U.S. patent number 3,560,694 [Application Number 04/792,557] was granted by the patent office on 1971-02-02 for microwave applicator employing flat multimode cavity for treating webs.
This patent grant is currently assigned to Varian Associates. Invention is credited to Jerome R. White.
United States Patent |
3,560,694 |
White |
February 2, 1971 |
MICROWAVE APPLICATOR EMPLOYING FLAT MULTIMODE CAVITY FOR TREATING
WEBS
Abstract
A microwave applicator is disclosed. The applicator includes a
flat multimode cavity having openings on opposite sides thereof for
passing therethrough a web of material to be treated with microwave
energy. The cavity is both designed and fed so as to be excited at
its operating frequency only in those TE.sub.l, m,n and TM.sub.l,
m,n classes of modes such that the value of l is limited to 1 and m
or n or both have a value greater than zero (preferably both m and
n have a range of values which includes 10) and such that the
E-vector of the microwave energy lies generally in the plane of the
treatment zone and has maximum intensity in the treatment zone. The
flat multimode cavity resonator is fabricated in two half sections
an upper half and a lower half which are joined together at their
edges. A mode-damping means is provided for attenuating a certain
undesired class of modes that could otherwise be supported within
the cavity. Air ducts are provided at opposite ends of the
resonator for directing air either parallel or antiparallel to the
direction of movement of the web to be treated.
Inventors: |
White; Jerome R. (San Carlos,
CA) |
Assignee: |
Varian Associates (Palo Alto,
CA)
|
Family
ID: |
25157318 |
Appl.
No.: |
04/792,557 |
Filed: |
January 21, 1969 |
Current U.S.
Class: |
219/693; 219/750;
219/757 |
Current CPC
Class: |
H01P
3/00 (20130101) |
Current International
Class: |
H01P
3/00 (20060101); H05b 009/06 (); H05b 005/00 () |
Field of
Search: |
;219/10.55,10.61 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
Other References
Foundations For Microwave Engineering, Collins 1966 pages 95-100
McGraw Hill.
|
Primary Examiner: Truhe; J. V.
Assistant Examiner: Bender; L. H.
Claims
I claim:
1. In an electromagnetic applicator, a multimode cavity resonator
having openings on opposite sides thereof for passing material to
be treated with electromagnetic energy through a thin wide
treatment zone contained within said cavity, said cavity having a
pair of parallel broad walls closed at their side edges by narrow
walls with said openings disposed in a pair of said narrow walls
and aligned in the plane of the thin wide treatment zone, means for
exciting said cavity with standing waves of electromagnetic of such
a class of resonant modes that the electric field vector in the
treatment zone is generally parallel to said broad walls of said
cavity and lies generally within the plane of the thin wide
treatment zone, the spacing between the pair of broad walls of said
cavity being at least equal to one-half wavelength and less than
one wavelength at the operating frequency of said cavity whereby
certain undesired classes of modes are not supported, and being
dimensioned to have sufficient length and width to support both the
TE.sub.l,m,n and TM.sub.l,m,n classes of modes of oscillation in
said cavity at the frequency of operation where l is 1 and the
range of both m and n is greater than 10, said means for exciting
said cavity resonator with microwave energy including a hollow
rectangular waveguide opening into said cavity at a narrow wall of
said cavity, said rectangular waveguide having a pair of broad
walls and a pair of narrow sidewalls with the planes of the broad
walls of said waveguide being generally perpendicular to the planes
of the broad walls of said cavity resonator to preferentially
excite in said cavity modes of oscillation having their electric
field vectors parallel to the cavity broad walls at the treatment
zone.
2. The apparatus of claim 1 including duct means for directing gas
into and out of said cavity, said duct means being disposed at said
pair of narrow sidewalls which have the openings therein for
passage of the material to be treated through the resonator.
