RELATED APPLICATION
BACKGROUND OF THE INVENTION
Field of the Invention
[0002] The present invention relates to a transformer device used in a LAN for networking
or the like, and more specifically, to a transformer device formed by winding a wire
material for a primary coil and a wire material for a secondary coil around an annular
core such as a toroidal core.
Description of the Prior Art
[0003] In recent years, size reduction of a transformer device used in a LAN for networking
or the like has been strongly demanded, and a material formed by winding a wire material
for a primary coil and a wire material for a secondary coil around a small core has
been known.
[0004] As one of such technologies, a technology is known, in which a transformer device
is formed, upon winding a wire material for a primary coil and a wire material for
a secondary coil around a toric core such as a toroidal core, by winding a bifilar
coil 211 formed by adjoining a primary coil 211A and a secondary coil 211B therearound
(see FIG. 15) to reduce leakage flux (Patent Document 1 described below).
[0005] This Patent Document 1 discloses a material in which a three-layer insulating coil
is used as a wire material for a bifilar wound coil.
[0006] Such a three-layer insulating coil has a high withstand voltage, and when the coil
is used as the wire material, the wire material for the primary coil and the wire
material for the secondary coil can also be wound around the core by allowing both
into close contact with each other even without interposing a separate insulating
tape or the like between the wire material for the primary coil and the wire material
for the secondary coil.
Related Prior Art
[0007] Patent Document 1: Japanese Laid-Open Patent Publication No.
H7-029755(A)
SUMMARY OF THE INVENTION
[0008] However, according to the Patent Document 1 described above, upon simultaneously
winding a plurality of wire materials for coils around a core by bifilar winding,
a difference in holding force is unavoidably produced among the wire materials for
the coils, resulting in difficulty in processing the wire materials for the coils
into a winding state, and characteristics have been liable to be degraded.
[0009] Further, when a three-layer insulating wire is used as the wire material, while the
use has an advantage of capability of increasing a withstand voltage, the use may
cause a problem of excessive increase of a cost to be over the range which can be
allowed by a user in a cost aspect.
[0010] When such a coil is selected, the best coil is not necessarily required in terms
of characteristics, and the coil is required to satisfy characteristics according
to an application and a purpose thereof and to be formed into a balanced configuration
in such a manner that the coil falls within a predetermined range according to the
application and the purpose also in terms of cost.
[0011] The present invention has been made in view of the circumstances described above,
and an object of the present invention is to provide a transformer device in which
two wire materials for coils can be efficiently processed into the same winding state
and a configuration in which various characteristics and a cost thereof fall within
a predetermined range is formed.
[0012] In order to solve the problems described above, a transformer device according to
the present invention has features described below.
[0013] More specifically, the transformer device according to the present invention includes
a transformer device to be mounted in a LAN for networking, in which a wire material
for a primary coil and a wire material for a secondary coil are wound around an annular
core to allow a signal component to pass from the wire material for the primary coil
to the wire material for the secondary coil,
wherein the primary coil wire is formed of a one-layer insulating wire material, and
the secondary coil wire is formed of a three-layer insulating wire material, respectively,
and a twisted wire formed by intertwisting the two insulating wire materials is wound
around the core.
[0014] In this case, the annular core is preferably formed into a toroidal core.
[0015] The annular core may be processed into a material in which a closed magnetic path
is formed by combining a pair of U-shaped cores or a pair of E-shaped cores.
[0016] Moreover, the twisted wire is preferably split into a first split wire to be wound
around a part on one side of the core and a second split wire to be wound around a
part on the other side of the core, and the first split wire and the second split
wire are electrically bonded thereto in a first terminal pin in the wire material
for the primary coil and in a second terminal pin in the wire material for the secondary
coil, respectively.
[0017] A twisting pitch of the twisted wire between the one-layer insulating wire material
and the three-layer insulating wire material is preferably adjusted to 3 mm or more
and 10 mm or less.
