U.S. patent number 3,838,367 [Application Number 05/408,512] was granted by the patent office on 1974-09-24 for microstrip filter comprising a ferromagnetic resonant body.
This patent grant is currently assigned to U.S. Philips Corporation. Invention is credited to Hans Bex.
United States Patent |
3,838,367 |
Bex |
September 24, 1974 |
MICROSTRIP FILTER COMPRISING A FERROMAGNETIC RESONANT BODY
Abstract
A YIG crystal filter, notably for use in mixing circuits, by
means of which, in addition to a frequency separation, a separation
of even and odd waves on a double line can be realized. According
to the invention, the transmission properties are substantially
improved by interconnecting points of the double line at the area
of the YIG crystal by means of a transmission line having a length
of one half wavelength related to the magnetic resonant frequency
of the YIG crystal.
Inventors: |
Bex; Hans (Aachen,
DT) |
Assignee: |
U.S. Philips Corporation (New
York, NY)
|
Family
ID: |
19817302 |
Appl.
No.: |
05/408,512 |
Filed: |
October 23, 1973 |
Foreign Application Priority Data
Current U.S.
Class: |
333/204;
455/325 |
Current CPC
Class: |
H01P
1/218 (20130101); H01P 1/203 (20130101) |
Current International
Class: |
H01P
1/203 (20060101); H01P 1/218 (20060101); H01P
1/20 (20060101); H01p 001/20 () |
Field of
Search: |
;333/73R,73C,73S |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Gensler; Paul L.
Attorney, Agent or Firm: Trifari; Frank R. Steinhauser; Carl
P.
Claims
What is claimed is:
1. An electric band-pass filter in which a first transmission line
is magnetically coupled to a second transmission line, extending
perpendicular thereto, by way of at least one body of
ferro-magnetic material which is magnetically pre-polarized in the
direction perpendicular to the directions of the transmission lines
with a strength such that magnetic resonance occurs at the desired
band-pass frequency, the first transmission line being formed by
two conductors and an earthed return conductor, it being possible
for even and odd waves to appear on the said two conductors, the
said two conductors being symmetrically arranged with respect to
the magnetic body such that the magnetic field of the even waves is
mainly perpendicular to the pre-polarization direction at the area
of the magnetic body, that of the odd waves extending mainly
parallel to the pre-polarization direction, characterized in that
the first transmission line is terminated on one end by a detour
line having an electrical length of approximately one half
wavelength related to the magnetic resonant frequency.
Description
The invention relates to an electric band-pass filter comprising at
least one body of ferromagnetic material.
Known filters of this kind comprise two transmission lines which
cross each other at right angles and which are magnetically
interconnected by way of a body of ferromagnetic material, for
example, a YIG crystal sphere which is magnetically pre-polarized
in the direction perpendicular to the directions of the
transmission lines. These two transmission lines which cross each
other at right angles are normally not coupled to each other. At
the magnetic resonant frequency (dependent of the strength of the
pre-polarizing field), however, a precession of the magnetic vector
occurs, with the result that coupling takes place. This coupling is
frequency-selective.
Also known are filters of this kind comprising a cascade of two or
more of such magnetic coupling bodies which are coupled to each
other, for example, via an opening in a conductive partition.
Also known is a diode mixing circuit for high frequencies (for
example, 2 GHz), in which use is made of such a magnetic filter for
filtering out the intermediate frequency and possibly for forming
directly therefrom a second intermediate frequency by a means of a
second transmission line. In this device a local oscillator is
connected to a diode mixing circuit via a first transmission line.
On this transmission line odd waves occur (that is to say, waves
whose currents are in phase-opposition) which have the frequency of
the local oscillator, and even waves (that is to say, waves whose
currents are in phase) which correspond to the desired intermediate
frequency signal.
This signal is filtered out by means of a YIG crystal filter.
Therefore, the two conductors are symmetrically arranged with
respect to the pre-polarized magnetic body such that the magnetic
field of the even waves on the transmission line is mainly
perpendicular to the pre-polarization direction at the area of the
body, so that coupling to the precession field takes place, whilst
the magnetic field of the odd waves is mainly parallel to the
pre-polarization direction, with the result that the coupling is
nil or at least insignificant.
Even though the frequency difference between the even and the odd
waves can often be comparatively small in practice, the filtering
action is very effective as a result of the difference in coupling
strength of the even and the odd waves with the magnetic body.
