TECHNICAL FIELD
[0001] The present invention relates to a phase shifting device used in, for example, a
transmitting device capable of high output through parallel operation of a plurality
of transmitters and a power supply apparatus for directional control of antennas.
BACKGROUND ART
[0002] When attempting to vary the direction of maximum radiation or side lobe characteristic
of an array antenna by appropriately controlling the driving phase of each of a plurality
of radiating elements forming the array antenna, or when attempting to realize a high-output
transmitting device by parallel-operating a plurality of transmitters and controlling
the output phase of each transmitter such that each is the same phase, line stretchers
constructed so as to mechanically vary the length of the transmission line of a signal,
or waveguide-type phase shifting devices formed by inserting a dielectric plate within
a waveguide have conventionally been used.
[0003] Fig. 1 presents several views of a waveguide-type phase shifting device of the prior
art, Fig. 1A showing a plan view, Fig. 1B showing a side view, Fig. 1C showing a sectional
view taken at the B-B line of Fig. 1B, and Fig. 1D showing a sectional view taken
at the A-A line of Fig. 1A.
[0004] In rectangular waveguide 11, flanges 12₁ and 12₂ are provided for inserting and connecting
such a waveguide-type phase shifting device within a rectangular waveguide circuit.
A dielectric plate 13 is provided within rectangular waveguide 11 such that the plate
surface is parallel to the electric field within the waveguide 11. As shown in Fig.
1D, the contour of this dielectric plate 13 is formed as a parallelogram, this parallelogram
having inclines on the edges of the radio-wave incident side and edges of the opposite
side which are formed so as to improve the radio-wave reflection characteristic at
these edge portions.
[0005] Instead of providing inclines to the edges of the radio-wave incident side and edges
of the opposite side of this dielectric 13, the radio-wave incident portion and opposite
side portion of the dielectric 13 may be formed such that the plate thickness gradually
varies.
[0006] Support fittings 14₁ and 14₂ for dielectric plate 13 pass through the opposing short
sides of rectangular waveguide 11 and dielectric plate 13. Support fittings 14₁ and
14₂ may freely slide at the portions where they pass through the opposing short sides
of rectangular waveguide 11 but are secured to the portions where they pass through
dielectric plate 13.
[0007] Coupling plate 15 links together support fittings 14₁ and 14₂. This coupling plate
15 serves as a handle for moving support fittings 14₁ and 14₂ either forward or backward
in the axial direction of each of support fittings 14₁ and 14₂ while maintaining dielectric
plate 13 in the attitude shown in Fig. 1D, thus allowing the plate surfaces of dielectric
plate 13 to be moved from a position coinciding with the central axis in the longitudinal
direction of rectangular waveguide 11 to a position close to either of the opposing
short sides as shown in Fig. 1C, thus enabling variation in the proportion of shift
change of radio waves propagated through rectangular waveguide 11.
[0008] In other words, such a phase shifting device uses the change in propagation speed
of radio waves within rectangular waveguide 11 according to the dielectric constant,
thickness, and length in the direction of wave propagation of dielectric plate 13.
When interposed at a position coinciding with the central axis in the longitudinal
direction of rectangular waveguide 11, where the electric field intensity is at maximum
strength, dielectric plate 13 exercises a large effect upon the propagation speed
of radio waves, but the electric field strength progressively weakens with distance
from the longitudinal central axis of the rectangular waveguide 11 and proximity to
either of the short sides, and consequently, as the position of insertion of dielectric
plate 13 shifts away from the central axis of rectangular waveguide 11 and approaches
either of the short sides, the effect upon the propagation speed of radio waves decreases.
Accordingly, the degree of phase shifting can be varied by changing the position of
insertion of dielectric plate 13.
[0009] Support fittings 14₁ and 14₂ are maintained parallel to each other, their relative
spacing (spacing in relation to the longitudinal direction of rectangular waveguide
11) being selected as λ
g/4 (λ
g is the wavelength within the waveguide corresponding to the employed frequency),
whereby reflected waves arising at the support fitting 14₁ closer to the radio-wave-incident
portion and reflected waves arising at support fitting 14₂ which travel back to the
position of support fitting 14₁ are of mutually reversed phase and cancel each other,
thereby enabling an improved reflection characteristic.
[0010] A line stretcher used in the prior art must regulate the line length according to
the required degree of phase shifting, and therefore, when the required degree of
phase shifting is great, not only is a large-scale mechanical structure required,
but a relatively time-consuming and labor-intensive adjustment is required to accurately
match the line length with the degree of phase shift.
[0011] The waveguide-type phase shifting device shown in Fig. 1 involves the drawbacks that
a long dielectric plate 13 is required when a large amount of phase shift is called
for, resulting in a phase shifting device of large overall size, and that a great
deal of time and effort is required to adjust the insertion point of the dielectric
plate 13 to accurately match the amount of phase shift with the required value.
[0012] Fig. 2 shows a power supply circuit configured using phase shifting devices of the
prior art for controlling the driving phase of subarray antennas and for varying the
direction of maximum radiation as well as the side lobe characteristic of an array
antenna. This power supply circuit is configured from subarray antennas 16₁-16₄ each
composed of a plurality of element antennas, phase shifting devices 17₁-17₃ of the
above-described prior art, transmission lines 18₁-18₃ having a degree of phase shift
that serves as a standard, and two-branch circuits 19₁-19₃.
[0013] A phase shifting device of the prior art not only entails the same drawbacks as the
above-described line stretcher, but when used as shown in Fig. 2, in which a power
supply circuit is configured for varying the direction of maximum radiation or side
lobe characteristic of an array antenna, further entails the drawback of complex structure
of the power supply circuit due to the need for transmission lines 18₁-18₃ having
an amount of phase shift that serves as a standard and two-branch circuits 19₁-19₃
for phase shifting devices 17₁-17₃, respectively.
DISCLOSURE OF THE INVENTION
[0014] The object of the present invention is to provide a phase shifting device which has
a simple and compact structure, and which allows easy adjustment at the time of manufacture
and easy handling during use.
[0015] To achieve the above-described objects, the present invention proposes a phase shifting
device that includes:
two-partition circuit for partitioning input power into two substantially equal
portions having a mutual phase difference of substantially 90°;
a first driver for generating circularly polarized waves that is driven by the
two-partitioned output of the two-partition circuit;
a second driver for coupling circularly polarized waves generated by the first
driver;
two sealed cases within which the first and second drivers are installed so as
to be rotatable relative to each other around the axis joining the centers of both
drivers; and
a combining circuit for combining the two outputs generated from circularly polarized
waves coupled in the second driver.
[0016] The two-partition output of the two-partition circuit, which distributes the input
power in two portions having a mutual phase difference of substantially 90°, is applied
to the first driver, which generates from its front surface a circularly polarized
wave. This circularly polarized wave couples at the second driver, and the two outputs
of the second driver arising from this coupled circularly polarized wave are combined
at the combining circuit. When the first and second drivers are rotated relative to
each other around the axis that joins the centers of each of the first and second
drivers, the phase difference between the input of the two-partition circuit that
applies driver power to the first driver and the combined output of the second driver
varies in accordance with this rotation.
[0017] This phase shifting device allows variation of the degree of phase shift over a range
of from 0° to 360°, and moreover, has a simple and compact structure that enables
extremely easy adjustment at the time of manufacture and service during use. In addition,
the relation between relative angle of rotation of the two sealed cases and the degree
of phase shift is proportional, and therefore, the degree of phase shift can be read
directly if graduations of degrees are added around the circumference of one of the
sealed cases and a pointer is added at a point on the circumference of the other sealed
case.
