BACKGROUND OF THE INVENTION
[0001] The present invention generally relates to an electrical filter, and more particularly,
to a dielectric filter which functions as a band elimination filter, and is especially
so arranged to be compact in an external size and capable of achieving a low cost
through simplification of the manufacturing process.
[0002] Conventionally, there has been provided a filter as shown in Figs. 8 and 9 for a
dielectric filter which functions as a band elimination filter for attenuating only
a signal in a specific frequency region. In Figs. 8 and 9, the dielectric filter 30
comprises a plurality of resonators 35 disposed side by side and each including a
cylindrical member 31 of a ceramic material formed with a through-bore 32 extending
therethrough along its axis, an inner-conductor layer 33 formed within the through-bore
32 and an outer conductor layer 34 formed over an outer peripheral surface of the
cylindrical member 31 except for its end face 31a at an open end side thereof, a capacitor
36 constituted by forming electrode films on opposite main faces of a ceramic disc,
and electrically connected to the end face 31a side at the open end of the through-bore
32 of each resonator 35, and a coaxial cable 37 having an electrical length of λ/4
wavelength, provided to connect the neighboring resonators 35 to each other thorugh
said capacitors 36.
[0003] However, sicne the conventional dielectric filter 30 as described above adopts a
construction is which the resonators 35 are connected to each other by the coaxial
cable 37 having the length at λ/4 wavelength, i.e. through couping by a so-called
distribution constant line, there is such a problem that the external size of the
dielectric filter 30 inevitably increases by the length of said coaxial cable 37.
Moreover, due to the fact that there is involved in its manufacture, such a complicated
work that the single unit of the resonator 35 is prepared in a pluarlity of pieces
so as to be connected by the λ/4 transmission line, troublesome procedures are required
by that extent, with a consequent rise in the manufacturing cost.
SUMMARY OF THE INVENTION
[0004] Accordingly, an essential object of the present invention is to provide an improved
dielectric filter which is capable of decreasing an external size thereof, with a
simultaneous reduction of cost through simplification in the manufacturing process.
[0005] Another object of the present invention is to provide a dielectric filter of the
above described type which is simple in construction and stable in functioning at
high reliability.
[0006] In accomplishing these and other objects, according to one preferred embodiment
of the present invention, there is provided a dielectric filter which functions as
a band elimination filter for attenuating only a signal of a particular frequency
region, and comprises a dielectric block formed with a plurality of through-bores
therein in a parallel relation to each other, inner-conductor layers respectively
formed within said through-bores, and outer-conductor layer formed at least on an
outer side face of said dielectric block, thereby to constitute a plurality of resonators,
coupling members respectively disposed within said through-bores for capacitor coupling
with said inner conductor layers, and a concentrated constant line respectively connecting
neighboring ones of said coupling members.
[0007] For the concentrated constant line as referred to above, for example, air-core coils,
pattern forming coils, etc. may be employed, while the capacitor coupling can be realized,
for example, by inserting a metallic pin in an axial direction of a resinous pin forced
into each of said through-bores.
[0008] In the dielectric filter according to the present invention as described above, since
the respective resonators are connected through the concentrated constant line, the
length for connection between said resonators may be shortened to a large extent,
while the respective resonators conventionally disposed as single units through intervals
equivalent to λ/4 wavelength therebetween, may be formed by one block member for reduction
of the external size by that extent.
[0009] Furthermore, owing to the concentrated constant arrangement, the troublesome work
conventionally required to be effected by maintaining a required length of the line
for connecting the resonators at high accuracy can be simplified, and moreover, since
it is not necessary to prepare a plurality of individual resonators, labor and the
number of parts during manufacture can be reduced to a large extent, thereby to decrease
the cost by that extent for improvement of productivity.
[0010] Subsequently, the reason why the conventional distribution constant line may be replaced
by the concentrated constant line in the above band elimination filter will be explained.