[0018] A wire diameter of each of a conducting wire of the one-layer insulating wire material
and the three-layer insulating wire material which constitute the twisted wire is
further preferably adjusted to 0.2 mm or more and 0.45 mm or less.
[0019] Moreover, a total thickness of a coating member of the one-layer insulating wire
material and a coating member of the three-layer insulating wire material interposed
between individual conducting wires of the wire material for the primary coil and
the wire material for the secondary coil is preferably adjusted to 0.1155 mm or more
and 0.1430 mm or less.
[0020] According to a transformer device of the present invention, a primary coil and a
secondary coil are each formed as a twisted wire formed by intertwisting a one-layer
insulating wire material and a three-layer insulating wire material into a spiral
form, and wire materials can be wound therearound in a state in which two wire materials
for coils are intertwisted, and therefore a plurality of wire materials for coils
can be processed into the same winding state in each of the wire materials for the
coils. Moreover, the wire materials can be formed into a closer contact state with
each other in comparison with a case where coils are wound therearound by bifilar
winding, and characteristics can be improved such that impedance can be adjusted to
a stabilized value in a high-frequency band. Moreover, workability during winding
the wire material for the coil around the core is also improved.
[0021] In the transformer device of the present invention, either the primary coil or the
secondary coil is applied as the one-layer insulating wire material and the other
is applied as the three-layer insulating wire material. Therefore, upon intertwisting
the primary coil and the secondary coil, a certain degree of withstand voltage can
be secured to maintain the characteristics, and simultaneously a significant rise
of a production cost can be suppressed.
[0022] In addition, such a technology is known, in which a material formed by intertwisting
a wire material for a primary coil and a wire material for a secondary coil into a
twisted form is used as an air-core coil without using a core to improve conversion
efficiency and to achieve size reduction of a device (Japanese Laid-Open Patent Publication
No.
H4-328812(A)). However, the technology described above is completely different from the invention
of the present application in a direction of a technical idea in a point of using
no core. Moreover, because the material has no core, leakage of magnetic flux is unable
to be prevented, and reduction of inductance is unable to be avoided, and therefore
the technology is different from the present invention in the direction of the technology
also in these points described above.
[0023] Further scope of applicability of the present invention will become apparent from
the detailed description given hereinafter. However, it should be understood that
the detailed description and specific examples, while indicating preferred embodiments
of the invention, are given by way of illustration only, since various changes and
modifications within the spirit and scope of the invention will become apparent to
those skilled in the art from this detailed description.
BRIEF DESCRIPTION OF THE DRAWINGS
[0024] The present invention will become more fully understood from the detailed description
given herein below and the accompanying drawings which are given by way of illustration
only and thus are not limitative of the present invention.
FIG. 1 is a schematic view showing a main part of a transformer device according to
an embodiment of the present invention.
FIG. 2 is a schematic view showing a form of a coil before winding a wire in the embodiment
shown in FIG. 1.
FIG. 3 is a perspective view showing an overall configuration of a transformer device
according to the embodiment of the present invention.
FIG. 4 is a conceptual diagram showing a connection relationship between pins and
wire materials for coils of the transformer device shown in FIG. 3 when viewed from
a back side of the transformer device.
FIG. 5 is a conceptual diagram showing a winding wire relationship between a core
and two kinds of wire materials for coils.
FIG. 6 is a graph showing a change in frequency characteristics of passage loss (insertion
loss) when a coil twisting pitch is changed with regard to the present embodiment.
FIG. 7 is a graph showing a change in frequency characteristics (primary side) of
reflection loss (return loss) when a coil twisting pitch is changed with regard to
the present embodiment.
FIG. 8 is a graph showing a change in frequency characteristics (secondary side) of
reflection loss (return loss) when a coil twisting pitch is changed in the embodiment.
FIG. 9 is a graph showing a change in frequency characteristics of passage loss (insertion
loss) when a coil diameter is changed with regard to the present embodiment.