[0018] Furthermore, the present invention provides a phase shifting device that includes:
a first driver for generating linearly polarized
waves that is driven by input applied by way of an input terminal;
a second driver for coupling two orthogonal components of linearly polarized waves
generated by the first driver;
two sealed cases within which the first and second drivers are installed so as
to be rotatable relative to each other around the axis joining the centers of both
drivers; and
a combining circuit for combining the two outputs generated by the two orthogonal
components of the linearly polarized wave coupled in the second driver.
[0019] When the first driver is driven, linearly polarized waves are generated from the
front surface of the driver, and the two orthogonal components of this linearly polarized
wave are coupled at the second driver. When the first and second drivers are rotated
relative to each other around the axis joining the centers of each of the first and
second drivers, the phase difference between the input applied to the first driver
and either of the two outputs of the combining circuit to which the two outputs of
the second driver are applied varies according to the angle of rotation; and in addition,
the phase difference between the two outputs of the combining circuit to which the
two outputs of the second driver are applied also varies according to the relative
angle of rotation between the first and second drivers.
[0020] This phase shifting device allows variation of the degree of phase shift over a range
of from 0° to 360°, and moreover, has a simple and compact structure and enables extremely
easy adjustment at the time of manufacture and handling during use. In addition, the
relation between relative angle of rotation of the two sealed cases and the degree
of phase shift is proportional, and therefore, the degree of phase shift can be read
directly if graduations of degrees are added around the circumference of one of the
sealed cases and a pointer is added at a point on the circumference of the other sealed
case.
[0021] This phase shifting device is well-suited for control of the direction of maximum
radiation or side lobe characteristics of an array antenna because it both allows
variation of the phase difference between the input and either one of the two outputs
of the combining circuit according to the relative angle of rotation between the sealed
cases, and moreover, allows variation of the phase difference between the two outputs
according to the relative angle of rotation between the sealed cases.
BRIEF DESCRIPTION OF THE DRAWING
[0022]
Figs. 1A - 1D show an example of a waveguide-type phase shifting device of the prior
art;
Fig. 2 shows an example of the use of the prior-art phase shifting device shown in
Fig. 1;
Fig. 3 is a side view of a phase shifting device according to an embodiment of the
present invention;
Fig. 4 is a side view of a coupler 21 shown in Fig. 3;
Fig. 5 is a plan view of coupler shown in Fig. 3;
Fig. 6 is a sectional view taken at line C-C of Fig. 4;
Fig. 7 is a sectional view taken at line D-D of Fig. 5;
Fig. 8 illustrates the operation of the phase shifting device according to the embodiment
of Fig. 3;
Fig. 9 shows the return loss characteristic in coaxial connection plug 21₃₁ of the
phase shifting device of the embodiment shown in Fig. 3;
Fig. 10 shows the transmission loss characteristic between coaxial connection plugs
21₃₁ and 21₃₄ of the phase shifting device of the embodiment shown in Fig. 3;
Fig. 11 shows the degree of phase shift in relation to the relative angle of rotation
φ between sealed cases 21₁ and 21₂ in the phase shifting device of the embodiment
shown in Fig. 3;
Fig. 12 shows the transmission loss characteristic between input terminal 22₁ and
output terminal 24₁ in the phase shifting device of the embodiment shown in Fig. 3;
Fig. 13 is a sectional view showing the principal parts of a phase shifting device
according to another embodiment of the present invention;
Fig. 14 is a sectional view showing the principal parts of a phase shifting device
according to another embodiment of the present invention;
Fig. 15 is a block diagram showing a phase shifting device according to the embodiment
of Fig. 13;
Fig. 16 is a side view of a phase shifting device according to another embodiment
of the present invention;
Fig. 17 is a side view of coupler 31 within Fig. 16;
Fig. 18 is a plan view of coupler 31 within Fig. 16;
Fig. 19 is a sectional view taken at line G-G of Fig. 17;
Fig. 20 is a sectional view taken at line H-H of Fig. 17;
Fig. 21 is a sectional view taken at line I-I of Fig. 18;
Figs. 22A and 22B show the electric field level produced by drive element 31 and the
outputs E₁ and E₂ of 90° 3-dB hybrid circuit 32 in the phase shifting device of Fig.
16;
Fig. 23 shows the reflection characteristic in coaxial connection plug 31₃₁ of the
phase shifting device of Fig. 16;
Fig. 24 shows the transmission loss characteristic between coaxial connection plugs
31₃₁ and 31₃₃ of the phase shifting device of Fig. 16;
Fig. 25 shows the degree of phase shift in relation to the relative angle of rotation
φ between sealed cases 31₁ and 31₂ in the phase shifting device of Fig. 16;
Fig. 26 shows the observation results of the transmission loss between coaxial connection
plug 31₃₁ of coupler 31 and the output terminal 32₃ of 90° 3-dB hybrid circuit 32,
and between coaxial connection plug 31₃₁ of coupler 31 and output terminal 32₄ of
90° 3-dB hybrid circuit 32;
Fig. 27 shows an example of the use of both outputs E₂ and E₁ of output terminals
32₃ and 32₄ of 90° 3-dB hybrid circuit 32; and
Fig. 28 is a sectional view showing the principal parts of the phase shifting device
according to another embodiment of the present invention.
DETAILED DESCRIPTION OF THE PREFFERED EMBODIMENTS
[0023] Fig. 3 is a side view of the phase shifting device according to an embodiment of
the present invention.
[0024] The phase shifting device according to this embodiment is constructed from coupler
21 which includes cylindrical sealed cases 21₁ and 21₂ which are each closed at one
end, and terminals 21₃₁-21₃₄ made up of coaxial connection plugs; 90° 3-dB hybrid
circuit 22 which is composed of a directional coupler including input terminal 22₁,
isolation terminal 22₂, and output terminals 22₃ and 22₄; reflectionless terminator
23 connected to isolation terminal 22₂; 90° 3-dB hybrid circuit 24 which is composed
of a directional coupler including output terminal 24₁, isolation terminal 24₂, and
input terminals 24₃ and 24₄; reflectionless terminator 25 connected to isolation terminal
24₂; coaxial cable 26₁ connecting output terminal 22₄ and terminal 21₃₁; coaxial cable
26₂ connecting output terminal 22₃ and terminal 21₃₂; coaxial cable 27₁ connecting
terminal 21₃₄ and input terminal 24₃; and coaxial cable 27₂ connecting terminal 21₃₃
and input terminal 24₄.
[0025] Here, the output power of each of output terminals 22₃ and 22₄ is 1/2 of the input
power to input terminal 22₁, and, for example, the phase of the output of output terminal
22₃ is substantially 90° delayed with respect to the phase of the output of output
terminal 22₄. Furthermore, inputs of equivalent magnitude are applied to each of input
terminals 24₃ and 24₄, the input to input terminal 24₃ being, for example, substantially
90° advanced with respect to the phase of input to input terminal 24₄.
[0026] The lengths of each of coaxial cables 26₁ and 26₂ are adjusted such that the phase
of the output of output terminal 22₃ of 90° 3-dB hybrid circuit 22 is delayed substantially
90° with respect to the phase of the output of output terminal 22₄, and moreover,
such that both outputs are applied to input coaxial connection plugs 21₃₁ and 21₃₂
of coupler 21 while being kept in a mutually equivalent relation. The lengths of coaxial
cables 27₁ and 27₂ are each adjusted such that the outputs from output coaxial connection
plugs 21₃₃ and 21₃₄ of coupler 21 are applied to the input terminals 24₃ and 24₄ of
90° 3-dB hybrid circuit 24 with the phase difference and the equal amplitude relation
between the outputs maintained unchanged.