[0011] Reference is made to equivalent circuit diagrams shown in Figs. 6(a), 6(b), 6(c),
6(d), 6(e), 6(f), 6(g), 6(h), and 6(i) for explaining the course through which the
present invention was realized.
[0012] In the first place, the λ/4 wavelength transmission line may be replaced by the
concentrated constant of a coil L and capacitors C under the conditions as follows
at a certain frequency f (Figs. 6(a), 6(b)).
ωL = Za · sinϑ
ωC = (1/Za) tanϑ/2
where Za: Characteristic impedance of the line,
ϑ : Electrical angle of the line,
ω = 2πf.
[0013] For example, upon setting as f = 400Mhz, Za = 50 , and ϑ = 90°,
L = (Za/2π · f) sinϑ = 50/(2 · π · 400 x 10⁶) x 1 = 1.99 x 10⁻⁸ [H]
C = (1/2π · f · Za) tanϑ/2 = 1/(2π · 400 x 10⁶ x 50) x 1 = 7.958 x 10⁻¹² [F]
[0014] Accordingly, the above transmission line may be converted as shown in Figs. 6(c)
to 6(d).
[0015] Here, upon consideration of the resonator as an L-C parallel resonance circuit, the
circuit shown in Fig. 6(d) can be converted into the equivalent circuit as shown in
Fig. 6(e).
[0016] Meanwhile, in Fig. 6(e), when Y-Δ conversion is effected by C-C′-Ce (2C-C′-Ce), the
equivalent circuits as shown in Figs. 6(f) to 6(h) are obtained.
[0017] Thus, the relations will be:
C₁ = (CC′ + C′Ce + CeC)/C′
C₂ = (CC′ + C′Ce + CeC)/Ce
C₃ = (CC′ + C′Ce + CeC)/C
L˝= L′ - (1/ω² C₃)
[0018] Therefore, the relation will be represented by the equivalent circuit as shown in
Fig. 6(i), and consequently, the distribution constant line will be replaced by the
concentrated constant line.
BRIEF DESCRIPTION OF THE DRAWINGS
[0019] These and other objects and features of the present invention will become apparent
from the following description taken in conjunction with the preferred embodiment
thereof with reference to the accompanying drawings, in which;
Fig. 1 is a schematic perspective view showing a dielectric filter according to one
preferred embodiment of the present invention,
Fig. 2 is a fragmentary side sectional view of the dielectric filter of Fig. 1,
Fig. 3(a) is a fragmentary perspective view of the dielectric filter of Fig. 1 further
provided with reactance elements,
Fig. 3(b) is an equivalent circuit of the dielectric filter of Fig. 3(a),
Fig. 4(a) is a fragmentary top plan view showing a dielectric filter according to
a modification of the embodiment of Fig. 1,
Fig. 4(b) is a fragmentary side elevational view of the modification of Fig. 4(a),
Fig. 5 is a fragmentary side sectional view of a dielectric filter according to a
further modification of the embodiment of Fig. 1,
Figs. 6(a) through 6(i) are equivalent circuit diagrams for explaining the course
through which the present invention was realized (already referred to),
Fig 7 is a perspective view showing one example in which the dielectric filter in
the above embodiment and a band pass filter are constituted as one unit,
Fig. 8 is an equivalent circuit diagram showing construction of a conventional dielectric
filter (already referred to), and
Fig. 9 is a fragmentary perspective view partly in section, showing the conventional
dielectric filter of Fig. 8 (already referred to).
DETAILED DESCRIPTION OF THE INVENTION
[0020] Before the description of the present invention proceeds, it is to be noted that
like parts are designated by like reference numerals throughout the accompanying drawings.