FIG. 10 is a graph showing a change in frequency characteristics (primary side) of
reflection loss (return loss) when a coil diameter is changed with regard to the present
embodiment.
FIG. 11 is a graph showing a change in frequency characteristics (secondary side)
of reflection loss (return loss) when a coil diameter is changed with regard to the
present embodiment.
FIG. 12 is a graph showing a change in frequency characteristics of passage loss (insertion
loss) when a coil coating thickness is changed with regard to the present embodiment.
FIG. 13 is a graph showing a change in frequency characteristics (primary side) of
reflection loss (return loss) when a coil coating thickness is changed with regard
to the present embodiment.
FIG. 14 is a graph showing a change in frequency characteristics (secondary side)
of reflection loss (return loss) when a coil coating thickness is changed with regard
to the present embodiment.
FIG. 15 is a schematic view showing a form of a coil before winding a wire in a conventional
technology.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0025] Hereinafter, an embodiment of a transformer device according to the present invention
will be described with reference to the drawings described above.
[0026] FIG. 1 is a schematic view showing a configuration of a transformer device according
to the present embodiment, and FIG. 2 shows a twisted coil 11 related to FIG. 1 in
a state before winding a wire around a core 31.
[0027] As shown in FIG. 2, the twisted coil 11 is formed of a twisted wire formed by intertwisting,
into a spiral form, a one-layer insulating wire (for example, a polyurethane enameled
wire (such as UEW), ordinarily also referred to as an insulating wire) 11A formed
by performing one-layer insulation coating on a conducting wire by a copper material
or the like, and a three-layer insulating wire (such as TEX and TIW) 11B formed by
performing three-layer insulation coating on the conducting wire by the copper material
or the like.
[0028] Thus, the twisted coil 11 is configured in such a manner that individual insulating
wires 11A and 11B are intertwisted into the spiral form. Thus, upon winding the twisted
coil around the core 31, the individual insulating wires 11A and 11B can be uniformly
crossed with magnetic flux. Moreover, two insulating wires 11A and 11B can be processed
into almost the same winding state relative to the core 31 in a closer contact state
to reduce magnetic leakage flux, and simultaneously impedance in a high-frequency
band can be adjusted to a stabilized value.
[0029] The twisted coil 11 is wound around the annular core 31 at a substantially uniform
pitch in a state of a twisted wire in which two kinds of insulating wires are intertwisted.
[0030] As the annular core 31, a material ordinarily referred to as a toroidal core (including
not only a circular shape, but also an elliptical shape, a barrel shape, a rectangular
shape or the like in an annular cross section) is preferably used, but is not necessarily
limited to the toroidal core. For example, the core may be a material in which a closed
magnetic path is formed by butting a pair of U-shaped cores or a pair of E-shaped
cores with each other. In addition, the shape is not limited to a toric shape, and
may be formed into a polygonal annular shape.
[0031] A main material of the core include ferrite, permalloy, a silicon steel plate and
the like, and a magnetic material other than the material described above can also
be used, and a dust core can also be used.
[0032] FIG. 3 is a perspective view showing an overall configuration of a transformer device
according to the present embodiment.
[0033] More specifically, as described above, the transformer device has a transformer body
1 formed by winding a twisted coil 11 formed by intertwisting two kinds of insulating
wires around a toroidal core (formed into almost a rectangular shape in a cross section
having an annular shape) 31 in a circumferential direction at almost the same pitch,
and a bobbin 41 for housing the transformer body 1, and six terminal pins 51(1) to
51(6) which extend from the bobbin 41 in a downward direction in the figure, and are
electrically connected hereto in end parts of predetermined insulating wires 11A and
11B of the twisted coil 11.
[0034] The bobbin 41 has left and right step parts (the step part on a deep side (right
side in the figure) is hidden by a front wall part 42) 44 formed between the front
wall part 42 and a rear wall part 43, a recessed part 46 surrounded on four sides
by the front and rear wall parts 42 and 43 and the left and right step parts 44, and
a pair of circuit board butting parts 45A and 45B projecting from a bottom part of
the recessed part 46 toward a downward direction in the figure.