[0027] Fig. 4 shows a side view of coupler 21 of Fig. 3, Fig 5 shows a plan view of the
sealed case 21₁ side of coupler 21 as seen from the bottom side, Fig. 6 is an enlarged
sectional view taken along line C-C of Fig. 4, and Fig. 7 is an enlarged sectional
view taken along line D-D of Fig. 5.
[0028] As can be clearly seen from Fig. 7, stepped portions are formed in the side walls
at the end portions of the openings of both of sealed cases 21₁ and 21₂, the end portion
of the opening of sealed case 21₂ fitting inside the end portion of the opening of
sealed case 21₁, the two sealed cases 21₁ and 21₂ being coupled together as a unit,
and sealed cases 21₁ and 21₂ being constructed so as to allow rotation relative to
each other around their cylindrical axis.
[0029] Sealed cases 21₁ and 21₂ are manufactured by first machining a metal block or press-forming
a metal sheet in the prescribed shape; by forming a suitable synthetic resin in a
preliminary form of the prescribed shape and subsequently applying a metal film to
the surface by a electroless plating or vacuum evaporation process; or by multilayer
stacking of dielectric plates having an appropriate dielectric constant and forming
as a cylinder with one closed end that shields electromagnetic energy in accordance
with Snell's law.
[0030] Coaxial connection plugs 21₃₁ and 21₃₂ each include internal conductors 21₄₁ and
21₄₂. A round insulation plate 21₅₁ composed of a material having excellent high-frequency
characteristics and a thickness less than the transmission wavelength such as an organic
material such as polyethylene or fluorinated ethylene or an inorganic material such
as a ceramic is adhered to the inner surface of the bottom wall of sealed case 21₁
using a suitable adhesive. Metal plate 21₆₁ is secured to the surface of round insulation
plate 21₅₁ using a suitable adhesive, and in addition, portions of the periphery of
metal plate 21₆₁ are connected to internal conductors 21₄₁ and 21₄₂ of coaxial connection
plugs 21₃₁ and 21₃₂, and the first driver composed of a microstrip antenna is formed
with sealed case 21₁ on the opposite side of round insulation plate 21₅₁ as the ground
conductor, metal plate 21₆₁ as the first driver element, and the contact points between
metal plate 21₆₁ and interior conductors 21₄₁ and 21₄₂ of coaxial connection plugs
21₃₁ and 21₃₂ as the driver points.
[0031] As can be seen from Fig. 6, a right angle is formed by the straight line joining
the center of metal plate 21₆₁ and the driving point constituted by the contact point
between metal plate 21₆₁ and the interior conductor 21₄₁ of coaxial connection plug
21₃₁ and the straight line joining the center of metal plate 21₆₁ and the driving
point constituted by the contact point between metal plate 21₆₁ and the internal conductor
21₄₂ of coaxial connection plug 21₃₁.
[0032] In addition, the exterior conductors of each of coaxial connection plugs 21₃₁ and
21₃₂ are electrically connected to sealed case 21₁, and as shown in Fig. 7, a portion
of sealed case 21₁ has been removed around the periphery of internal conductor 21₄₁
to form a gap such that internal conductor 21₄₁ makes no mechanical contact with sealed
case 21₁, and a gap is similarly formed in sealed case 21₁ at the portion around the
periphery of internal conductor 21₄₂.
[0033] As the method for securing metal plate 21₆₁ to the surface of round insulation plate
21₅₁, a setscrew in the center of metal plate 21₆₁ (the portion wherein electric field
intensity is 0) may also be used to secure the plate to round insulation plate 21₅₁
rather than an adhesive, or metal plate 21₆₁ may be screwed at its center to the bottom
wall of sealed case 21₁ through round insulation plate 21₅₁.
[0034] Instead of using metal plate 21₆₁, the driver element of the microstrip antenna making
up the first driver may be formed by applying a metal film to the surface of round
insulation plate 21₅₁ by a process such as vacuum evaporation and finishing to the
required outline shape by a process such as etching.
[0035] Whether the driver element is formed from a metal plate or metal film, its outline
shape may instead of a circle be formed as a square, electrical connection with the
internal conductors 21₄₁ and 21₄₂ of coaxial connection plugs 21₃₁ and 21₃₂ being
effected in the corner portions of the square.
[0036] Next will be explained the dimensions of driver element 21₆₁ for a case in which
driver element 21₆₁ is driven in basic mode. When the outline shape of driver element
21₆₁ is formed as a circle as shown in Fig. 6, if the specific inductive capacity
of round insulation plate 21₅₁ is ε
r and the design frequency is f
o, the radius of driver element 21₆₁ is preferably selected as substantially

, and when the outline shape of driver element 21₆₁ is formed as a square, the length
of one side of driver element 21₆₁ is preferably selected as substantially

(C being the speed of light).
[0037] Next, in Fig. 7, 21₄₃ and 21₄₄ are the internal conductors of coaxial connection
plugs 21₃₃ and 21₃₄, respectively, 21₅₂ is a round insulation plate, and 21₆₂ is the
second driver element; the material, method of fabrication, and mutual electrical
and mechanical relation of each of these parts being identical to the material, method
of fabrication, and mutual electrical and mechanical relation of each of respective
coaxial connection plugs 21₃₁ and 21₃₂, internal conductors 21₄₁ and 21₄₂, round insulation
plate 21₅₁, and first driver element 21₆₁ on the side of sealed case 21₁.
[0038] Fig. 8 illustrates the operation of this phase shifting device. The input power E
applied to the input terminal of 90° 3-dB hybrid circuit 22 is distributed into two
substantially equal portions and outputted from output terminals 22₃ and 22₄, the
phase of output E₁ of output terminal 22₃ being delayed substantially 90° with respect
to the phase of output E₂ of output terminal 22₄.
[0039] Output is outputted to isolation terminal 22₂ according to the difference between
the impedance viewing the load side from output terminal 22₃ and the impedance viewing
the load side from output terminal 22₄, and this output is absorbed by reflectionless
terminator 23; however, in a state in which output terminal 22₃ and the load are matched
and output terminal 22₄ and the load are matched, the output outputted to isolation
terminal 22₂ becomes extremely small, and as a result, the permissible power of reflectionless
terminator 23 may be extremely low.
