U.S. patent number 3,783,221 [Application Number 05/210,742] was granted by the patent office on 1974-01-01 for device for adjusting the microwave energy applied to a band or a sheet to be treated in a resonant cavity furnace.
Invention is credited to Joel Henri Auguste Soulier.
United States Patent |
3,783,221 |
Soulier |
January 1, 1974 |
DEVICE FOR ADJUSTING THE MICROWAVE ENERGY APPLIED TO A BAND OR A
SHEET TO BE TREATED IN A RESONANT CAVITY FURNACE
Abstract
A wave-guide has a slot whose area increases in the direction of
reduction of the energy transmitted by a microwave generator.
Inventors: |
Soulier; Joel Henri Auguste
(Eaubonne, FR) |
Family
ID: |
26216137 |
Appl.
No.: |
05/210,742 |
Filed: |
December 22, 1971 |
Foreign Application Priority Data
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Dec 31, 1970 [FR] |
|
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70.47568 |
Dec 31, 1970 [FR] |
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70.47569 |
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Current U.S.
Class: |
219/693; 333/248;
219/750; 219/696 |
Current CPC
Class: |
H05B
6/68 (20130101); H05B 6/788 (20130101) |
Current International
Class: |
H05B
6/78 (20060101); H05B 6/68 (20060101); H05b
009/06 () |
Field of
Search: |
;219/10.55,10.61 ;34/1
;333/98R |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Albritton; C. L.
Assistant Examiner: Jaeger; Hugh D.
Attorney, Agent or Firm: Jecies; Saul
Claims
I claim:
1. A micro-wave cavity furnace comprising, in combination,
a resonant wave guide cavity having longitudinally spaced end
portions and a wall extending from one to the other end
thereof;
a source of microwaves arranged in one of said end portions and
operative for radiating microwaves whose axis of propagation
extends from said one towards the other of said end portions;
advancing means for advancing a band of microwave-absorbing
material to be treated over said wall exteriorly of said resonant
cavity and transversely of said axis of propagation; and
aperture means provided in said wall extending along said axis and
having a cross-sectional area which divergingly increases in
direction from said one toward said other end portion, the increase
in said cross-sectional area compensating for the microwave energy
attenuation which takes place in said direction so as to assure
uniform treating of said band as the latter becomes incrementally
exposed to the microwave energy through said aperture means.
2. A furnace as defined in claim 1, wherein said aperture means
comprises at least one slot which diverges in said direction.
3. A furnace as defined in claim 2, wherein said band has a given
width in said direction; and wherein said slot has a length in said
direction which corresponds to said given width.
4. A furnace as defined in claim 2, wherein said slot diverges in
said direction in inverse ratio to the degree of microwave energy
attenuation in said direction.
5. A furnace as defined in claim 1, wherein said aperture means
comprises an elongated slot extending in said direction, and a
plurality of apertures located laterally adjacent saod slot, and
wherein the combined cross-sectional area of said slot and
apertures increases in said direction.
6. A furnace as defined in claim 5, wherein said apertures are
elongated substantially normal to the elongation of said slot and
are spaced from one another in said direction.
7. A furnace as defined in claim 6, wherein the distance between
consecutive ones of said slots equals substantially one-half of the
length of microwaves radiated by said source.
8. A furnace as defined in claim 1, wherein said aperture means
comprises a plurality of slot-shaped apertures all elongated in
said direction, and wherein the combined cross-sectional area of
said slot-shaped apertures increases in said direction.
9. A furnace as defined in claim 1, wherein said aperture means
comprises at least one slot which is elongated in said direction,
and a plurality of additional slots located at opposite lateral
sides of said one slot and extending transverse to the elongation
of the same; and wherein the combined cross-sectional area of said
slots increases in said direction.
10. A furnace as defined in claim 1; and further comprising a plate
member located in said resonant cavity and having an edge face
located inwardly adjacent and facing said aperture means.
11. A furnace as defined in claim 10, wherein said edge face is
inclined towards said aperture means in said direction.
12. A furnace as defined in claim 1; and further comprising a grid
element juxtaposed with said wall and having additional aperture
means configurated in correspondence with the aperture means in
said wall; and operating means associated with said grid element
for shifting the same relative to said wall so as to obtain varying
degrees of registry between said aperture means of said wall and of
said grid element.
13. A furnace as defined in claim 1; further comprising a detector
component located in said resonant cavity in the region of said
other end portion and operative for producing a signal upon
detecting microwave energy in excess of a predetermined amount;
amplifier means connected with said detector component for
amplifying the signal thereof; and a control circuit connected with
said amplifier means and said source for receiving the amplified
signal from the former and for varying the operation of said source
in dependence upon the magnitude of the signal.
14. A furnace as defined in claim 13, wherein said detector
component comprises a neon lamp which is energized in the presence
of said excess microwave energy, and a photosensitive cell
positioned so as to detect energization of said neon lamp and
produce said signal.
15. A furnace as defined in claim 13, wherein said detector
component comprises a thermo-electric probe.
16. A furnace as defined in claim 13, wherein said detector
component comprises a ferrite probe.