[0035] Moreover, the transformer device has primary side terminal pins 51(1) to 51(3) which
extend from a lower surface of the step part 44 on a left side in the figure in the
bobbin 41 to a downward direction in the figure, and are arranged in parallel to each
other, and secondary side terminal pins 51(4) to 51(6) which extend from the lower
surface of the step part (not shown) 44 on a right side in the figure in the bobbin
41 to the downward direction in the figure, and are arranged in parallel to each other.
[0036] The transformer body 1 is stored therein in such a manner that, in a state in which
a central axis extends in a direction of the front and rear wall parts 42 and 43,
a part thereof is fitted into the recessed part 46 described above. Moreover, among
parts of the twisted coil 11 wound therearound, the end parts of the one-layer insulating
wire (such as UEW) 11A being a primary side coil are electrically connected to the
terminal pins 51(1) to 51(3), and meanwhile, the end parts of the three-layer insulating
wire (such as TEX and TIW) 11B being a secondary side coil are electrically connected
to the terminal pins 51(4) to 51(6).
[0037] Moreover, the pair of circuit board butting parts 45A and 45B each are a columnar
member long in a front-rear direction and having a bottom surface formed into a planar
form, and are formed into almost the same shape. When the transformer device is mounted
on a circuit board (not shown), operation of bringing the transformer device to relatively
close toward the circuit board is performed by placing the transformer device in a
predetermined position. Upon the operation, the terminal pins 51(1) to 51(6) are first
passed through through-holes of the circuit board (not shown), and then the bottom
surfaces of the circuit board butting parts 45A and 45B are butted on a surface of
the circuit board. Thus, relative movement of the transformer device is stopped. More
specifically, a distance between a bottom surface of the bobbin 42 and the surface
of the circuit board is regulated by the circuit board butting parts 45A and 45B,
and the terminal pins 51(1) to 51(6) are exposed above the surface of the circuit
board over a predetermined length from root parts thereof.
[0038] More specifically, a spacing in which the primary side coil and the secondary side
coil are to be connected can be secured in the root parts of the terminal pins.
[0039] FIG. 4 shows an arrangement of individual terminal pins 51(1) to 51(6), and a connection
state of coils to the terminal pins 51(1) to 51(6) when the terminal pins 51(1) to
51(6) are viewed from a back side of the transformer device shown in FIG. 3. Moreover,
FIG. 5 shows a winding state of primary side coils (UEW) 11A1 and 11A2 and secondary
side coils (TEX) 11B1 and 11B2 wound around a core 31A.
[0040] In addition, as shown in FIG. 5, the twisted coil 11 to be wound around the core
31A is split into a first twisted coil 111A to be wound around a part on a left side
of the core 31A in the figure, and a second twisted coil 111B to be wound around a
part on a right side of the core 31A in the figure, and both coils are configured
to be electrically coupled to the terminal pin 51(1) in the primary side coil, and
to the terminal pin 51(4) in the secondary side coil, respectively.
[0041] The end parts of the one-layer insulating wire (UEW) 11A being the primary side coil
are configured to be electrically connected to the terminal pins 51(1) to 51(3), and
meanwhile, the end parts of the three-layer insulating wire (TEX) 11B being the secondary
side coil are configured to be electrically connected to the terminal pins 51(4) to
51(6).
[0042] More specifically, as shown in FIG. 5 (see FIG. 4), the primary side coil (UEW) 11A1
(first twisted coil 111A) which extends from the terminal pin 51(2) (a symbol S standing
for START is provided), and is started in winding the wire around the core 31A is
wound around the part on the right side of the core 31A, in the figure, and then connected
to the terminal pin 51(1). Meanwhile, the primary side coil (UEW) 11A2 (second twisted
coil 111B) is connected to the terminal pin 51(1), in the figure, and wound around
the part on the left side of the core 31A, and then connected to the terminal pin
51(3) (a symbol F standing for FINISH is provided).