3. The apparatus of claim 2 wherein said duct means includes a
plurality of adjacent conductive passageways having transverse
inside dimensions below cutoff at the operating frequency of said
cavity resonator.
4. The apparatus of claim 3 wherein the ducts are arranged to
direct a pair of gas streams through said cavity resonator on
opposite sides of said treatment zone, with the direction of the
gas streams being generally parallel or antiparallel to the
direction of movement of the material being treated through said
resonator.
5. The apparatus of claim 1 wherein said waveguide opens into said
cavity substantially at one of the corners of said cavity.
6. The apparatus of claim 1 wherein said cavity resonator comprises
two similar half portions joined together along a joint formed in
and disposed intermediate the height of two narrow sidewalls which
extend generally in the direction of movement of the material to be
treated through said resonator, and means forming a microwave
attenuator structure disposed in said joint to suppress undesired
classes of modes of oscillation in said cavity.
7. The apparatus of claim 1 wherein means forming an attenuator
structure are disposed in said openings in said narrow cavity walls
for passing material to be treated to suppress undesired classes of
modes of oscillation in said cavity.
8. An electromagnetic applicator comprising an electromagnetic
treatment chamber capable of supporting within its interior
electromagnetic wave energy and defined by a pair of generally
parallel conductive broad walls closed along opposite side edges by
narrow conductive sidewalls, the spacing between said pair of broad
walls of said cavity being at least equal to one-half wavelength
and less than one wavelength at the operating frequency of said
electromagnetic wave energy, means for exciting said chamber with
electromagnetic energy of a class of modes of oscillation producing
electric field vectors in the midplane between and generally
parallel to said broad walls, means for supporting at said midplane
within said chamber material to be treated with said energy, and
lossy mode-damping means extending along each of said sidewalls at
said midplane and generally parallel to said broad walls to
attenuate any modes within said chamber having at said midplane an
electric field vector not parallel to said broad walls.
Description
DESCRIPTION OF THE PRIOR ART
Heretofore, multimode cavity resonators, excited such that the
E-vector is parallel to the plane of a web of material to be
treated, have been employed for treating webs of dielectric
material. One such prior art applicator is disclosed in U.S. Pat.
No. 2,650,291 issued Aug. 25, 1953. One of the problems with this
prior art applicator is that the cavity is relatively deep in the
direction perpendicular to the plane of the web such that the
cavity can support certain undersired modes of oscillation with the
electric vector perpendicular to the plane of the web at the plane
of the web. These modes, with the E-vector perpendicular to the
web, are generally undesired since they contribute very little to
heating of the material being treated and being therefore lightly
loaded can cause arcing and breakdown of the air dielectric in the
cavity. Such modes also cause excessive leakage of microwave energy
through the openings provided for the web material.
Others have built waveguide-type applicators wherein the waveguide
was formed in a serpentine manner, thereby producing a relatively
flat applicator. The waveguide was sometimes formed in two half
sections and hinged at one side of the web of material to be
treated to facilitate threading of the web into the applicator
structure and to facilitate cleaning and maintenance of the
structure. However, one problem with the prior waveguide applicator
is that the serpentine arrangement of the waveguide makes it
difficult to duct air through the applicator and the applicator is
generally a relatively complex structure. Due to their structural
complexity waveguide applicators are more costly to fabricate, tend
to be physically larger and heavier and are inherently more lossy
and thus less efficient than cavity-type applicators. They are also
more difficult to ventilate and clean and have a tendency to
collect undesired matter in their physically intricate interior.
Finally, the space which is allowed for the passing of material to
be treated is quite critical for efficient transfer of microwave
energy to the material, thus requiring careful control over the
dimensions and motion of such material. Such a waveguide applicator
is disclosed in U.S. Pat. No. 2,560,903 issued Jul. 17, 1951.
SUMMARY OF THE PRESENT INVENTION
The principle object of the present invention is the provision of
an improved microwave applicator.
