U.S. patent number 3,668,574 [Application Number 05/029,626] was granted by the patent office on 1972-06-06 for hybrid mode electric transmission line using accentuated asymmetrical dual surface waves.
This patent grant is currently assigned to British Railways Board. Invention is credited to Harold Monteagle Barlow.
United States Patent |
3,668,574 |
Barlow |
June 6, 1972 |
HYBRID MODE ELECTRIC TRANSMISSION LINE USING ACCENTUATED
ASYMMETRICAL DUAL SURFACE WAVES
Abstract
A method and means for reducing net transmission losses and
frequency dispersion within an electrical transmission line having
dual conducting surfaces and carrying a hybrid mode electromagnetic
wave comprising both a TEM component and a dual surface wave
component. One of the two conducting surfaces is caused to have
more surface resistance than the other by a predetermined amount
thereby making the surface wave part of the field asymmetric and
enhancing the energy particularly associated with the surface wave
to the detriment of the other existing components such as the TEM
field. The predetermined amount of surface reactance is controlled
to reduce the product of transverse attenuation and phase-change
coefficients for the hybrid wave thereby causing a reduction in its
overall axial attenuation coefficient in the direction of
propogation. Thus the wave is slowed down by the dielectric
loading, its phase-change coefficient is increased and made more
nearly proportional directly to frequency.
Inventors: |
Barlow; Harold Monteagle
(Banstead, EN) |
Assignee: |
British Railways Board (London,
EN)
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Family
ID: |
26239390 |
Appl.
No.: |
05/029,626 |
Filed: |
April 17, 1970 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
Issue Date |
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672560 |
Oct 3, 1967 |
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Foreign Application Priority Data
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Oct 7, 1966 [GB] |
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45,14/66 |
Feb 1, 1967 [GB] |
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4,818/67 |
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Current U.S.
Class: |
333/240; 333/222;
333/219 |
Current CPC
Class: |
H01P
3/02 (20130101); H01P 3/04 (20130101); H01B
11/1895 (20130101); H01B 11/14 (20130101) |
Current International
Class: |
H01B
11/18 (20060101); H01B 11/02 (20060101); H01B
11/14 (20060101); H01P 3/02 (20060101); H01P
3/04 (20060101); H01p 001/16 (); H01p 003/06 ();
H01p 011/00 () |
Field of
Search: |
;333/84R,95S,96 ;174/12C
;156/53 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
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1,076,211 |
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Feb 1960 |
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DT |
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1,022,279 |
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Jan 1958 |
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DT |
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694,622 |
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Jul 1953 |
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GB |
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Other References
Barlow 1965, "Screened Surface Waves and Some Possible
Applications" Proc IEE Vol. 112 No. 3, 3-1965, pp. 477-482 .
Discussion, "Screened Surface Waves and Some Possible
Applications," Proc IEE Vol. 112, No. 10, 10-1965, pp. 1894-1895
.
Barlow et al.; 1954, "An Experimental Investigation of the
Properties of Corrugated Cylindrical Surface waveguides," Proc IEE,
101, PT. III, 1954, pp. 182-188 .
Barlow et al.; 1953, "Surface Waves," Proc IEE, 100, pt. III,
11-1953, pp. 329, 337-338 .
Barlow, 1967; "New Features of Wave Propogation Not Subject to
Cutoff Between Two Parallel Guiding Surfaces," Proc IEE, 114, No.
4, 4-67, pp. 421-427 .
Barlow 1968; "High-Frequency Coaxial Cables," Proc IEE, 115 No. 2,
2-1968, pp. 243-246 .
Barlow 1969, "Hybrid Tem-Dial Surface Wave in Coaxial Cable" Proc
IEE, 116, No. 4, 4-1969, pp. 489-494 .
Millington et al.; "Riccati Approach to the Propogation of Axially
Symmetric Waves in a Coaxial Guide," Proc IEE, 115, No. 8, 8-1968,
pp. 1079-1088.
|
Primary Examiner: Saalbach; Herman Karl
Assistant Examiner: Punter; Wm. H.
