U.S. patent number 3,843,860 [Application Number 05/399,676] was granted by the patent office on 1974-10-22 for twisted microwave applicator.
This patent grant is currently assigned to Varian Associates. Invention is credited to Howard R. Jory, Charles H. Will, Jr..
United States Patent |
3,843,860 |
Jory , et al. |
October 22, 1974 |
TWISTED MICROWAVE APPLICATOR
Abstract
A twisted microwave applicator is provided to avoid the heating
non-uniformities inherently resulting from non-twisted microwave
applicators. The invention comprises a section of waveguide twisted
about its axis, preferably twisted 90.degree. or more. The
applicator is coupled to a microwave generator by conventional
techniques. The objects to be treated are introduced into one end
of the applicator, transported through the applicator and removed
at the other end. The twisted waveguide provides for rotation of
the field pattern, which tends to subject all portions of the
objects to the same overall heating effect.
Inventors: |
Jory; Howard R. (Menlo Park,
CA), Will, Jr.; Charles H. (San Jose, CA) |
Assignee: |
Varian Associates (Palo Alto,
CA)
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Family
ID: |
26903481 |
Appl.
No.: |
05/399,676 |
Filed: |
September 21, 1973 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
Issue Date |
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208768 |
Dec 16, 1971 |
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Current U.S.
Class: |
219/693; 219/746;
333/248; 333/252 |
Current CPC
Class: |
H05B
6/80 (20130101); H01P 1/022 (20130101); H05B
6/70 (20130101); H05B 6/6402 (20130101) |
Current International
Class: |
H05B
6/78 (20060101); H01P 1/02 (20060101); H05b
009/06 () |
Field of
Search: |
;219/10.55 ;333/98R |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Truhe; J. V.
Assistant Examiner: Jaeger; Hugh D.
Attorney, Agent or Firm: Cole; Stanley Z. Herbert; Leon F.
Morrissey; John J.
Parent Case Text
This is a continuation of application Ser. No. 208,768 filed Dec.
16, l971 now abandoned.
Claims
What is claimed is:
1. An electromagnetic energy applicator comprising a waveguide
section elongate about an axis and having electromagnetic energy
input means connected thereto, said waveguide section having two
rectangular end walls with openings therein for passage of an
object along a path through said waveguide section, said end walls
being substantially opague to said electromagnetic energy, said
waveguide section being configured so that the longer rectangular
dimension of one of said end walls is nonparallel to the longer
rectangular dimension of the other of said end walls, said
waveguide section being further configured so that as said object
passes along said path from said one end wall to said other end
wall said object is exposed for the greater portion of said path to
a continuously varying orientation of the electric field of said
electromagnetic energy.
2. The applicator of claim 1 wherein said waveguide section forms a
resonant cavity; and wherein said waveguide section comprises a
twisted portion interposed between two nontwisted portions; said
end walls being disposed to permit passage of said object
sequentially through one of said non-twisted portions, then through
said twisted portion, and then through the other of said
non-twisted portions along said path; each of said non-twisted
portions having a length along said path sufficient to provide a
non-zero electric field intensity at the boundary between said
non-twisted portion and said twisted portion; said twisted portion
having a length along said path sufficient to provide that said
object is exposed to more of said energy in said twisted portion
than in said non-twisted portions.
3. The applicator of claim 2 wherein said twisted portion of said
waveguide section is twisted by at least 90.degree..
4. The applicator of claim 2 wherein the length of each of said
non-twisted portions of said waveguide section is on the order of
one-quarter of the waveguide wavelength of said electromagnetic
energy.
5. The applicator of claim 1 wherein said waveguide section
comprises a twisted portion interposed between two non-twisted
portions; said end walls being disposed to permit passage of said
object sequentially through one of said non-twisted portions, then
through said twisted portion, and then through the other of said
non-twisted portions along said path; the length of each of said
non-twisted portions along said path being sufficient to provide
maximum electric field intensity of said energy at the boundary
between said non-twisted portion and said twisted portion.
6. The applicator of claim 5 wherein the length of each of said
non-twisted portion along said path is substantially no longer than
one-quarter of the waveguide wavelength of said energy.
7. The applicator of claim 1 wherein said applicator further
comprises electromagnetic energy output means connected to said
waveguide section; said waveguide section comprising a twisted
portion interposed between two non-twisted portions; said end walls
being disposed to permit passage of said object sequentially
through one of said nontwisted portions, then through said twisted
portion, and then through the other of said non-twisted portions
along said path; one of said non-twisted portions having a length
sufficient to accommodate thereon the connection of said
electromagnetic energy input means to said waveguide section and
the other of said non-twisted portions having a length sufficient
to accommodate thereon the connection of said electromagnetic
energy output means to said waveguide section; said twisted portion
having a length along said path sufficient to provide that said
object is exposed to more of said energy in said twisted portion
than in said nontwisted portions.