One feature of the present invention is the provision of a
relatively flat applicator cavity resonator which supports classes
of resonant modes such that the electric vector of the field midway
between the broad walls of the cavity is parallel to the plane of
the broad walls of the cavity, such cavity having a height in a
direction perpendicular to the broad walls, which is less than a
wavelength at the operating frequency, whereby certain undesired
classes of modes (specifically l>2) modes having electric field
vectors perpendicular to the broad walls midway between the broad
walls of the cavity are not supported. Another feature of the
present invention is the same as the preceding feature wherein the
broad walls are dimensioned to have sufficient length and width to
support the TE.sub.l m, n and TM.sub.l,m,n modes at the frequency
of operation, where l is 1 and at least m or n is greater than 10,
whereby mode stirring is readily achieved by frequency modulating
the exciting microwave energy applied to the cavity.
Another feature of the present invention is the same as any one or
more of the preceding features wherein a rectangular waveguide is
coupled to the cavity for exciting the cavity with microwave
energy, the waveguide being oriented relative to the cavity such
that the broad walls of the rectangular waveguide are perpendicular
to the planes of the broad walls of the cavity, whereby the desired
classes of modes of oscillation are excited to the exclusion of
other possible modes.
Another feature of the present invention is the same as any one or
more of the preceding features wherein the cavity resonator
comprises two similar half resonator portions joined together along
a joint formed in the narrow sidewalls and including a lossy,
mode-damping material disposed in the joint for suppressing certain
undesired modes of oscillation having their electric field vectors
perpendicular to the broad walls of the cavity (specifically, the
TE.sub.o,m,n class of modes).
Another feature of the present invention is the same as any one or
more of the preceding features including the provision of air ducts
disposed at the narrow end walls of the cavity for directing air or
other gasses through the cavity in a direction parallel or
antiparallel to the direction of movement of the material being
treated within the cavity.
Other features and advantages of the present invention will become
apparent upon a perusal of the following specification taken in
connection with the accompanying drawings wherein:
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a schematic, perspective, line diagram, partly in block
diagram form, depicting a microwave applicator incorporating
features of the present invention;
FIG. 2 is a simplified schematic line diagram of a flat multimode
cavity incorporating features of the present invention;
FIGS. 3A and 3B depict the desired mode patterns to be excited in
the cavity of FIG. 2 the mode patterns being shown for a portion of
the structure of FIG. 2 delineated by line 3-3;
FIG. 4 is a schematic line diagram of a portion of the structure of
FIG. 1 delineated by line 4-4;
FIG. 5 is a fragmentary perspective view of a portion of the
structure of FIG. 1 delineated by line 5-5; and
FIG. 6 is a fragmentary perspective view, partly in section, of a
portion of the structure of FIG. 1 delineated by line 6-6.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
Referring now to FIG. 1 there is shown the microwave applicator of
the present invention. The applicator includes a flat multimode
rectangular cavity resonator 2 defining a relatively thin
rectangular treatment zone centrally disposed within the cavity 2
in a plane midway between the broad walls 3 of the resonator. The
resonator 2 includes opposite pairs of narrow sidewalls 4 and 5.
Narrow sidewalls 5, at the ends of the resonator 2, include
elongated apertures 6 for the passage of a web 7 of dielectric
material to be treated with microwave energy within the cavity 2.
The applicator is particularly useful for heating and drying flat
webs, sheets, or films of material, such as drying a polyvinylidene
coating of a thickness of between 0.1 to 1.0 mils on a 1 to 5 mil
thick 3 to 4 foot wide continuously moving paper web, such web
moving at speeds between 200 and 600 feet per minute.
Systems of air ducts 8, more fully described below with regard to
FIG. 6, are provided in the end walls 5 of the resonator 2 for
directing streams of air adjacent the moving web 7. The direction
of flow is antiparallel (i.e., parallel and counter) to the
direction of movement of the web and the stream is on both sides of
the web 7 through the treatment zone.