Parent Case Text
The subject matter of this specification constitutes a
continuation-in-part of the subject matter of my previous
application, Ser. No. 672,560, filed Oct. 3, 1967, now abandoned,
which also relates to an electric transmission line.
Claims
1. In a hybrid mode dual surface electrical transmission line, a
new use for dielectric material on one conducting surface of said
line which is of the type that inherently transmits a hybrid wave
comprising at least a TEM mode and a dual surface wave mode and
which has a pair of spaced-apart generally parallel conducting
surfaces with a second dielectric material in between, said new use
comprising the method steps of:
adding to said one conducting surface a predetermined thickness of
the first-mentioned dielectric material having a permittivity
greater than said second dielectric material to increase the
surface reactance of said one surface and to product an accentuated
asymmetrical dual surface wave mode thereby reducing the dispersion
and attenuation of the resulting hybrid mode while simultaneously
introducing additional line losses caused by the addition of said
first dielectric material, and
controlling the predetermined thickness of said first dielectric
material to produce a substantially constant phase velocity over a
relatively wide frequency range and to produce an increase in
overall line attenuation due to said additional losses that is
significantly less than an accompanying reduction in overall line
attenuation due to said accentuated asymmetrical dual surface wave
whereby a net reduction in overall line attenuation is
2. A new use method as in claim 1, wherein said thickness
controlling step
3. A method for decreasing frequency dispersion and net line
attenuation in a two conductor transmission line system comprising
a pair of spaced-apart generally parallel conducting surfaces
having a dielectric medium disposed between said surfaces wherein a
hybrid wave inherently exists having both TEM and dual surface wave
components, said method comprising the step of
introducing a predetermined thickness of a further dielectric
medium along the length of one of said conducting surface, said
predetermined thickness and the relative permittivity of said
further dielectric material being chosen to enhance the dual
surface wave component relative to the TEM component and to make
said dual surface wave component asymmetric whereby the frequency
dispersion and net line attenuation of the overall hybrid mode are
decreased in spite of added losses introduced by the addition of
said further dielectric medium.
Description
Minimizing net electrical transmission line losses and reducing
frequency dispersion has long been recognized as an important and
worthwhile goal in the electrical art. These objectives are often
given special emphasis wherever long transmission distance and/or
large amounts of power are involved to make such minimization
economically imperative. However, before this invention, such
efforts at minimization were largely restricted to increasing the
conductivity of conductors, increasing the cross-sectional area of
conductors, increasing the effective skin depth of electrical
current in conductors, providing special line terminations and
adding distributed or lumped inductive loading to the line. All of
these previous efforts to minimize losses were made in the art
while it was generally believed that the only significant mode of
propagation in dual conducting surface line was a simple TEM
mode.
It has now been discovered that the normal transmission mode of
electromagnetic energy in a dual conducting surface transmission
line, for example, a strip line or a coaxial cable, is, contrary to
generally accepted belief, an overall hybrid mode and not a simple
TEM mode. This hybrid mode comprises a combination of at least a
dual surface wave field and a TEM field with the magnitude of the
former depending to a large extent on the surface reactance of the
two conducting surfaces. If, as is usually the case, the surface
reactances of the two conducting surfaces are equal, then with a
symmetrical disposition of conductors there will be a dual surface
wave mode with fields of equal magnitude associated with each of
the two conducting surfaces.
This invention is based upon the discovery that the net attenuation
of electrical energy propagated along a two conductor line and the
departure from the required linear relationship between
phase-change coefficient and frequency may be reduced by
purposefully increasing the surface reactance of one of the two
conducting surfaces by a controlled amount. This controlled
increase enhances the dual surface wave fields associated with the
one surface having increased surface reactance to the detriment of
other existing propagation modes thereby producing an asymmetrical
hybrid wave which has been found to cause appreciably less net
attenuation and less distortion than if no such asymmetry exists,
provided that the amount of increased surface reactance is
carefully controlled and kept within certain ranges or limits. In
the preferred embodiment of this invention, the degree of asymmetry
produced is such that the hybrid wave contour of minimum axial
electric field occurs as close as possible. to the conducting
surface opposite the one which is provided with increased surface
reactance.