[0040] Output E₁ of output terminal 22₃ of 90° 3-dB hybrid circuit 22 is applied by way
of coaxial cable 26₂ to the driver point at which internal conductor 21₄₂ of coaxial
connection plug 21₃₂ of coupler 21 connects to first driver element 21₆₁. The instantaneous
value of the electric field propagated from this driving point in the Z direction
(the X-axis and Y-axis are determined as shown in Fig. 6, and the direction perpendicular
to the X- and Y-axis is the Z direction) is E
X. Output E₂ of output terminal 22₄ of 90° 3-dB hybrid circuit 22 is applied by way
of coaxial cable 26₁ to the driver point at which internal conductor 21₄₁ of coaxial
connection plug 21₃₁ of coupler 21 is connected to first driver element 21₆₁, and
the instantaneous value of the electric field propagated in the Z direction from this
driver point is E
Y. The instantaneous values E
X and E
Y of the electric field are:

The electric field propagated in the Z direction couples at the second driver
element 21₆₂, which together with round insulation plate 21₅₂ and the bottom wall
of the second sealed case 21₂ forms the second driver; but if the angle formed between
the straight line joining the center of first driver element 21₆₁ with the driver
point at which internal conductor 21₄₁ of coaxial connection plug 21₃₁ of coupler
21 connects to first driver element 21₆₁ and the straight line joining the center
of second driver element 21₆₂ with the driver point at which internal conductor 21₄₄
of coaxial connection plug 21₃₄ of coupler 21 connects to second driver element 21₆₂
is represented by φ, the output of coaxial connection plug 21₃₄ is represented by
E₃, and the output of coaxial connection plug 21₃₃ is represented by E₄, the outputs
E₃ and E₄ are:

The output E₃ of coaxial connection plug 21₃₄ is applied through input terminal
24₃ to 90° 3-dB hybrid circuit 24, and output E₄ of coaxial connection plug 21₃₃ is
applied through input terminal 24₄ to 90° 3-dB hybrid circuit 24. If the output of
isolation terminal 24₂ of 90° 3-dB hybrid circuit 24 is represented by E₅, and the
output of output terminal 24₁ is represented by E₆, outputs E₅ and E₆ are respectively:

In other words, in this phase shifting device, the phase of the output of output
terminal 24₁ of 90° 3-dB hybrid circuit 24 can be shifted by φ with respect to the
phase of the input to input terminal 22₁ of 90° 3-dB hybrid circuit 22 by simply rotating
the sealed cases 21₁ and 21₂ with respect to each other by the angle φ.
[0041] Fig. 9 shows the reflection characteristics at coaxial connection plug 21₃₁ for a
case in which the inside diameter of the cylinders having one closed end that form
sealed cases 21₁ and 21₂ of coupler 21 are selected as 0.285 λ
o (λ
o being the free space wavelength corresponding to the designed frequency f
o), the distance between the bottom wall of sealed case 21₁ and the bottom wall of
sealed case 21₂ is set at 0.089 λ
o, the specific inductive capacity of each of round insulation plates 21₅₁ and 21₅₂
is set at 10, the dielectric dissipation factor of each of round insulation plates
21₅₁ and 21₅₂ is set at 0.0055, the thickness of round insulation plates 21₅₁ and
21₅₂ is set at 0.023 λ
o, and each of the first and second driver elements 21₆₁ and 21₆₂ are formed in a circular
shape of diameter 0.21 λ
o. Here, the axis of abscissas shows the relative frequency with respect to the design
frequency f
o, and the axis of ordinates shows the amount of return loss (dB).
[0042] Fig. 10 shows the transmission characteristics between coaxial connection plugs 21₃₁
and 21₃₄ for a case in which each of the dimensions of coupler 21 is the same as for
Fig. 9, the axis of abscissas being equivalent to Fig. 9 and the axis of ordinates
showing the amount of transmission loss (dB).
[0043] As can be seen from Fig. 9 and Fig. 10, coupler 21 exhibits excellent reflection
characteristics and transmission characteristics over a broad band.
[0044] Furthermore, the thickness of round insulation plates 21₅₁ and 21₅₂ of coupler 21
can be selected according to the transmission frequency band, and the bandwidth can
be broadened by increasing the thickness from the selected thickness.
[0045] Fig. 11 shows observation results of changes in phase of the output from output terminal
24₁ of 90° 3-dB hybrid circuit 24 with respect to the phase of the input to input
terminal 22₁ of 90° 3-dB hybrid circuit 22, the axis of abscissas showing the frequencies
relative to the design frequency f
o and the axis of ordinates showing the amount of phase shift (
·) with respect to the angle of rotation φ, each of the dimensions of coupler 21 being
selected in the same way as explained for Fig. 9, the phase shifting device being
configured with 90° 3-dB hybrid circuit 22 connected to coupler 21 by way of coaxial
cables 26₁ and 26₂ and 90° 3-dB hybrid circuit 24 connected to coupler 21 by way of
coaxial cables 27₁ and 27₂ as shown in Fig. 3, and φ representing the angle of rotation
by which the sealed cases 21₁ and 21₂ forming coupler 21 have been rotated relative
to each other around their common cylindrical axis.
[0046] As is clear from Fig. 11, regardless of the transmission frequency, the amount of
phase shift always coincides with the angle of rotation φ of sealed cases 21₁ and
21₂ making up coupler 21 with respect to each other around their common cylindrical
axis.
[0047] Fig. 12 shows the observation results of the amount of transmission loss between
input terminal 22₁ of 90° 3-dB hybrid circuit 22 and output terminal 24₁ of 90° 3-dB
hybrid circuit 24 under the same conditions as for the observations in which the results
of Fig. 11 were obtained, the axis of abscissas being the same as for Fig. 11 and
the axis of ordinates showing the amount of transmission loss (dB).
[0048] As is clear from Fig. 12, compared to the amount of transmission loss shown in Fig.
10 for coupler 21 alone, the addition of 90° 3-dB hybrid circuits 22 and 24, coaxial
cables 26₁ and 26₂, as well as 27₁ and 27₂ increases the transmission loss, but the
degree of change in the frequency characteristic of the amount of transmission loss
is as for coupler 21 alone.
[0049] The foregoing explanation relates to a case in which sealed cases 21₁ and 21₂ of
coupler 21 are formed from metal; the first driver installed within coupler 21 is
formed from a microstrip antenna composed of sealed case 21₁, which is the ground
conductor, round insulation plate 21₅₁, and driver element 21₆₁; and the second driver
is formed from a microstrip antenna composed of sealed case 21₂, which is the ground
conductor, round insulation plate 21₅₂, and driver element 21₆₂. However, in a case
in which sealed cases 21₁ and 21₂ are formed by applying a metal film to the outer
surface of a body composed of a suitable synthetic resin, the metal film applied to
the outer surface of the body of sealed case 21₁ can serve as the ground conductor,
the body of sealed case 21₁ can serve as round insulation plate 21₅₁, and the first
driver composed of a microstrip antenna can therefore be formed by attaching driver
element 21₆₁ to the inner surface of the bottom wall of sealed case 21₁, and the second
driver composed of a microstrip antenna can similarly be formed by attaching driver
element 21₆₂ to the inner surface of the bottom wall of sealed case 21₂.
[0050] In a case in which sealed cases 21₁ and 21₂ are formed by multilayer stacking of
dielectric plates, the first driver composed of a microstrip antenna can be formed
by attaching driver element 21₆₁ to the inner surface of the bottom wall of sealed
case 21₁ and attaching a ground conductor to the outer surface of the bottom wall;
and the second driver composed of a microstrip antenna can be formed by attaching
driver element 21₆₂ to the inner surface of the bottom wall of sealed case 21₂ and
attaching a ground conductor to the outer surface of the bottom wall.
[0051] Instead of forming the driver as a microstrip antenna, the driver can also be formed
from a slot antenna formed by providing a cross-shaped slot 21₇₁ in the central portion
of metal plate or metal film 21₆₁ forming the driver element as shown in Fig. 13,
which is a sectional view taken along the same line as Fig. 6. Other construction
and reference numerals in Fig. 13 are as for Fig. 6.
[0052] In Fig. 14, which is a sectional view taken along the same line as Fig. 7, 21₇₁ is
cross-shaped slot, and 21₇₂, like 21₇₁, is a cross-shaped slot provided in the central
portion of the metal plate or metal film 21₆₂ forming the driver element, the other
construction and reference numerals being the same as for Fig. 7.