[0021] Referring now to the drawings, there is shown in Figs. 1 and 2, a dielectric filter
1A which functions as a band elimination filter according to one preferred embodiment
of the present invention, which generally includes a dielectric block 2 of a ceramic
material in cubic rectangular box-like configuration and formed therein with, for
example, five through-bores 3 through a predetermined interval therebetween and in
a parallel relation to each other, an inner conductor layer 4 formed on the inner
peripheral face of each of said through-bores 3, an outer conductor layer 5 formed
on four side walls 2b of said dielectric block 2 except for an end face 2a at an open
end side (i.e. upper face 2a in Fig. 1), a short-circuiting conductive layer 6 formed
on a bottom face 2c of said dielectric block 2 for short-circuiting between the outer
conductor layer 5 and the inner conductor layers 4 for generating a resonance mode
of λ/4 wavelength, thereby to constitute five resonators 7, a resinous pin 8 forced
into each of said through-bores 3 at the end face 2a on the open end side of the block
2, a metallic pin 9 inserted into the center of each resinous pin 8 in its axial direction
as a coupling member for capacitive coupling with the inner conductor layer 4, with
the upper end of said metallic pin 9 projecting upwardly from the open end face 2a
to a certain extent, and air-core coils 10 as a concentrated constant line for connecting
neighboring ones of said metallic pins 9 as illustrated (in Fig. 1, IP indicates a
circuit symbol showing an input terminal and OP represents a circuit symbol showing
an output terminal).
[0022] Subsequently, the function and effect of the dielectric filter 1A in the embodiment
of the present invention as described above will be explained.
[0023] Since the dielectric filter 1A of the present embodiment functions as a band elimination
filter for attenuating only the signal in the particular frequency region, it may
be employed, for example, for an antenna duplexer, filter diplexer, etc., in which
more than two filters 1A are combined.
[0024] As described above, according to the dielectric filter of the present embodiment,
since the resonators 7 neighboring each other are connected by the air-core coil 10
through the metallic pins 9, i.e. since the distribution constant line is replaced
by the concentrated constant line, the conventional construction in which a plurality
of single resonators are arranged side by side, may be accommodated in one block,
and thus, the connecting length between the resonators 7 may be remarkably reduced
as compared with that in the conventional transmission line, thereby reducing the
size of the filter by that extent.
[0025] Moreover, since the troublesome connecting work conventionally required for achieving
the electrical length of λ/4 may be omitted for facilitation of the connecting procedure,
and furthermore, only one block may be prepared for the filter, the process during
manufacture can be simplified so as to reduce the cost by that degree, with a consequent
improvement of productivity.
[0026] It is to be noted here that, in the dielectric filter 1A as described so far, although
the capacity component to be produced by the replacement of the transmission line
with the concentrated constant, may be absorbed by the resonators, this is limited
to a theoretical assumption, and in the actual practice, such capacity component can
not necessarily be absorbed entirely.
[0027] Therefore, in a modified dielectric filter 1B as shown in Figs. 3(a) and 3(b), a
reactance element Z is connected between a junction of the metallic pin 9 and the
air-core coil 10 and the outer conductor layer 5 for fine adjustment of the filter
characteristics. In the above case, such reactance element Z may be added to all of
the connecting portions or to the connecting portions arbitrarily selected, and the
reactive element of a capacitive nature or inductive nature may be provided singly
or in combination.
[0028] Additionally, in the dielectric filter 1A in Fig. 1, there is a case where a fringing
capacity is generated at the open side end face 2a of the inner conductor layer 4
of the resonator 7, thereby to produce a capacitive coupling between the neighboring
resonators 7, which may be, however, advantageously absorbed through variation of
the value for the air-core coil 10.
[0029] It should also be noted here that, in the foregoing embodiment, although the case
where the air-core coils 10 are employed for the concentrated constant line, is described
as one example, the arrangement may be, for example, so modified as in a modification
1C in Figs. 4(a) and 4(b) in which the air-core coils 10 are replaced by a coil line
pattern plate CL, which includes an insulative substrate 15, and a coil line pattern
16 formed thereon. For attachment onto the block 2, the substrate 15 with the coil
line pattern 16 is applied onto the metallic pins 9 through corresponding holes formed
in the substrate 15, and the pins 9 and the coil line pattern 16 are connected by
soldering for fixing. in this case also, effects similar to those in the foregoing
embodiment may be obtained.