[0043] Meanwhile, the secondary side coil (TEX) 11B1 (first twisted coil 111A) which extends
from the terminal pin 51(6) (a symbol S standing for START is provided), and is started
in winding the wire around the core 31A is wound around the part on the left side
of the core 31A, in the figure, and then connected to the terminal pin 51(4). Meanwhile,
the secondary side coil (TEX) 11B2 (second twisted coil 111B) is connected to the
terminal pin 51(4), in the figure, and wound around the part on the right side of
the core 31A, and then connected to the terminal pin 51(5) (a symbol F standing for
FINISH is provided) .
[0044] Incidentally, regarding to what degree a twisting pitch P of the twisted coil 11
should be adjusted, what is important is whether or not a shape as the twisted coil
can be actually kept and whether or not winding work can be efficiently performed.
[0045] If the twisting pitch P of the twisted coil 11 is adjusted to a level less than 3
mm, it becomes hard to maintain a linear shape of the twisted wire, resulting in difficulty
in satisfactorily winding the wire around the core 31. On the other hand, if the twisting
pitch P of the twisted coil 11 is over 10 mm, it becomes hard to suppress loosening
or untwisting of twist during winding the wire for the twisted coil 11, and efficiency
of the winding work is significantly reduced.
[0046] Accordingly, from the viewpoints described above, it is preferably to set the twisting
pitch P of the twisted coil 11 to the range:

in efficiently winding the twisted coil 11 around the core 31 in an original shape.
[0047] It is further preferably to set the twisting pitch P to the range:

[0048] Thus, the working effect described above can be further secured.
[0049] However, in the case where the twisting pitch P of the twisted coil 11 is set in
the range of 3 mm or more and 10 mm or less, it is hard to use such a material unless
the material can maintain a satisfactory state also in view of the characteristics.
Then, in the range in which the twisting pitch P of the twisted coil 11 is 3 mm or
more and 10 mm or less, verification has been made on whether or not a satisfactory
value can be obtained in view of the characteristics (frequency characteristics of
passage loss (insertion loss), frequency characteristics of reflection loss (return
loss) (primary side: between terminal pins 51(2) and 51(3)) and frequency characteristics
of reflection loss (return loss) (secondary side: between terminal pins 51(5) and
51(6))).
[0050] FIG. 6 represents each graph showing frequency characteristics of passage loss (insertion
loss) when a coil twisting pitch P is changed with regard to the present embodiment.
[0051] In the twisted coil 11 being an evaluation object upon obtaining the graph shown
in FIG. 6, the twisting pitch P is changed from 3 mm to 10 mm at an increment of 1
mm, and each graph in FIG. 6 to FIG. 8 shows a change in the characteristics for a
material having each pitch. In addition, a primary side coil of the twisted coil 11
at this time is a one-layer insulating wire (2UEW: 0.0155 mm-thick) 11A, and a secondary
side coil of the twisted coil 11 is a three-layer insulating wire (TEX-E: 0.1 mm-thick)
11B. A coil diameter D is 0.23 mm (the same in the graphs shown in FIG. 7 and FIG.
8).
[0052] As shown in FIG.6, verification has been made in such a manner that the frequency
characteristics of passage loss (insertion loss) become more satisfactory accordingly
as the twisting pitch P is reduced, and are within an allowable range at least in
the region from 3 mm to 10 mm in P.
[0053] FIG. 7 represents each graph showing frequency characteristics of reflection loss
(return loss) (primary side: between terminal pins 51(2) and 51(3)) when a coil twisting
pitch P is changed with regard to the present embodiment.
[0054] As shown in FIG. 7, verification has been made in such a manner that the frequency
characteristics of reflection loss (return loss) (primary side) become more satisfactory
accordingly as the twisting pitch P is reduced, and are within an allowable range
at least in the region from 3 mm to 10 mm.