In other words, it is now established that a hybrid wave
propagation of energy is not only unavoidable in any parallel
conductor electrical transmission system but that the deliberate
accentuation of the surface wave content thereof, to a limited and
controlled extent, can be very beneficial. This technique, is, of
course, applicable to the standard two-wire transmission line
normally used for the lower poser frequencies as well as other
lines such as coaxial and strip lines which are used for higher
electrical frequencies.
The essence of this invention is based on the application of just
sufficient reactive loading (achieved in the preferred embodiment
with a thin dielectric coating) to one of the conductors thus
enhancing and making asymmetrical the surface wave mode content up
to the point where the overall net line attenuation and distortion
is a minimum or thereabouts. In the preferred embodiment, this
requires only a very thin layer of dielectric coating. If an
excessive thickness of dielectric or other reactive loading is
utilized, the net line attenuation will be increased from a minimum
and, in fact, will eventually exceed the attenuation of the line
without any coating or loading at all.
It has also been discovered that the production of an asymmetrical
surface wave on a two conductor line by the previously described
principles tends, at the same time, to reduce the undesirable
frequency dispersion characteristics of the resulting line by
making the axial propagation phase-change coefficient almost
directly proportional to frequency.
The effect of adding a controlled amount of surface reactance to
one of the two conducting surfaces (obtained in the preferred
embodiment by a thin dielectric coating) causes very significant
and complex changes in field distributions of electromagnetic
fields within the space between the conducting surfaces. Over at
least a small range of added reactance values, the result of such
complex changes has been found to be a reduction in the product of
transverse attenuation and transverse phase-change coefficients for
the hybrid wave with enhanced asymmetrical surface wave content. At
the same time, many other parameters of the hybrid wave are also
changed. For example, the longitudinal or axial hybrid wave
impedance and the longitudinal or axial phase-change coefficient
are both increased and, as previously pointed out, the axial
phase-change coefficient is also made more nearly proportional to
frequency thereby producing a more desirable frequency dispersion
characteristic.
A particularly important result of these changes is a reduction in
the product of transverse attenuation and phase-change coefficients
since the overall attenuation in the axial propagation direction of
the hybrid wave with enhanced surface wave component is
proportional to and thus directly dependent upon this product
divided by the axial phase-change coefficient. Thus, over a
predetermined range of added surface reactance, a controlled
enhancement of the surface wave content increases the proportion of
total energy propagating in that mode and may result in a reduced
attenuation of the energy propagating in that mode. Thus, by
carefully controlling the amount of added surface reactance, not
only is the dispersion less but the reduction in overall net
attenuation can exceed any additional losses that may be caused by
the introduction of the added dielectric medium or other reactive
loading. Actually, the transverse attenuation coefficient increases
with added surface reactance while the transverse phase-change
coefficient falls rapidly and the product is reduced over a limited
range of surface reactance loading.
While in the prior art surface reactance has been added to a single
conducting surface for the purpose of trapping a surface wave mode
in the close proximity of the conducting surface and thus providing
a single conductor surface wave transmission line, the amount of
added surface reactance used for these single conductor surface
wave transmission lines is greatly in excess of the limited range
of surface reactance loading which may be profitably utilized with
this invention. In fact, the excessive surface reactance loading
required to achieve a single conductor surface wave transmission
line would, in most cases, actually increase the net line
attenuation in a dual surface transmission line supporting hybrid
modes of propagation.
Accordingly, it is an object of this invention to provide means for
producing an asymmetrical TEM dual surface wave on a two conductor
line by adding a controlled amount of surface reactance to one
conductor, the added reactance comprising a thin coating of a
low-loss dielectric medium on the one conducting surface with the
coating relative permittivity and thickness being carefully
controlled to insure a greater decrease in attenuation (due to the
resulting asymmetrical surface wave) than increase in attenutation
(due to added losses in the coating medium) thereby insuring a
reduced overall net line attenuation and at the same time reduced
frequency dispersion.