[0030] furthermore, the metallic pin 9 described as employed in the foregoing embodiment
for the capacitor coupling member, may be replaced by a capacitor member 13 constituted
by forming electrode layers 12 on opposite main faces of a cylindrical ceramic member
11 as shown in a further modification 1D in Fig. 5. In this case, a cylindrical metallic
capacitor base 14 is inserted into the through-bore 3 instead of the resinous pin
8, and the lower face of said capacitor member 13 is connected to the upper face of
said capacitor base 14, while the air-core coil 10 is connected to the electrode layer
12 on the upper face of said capacitor member 13.
[0031] It may further be so arranged to connect the dielectric filter of the foregoing embodiment
in series with other filter, so as to accommodate such series-connected filters in
a casing for application as a shared unit, or to form a conventional band-pass filter
21 and the dielectric filter 1 in the foregoing embodiment into one unit in a single
dielectric block 20 as shown in Fig. 7.
[0032] It should further be noted that, in the foregoing embodiment, although the λ/4 wavelength
resonator is taken up as one example, the present invention is also applicable to
a λ/2 wavelength resonator as well.
[0033] As is clear from the foregoing description, according to the dielectric filter of
the present invention, the resonators are constituted by forming a plurality of through-bores
in the dielectric block, and forming the inner conductor layers and the outer conductor
layer within the through-bores and the outer side walls of the block respectively,
while the neighboring resonators are connected to each other through the capacitor
coupling members by the concentrated constant line, and therefore, not only the connecting
length between the resonators can be reduced, but also a plurality of resonators are
integrally formed in one block-member, with a consequent reduction of the filter size
by that extent. Additionally, troublesome work while maintaining the predetermined
electrical length may be dispensed with for saving labor during manufacture to a large
extent, and also for decreasing of the number of parts involved, with a corresponding
reduction in cost.
[0034] Although the present invention has been fully described by way of example with reference
to the accompanying drawings, it is to be noted here that various changes and modifications
will be apparent to those skilled in the art. Therefore, unless otherwise such changes
and modifications depart from the scope of the present invention, they should be
construed as included therein.
1. A dielectric filter which functions as a band elimination filter for attenuating
only a signal of a particular frequency region, said dielectric filter comprising
a dielectric block formed with a plurality of through-bores therein in a parallel
relation to each other, inner-conductor layers respectively formed within said through-bores,
an outer-conductor layer formed at least on an outer side face of said dielectric
block, thereby to constitute a plurality of resonators, a coupling means respectively
disposed within said through-bores for capacitive coupling with said inner conductor
layers, and a concentrated constant line means for respectively connecting neighboring
ones of said coupling means.
2. A dielectric filter as claimed in Claim 1, wherein said coupling means includes
metallic pins respectively inserted in an axial direction, into resinous pins forced
into said through-bores.
3. A dielectric filter as claimed in Claim 1, wherein said coupling means includes
capacitor members each constituted by forming electrode layers on opposite main faces
of a cylindrical ceramic member, and connected at its under face, with an upper face
of a cylindrical metallic capacitor base inserted in each of said through-bores.
4. A dielectric filter as claimed in Claim 1, wherein said concentrated constant line
means includes air-core coils each connecting neighboring ones of said coupling means.
5. A dielectric filter as claimed in Claim 1, wherein said concentrated constant line
means includes a coil line pattern plate constituted by an insulative substrate and
a coil line pattern formed thereon so as to connect neighboring ones of said coupling
means.
6. A dielectric filter as claimed in Claim 1, further including a reactance element
means connected between junctions of said coupling means and said concentrated constant
line means, and said outer conductor layer for fine adjustment of the filter characteristics.