8. The applicator of claim 7 wherein said twisted portion of said
waveguide section is twisted by at least 90.degree..
9. The applicator of claim 1 wherein said waveguide section
comprises a twisted portion interposed between two non-twisted
portions; said end walls being disposed to permit passage of said
object sequentially through one of said non-twisted portions, then
through said twisted portion, and then through the other of said
non-twisted portions along said path; the length of each of said
non-twisted portions along said path being sufficiently small to
provide that said object is exposed to more of said energy in said
twisted portion than in said non-twisted portions.
10. The applicator of claim 1 wherein said waveguide section forms
a resonant cavity.
11. The applicator of claim 1 wherein said rectangular end walls
are perpendicular to said axis of said waveguide section.
12. The applicator of claim 1 wherein said electromagnetic energy
input means comprises an energy input waveguide which is
electromagnetically coupled to said object-treating waveguide
section through an iris opening.
13. The applicator of claim 1 wherein said electromagnetic energy
input means comprises an energy input waveguide which is elongate
about an axis, said energy input waveguide axis being perpendicular
to the axis of said object-treating waveguide section.
14. The applicator of claim 13 wherein the interface between said
energy input waveguide and said object-treating waveguide section
lies in a plane which is perpendicular to said axis of said energy
input waveguide.
Description
BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention is a further deveopment in the field of microwave
treatment applicators, particularly in the technique of providing a
uniform heating effect on all parts of an object passing through
the applicator.
2. Description of the Prior Art
In conventional microwave applicators, the electric field varies in
intensity over any given cross section of the applicator at any
given instant of time depending upon the distance from the
conductive walls of the applicator to the point at which the
electric intensity is measured. In addition, further variations in
field intensity will be introduced over the given cross-section
because of field distortions caused by the dielectric properties of
the objects to be treated. An object passing through a conventional
microwave applicator will experience different heating effects on
its various surfaces and internal portions because of these
non-uniformities in the electric field intensity which are inherent
in conventional applicators.
SUMMARY OF THE INVENTION
It is an object of this invention to provide for the exposure of
all surfaces and internal portions of material treated in a
microwave applicator to a heating effect of increased uniformity
within the applicator.
It is a further object of this invention to achieve a heating
effect of increased uniformity within a microwave applicator by
providing for relative rotation between the field pattern in the
applicator and the material to be treated.
It is a further object of this invention to provide for rotation of
the field pattern within a microwave applicator by means of a
twisted waveguide section.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a perspective view of a twisted microwave applicator
illustrating the invention embodied in a resonant cavity
applicator;
FIG. 2 is a cross-section of the applicator taken on line 2--2 of
FIG. 1;
FIG. 3 illustrates the non-uniformity of the electric field
intensity over a cross-section of a microwave applicator;
FIG. 4 illustrates the distortion of the electric field intensity
in a microwave cavity caused by the dielectric properties of an
object being treated; and
FIG. 5 is a view similar to FIG. 1 illustrating the invention
embodied in a traveling wave applicator.
DESCRIPTION OF THE INVENTION
FIG. 1 shows a perspective view of a twisted microwave applicator 1
which effectively embodies the concept of this invention. The
applicator comprises a waveguide section 2 twisted about its
longitudinal axis. In the drawing a 90.degree. twist is shown.
Waveguide section 2 is fitted with conductive end walls 3 and 4 to
form a resonant cavity. Except for the twist, waveguide section 2
is made like conventional straight waveguide sections; namely
section 2 is made of metal walls to form a container for microwave
energy. Waveguide section 2 is rectangular in cross section at
every point along its length as shown for example in FIG. 2.
Although a rectangular cross-section is preferred, the principle of
the invention applies to any cross-section shape which tends to
increase uniformity of heating when it is twisted. The objects to
be treated within the cavity are introduced and removed through
openings in the end walls. In one approach the objects are
introduced through a tube 5 and removed through a tube 6. Tubes 5
and 6 are made of conductive material and are designed in
conventional manner to be non-propagating at the frequency of
operation of the applicator so that microwave energy will not
escape from the cavity. Tubes 5 and 6 are secured to the end walls
but do not extend inside the waveguide 2. The objects to be treated
are preferably enclosed inside the cavity by a dielectric tube 7
extending between the end walls and coaxial with tubes 5 and 6. In
this way the objects to be treated can be inserted into tube 5 and
push one another through the tube 7 and out tube 6. Also, the
waveguide section 2 can be oriented to slope downward from the
input to the output end to provide a gravity transport. Another
alternative is to run a conventional conveyer belt (not shown)
through the waveguide section 2 to carry the objects. If tube 7 is
employed, the belt would go through the tube. If the action of the
belt transport and the shape of the objects would tend to cause
random rotation of the objects on top of the belt, the objects
should be clipped or otherwise fastened to the belt to avoid the
possibility that some objects might rotate in a way which would
tend to offset the twisting effect of the twisted waveguide.