[0053] In this embodiment as well, if sealed cases 21₁ and 21₂ are formed by applying a
metal film to the outer surface of a base body composed of a suitable synthetic resin,
the metal film applied to the outer surface of the base body can serve as the ground
conductor and the base body itself can be used as round insulation plates 21₅₁ and
21₅₂ of Fig. 14; and if sealed cases 21₁ and 21₂ are formed by multilayer stacking
of dielectric plates, the first and second drivers composed of slot antennas can be
formed by attaching driver elements 21₆₁ and 21₆₂ composed of metal films or metal
plates provided with cross-shaped slots to the inner surface of each of the bottom
walls of sealed cases 21₁ and 21₂, and providing a ground conductor on the outer surface
of each bottom wall.
[0054] Further, probes may be connected to internal conductors 21₄₁ and 21₄₂ of coaxial
connection plugs 21₃₁ and 21₃₂ shown in Fig. 6 or Fig. 13, these probes being formed
such that the longitudinal direction of both probes is parallel to metal plate or
metal film 21₆₁, the portions of both probes extending in the longitudinal direction
intersect at the center point of metal plate or metal film 21₆₁, and this intersecting
angle is a right angle. A driver composed of probes similar to the sealed case 21₁
side may then be provided on the sealed case 21₂ side.
[0055] Whichever of the above constructions is adopted for the drivers installed in each
of sealed cases 21₁ and 21₂, the amount of phase shift between the input and output
is determined by the angle of relative rotation between sealed cases 21₁ and 21₂,
and in order for sealed cases 21₁ and 21₂ to rotate with respect to each other, any
of the following constructions may be adopted: coaxial cables 26₁, 26₂, 27₁, and 27₂
are formed as flexible cables; the sealed case 21₂ side is fixed and sealed case 21₁,
coaxial cables 26₁ and 26₂, and 90° 3-dB hybrid circuit 22 rotate as a unit; the sealed
case 21₁ side is fixed and sealed case 21₂, coaxial cables 27₁ and 27₂, and 90° 3-dB
hybrid circuit 24 rotate as a unit; or sealed case 21₁, coaxial cables 26₁ and 26₂,
and 90° 3-dB hybrid circuit 22 are formed as one rotatable unit and sealed case 21₂,
coaxial cables 27₁ and 27₂ and 90° 3-dB hybrid circuit 24 are formed as another rotatable
unit.
[0056] The foregoing explanations relate to cases in which sealed cases 21₁ and 21₂ are
each formed as a cylinder with one closed end, but either of sealed case 21₁ or 21₂
may be formed as a cylindrical case with one closed end in which is installed either
the first or second driver, and the other side, i.e., sealed case 21₂ or 21₁, may
be formed as a disk-shaped cover with the second or first driver attached to the inner
surface, this cover being formed to rotatably fit with the end portion of the opening
of the closed cylinder body.
[0057] As is clear from the foregoing explanation, in this phase shifting device, the side
of coaxial cables 26₁ and 26₂ and 90° 3-dB hybrid circuit 22 and the side of coaxial
cables 27₁ and 27₂ and 90° 3-dB hybrid circuit 24 are formed symmetrically to each
other across the plane cutting through the midsection of the coupler 21 at F-F in
Fig. 15; and consequently, precisely identical operation can be achieved as explained
in conjunction with Fig. 8 even if terminal 24₁ of 90° 3-dB hybrid circuit 24 is made
the input terminal and terminal 22₁ of 90° 3-dB hybrid circuit 22 is made the output
terminal. The other reference numerals of Fig. 15 are equivalent to those of Fig.
3.
[0058] The foregoing explanation relates to an example in which 90° 3-dB hybrid circuits
22 and 24 and reflection-less terminators 23 and 25 have been used for the two-partition
circuit of the input and the combining circuit of the output, but for a case in which
the transmission frequency bandwidth is relatively narrow, the input- and output-side
90° 3-dB hybrid circuits 22 and 24 and reflectionless terminators 23 and 25 can be
replaced by two-branch terminal circuits, with one of coaxial cables 26₁ and 26₂ connecting
coaxial connection plugs 21₃₁ and 21₃₂ of coupler 21 with the two output terminals
of the two-branch terminal circuit on the input side, for example, coaxial cable 26₂,
being formed exactly one transmission quarter-wavelength longer than coaxial cable
26₁, and one of coaxial cables 27₁ and 27₂ connecting coaxial connection plugs 21₃₃
and 21₃₄ of coupler 21 to the two input terminals of the two-branch terminal circuit
on the output side, for example coaxial cable 27₁, being formed exactly one transmission
quarter-wavelength longer than coaxial cable 27₂.
[0059] In this embodiment, although the lengths of coaxial cables 26₁ and 26₂ must be made
to differ by exactly one transmission quarter-wavelength, and the lengths of coaxial
cables 27₁ and 27₂ similarly must be made to differ by exactly one transmission quarter-wavelength,
the difference in lengths for both sets of cables is fixed at one transmission quarter-wavelength,
and fabrication is therefore relatively easy.
[0060] If the difference in lengths between coaxial cables 26₁ and 26₂ and the difference
in lengths between coaxial cables 27₁ and 27₂ is selected to be one quarter-wave-length
of the center frequency of the transmission band, the difference in length between
the coaxial cables will not precisely match the quarter-wavelength for frequencies
outside the center frequency, but since this embodiment is intended for applications
in which the transmission frequency band is relatively narrow, any operational error
arising due to variance from the quarter-wavelength is minute and presents no practical
problem.
[0061] The foregoing explanation relates to a case in which the phase shifting device of
the present invention is constructed by assembling three-dimensional constituent elements,
but the entire structure can be miniaturized by forming 90° 3-dB hybrid circuits 22
and 24 and reflectionless terminators 23 and 25 on a printed circuit board using a
printed wiring method, and forming coaxial cables 26₁, 26₂, 27₁ and 27₂ as microstrip
wiring.
[0062] The entire structure may also be made extremely compact and concise by providing
dielectric layers on the outer surfaces of sealed cases 21₁ and 21₂ of coupler 21,
and then forming by a printed wiring method on the dielectric layer provided on the
outer surface of sealed case 21₁ microstrip wiring that takes the place of 90° 3-dB
hybrid circuit 22, reflectionless terminator 23 and coaxial cables 26₁ and 26₂, and
forming by a printed wiring method on the dielectric layer provided on the outer surface
of sealed case 21₂ microstrip wiring that takes the place of 90° 3-dB hybrid circuit
24, reflectionless terminator 25 and coaxial cables 27₁ and 27₂.
[0063] In a case in which two-branch terminal circuits are used in place of 90° 3-dB hybrid
circuits 22 and 24 and reflectionless terminators 23 and 25, the entire structure
can be miniaturized through formation on printed circuit boards or on dielectric layers
provided on the outer surfaces of each of sealed cases 21₁ and 21₂.
[0064] Fig. 16 presents a phase shifting device according to another embodiment of the present
invention.