[0055] FIG. 8 represents each graph showing frequency characteristics of reflection loss
(return loss) (secondary side: between terminal pins 51(5) and 51(6)) when a coil
twisting pitch P is changed with regard to the present embodiment.
[0056] As shown in FIG. 8, verification has been made in such a manner that the frequency
characteristics of reflection loss (return loss) (secondary side) become more satisfactory
accordingly as the twisting pitch P is reduced, and are within an allowable range
at least in the region from 3 mm to 10 mm.
[0057] Next, verification has been made on a coil diameter D of a conducting wire of insulating
wires 11A and 11B of a twisted coil 11 as to whether or not a satisfactory value can
be obtained in view of characteristics (frequency characteristics of passage loss
(insertion loss), frequency characteristics of reflection loss (return loss) (primary
side: between terminal pins 51(2) and 51(3)) and frequency characteristics of reflection
loss (return loss) (secondary side: between terminal pins 51(5) and 51(6)), when the
diameter is adjusted to an ordinarily used range of 0.20 mm or more and 0.45 mm or
less.
[0058] In addition, referring to as the coil diameter in the description of the present
application represents a cross sectional diameter of the conducting wire, excluding
the insulation coating.
[0059] FIG. 9 represents each graph showing frequency characteristics of passage loss (insertion
loss) when a coil diameter D is changed with regard to the present embodiment.
[0060] In a twisted coil 11 being an evaluation object upon obtaining the graph shown in
FIG. 9, a coil diameter D is sequentially changed from 0.2 mm to 0.45 mm, and each
graph in FIG. 9 to FIG. 11 shows a change in the characteristics for a material having
each diameter.
[0061] In addition, a primary side coil of the twisted coil 11 at this time is a one-layer
insulating wire (2UEW: 0.0155 mm-thick), and a secondary side coil of the twisted
coil 11 is a three-layer insulating wire (TEX-E: 0.1000 mm-thick), and a twisting
pitch P of the twisted coil 11 is 5 mm (the same in the graphs shown in FIG. 10 and
FIG. 11).
[0062] As shown in FIG.9, verification has been made in such a manner that the frequency
characteristics of passage loss (insertion loss) become more satisfactory accordingly
as the coil diameter D is increased, and are within an allowable range at the coil
diameter D at least in the region from 0.2 mm to 0.45 mm.
[0063] FIG. 10 represents each graph showing frequency characteristics of reflection loss
(return loss) (primary side: between terminal pins 51(2) and 51(3)) when a coil diameter
D is changed with regard to the present embodiment.
[0064] As shown in FIG. 10, verification has been made in such a manner that the frequency
characteristics of reflection loss (return loss) (primary side) become more satisfactory
accordingly as the coil diameter D is increased, and are within an allowable range
at least in the region from 0.2 mm to 0.45 mm.
[0065] FIG. 11 represents each graph showing frequency characteristics of reflection loss
(return loss) (secondary side: between terminal pins 51(5) and 51(6)) when a coil
diameter D is changed with regard to the present embodiment.
[0066] As shown in FIG. 11, verification has been made in such a manner that the frequency
characteristics of reflection loss (return loss) (secondary side) become more satisfactory
accordingly as the coil diameter D is reduced, and are within an allowable range at
least in the region from 0.2 mm to 0.45 mm.
