
a magnetic alloy thin belt, the former method is employed
because the shape of the magnetic core is almost annular.
Incidentally, when the magnetic core is enclosed in a
casing, the magnetic core moves in the casing and collides
with the wall of the casing during transportation if the
magnetic core is not fixed in the casing.
When the magnetic core collides with the wall of the
casing, it may be destroyed by stress applied to the magnetic
core or the magnetic characteristics of the magnetic core may
deteriorate.
Further, the impact may be transmitted to other
component and exert a bad influence on the component.
Still further, a soldered portion of the coil may peel
off due to the impact of the collision.
Therefore, in order to form a casing enclosed type
magnetic core, the movement of the magnetic core in the casing
must be prevented to ensure the reliability of the magnetic
core as a magnetic component.
In this case, to prevent the movement of the magnetic
core in the casing, it is conceivable to make the size of the
inner wall of the casing the same as the outer size of the
magnetic core.
However, when a core is formed by winding a wire round
the casing enclosed type magnetic core, the casing may be
deformed by the wound wire and stress may be applied to the
magnetic core.
Further, since the magnetic core is in direct contact
with the casing, the vibration of the magnetic core is easily
transmitted to the casing and a big sound is generated when
the magnetic core is excited.
For that reason, as conventional means for preventing
the generation of a sound, a casing having an inner diameter
larger than the outer size of the magnetic core is prepared
and an adhesive is filled in or applied to a space between the
casing and the magnetic core.
Meanwhile, when the casing is made much larger than the
magnetic core, a magnetic flux in the space between the
magnetic core and the casing must be taken into account.
Therefore, to produce the above casing enclosed type
magnetic core, a casing slightly larger than a magnetic core
is used.
As described above, by filling or applying an adhesive
to the space between the magnetic core and the casing, the
movement and vibration of the magnetic core in the casing are
prevented from being transmitted to the casing.
However, when the adhesive is used and temperature
inside the casing becomes higher than room temperature, the
adhesive fixing the casing and the magnetic core expands.
Therefore, the vibration absorption power of the
adhesive may be lost by a distortion caused by a volume
increase due to the expansion of the adhesive depending on the
amount of the adhesive filled or coated.
It is an object of the present invention to provide a
casing enclosed type magnetic core which has high reliability
as a magnetic component and makes a small sound.
DISCLOSURE OF THE INVENTION
A first feature of the present invention resides in a
casing enclosed type magnetic core which comprises (a) a
magnetic core, (b) a casing for containing the magnetic core,
and (c) powders filled at least partially in a space between
the magnetic core and the casing.
That is, the powders are filled in the space between
the casing and the magnetic core to fix the casing and the
magnetic core, prevent vibration absorption power from being
lost by using an adhesive, and prevent and suppress the
transmission of the vibration of the magnetic core to the
casing.
In this case, the charging rate of the powders filled
in the space between the magnetic core and the casing is, for
example, 1 to 150%, preferably 10 to 150%, more preferably 10
to 120%, the most preferably 10 to 100%.
Incidentally, the charging rate of the powders is
calculated from the following equation.
charging rate (%) = mass of powders (g)/(volume of
space [cm3] x bulk density of powders [g/cm3]) x 100
The bulk density of the powders [g/cm3] was measured in
accordance with ASTM D1895-69.
Further, in the casing enclosed type magnetic core of
the present invention, either magnetic or non-magnetic powders
can be used.
Subsequently, a second feature of the present invention
resides in a casing enclosed type magnetic core, wherein the
maximum value of short diameter of the powder filled is in the
range of 5 to 500 µm.
Incidentally, the maximum value of short diameter of
the powder filled is particularly preferably in the range of
100 to 400 µm.
In this case, the short diameter of the powder is the
diameter of the powder when the powder is spherical (having a
circular section) and the shortest diameter of the powder when
the powder does not have an indeterminate form like a powder
having an elliptical section.
Next, a third feature of the present invention resides
in a casing enclosed type magnetic core, wherein the powder is
a nylon resin or silica having silicone oil adhered
therearound.
It should be noted that, as the powder, there can be
used the powder of a polyolefin such as polyethylene,
polypropylene or polymethyl pentene, alumina powder, silicon
dioxide powder or the like.
Next, a fourth feature of the present invention resides
in a casing enclosed type magnetic core, wherein the casing
has a closed structure.
Therefore, the casing enclosed type magnetic core of
the present invention can insulate a sound generated by the
vibration of the magnetic core by covering the magnetic core
tightly with the casing.
Then, a fifth feature of the present invention resides
in a casing enclosed type magnetic core, wherein the magnetic
core is composed of an amorphous magnetic alloy thin belt.