Waveguide section 2 is coupled to a microwave generator (not shown)
by a conventional inlet waveguide section 10 coupled to waveguide 2
through an iris opening 11. Alternatively, coaxial line and
coupling loop type of coupling can be employed although such a
coupling would be made in a wide wall of waveguide section 2,
rather than in a narrow wall.
Waveguide section 2 is twisted to achieve rotation of the
electromagnetic field pattern from one end of the microwave
treatment cavity to the other. This rotation of the field pattern
will cause the surfaces and internal portions of objects passing
through the treatment cavity to experience a uniform heating
effect. The heating effect at any point within the cavity is
proportional to the square of the electric field strength at that
point. If there are local variations in the field strength within
the cavity, then objects having different shapes, objects having
different paths through the waveguide, and different portions of a
specific object will experience non-uniform heating effects unless
all portions of each object are exposed to the same net field
integrated over the path of the object through the cavity. In a
conventional straight waveguide section the non-uniformity remains
constant along the section, so for example, a portion of an object
which is exposed to a low energy field, is exposed to the same low
field throughout its travel through the waveguide. By rotating the
field pattern about an object as it passes through the cavity, this
invention provides the desired integration so that all objects and
all parts of the same object tend to experience the same net
exposure to the microwave energy within the cavity as they pass
through the cavity.
FIG. 3 illustrates the variation in electric field intensity over
the cross-section of a rectangular microwave applicator (such as
any cross-section of waveguide section 2) at any given instant of
time. The field variation is shown by individual field vector lines
E and the line 12 which depicts the envelope of the changing field
strength across the waveguide section. This variation results from
the fact that the components of the electric field parallel to the
narrow conducting walls decrease in magnitude as the distance from
the narrow walls decrease, until E = 0 at the narrow walls. FIG. 4
illustrates the distortion of the electric field intensity over a
given cross-section caused by the non-uniform cross section or
non-uniform dielectric properties of an object 14 to be treated.
The non-uniformities in the electric field intensity such as
illustrated in FIG. 3 and FIG. 4 cause non-uniform heating effects
upon objects passing through a microwave applicator in which the
field pattern remains constant. However, in accordance with this
invention, rotating the field pattern about the objects as they
pass through the applicator, causes the objects to experience
changing fields which tend to provide a uniform heating effect on
the objects in the course of their travel through the applicator.
As indicated by the E arrows in FIG. 1 the applicator formed by the
90.degree. twisted waveguide section 2 provides an E field which
changes from vertical at the inlet end of section 2 to horizontal
at the outlet end.
Use of a straight waveguide section in which the material to be
treated is rotated in controlled manner as it passes through the
waveguide section can be used to simulate the result achieved with
a twisted waveguide. However, this requires a complex mechanical
system for rotating the material. The complexity of such a system
involves inherently poorer reliability and greater maintenance
problems than the twisted waveguide.
Although the 90.degree. twist of waveguide section 2 is shown in
FIG. 1, it will be understood that twisting of more or less than
90.degree. can be employed to achieve heating uniformity which is
better than with a straight waveguide. However, at least 90.degree.
twist is required to cause the electric field lines to pass through
the objects parallel to the vertical axis of the objects and also
parallel to the horizontal axis of the objects. Where more than
90.degree. is used, the twist is preferably in multiples of
90.degree., and preferably the number of multiples is selected so
that the object to be treated is not exposed to electrical field
more in one direction than in another direction. As is known by
those skilled in the art, the electrical field axially along the
resonant cavity applicator 1 is in form of a sine wave with zero
intensity at the end walls. Thus if the twist starts immediately at
the end walls 3 and 4, the full effect of the twist is not
realized. Accordingly it is preferred to have straight waveguide
lengths L at the inlet and outlet ends, particularly where a twist
of only 90.degree. is used. Although any length L is beneficial,
the straight end portions preferably have a length L on the order
of 1/4 of the wavelength of the waveguide wavelength, as
distinguished from free space wavelength.
It is also possible to use a twisted waveguide section in a
traveling wave applicator as shown at 1' in FIG. 5. The differences
between the resonant cavity applicator 1 of FIG. 1 and the
traveling wave applicator 1' in FIG. 2 are that the traveling wave
applicator has a waveguide output 16 which goes to a dummy load
(not shown), and the coupling from the inlet waveguide 10 opens
completely into the waveguide section 2 so that microwave energy
passes into section 2 through the fully open end of section 10
rather than through the small iris hole 11. In the traveling wave
embodiment, the field strengths lengthwise along section 2 are not
held to zero at the end walls 3 and 4 so the straight end sections
L are not required for the reason discussed in connection with FIG.
1. However, as a practical matter straight sections L are preferred
in the traveling wave case to simplify connection of the input and
output sections 10.
* * * * *