The desired intermediate frequency signal is derived by means of a
second transmission line which crosses the first transmission line
at right angles and which is magnetically coupled to the magnetic
body, possibly via a cascade of inter-connected magnetic bodies.
Like the first transmission line, the second transmission line can
also consist of a plurality of conductors.
The invention relates notably to an electric band-pass filter in
which a first transmission line is magnetically coupled to a second
transmission line, extending perpendicular thereto, by way of at
least one body of ferromagnetic material which is magnetically
pre-polarized in the direction perpendicular to the directions of
the transmission lines with a strength such that magnetic resonance
occurs at the desired band-pass frequency, the first transmission
line being formed by two conductors and an earthed return
conductor, it being possible for even and odd waves which can have
frequencies of the same order of mangitude to appear on the said
two conductors, the said two conductors being symmetrically
arranged with respect to the magnetic body such that the magnetic
field of the even waves is mainly perpendicular to the
pre-polarization direction at the area of the magnetic body, that
of the odd waves extending mainly parallel to the prepolarization
direction.
The invention is characterized in that the first transmission line
is terminated on one end by a detour line having an electrical
length of approximately one half wavelength related to the magnetic
resonant frequency.
This detour line substantially has a short-circuit between the
conductors and the return conductor for the even waves at the area
of the magnetic body, whilst for the odd waves a comparatively high
impedance is present between the conductors and the return
conductor (at this area).
The invention will be described in detail hereinafter with
reference to the drawing.
FIG. 1 is a diagrammatic representation of a double mixing circuit
of a known kind in which the filter according to the invention is
used.
FIGS. 2 and 3 show the shape of the magnetic field generated by
currents on the conductors in the same direction and by currents in
the opposite direction, respectively.
FIG. 4 is a plan view of a given embodiment of the filter.
FIG. 5 is a cross-sectional view taken along the line V--V, and
FIG. 6 is a perspective view of a detail.
The double mixing circuit shown in FIG. 1 can be used, for example,
as the input mixing circuit in a television receiver by means of
which all television bands with a frequency range of, for example,
50 MHz to 900 MHz can be covered merely by variation of the
frequency of a local oscillator, without the switching over of
tuned circuits being necessary. For this purpose, the input signal
is first stepped up in a first mixing stage, comprising an
oscillator of fixed frequency, to an intermediate frequency of, for
example, 2,000 MHz to which the filter is tuned, and is
subsequently stepped down in a second mixing stage to the normal
intermediate frequency of approximately 35 MHz of the television
receiver.
The input signal of the signal source S is applied, via the
conductors L1, L2 to the diode bridge R1, the output terminals of
which are connected to the YIG crystal filter F via the conductors
L3, L4.
The conductors L3, L4, are arranged to be symmetrical with respect
to a sphere Y1, made of YIG-crystal, which is magnetically
pre-polarized by a magnetic field H.sub.a perpendicular to the
plane of the conductors (FIG. 2) such that magnetic resonance
(Kittel mode) occurs at 2,000 MHz.
In the points 1 and 2 just below the sphere Y1 the conductors L3,
L4, are terminated by a detour line L5, the length of which is
equal to one half wavelength at the resonant frequency.
Furthermore, the points 1 and 2 are connected, by way of conductors
L6, L7, to the local oscillator G1 whose frequency can be varied
between 2050 MHz and 2900 MHz. The signal of the oscillator G1 is
thus applied, via the conductors L6, L3 and L7, L4, to the diode
bridge R1 such that the currents in the conductors are in
phase-opposition (odd waves).
Under the influence of the signal of generator G1 and the input
signal, the diode bridge R1 forms mixing products, including the
intermediate frequency signal of 2,000 MHz, which is applied in the
same phase (even wave) to the conductors L3 and L4.
FIGS. 2 and 3 show a cross-sectional view at the area of the sphere
Y1. The conductors L3 and L4 are constructed as microstrips and are
provided on one side of a dielectric carrier D. Provided on the
other side of the carrier D is an earthed metal plate A having a
coupling opening K. The sphere Y1 is situated in a recess in the
carrier D and is pre-polarized by a magnetic field H.sub.a.
FIG. 2 also shows lines of force M of the high-frequency magnetic
field which is generated by even waves on the conductors L3 and L4.
These lines of force enclose the two conductors L3 and L4 and are
directed mainly perpendicular to the magnetic field H.sub.a at the
area of the sphere Y1. As is known, under these circumstances a
precession of the magnetic vector about the direction of the field
H.sub.a occurs. This precession is maximum if the frequency of the
waves corresponds to the magnetic resonant frequency of the medium
which is determined by the strength of the field H.sub.a. The even
waves, representing the desired intermediate frequency signal of
2,000 MHz, therefore, as strongly magnetically coupled to the
sphere Y1.