[0065] The phase shifting device of this embodiment is constructed from a coupler 31 composed
of cylindrical sealed cases 31₁ and 31₂ having one closed end, and terminals 31₃₁-31₃₃
composed of, for example, coaxial connection plugs; 90° 3-dB hybrid circuit 32 composed
of, for example, a quarter-wave coupled line-type directional coupler including input
terminal 32₁, isolation terminal 32₂, and output terminals 32₃ and 32₄; coaxial cable
33₁ connecting terminal 31₃₃ and input terminal 32₁; and coaxial cable 33₂ connecting
terminal 31₃₂ and isolation terminal 32₂. Here, considering a signal inputted to input
terminal 32₁, the phase of the output from output terminal 32₃ is delayed substantially
90° with respect to the phase of the output of output terminal 32₄. In addition, the
length of each of coaxial cable 33₁ and 33₂ is adjusted such that the phase difference
between inputs at the input end of each of coaxial cables 33₁ and 33₂ is maintained
unchanged when outputted from the output end of each of coaxial cables 33₁ and 33₂.
[0066] Fig. 17 shows a side view of coupler 31 of Fig. 16, and Fig. 18 shows a plan view
of the sealed case 31₁ side of coupler 31 as seen from the side of the bottom wall,
the reference numerals used in Figs. 17 and 18 being the same as those used in Fig.
16. Fig. 19 is an enlarged sectional view taken at line G-G of Fig. 16, Fig. 20 is
an enlarged sectional view taken at line H-H of Fig. 17, and Fig. 21 is an enlarged
sectional view taken at line I-I of Fig. 18.
[0067] As can be clearly seen from Fig. 21, stepped portions are formed in the side walls
at the end portions of the openings of each of sealed cases 31₁ and 31₂, the end portion
of the opening of one of the sealed cases, in this case sealed case 31₂, fitting inside
the end portion of the opening of the other sealed case 31₁, the two sealed cases
31₁ and 31₂ being mechanically and electrically coupled, and sealed cases 31₁ and
31₂ able to rotate relative to each other around their cylindrical axis.
[0068] Sealed cases 31₁ and 31₂ are manufactured by machining a metal block or press-forming
a metal sheet in the prescribed shape; by forming a suitable synthetic resin in a
preliminary form of the prescribed shape and subsequently applying a metal film to
the surface by an electroless plating or vacuum evaporation process; or by multilayer
stacking of dielectric plates having an appropriate dielectric constant and forming
as a cylinder with one closed end that shields electromagnetic energy in accordance
with Snell's law.
[0069] Coaxial connection plugs 31₃₁ to 31₃₃ have internal conductors 31₄₁ to 31₄₃. Round
insulation plates 31₅₁ and 31₅₂ are composed of a material having excellent high-frequency
characteristics such as an organic material such as polyethylene or fluorinated ethylene
or an inorganic material such as a ceramic and have a thickness less than the transmission
wavelength, round insulation plate 31₅₁ being secured to the inner surface of the
bottom wall of sealed case 31₁, round insulation plate 31₅₂ being secured to the inner
surface of the bottom wall of sealed case 31₂, and each being secured using a suitable
adhesive.
[0070] Metal plate 31₆₁ is secured to the surface of round insulation plate 31₅₁ using a
suitable adhesive, and in addition, a portion of its periphery is electrically connected
to internal conductor 31₄₁ of coaxial connection plug 31₃₁. First driver composed
of a microstrip antenna is formed with sealed case 31₁ on the opposing side of insulation
plate 31₅₁ serving as ground conductor, metal plate 31₆₁ serving as first driver element,
and the connection point between internal conductor 31₄₁ of coaxial connection plug
31₃₁ and metal plate 31₆₁ serving as the driver point.
[0071] Metal plate 31₆₂ is secured to the surface of round insulation plate 31₅₂ using a
suitable adhesive, and in addition, portions of its periphery are electrically connected
to internal conductors 31₄₂ and 31₄₃ of coaxial connection plugs 31₃₂ and 31₃₃. Second
driver composed of a microstrip antenna is formed with sealed case 31₂ on the opposing
side of insulation plate 31₅₂ serving as ground conductor, metal plate 31₆₂ serving
as second driver element, and the connection points between metal plate 31₆₂ and internal
conductors 31₄₂ and 31₄₃ of coaxial connection plugs 31₃₂ and 31₃₃ serving as the
driver points.
[0072] As can be seen from Fig. 20, a right angle is formed by the intersection of the straight
line joining the center of metal plate 31₆₂ with the driving point composed of the
connection point between internal conductor 31₄₂ of coaxial connection plug 31₃₂ and
metal plate 31₆₂, and the straight line joining the center of metal plate 31₆₂ with
the driving point formed by the connection point between internal conductor 31₄₃ of
coaxial connection plug 31₃₃ and metal plate 31₆₂.
[0073] In addition, the spacing between first driver element 31₆₁ and second driver 31₆₂
is set at less than the transmission wavelength.
[0074] The external conductor of coaxial connection plug 31₃₁ is electrically connected
to sealed case 31₁, and the external conductors of each of coaxial connection plugs
31₃₂ and 31₃₃ are connected to sealed case 31₂; but, as shown in Fig. 21, a gap is
provided by removing a portion of the sealed case 31₁ in the vicinity of internal
conductor 31₄₁ and a gap is provided by removing a portion of sealed case 31₂ in the
vicinity of internal conductor 31₄₃ such that internal conductors 31₄₁ and 31₄₃ of
coaxial connection plugs 31₃₁ and 31₃₃ do not mechanically contact sealed cases 31₁
and 31₂. Although not shown in Fig 21, a gap is similarly provided in sealed case
31₂ in the vicinity of internal conductor 31₄₂ of coaxial connection plug 31₂₁.
[0075] Rather than using an adhesive as a means of securing metal plate 31₆₁ or 31₆₂ to
the surface of round insulation plate 31₅₁ or 31₅₂, the center of metal plate 31₆₁
or 31₆₂ (the portion where electric field intensity is 0) may be secured to round
insulation plate 31₅₁ or 31₅₂ using a setscrew, or alternatively the center of metal
plate 31₆₁ or 31₆₂ may be screwed to the bottom wall of sealed case 31₁ or 31₂ through
round insulation plate 31₅₁ or 31₅₂.
[0076] Rather than forming the driver element of the microstrip antenna constituting the
first or second driver from metal plate 31₆₁ or 31₆₂, the driver element may be formed
by applying a metal film to the surface of round insulation plate 31₅₁ or 31₅₂ using
a vacuum evaporation process and finishing to the required outline shape by a process
such as etching.
[0077] Whether the driver element is formed from a metal plate or metal film, its outline
shape may be formed as a square instead of the circle shown in Fig. 19 and Fig. 20.
[0078] Regarding the dimensions of driver elements 31₆₁ and 31₆₂ for cases in which driver
elements 31₆₁ and 31₆₂ are driven in basic mode, if the outline shape of these elements
is formed as a circle, the specific inductive capacity of round insulation plates
31₅₁ and 31₅₂ is ε
r and the design frequency is f
o, the radius of driver elements 31₆₁ and 31₆₂ is preferably selected to be substantially

; and if the outline shape of driver elements 31₆₁ and 31₆₂ is formed as a square,
the length of one side is preferably selected to be substantially

(where C is the speed of light).
[0079] Fig. 22 illustrates the operation of the present phase shifting device.
[0080] The input applied to coaxial connection plug 31₃₁ of coupler 31 passes through internal
conductor 31₄₁ and drives driver element 31₆₁ in the first driver.