A source of microwave energy 9, such as a magnetron oscillator, is
coupled to the cavity 2 via a rectangular waveguide 11. The
waveguide 11 is arranged such that the broad walls of the waveguide
11 are perpendicular to the broad walls 3 of the cavity, such that
classes of modes of oscillation are excited within the cavity
having their electric vectors parallel to the broad walls 3 of the
cavity 2 at the plane of the web 7. In this manner, the strong
electric field vector is disposed in the plane of the web 7 within
the centrally disposed treatment zone of the resonator 2. When the
electric vector is in the plane of the web 7, the most effective
heating effect is obtained. The cavity modes, methods of
excitation, and the dimensions of the cavity are more fully
described below with regard to FIGS. 2--4.
The cavity 2 is formed in two similar half sections which are
fitted together along joint 12 in the narrow sidewalls 4 on
opposite sides of the web 7. The nature of the joint 12 is more
fully described below with regard to FIG. 5. The two halves of the
cavity resonator 2 are held together by suitable fasteners such as
screws, clamps or the like, not shown.
Referring now to FIGS. 2--4, the desired classes of modes of
oscillation within the cavity are described together with
dimensional considerations to obtain the desired classes of modes.
The desired classes of modes of oscillation within the cavity 2 are
those in which the electric field vectors E lie in a plane parallel
to the broad walls 3 of the cavity 2 at the plane of the web 7. In
addition, the electric vectors should have their maximum intensity
at a point midway in the thickness T of the cavity, where the
thickness T is the spacing between the broad walls 3. The desired
TE.sub.l,m,n and TM.sub.l,m,n modes are generally depicted in FIGS.
3A and 3B, respectively.
The cavity 2 preferably has a length L and a width W sufficiently
great such that the cavity will support the aforedescribed modes of
oscillation where either m or n or both are greater than 10, and
the cavity should have a thickness T such that l is no greater than
1. This means that the thickness T of the cavity 2 must be between
one half and one wavelength.
If the thickness T is less than a half wavelength the desired
classes of modes cannot be supported within the cavity and if the
thickness T is greater than one wavelength the cavity can support
certain undesired classes of modes of oscillation, wherein the
electric vector E is perpendicular to the broad walls. Such modes
are particularly troublesome since they lead to voltage breakdown
at high power levels resulting in undesired arcing and excessive
leakage of microwave energy from the apertures 6. Furthermore, such
modes contribute very little to heating since their electric
vectors are perpendicular to the plane of the thin web 7 being
treated.
By making the length L and width W dimensions of the cavity 2
sufficiently large such that the range of the m or n designators of
the excited modes is in excess of 10 it is assured that the various
resonant frequencies of the excited modes within the cavity are
closely spaced in frequency. This has the advantage of enabling
mode starring to be more readily accomplished.
Referring now to FIG. 4, there is shown the waveguide coupling
arrangement for exciting the desired TE.sub.l,m,n or TM.sub.l,m,n
modes within the resonator 2. The desired modes have strong
electric field vectors E in the plane midway between the broad
walls 3 with the E vectors being parallel to the broad walls. These
desired classes of modes are excited by the dominant modes in the
input waveguide 11 when the waveguide is coupled near a corner of
the cavity 2 and when the waveguide 11 is arranged with the broad
walls of the guide perpendicular to the broad walls 3 of the cavity
2.
The waveguide 11 is split to form a joint 23, such that the
waveguide is divided into two mating portions, one portion being
fixedly secured as by welding to each of the separate half sections
of the cavity 2. Very little leakage of microwave energy through
the joint 23 is obtained because the dominant mode of the waveguide
11 has essentially no coupling to the longitudinal joint 23 located
in the center of the broad walls.