FIG. 3 shows lines of force M of the high-frequency magnetic field
generated by odd waves on the conductors L3 and L4. These lines of
force enclose the conductors L3 and L4 separately and are directed
mainly parallel to the field H.sub.a at the area of the sphere Y1.
Consequently, the odd waves are very weakly mangetically coupled to
the sphere, on the one hand because the lines of force parallel to
the field H.sub.a do not initiate the precession, and on the other
hand because the generator frequency deviates substantially from
the magnetic resonant frequency.
The two wave types are thus very effectively separated.
The sphere Y1 is magnetically coupled to the further circuit, via
the coupling opening K, as will be described hereinafter.
The detour line L5 constitutes a short-circuit between the points 1
and 2 and earth for the even waves, with the result that at the
area of the YIG crystal sphere Y1 a current loop appears for the
intermediate frequency signal. The magnetic coupling between the
even waves and the sphere Y1, consequently, is maximum.
In the known mixing circuit the detour line L5 is absent, with the
result that the currents of the even waves in the vicinity of the
sphere can be much smaller than the maximum value.
Moreover, the enen waves on the conductors L3 and L4 can proceed
further over the conductors L6 and L7 in the direction of the
generator G1, which causes additional losses and which has an
adverse effect on the stability of the generator.
One consequence is that a high insertion loss of, for example, 16
dB can occur in the filter.
However, for the odd waves of the generator signal the detour line
has a high impedance between the points 1 and 2. This implies a
given loading of the generator, but is of no further
importance.
The conductors system L3, L4, L5, L6, L7 is arranged, as is shown
in the plan view of FIG. 4, on one side of the filter plate. The
diameter of the spheres amounts to, for example, 0.8 mm and that of
the coupling opening to 4 mm. As is denoted by broken lines in FIG.
4, a conductor system L8, L9, L10, L11, L12, of the same shape as
the first system but rotated through 90.degree. with respect
thereto, is provided on the other side. FIG. 5 shows a
cross-sectional view. Analogous to the FIGS. 2 and 3, the first
condutor system is provided on a dielectric carrier D1 and is
coupled to the sphere Y1. Similarly, the second conductor system is
provided on a carrier D2 and is coupled to the YIG crystal sphere
Y2. Present between the carriers D1 and D2 is a metal plate A
having a coupling opening K, a detail of which is shown in FIG.
6.
The spheres Y1 and Y2 are connected to carrier rods H1 and H2 which
are inserted into holes in the carriers D1 and D2. By means of the
carrier rods H1 and H2, the crystal axes of the spheres Y1 and Y2
can be oriented such that the temperature influence is minimum. The
spheres are magnetically coupled to each other via the opening K
and are tuned to the same frequency. As is known, a band-filter
action is thus obtained.
As appears from FIG. 1, the conductors L11 and L12 are connected to
a generator G2 whose frequency has the fixed value 1965 MHz. The
generator G2 generates odd waves on the condutor system L8, L11 and
L9, L12, respectively.
The magnetic rotary field in the sphere Y2 induces even waves in
the conductors L8 and L9, the said waves proceeding at a frequency
of 2,000 MHz in the direction of the diode bridge R2 where they are
mixed with the generator signal. The intermediate frequency signal
having a frequency of 35 MHz appears on the output terminals U1 and
U2.
The detour line L10, the electric length of which is equal to one
half wavelength at the resonant frequency of 2,000 MHz and which is
connected between the points 3 and 4, constitutes a short-circuit
for the even waves between the conductors L8 and L9 and the earthed
intermediate plate A. It is thus prevented that the even waves can
proceed on the conductors L11 and L12 to the generator G2, which
would lead to losses.
As a result of the use of the detour lines L5 and L10 according to
the invention, it was found to be possible to achieve a drastic
reduction of the insertion loss of the filter, for example, from 16
dB to 2.6 dB. Moreover, the filter action was improved by this step
because the strength ratio of the even and the odd waves is
improved in the vicinity of the YIG crystal spheres.
The filter can be modified in various manners within the scope of
the invention.
For example, a single sphere can be used instead of two
spheres.
If the filter is used in a single mixing circuit, it is not
necessary for the two crossed transmission lines to consist of two
conductors each. In such a case one of the transmission lines can
consist of a single conductor like in the known filters.
* * * * *