[0081] If the X-axis and Y-axis are established as shown in Fig. 19, Fig. 20, and Fig. 22A,
electric field vector E produced by driver element 31₆₁ driven as described above
can be divided between two orthogonal components E
X and E
Y as shown in Fig. 22A. These couple at driver element 31₆₂ of the second driver in
the form:

As described hereinabove, this device is formed such that a right angle is formed
by the intersection of the straight line joining the center of driver element 31₆₂
with the driving point constituted by the connection point between driver element
31₆₂ and internal conductor 31₄₂ of coaxial connection plug 31₃₂ and the straight
line joining the center of driver element 31₆₂ with the driving point constituted
by the connection point between driver element 31₆₂ and internal element 31₄₃ of coaxial
connection plug 31₃₃; and therefore, when driver element 31₆₂ is driven in basic mode,
coupling between coaxial connection plugs 31₃₂ and 31₃₃ becomes sparse and quadrature
mode coupling is enabled.
[0082] The quadrature mode coupling to driver element 31₆₂ causes component E
X to be outputted from coaxial connection plug 31₃₂ and component E
Y to be outputted from coaxial connection plug 31₃₃, the two outputs being respectively
inputted to terminals 32₁ and 32₂ of 90° 3-dB hybrid circuit 32 by way of coaxial
cables 33₁ and 33₂.
[0083] If the output of output terminals 32₄ and 32₃ of 90° 3-dB hybrid circuit 32 are E₁
and E₂, respectively:

Although the phase of output E₁ shifts in a counter-clockwise direction with increase
in declination angle φ of electric field vector E from the X-axis as shown in Fig.
22A, the amplitude remains unchanged. The phase of output E₂ also shifts in a clockwise
direction with increase in declination angle φ of electric field vector E from the
X-axis, but again, the amplitude remains unchanged. Accordingly, if the declination
angle φ of electric field vector E from the X-axis is 45° or 225°, the amplitude as
well as the phase of both outputs E₁ and E₂ are equal, but if the declination angle
φ increases from 45° or 225°, the phase of output E₁ shifts in the advance direction,
and the phase of output E₂ shifts in the delay direction. If the declination angle
φ of electric field vector E from the X-axis further increases to 135° or 315°, the
phase relation between outputs E₁ and E₂ is mutually reversed.
[0084] Fig. 23 shows the reflection characteristic at coaxial connection plug 31₃₁ observed
after removing coaxial cables 33₁ and 33₂ from coaxial connection plugs 31₃₂ and 31₃₃,
the inner diameter of the cylinders with one closed end forming sealed cases 31₁ and
31₂ of coupler 31 being selected as 0.285 λ
o (λ
o being the free-space wavelength corresponding to the design frequency f
o), the distance of opposition between the bottom wall of sealed case 31₁ and the bottom
wall of sealed case 31₂ as 0.089 λ
o, the specific inductive capacity of round insulation plates 31₅₁ and 31₅₂ as 10,
the dielectric dissipation factor of each of round insulation plates 31₅₁ and 31₅₂
as 0.0055, the thickness of each of round insulation plates 31₅₁ and 31₅₂ as 0.023
λ
o, the outline shape of first and second driver elements 31₆₁ and 31₆₂ being formed
as a circle with a diameter of 0.21 λ
o, the axis of abscissas in the figure being the relative frequency for the design
frequency f
o, and the axis of ordinates being the amount of return loss (dB). Fig. 24 shows the
transmission characteristics between coaxial connection plugs 31₃₁ and 31₃₃ observed
with coaxial cable 33₁ and 33₂ removed from coaxial connection plugs 31₃₂ and 31₃₃
and the selected values of the dimensions of each of the parts of coupler 31 being
the same as described for Fig. 23, the horizontal axis of the figure being the same
as for Fig. 23 and the vertical axis being the amount of transmission loss (dB).
[0085] As is clear from Fig. 23 and Fig. 24, coupler 31 exhibits excellent reflection characteristics
and transmission characteristics across a broad band.
[0086] In addition, the thickness of round insulation plates 31₅₁ and 31₅₂ in coupler 31
can be selected according to the transmission frequency band, and the bandwidth can
be broadened by increasing the selected thickness.
[0087] Fig. 25 shows the results of observing the phase shift of output E₁ of coaxial connection
plug 31₃₃ and output E₂ of coaxial connection plug 31₃₂ upon change of declination
angle φ to 90° or 135° with 45° as a standard. Here, the same values are selected
for the dimensions of each part of coupler 31 as described for Fig. 23; the phase
shifting device is configured as shown in Fig. 16, wherein 90° 3-dB hybrid circuit
32 is connected to coupler 31 by way of coaxial cables 33₁ and 33₂; and sealed cases
31₁ and 31₂, which make up coupler 31, are rotated relative to each other around their
common cylindrical axis. The angle of declination φ is formed by the straight line
joining the center of driver element 31₆₂ with the connection point between internal
conductor 31₄₂ of coaxial connection plug 31₃₂ and driver element 31₆₂ in the second
driver installed on the sealed case 31₂ side, i.e., the X-axis, and the electric field
vector E arising due to drive of driver element 31₆₁ in the first driver installed
on the sealed case 31₁ side. For both outputs E₁ and E₂, the absolute value of the
change in phase and the change in declination angle φ match without any dependence
on transmission frequency, and the code of phase of outputs E₁ and E₂ differ. Accordingly,
the phase difference between outputs E₁ and E₂ with respect to change in declination
angle φ is 2φ.
[0088] The axis of abscissas of Fig. 25 is the same as for Fig. 23, and the axis of ordinates
shows declination angle φ, i.e., the amount of phase shift (
·) with respect to the relative angle of rotation φ between sealed cases 31₁ and 31₂.
[0089] Fig. 26 shows the amount of transmission loss between coaxial connection plug 31₃₁
of coupler 31 and output terminal 32₃ of 90° 3-dB hybrid circuit 32, and between coaxial
connection plug 31₃₁ of coupler 31 and output terminal 32₄ of 90° 3-dB hybrid circuit
32, the observation results being obtained under the same conditions as those for
Fig. 25, the axis of abscissas being the same as Fig. 25 and the axis of ordinates
showing the amount of transmission loss (dB).
[0090] As is clear from Fig. 26, although the addition of 90° 3-dB hybrid circuit 32 and
coaxial cables 33₁ and 33₂ results in increased transmission loss as compared with
the amount of transmission loss for the case shown in Fig. 24 in which coupler 31
alone is used, the differences in the change of phase shift of outputs E₁ and E₂ with
respect to the change in angle φ or in amplitude of outputs E₁ and E₂ are virtually
negligible.
[0091] Fig. 27 shows an example which employs both outputs E₂ and E₁ of output terminals
32₃ and 32₄ of 90° 3-dB hybrid circuit 32. Reference numeral 34 indicates the phase
shifting device shown in Fig. 16, 31₃₁ is the input terminal of coupler 31 in phase
shifting device 34, 32₃ and 32₄ are the output terminals of 90° 3-dB hybrid circuit
32 in phase shifting device 34, and 35₁ and 35₂ are both subarray antennas composed
of a plurality of element antennas.
[0092] The locus joining the peaks of each of output vectors E
X and E
Y corresponding to the change in the relative angle of rotation φ between sealed cases
31₁ and 31₂ which make up coupler 31 in phase shifting device 34 is an oval, but the
angle at which output vectors E
X and E
Y begin to describe an oval both differs by 90° and is in the opposite direction of
rotation, and consequently, the phase difference between outputs E₂ and E₁ can be
freely selected. Accordingly, the direction of maximum radiation and the side-lobe
characteristics of the array antenna composed of subarray antennas 35₁ and 35₂ can
be controlled by supplying outputs E₂ and E₁ of output terminals 32₃ and 32₄ as the
driving power of subarray antennas 35₁ and 35₂.