A further object of this invention is to provide means for
producing an asymmetrical hybrid TEM dual surface wave by adding a
controlled amount of surface reactance to one conductor in the form
of corrugations or grooves substantially at right angles to the
direction of the hybrid wave propagation. These grooves preferably
have a depth much less than a quarter wave length such that the
surface reactance is of the same order as that employed with the
dielectric coated conductor previously described.
It is also an object of this invention to apply the foregoing
principles to standard a.c. power (50-60 Hz.). dual conductor
transmission lines by using on one of the line conductors a
controlled coating of a dielectric medium having a very high
permittivity, as for example, a ferrite material.
Another object of this invention is application of the above
principles to resonators where such resonators comprise a length of
transmission line embodying the invention as previously discussed
together with electrical reflectors or short-circuits at opposite
ends thereof.
A more complete understanding of this invention may be obtained by
carefully studying the following detailed explanation and the
accompanying drawings of which:
FIG. 1 illustrates in cross-section a coaxial cable embodying this
invention,
FIG. 2 is an axial cross-section of the cable illustrated in FIG.
1,
FIG. 3 is a graph generally showing the relationship between net
line attenuation and thickness of the dielectric coating or other
equivalent surface reactance,
FIG. 4 shows a spiral wrapping of a sandwiched dielectric material
about a conductor according to this invention,
FIG. 5 is a detailed cross-sectional view of the sandwiched
material taken along line 5-5 in FIG. 4,
FIG. 6 illustrates an axial cross-section of the center conductor
of an alternate embodiment of this invention utilizing a corrugated
or grooved conductor surface to achieve increases surface
reactance,
FIG. 7 illustrates an end view of a low-frequency power cable
embodying this invention,
FIG. 8 illustrates a plan view of the power cable shown in FIG.
7,
FIG. 9 illustrates a resonator constructed according to the
principles of this invention, and pp FIG. 10 is a graph of
experimentally determined approximately optimum dielectric
thickness versus operating frequency.
The standard coaxial dual conductor line having an inner conductor
10 surrounded by an outer conductor 12 as shown in FIGS. 1 and 2
(for the moment disregarding dielectric coating 14) has long been
known to support propagation of energy in a TEM mode characterized
by radial electrical fields and circumferential magnetic fields.
With this invention it has been discovered that the propagation of
energy along such a dual conductor line as shown in FIGS. 1 and 2
actually includes significant surface wave modes as well as the
long-accepted TEM mode which together constitute a resulting hybrid
wave. It has been further discovered that, by a controlled
enhancement of the magnitude of the surface wave fields associated
with one of the two conducting surfaces, the overall net
attenuation of hybrid mode energy propagated along the line may be
reduced, while the phase velocity of propagation becomes
substantially constant at all operating frequencies.
Referring now to FIG. 1, there is shown, in cross-section, a
coaxial cable embodying this invention. Inner conductor 10 has a
coating 14 with a thickness t of a dielectric material. If desired,
the cable illustrated in FIG. 1 may be air-spaced in which case the
space volume existing between dielectric coating 14 and outer
conductor 12 would be filled with air or some inert gas and the
conductor 10 would be held in proper spaced-apart relationship from
outer conductor 12 by insulating spacers 16 as shown by dotted
lines in FIG. 2.
It has been discovered that when a high frequency wave is launched
into a cable as illustrated by FIGS. 1 and 2, the total energy
propagation is in fact in the form of a hybrid mode comprising both
a TEM mode and a dual surface wave mode having surface wave fields
associated with each of the two conducting surfaces. The effect of
dielectric coating 14, which increases the surface reactance of
conductor 10, is to cause the surface wave field associated with
conducting surface 10 to be enhanced, thus causing the total dual
surface wave mode to become increasingly asymmetric. That is, more
of the total propagated energy is caused to travel in the surface
wave field associated with conductor 10 than before. As illustrated
by the electric field pattern shown in FIG. 2, electric field 18
associated with conducting surface 10 is of a much greater
magnitude than electric field 20 which is associated with conductor
12. At some point between these two electric fields there is a
contour of minimum axial electric field which is preferably caused
to be as close to conductor 12 as possible.