[0067] Next, with regard to a coating thickness (thickness of an insulating material coating
a circumference of a metal conducting wire) T of the twisted coil 11, either 1UEW
(0.0230 mm-thick) or 2UEW (0.0155 mm-thick) each ordinarily used is selected for a
primary side coil, and either TEX-E (0.1000 mm-thick) or TIW-2 (0.1200 mm-thick) each
ordinarily used is selected for a secondary side coil, and a total coating thickness
T has been set by combining coating thicknesses of individual insulating wires 11A
and 11B selected. Thus, with regard to the coating thickness T, a combination of TEX-E
(0.1000 mm-thick) and 1UEW (0.0230 mm-thick) results in a thickness of 0.1230 mm,
a combination of TEX-E (0.1000 mm-thick) and 2UEW (0.0155 mm-thick) results in a thickness
of 0.1155 mm, a combination of TIW-2 (0.1200 mm-thick) and 1UEW (0.0230 mm-thick)
results in a thickness of 0.1430 mm, and a combination of TIW-2 (0.1200 mm-thick)
and 2UEW (0.0155 mm-thick) results in a thickness of 0.1355 mm.
[0068] More specifically, verification has been made as to whether or not a satisfactory
value can be obtained by measuring four twisted coils 11 in which a coating thickness
T is changed as an object to be measured in view of characteristics (frequency characteristics
of passage loss (insertion loss), frequency characteristics of reflection loss (return
loss) (primary side: between terminal pins 51(2) and 51(3)) and frequency characteristics
of reflection loss (return loss) (secondary side: between terminal pins 51(5) and
51(6)), when the coating thickness T is adjusted in the range of 0.1155 mm or more
and 0.1430 mm or less.
[0069] FIG. 12 represents each graph showing frequency characteristics of passage loss (insertion
loss) when a coil coating thickness T is changed with regard to the present embodiment.
In the twisted coil 11 being an evaluation object upon obtaining the graph shown in
FIG. 12, a coil coating thickness T is changed from 0.1155 mm to 0.1430 mm in four
stages, and the graph in FIG. 12 shows each change in the characteristics for a material
having each thickness.
[0070] In addition, a twisting pitch P of the twisted coil 11 at this time is 5 mm and a
coil diameter D is 0.20 mm (the same in the graphs shown in FIG. 13 and FIG. 14).
[0071] As shown in FIG. 12, verification has been made in such a manner that the frequency
characteristics of passage loss (insertion loss) become more satisfactory accordingly
as the coil coating thickness T is reduced, and are within an allowable range at least
in the region from 0.1155 mm to 0.1430 mm.
[0072] FIG. 13 represents each graph showing frequency characteristics of reflection loss
(return loss) (primary side: between terminal pins 51(2) and 51(3)) when a coil coating
thickness T is changed with regard to the present embodiment.
[0073] As shown in FIG. 13, verification has been made in such a manner that the frequency
characteristics of reflection loss (return loss) (primary side) become more satisfactory
accordingly as the coil coating thickness T is reduced, and are within an allowable
range at least in the region from 0.1155 mm to 0.1430 mm.
[0074] FIG. 14 represents each graph showing frequency characteristics of reflection loss
(return loss) (secondary side: between terminal pins 51(5) and 51(6)) when a coil
coating thickness T is changed with regard to the present embodiment.
[0075] As shown in FIG.14, verification has been made in such a manner that the frequency
characteristics of reflection loss (return loss) (secondary side) become more satisfactory
accordingly as the coil coating thickness T is reduced, and are within an allowable
range at least in the region from 0.1155 mm to 0.1430 mm.
[0076] As described above, the embodiment of the present invention is described, but the
present invention is not limited to the material in the embodiment described above,
and the embodiments can be modified in various manners.
[0077] For example, all of the coil twisting pitch P, the coil diameter D and the coil coating
thickness T are preferably set to set values verified in the embodiment for the twisted
coil 11 described above. However, even if one or two of the elements are out of the
verified range, the transformer device can have satisfactory characteristics to a
certain degree.
[0078] Moreover, constituent materials of the core, the conducting wire of the coil, the
bobbin and the insulation coating are not limited to the materials in the embodiment
described above, and various other materials can be used.
[0079] The invention being thus described, it will be obvious that the same may be varied
in many ways. Such variations are not to be regarded as a departure from the spirit
and scope of the invention, and all such modifications as would be obvious to one
skilled in the art are intended to be included within the scope of the following claims.