Incidentally, this casing enclosed type magnetic core
can be applied to magnetic cores made from various materials
such as amorphous alloys (for example, Fe-based amorphous
alloy), silicon steel, ferrite, dust and the like.
BRIEF DESCRIPTION OF THE DRAWINGS
Fig. 1 is a diagram showing the configuration of a
casing enclosed type magnetic core of the present invention.
Fig. 2 is a diagram outlining a sound measurement test
to be made on the casing enclosed type magnetic core.
Fig. 3 is a diagram showing the waveform of an
excitation signal supplied to the coil at the time of the
sound measurement test.
Fig. 4 is a table showing the test result of each
casing enclosed type magnetic core.
Fig. 5 is a graph showing the sound level of each
casing enclosed type magnetic core with respect to the
charging rate of powders.
BEST MODE FOR CARRYING OUT THE INVENTION
Preferred embodiments of the present invention will be
described below with reference to the accompanying drawings.
[Embodiment 1]
First, a casing enclosed type magnetic core according
to this embodiment will be outlined with reference to Fig. 1.
Here, Fig. 1 is a diagram showing the configuration of
the casing enclosed type magnetic core of the present
invention.
Then, the casing enclosed type magnetic core 10
according to this embodiment comprises a magnetic core 11,
casings 121 and 122, and powders 13 as shown in Fig. 1.
Next, the casing enclosed type magnetic core 10 is
constructed by enclosing the magnetic core 11 in the casing 12
and filling the powders 13 in a space between the magnetic
core and the casing.
Hereinafter, the constitution and performance of the
casing enclosed type magnetic core according to this
embodiment will be described with reference to Figs. 2 to 5.
In this case, Fig. 2 is a diagram outlining a sound
measurement test to be made on the casing enclosed type
magnetic core, Fig. 3 is a diagram showing the waveform of an
excitation signal to be supplied to the coil at the time of
the sound measurement test.
The magnetic core 11 used in the casing enclosed type
magnetic core is obtained by heating at about 470°C a roll
having an outer diameter of 27.0 mm, an inner diameter of 15.0
mm and a height of 10.0 mm of a Fe-based amorphous magnetic
alloy thin belt (manufactured by Allied Signal Co. of the US,
trade name: Metglas 2605S-2, [composition Fe78B13Si9 (%)])
containing Si and B.
The casing 12 is a casing having an outer diameter of
27.7 mm, an inner diameter of 14.7 mm and a height of 10.3 mm
(all are the sizes of the inner casing) (manufactured by Toray
Industries, Inc., trade name: TORAYCON 1184G-30).
Further, two kinds of powders are used such as the
powders 13 filled in the space between the magnetic core 11
and the casing 12 are composed of nylon resin powders having a
maximum value of short diameter of 180 µm (manufactured by
Sumitomo Seika Co., trade name: Flolon) and silica powders
having a maximum value of short diameter of 300 µm and
silicone oil adhered therearound (manufactured by Toray Dow
Corning Silicone Co., trade name: Trefil).
Then, several casing enclosed type magnetic cores
having different charging rates of powders using the above
materials were fabricated.
Thereafter, a coil was formed by making 31 turns of a
magnetic wire having a diameter of 1.0 mm⊘ around each of the
magnetic cores provided by the above process to prepare
evaluation samples.
Then, a fixation test for evaluating reliability as a
magnetic component and a sound measuring test were made on
each of the evaluation samples. The methods of the above
tests will be described in detail hereinunder.
First, the fixation test was carried out by holding the
case enclosed type magnetic core with hand and strongly
shaking it in a direction parallel to the section of the
laminate of the magnetic core. When the movement of the
magnetic core was felt, the magnetic core was judged as
defective.
Subsequently, the sound measuring test was carried out
by measuring the level of a sound generated by the casing
enclosed type magnetic core 10 when an excitation signal was
supplied to the coil 15 formed around the casing enclosed type
magnetic core 10 as shown in Fig. 2 by a microphone 21
installed at a position 200 mm away from the center of the
casing enclosed type magnetic core 10.
Thereafter, a sound pressure level having a central
frequency of 1/3 octave band measured by the microphone 21 of
10 kHz is taken as a sound level and whether the casing
enclosed type magnetic core passes the sound measuring test is
judged based on whether the sound level thereof is 45.0 dB or
lower.
This target value of 45.0 dB is determined based on a
sound level which is apparently perceived to be a lower sound
than 58.0 dB, the sound level of a casing enclosed type
magnetic core using an adhesive.
Incidentally, the excitation signal to be supplied to
the coil 15 is a sweep sinusoidal wave having a frequency of
500 to 20,000 Hz which changes at a current value of 0 to 6A
as shown in Fig. 3.
Further, evaluation on each sample was carried out
mainly at room temperature and part of the samples were
evaluated at a high temperature of 110°C.