It has been also discovered that, as the thickness t of coating 14
is increased from zero value upwards, the net attenuation of
axially propagating energy within the cable falls to a minimum and
thereafter increases. A general indication of this relationship
between an axial attenuation coefficient .alpha. and thickness t of
coating 14 is shown in FIG. 3.
The thickness t of the coating 14 required to minimize net line
attenuation of axial propagating energy is dependent upon many
parameters including the relative permittivity of the dielectric
coating and its value with respect to the permittivity of the main
dielectric medium existing between dielectric coating 14 and outer
conductor 12 and the frequency range of propagating waves.
Although, as yet, no rigorously derived mathematical formulas have
been shown to predict the optimum value of thickness t or other
reactive loading, the following table of operating frequency versus
approximate optimum thickness of dielectric coating has been
discovered by an experiment in which the relative permittivity of
the dielectric coating 14 is approximately two or three times
greater than the relative permittivity of the surrounding
dielectric medium of the transmission line.
Approximate Optimum Operating Frequency Thickness of Dielec- tric
Coating
__________________________________________________________________________
10 Ghz. 0.0003-0.0015 inches 3 Ghz. 0.0005-0.0030 inches 100-300
Mhz. 0.0050-0.0080 inches 1-30 Mhz. 0.0100-0.0300 inches
__________________________________________________________________________
The information given in the above table is presented in graphical
form in FIG. 10 with operating frequency shown on a horizontal
logarithmic scale and thickness shown by a linear vertical scale.
Operation within the cross-hatched region will result in reduced
net line attenuation as taught by this invention.
If the main dielectric is solid polythene, the inner conductor must
be coated with a low-loss dielectric having a relative permittivity
between 7 and 8, or thereabouts while if the main dielectric medium
of the line is air, the coating may comprise polythene or
polystrene. Instead of coating the inner conductor 10 with
dielectric medium, the inner surface of outer conductor 12 may be
coated, but it is preferable from the point of view of simplicity
in manufacture to coat the inner conductor as shown in FIG. 2.
In the case of a cable filled with a solid dielectric medium where,
as previously noted, it is necessary for the coating 14 to have a
higher permittivity than the main dielectric medium, suitable
materials for such a coating 14 are polystyrene loaded with
titanium dioxide, calcium titanate, or strontium titanate. These
materials may be applied as a coating to the inner conductor
preferably by extrusion or as shown in FIGS. 4 and 5 by crushing
the loading material into a powdered form and sandwiching the
powder 22 between two layers of insulating flexible tape 24, for
example, cellulose tape such as "Sellotape." The resulting sandwich
26 of flexible tape and powdered dielectric material is then wound
spirally about inner conductor 10 to provide the necessary coating
14 as shown in FIG. 4.
In accordance with another embodiment of this invention shown in
FIG. 6, corrugations or grooves 28 may be provided in the surface
of one of the conducting surfaces (inner conductor 10 as shown in
FIG. 6) instead of providing a coating such as coating 14 to
increase the surface reactance. These corrugations or grooves 28
are preferably about the inner conductor if the transmission line
is coaxial as shown in FIGS. 1 and 2. The circumferential grooves
or channels 28 shown in FIG. 6 have effective depths much less than
a quarter wave-length thereby producing a surface reactance
comparable to that produced by the dielectric coating previously
considered. The ratio of slot width b to slot pitch B is such that
b /B is equal very nearly to the ratio of slot reactance to surface
reactance. A cable constructed as described and illustrated in FIG.
6 behaves similarly to the cable illustrated in FIGS. 1 and 2 which
utilizes the dielectric coating 14 in lieu of such corrugations or
grooves to increase the surface reactance of conductor 10.