[0093] A comparison of Fig. 27 and Fig. 2 clearly shows that, while the structure of a power
supply circuit using a phase shifting device of the prior art was complicated by the
requirement for a transmission path having a standard amount of phase shift and a
two-branch circuit for each phase shifter, the use of a phase shifting device of the
present invention results in a power supply circuit of extremely simple construction
because the phase shifting device of the present invention has an effect equivalent
to the combination of a prior-art phase shifting device, a transmission path having
a standard amount of phase shift, and a two-branch circuit.
[0094] The foregoing description relates to an example in which sealed cases 31₁ and 31₂
of coupler 31 are formed from metal; the first driver installed in coupler 31 is formed
from a microstrip antenna composed of sealed case 31₁ which serves as a ground conductor,
round insulation plate 31₅₁, and driver element 31₆₁; and the second driver is formed
from a microstrip antenna composed of sealed case 31₂ which serves as a ground conductor,
round insulation plate 31₅₂, and driver element 31₆₂. However, if sealed cases 31₁
and 31₂ are each formed by applying a metal film to the outer surface of a base body
composed of a suitable synthetic resin, the metal film applied to the outer surface
of the base body of sealed case 31₁ can be used as a ground conductor, the base body
itself of sealed case 31₁ can be used as round insulation plate 31₅₁, and as a result,
the first driver composed of a microstrip antenna can be formed by attaching driver
element 31₆₁ to the inner surface of the bottom wall of sealed case 31₁, and the second
driver composed of a microstrip antenna can be formed by attaching driver element
31₆₂ to the inner surface of the bottom wall of sealed case 31₂.
[0095] For a case in which sealed cases 31₁ and 31₂ are formed by multilayer stacking of
dielectric plates, the first driver composed of a microstrip antenna can be formed
by attaching driver element 31₆₁ to the inner surface and attaching a ground conductor
to the outer surface of the bottom wall of sealed case 31₁, and the second driver
composed of a microstrip antenna can be formed by attaching driver element 31₆₂ to
the inner surface and attaching a ground conductor to the outer surface of the bottom
wall of sealed case 31₂.
[0096] As shown in Fig. 28 in a sectional view similar to that of Fig. 20, instead of being
formed from a microstrip antenna, the second driver may be formed from a slot antenna
achieved by providing a cross-shaped slot 31₇ in the center of metal plate or metal
film 31₆₂ forming the driver element; and the first driver may be formed as a slot
antenna composed of only a slot in the vertical direction or in the horizontal direction
of the cross-shaped slot of Fig. 28. Other reference numerals and construction in
Fig. 28 is as for Fig. 20.
[0097] In this embodiment as well, if sealed cases 31₁ and 31₂ are formed by applying a
metal film to the outer surface of a base body composed of a suitable synthetic resin,
the metal film applied to the outer surface of the base body may be used as the ground
conductor, and the base body itself can be used as round insulation plates 31₅₁ and
31₅₂; and if sealed cases 31₁ and 31₂ are formed by multilayer stacking of dielectric
plates, first and second drivers composed of slot antennas can be formed by attaching
driver elements 31₆₁ and 31₆₂ composed of a metal plate or metal film provided with
a single-line slot or a cross-shaped slot to the inner surfaces of the bottom walls
of each of sealed cases 31₁ and 31₂ and attaching ground conductors to the outer surfaces
of each bottom wall.
[0098] In addition, the first driver may be formed by connecting a probe to internal conductor
31₄₁ of coaxial con nection plug 31₃₁ shown in Fig. 19; and the second driver may
be formed by connecting probes to internal conductors 31₄₂ and 31₄₃ of coaxial connection
plug 31₃₂ and 31₃₃ shown in Fig. 20, the longitudinal direction of both probes being
parallel to metal plate or metal film 31₆₂ and the portions extending in the longitudinal
direction of both probes intersecting at the center point of metal plate or metal
film 31₆₂, this intersection being a right angle.
[0099] In either of the above-described constructions of the first and second drivers installed
in sealed cases 31₁ and 31₂, respectively, the amount of phase shift between input
and output is determined according to the relative angle of rotation between sealed
cases 31₁ and 31₂, and to rotate sealed cases 31₁ and 31₂ relative to each other,
a construction may be adopted wherein sealed case 31₂, coaxial cables 33₁ and 33₂,
and 90° 3-dB hybrid circuit 32 are fixed and sealed case 31₁ is caused to rotate;
wherein sealed case 31₁ is fixed and sealed case 31₂, coaxial cables 33₁ and 33₂,
and 90° 3-dB hybrid circuit 32 are caused to rotate as a unit; or wherein sealed case
31₁ and 90° 3-dB hybrid circuit 32 are fixed, coaxial cables 33₁ and 33₂ is formed
from a flexible cable, and sealed case 31₂ is caused to rotate.
[0100] The foregoing explanation relates to a case in which sealed cases 31₁ and 31₂ are
both formed as cylinders with one closed end, but either sealed case 31₁ or 31₂ may
be formed as a cylinder with one closed end in which the first or second driver is
installed, and the other sealed case, i.e., sealed case 31₂ or 31₁ may be formed as
a disk-shaped cover with the second or first driver attached to its inner surface
and formed such that the cover rotatably fits with the end portion of the opening
of the cylinder with one closed end.
[0101] The foregoing explanation relates to a case in which 90° 3-dB hybrid circuit 32 is
formed as a quarter-wave coupled-line directional coupler, but the hybrid circuit
may also be formed as a branch line directional coupler.
[0102] In addition, for cases in which the transmission fre quency bandwidth is relatively
narrow, a two-branch terminal circuit may take the place of 90° 3-dB hybrid circuit
32, and the length of one of coaxial cables 33₁ and 33₂, for example coaxial cable
33₂, may be formed exactly one transmission quarter-wavelength longer than coaxial
cable 33₁.
[0103] In this embodiment, the lengths of coaxial cable 33₁ and 33₂ must differ by exactly
one transmission quarter-wavelength, but fabrication is relatively easy because the
difference in length between coaxial cables 33₁ and 33₂ is fixed at one transmission
quarter-wavelength.
[0104] If the difference in lengths between coaxial cables 33₁ and 33₂ is selected to be
one transmission quarter-wavelength for the center frequency of the transmission band,
the difference in length between the coaxial cables will not precisely match the quarter-wavelength
for frequencies outside the center frequency, but since this embodiment is intended
for applications in which the transmission frequency band is relatively narrow, any
operational error arising due to variance from the quarter-wavelength is minute and
presents no practical problem.
[0105] The foregoing explanation relates to a case in which the phase shifting device is
constructed by assembling three-dimensional constituent elements, but the entire structure
can be miniaturized by forming 90° 3-dB hybrid circuit 32 on a printed circuit board
using a printed wiring method and forming coaxial cables 33₁ and 33₂ as microstrip
wiring.
[0106] The entire structure may also be made extremely compact and concise by providing
a dielectric layer on the outer surface of sealed case 31₂ of coupler 31, and then
employing a printed wiring method to form 90° 3-dB hybrid circuit 32 and microstrip
wiring that takes the place of coaxial cables 33₁ and 33₂.
[0107] In a case in which a two-branch terminal circuit takes the place of 90° 3-dB hybrid
circuit 32, the entire structure can be miniaturized by forming this component on
a printed circuit board or on a dielectric layer provided on the outer surface of
sealed cases 31₂.