The evaluation results of the casing enclosed type
magnetic cores will be now described with reference to Figs. 4
and 5.
In this case, Fig. 4 is a table showing the evaluation
results of each sample and Fig. 5 is a diagram showing the
relationship between the sound level of each sample and
charging rate for each type of powders.
As shown in Fig. 4, out of 10 prepared samples, Samples
1 to 3 used nylon resin powders and Samples 4 to 10 used
silica powders having silicone oil adhered therearound.
First, the fixation test was made on Sample 1 and the
sound level thereof was measured based on a nylon resin powder
charging rate calculated from the above equation of 10.6%.
As a result, the sample passed the fixation test and
the sound level thereof was found to be 34.9 dB, lower than
the target value.
Subsequently, the fixation test was then made on Sample
2 at room temperature and a high temperature of 110°C and the
sound level thereof was measured based on a nylon resin powder
charging rate of 24.5%.
As a result, the sample passed the fixation test at
room temperature and a high temperature of 110°C and the sound
level thereof was found to be 35.9 dB, lower than the target
value.
The fixation test was also made on Sample 3 and the
sound level thereof was measured based on a nylon resin powder
charging rate of 49.7%.
As a result, the sample passed the fixation test and
the sound level thereof was found to be 43.5 dB, lower than
the target value.
Therefore, in the test using nylon resin powders, all
the samples had a sound level of 45.0 dB or lower which was
lower than the target value.
Then, the fixation test was made on Sample 4 at room
temperature and a high temperature of 110°C and the sound level
thereof was measured based on a silica powder charging rate of
30.0%.
As a result, the sample passed the fixation test at
room temperature and a high temperature of 110°C and the sound
level thereof was found to be 35.9 dB, lower than the target
value.
The fixation test was also made on Sample 5 and the
sound level thereof was measured based on a silica powder
charging rate of 50.0%.
As a result, the sample passed the fixation test and
the sound level thereof was found to be 32.8 dB, lower than
the target value.
Then, the fixation test was made on Sample 6 and the
sound level thereof was measured based on a silica powder
charging rate of 60.0%.
As a result, the sample passed the fixation test and
the sound level thereof was found to be 32.9 dB, lower than
the target value.
Next, the fixation test was made on Sample 7 and the
sound level thereof was measured based on a silica powder
charging rate of 70.0%.
As a result, the sample passed the fixation test and
the sound level thereof was found to be 32.1 dB, lower than
the target value.
The fixation test was further made on Sample 8 and the
sound level thereof was measured based on a silica powder
charging rate of 80.0%.
As a result, the sample passed the fixation test and
the sound level thereof was found to be 36.2 dB, lower than
the target value.
The fixation test was further made on Sample 9 and the
sound level thereof was measured based on a silica powder
charging rate of 90.0%.
As a result, the sample passed the fixation test and
the sound level thereof was found to be 32.3 dB, lower than
the target value.
It should be noted that the fixation test was further
made on Sample 10 and the sound level thereof was measured
based on a silica powder charging rate of 100.0%.
As a result, the sample passed the fixation test and
the sound level thereof was found to be 34.3 dB, lower than
the target value.
Therefore, in the test using silica powders, all the
samples had a sound level of 45.0 dB or lower which was lower
than the target value.
That is, it was found that a sound generated from the
magnetic core and the movement of the magnetic core in the
casing can be suppressed by filling powders in the space
between the magnetic core and the casing.
As described above, when the powders are filled in the
space between he magnetic core and the casing, a casing
enclosed type magnetic core having high reliability as a
magnetic component and making a sound small can be obtained.
Further, as is obvious from the results of a test made
on Sample 2 and Sample 4 at a temperature of 110°C, the casing
enclosed type magnetic core can be used stably at a high
temperature.
Also, as is evident from the evaluation results of the
samples, the powder charging rate is preferably in the range
of 1 to 150%, more preferably 10 to 150%, much more preferably
10 to 120%, the most preferably 10 to 100%.
The maximum value of short diameter of the powder used
in the present invention is preferably in the range of 5 to
500 µm, particularly preferably 100 to 400 µm.
Industrial Feasibility
Since the casing enclosed type magnetic core of the
present invention is able to prevent or suppress the movement
of the magnetic core in the casing and the transmission of the
vibration of the magnetic core to the casing, a casing
enclosed type magnetic core making a sound small during use
and having high reliability as a magnetic component can be
obtained.
Further, since the casing enclosed type magnetic core
of the present invention does not use an adhesive, its
vibration absorption power is not lost even when it is used at
high temperatures.
For that reason, according to the present invention, a
casing enclosed type magnetic core having a wider usable
temperature range than the conventional casing enclosed type
magnetic core can be obtained.