Obviously an advantage of transmission lines embodying this
invention as described above is that since the overall net axial
propagation attenuation of the line may be less than that of the
usual type of line carrying a quasi-TEM wave, (i.e., one with most
of the power in a TEM mode as would be the case without any surface
wave accentuating means), the number of repeaters that are required
when this form of line is used for a long distance signal
transmission, as in a submarine cable, is reduced. Furthermore,
these new lines result in noticeably less frequency dispersion than
in a conventional cable so that the requirements for equalizing
networks are reduced and the cables may be operated over wider
frequency bands.
The previously discussed transmission lines are, of course, only
representative of any dual surface electric transmission line
having two conducting surfaces, such as, for example, coaxial
lines, strip lines, twin lines, etc. While these transmission lines
have their main application in the transmission of signals at hf
and higher frequencies, the invention is also applicable to the
transmission of power usually at frequencies of only 50 or 60 Hz.
However, in order to increase sufficiently the surface reactance of
a conductor at these low frequencies without utilizing excessively
thick dielectric coatings, materials having very high
permittivities are required. One suitable material is manganese
zinc ferrite which has a relative permittivity of about 10.sup. 5,
a relative permeability of 10.sup. 3 and a conductivity in the
range of 3 .times. 10.sup.-.sup. 6 mho/m giving a loss tangent of
10.sup.-.sup. 2.
Because these ferrites are hard, brittle materials, the coating of
a conductor with such materials may be in the form of a series of
individual axially spaced apart rings of the material thus enabling
the resulting reactively loaded cable to maintain the required
degree of mechanical flexibility without damage to the dielectric
material. Alternatively, the ferrite material may be sandwiched in
powdered form between supporting flexible tapes, as previously
discussed for higher frequency lines and depicted in FIGS. 4 and 5.
The use of such sandwiched tapes wound spirally about the conductor
will also result in less longitudinal or axial induced current
within the ferrite material than with the ring configuration.
It is desirable to insure that as high a proportion of the total
energy as possible is contained in the surface wave content of the
field rather than in the TEM part and at 50 Hz. this feature is
best achieved either by a pair of spaced apart conductors of
circular cross-section or by a coaxial configuration of conductors.
An example illustrating the first-mentioned arrangement for power
frequency transmission lines is shown in FIGS. 7 and 8 in which two
parallel spaced-apart conductors 30 and 32 of circular
cross-section constitute a high power transmission line. Conductor
30 is coated with a series of axially aligned, individually
spaced-apart rings 34 of manganese zinc ferrite.
Of course, in any of the previously described embodiments, it is
permissible to apply surface reactance loading to both of the two
conducting surfaces but in unequal amounts such that the requisite
asymmetric TEM surface wave field is still produced by the
supporting surfaces; however, it is preferable that only one of the
conductors is coated or otherwise loaded with additional surface
reactance.
One application for the low-loss transmission line of this
invention is in a resonator as shown in FIG. 9. Here a fixed length
l of electric transmission line constructed according to this
invention is terminated at both ends by electrical reflectors or
short-circuits 36 and 38. Electrical energy may be transferred to
and from the resonator 40 by way of line 42 through reflector 38.
As is usual with resonators of this type, resonance will be
observed at a plurality of frequencies having wavelengths in the
medium of resonator 40 corresponding to 2(1/n ) where n is an
integer.
Although only a few embodiments of this invention have been
specifically described above, it should be appreciated that this
invention encompasses the whole of a dramatic new discovery of
means for reducing the net line attenuation and dispersion of dual
conductor electric transmission lines by providing surface-wave
accentuating means for causing a significant portion of the total
propagated energy to be in the form of an asymmetrical surface wave
rather than in the usual TEM mode and for controlling this means
both to cause a greater reduction in net line attenuation than any
increase, thereof caused by the presence of said means and to cause
a wider range of frequencies to travel along the line with the same
phase velocity. Accordingly, many possible modifications of the
disclosed embodiments are within the scope of this invention.
* * * * *