Although the resonator 2 is specifically designed and fed so that
undesired classes of modes are neither supported nor excited, it is
impossible to avoid supporting and weakly exciting at least one
undesired class of modes, namely, the TE.sub.o,m,n, class. This
class of modes is typical of the undesired classes of modes,
wherein the electric vector is perpendicular to the broad walls 3
and these modes are, of course, the undesired modes since they
contribute very little to the heating of the web 7 and since they
can cause arcing and breakdown within the cavity 2. Thus, according
to a teaching of this invention, a mode-damping means is included
in the cavity 2 which preferentially couples to these undesired
modes and suppresses them.
Referring now to FIG. 5, there is shown a preferred mode-damping
structure for suppressing undesired classes of modes of resonance
within the cavity 2. More specifically, the joint 12 between the
mating lip portions 22 of the narrow sidewalls 4 include a lossy
mode-damping element 21. In FIG. 5, the lip portions 22 are shown
separated for ease of explanation. The lossy mode-damping element
21 may comprise, for example, a sheet of rubber loaded with lossy
powders, such as powders of iron, carbon or ferrites. The
mode-damping element 21 serves to heavily attenuate any mode within
the cavity 2 having currents in the sidewall 4 which tend to flow
across the joint 12.
Referring now to FIG. 6, there is shown the system of air ducts 8
for ducting air through the treatment zone in a direction counter
to the direction of movement of the web 7. The end walls 5 of the
resonator 2 are formed by a plurality of conductive septums 15 as
of aluminum. The planes of the septums 15 are perpendicular to the
plane of the broad walls 3 and the inner side edges of the septums
15 define the conductive path for the end wall portions 5 of the
resonator 2. The septums 15 are closed off at their inner end by
means of a conductive plate 16 which also defines the marginal lip
of the opening 6 in the end wall 5, which opening permits the web 7
to pass through the cavity 2. A plate 17, as of aluminum, closes
off the outside side edges of the septums 15 and a similar plate 18
closes off the inner side edges of the septums 15, externally of
the cavity 2, to define a plurality of air passageways through the
end wall 5 of the resonator 2. The inside cross-sectional
dimensions of each of the air ducts is dimensioned such that it is
below cutoff for microwave energy at the operating frequency of the
cavity 2. In this manner microwave energy is not transferred into
the tubular air duct system. A flange 19 is provided at the outer
end of the ducts 8 for bolting the air ducts to a suitable exhaust
pan or blower, now shown.
The flat multimode cavity of the present invention has many
advantages over the prior cavity resonator microwave applicators.
Its short height makes it difficult to excite undesired modes of
oscillation with the electric vector other than parallel to the
broad walls. The short height of the cavity further facilitates
directing air flow immediately adjacent the surface of the web or
treatment zone. Decreasing the height of the cavity also
facilitates impedance matching because, in a higher cavity, the
modes would have higher Q, thereby making it more difficult to
match the high impedance of the high Q modes to the relatively low
output impedance of the microwave source 9. Furthermore, by
arranging the waveguide feed with the broad walls of the waveguide
11 perpendicular to the broad walls 3 of the cavity, the desired
modes are excited to the exclusion of certain undesired modes. The
provision of the lossy mode absorbing element 21 in the joint 12
further suppresses undesired modes.
In addition, the flat multimode cavity of the present invention
exhibits all of the advantages of the cavity resonator applicator
over the waveguide applicator. It is a physically simple structure
which can be fabricated inexpensively, tends to be smaller and
lighter in weight and has lower inherent loss than the waveguide
type of applicator. As will be apparent it is easy to ventilate and
clean and will not tend to collect foreign matter. Finally, it has
a sufficient unobstructed volume adjacent the path of the material
being treated to minimize the need for careful control over the
dimensions and motion of such material.
Since many changes could be made in the above construction and many
apparently widely different embodiments of this invention could be
made without departing from the scope thereof, it is intended that
all matter contained in the above description or shown in the
accompanying drawings shall be interpreted as illustrative and not
in a limiting sense.
* * * * *