17. A micro wave furnace for treating a work piece in the form of
an elongated band, comprising
a substantially electrically continuous cavity having a
longitudinal axis;
a source of microwave power to energize the cavity for propagating
therein microwave energy along said longitudinal axis;
at least one longitudinal aperture provided on the cavity on one of
the walls thereof, said at least one aperture having a surface
extent increasing along said longitudinal axis;
travelling means for moving said band along its own longitudinal
plane and transversely to said longitudinal axis in front of said
at least one aperture;
thereby providing a substantially even distribution of the
microwave power applied to said band.
18. A furnace as defined in claim 17, wherein at least one
longitudinal aperture has a length substantially equal to the width
of the band.
19. A furnace as defined in claim 17, wherein the microwave energy
propagated along the longitudinal axis is regularly attenuated from
the source of microwave power and wherein the at least one aperture
has a surface extent increasing along said longitudinal axis in
inverted ratio to attenuation of microwave energy along said
longitudinal axis.
20. A furnace as defined in claim 17, wherein the at least one
longitudinal aperture is delimited by sets of longitudinally
extending slots, said slots being in a number and extension
increasing along said longitudinal axis, said slots being moreover
staggered whereby said travelling means are moving the band in
front of at least one slot.
21. A furnace as defined in claim 17, further comprising at least
one set of transversely extending slots placed in a fringed
arrangement around the at least one longitudinally extending
aperture.
22. A furnace as defined in claim 17, wherein two of said
transversely extending slots are distant from each other by
approximately one-half of the microwave length into the resonant
cavity.
23. A furnace as defined in claim 17, further comprising a field
concentrating plate, said plate being placed inside the resonant
cavity in front of the at least one slot and transversely to a
plane limited thereby.
24. A furnace as defined in claim 23, wherein said field
concentrating plate is a tapered ridge having a slope increasing
from the source.
25. A furnace as defined in claim 17, further comprising a grid
having at least one hole of a shape corresponding to the shape of
the at least one aperture, said grid being placed in parallel
relationship to a plane limited by said at least one aperture, and
one operating device being connected to said grid for moving it,
whereby controlling the opening surface of the at least one
aperture.
26. A furnace as defined in claim 17, further comprising a detector
component placed inside the resonant cavity downstream from the
band while considering propagation direction of the microwaves,
said detector component providing a signal at output thereof when
it is energized by microwave energy, said detector component being
connected to the source of microwave power through a control
circuit whereby the source of microwave power is adjusted by means
of the signal from said detector.
27. A furnace as defined in claim 26, wherein the detector
component comprises a neon lamp and a cell placed in front of said
lamp, said cell detecting lighting up the neon lamp when the same
is submitted to a radiation and being connected to input of said
control circuit.
28. A furnace as defined in claim 26, wherein the detector
component is constituted of a thermoelectric probe.
29. A furnace as defined in claim 26, wherein the detector is
constituted of a ferrite probe.
30. A method of uniformly heating sheets and bands, comprising the
steps of
radiating microwave energy from a location in a wave-guide which is
provided in a boundary wall thereof with aperture means that is
elongated along the axis of wave propagation and whose
cross-sectional area increases along said axis in direction away
from said location; and
advancing a sheet or band to be treated over said aperture means
transversely to the elongation thereof and outside said wave-guide,
so that the increments of said sheet or band which are exposed
through said aperture means to said microwave energy will be
uniformly heated despite the attenuation of microwave energy along
said axis in said direction away from said location.
31. A method as defined in claim 30, wherein said sheet or band is
advanced continuously.
32. A method as defined in claim 30, wherein the width of said
sheet or band is at most equal to the length of said aperture means
along said axis, so that the entire width of said sheet or band is
exposed simultaneously in said aperture means to said microwave
energy.
33. A micro-wave cavity furnace comprising, in combination,
a wave-guide cavity having longitudinally spaced end portions and a
wall extending from one to the other thereof;
a source of microwaves arranged in one of said end portions and
operative for radiating microwaves whose axis of propagation
extends from said one towards the other of said end portions, said
source having a protruding antenna;
advancing means for advancing a band of microwave-absorbing
material to be treated over said wall exteriorly of said resonant
cavity and transversely both to said axis of propagation and to
said axis of the protruding antenna;
aperture means provided in said wall extending along said axis and
axis of the aperture means lying in the same plane with the
antenna, said aperture means having a cross-sectional area which
divergingly increases in direction from said one toward said other
end portion, the increase in said cross-sectional area compensating
for the microwave energy attenuation which takes place in said
direction so as to assure uniform treating of said band as the
latter becomes incrementally exposed to the micro-wave energy
through said aperture means.
34. A microwave cavity furnace for treating a workpiece in the form
of an elongated band, comprising
a substantially electrically continuous cavity having a
longitudinal axis;
a source of microwave power to energize the cavity for propagating
therein microwave energy along said longitudinal axis, said source
having an antenna protruding in the cavity;
at least one longitudinal aperture provided on the cavity on a wall
perpendicular to the protruding antenna, said aperture having an
axis lying in the same plane with the antenna and a surface extent
increasing along said longitudinal axis;
travelling means for moving said band along its own longitudinal
plane and transversely to said longitudinal axis in front of said
aperture;
thereby providing a substantially even distribution of the
microwave power applied to said band.
Description
In microwave heating it is well known to use waveguide furnaces for
the treatment of materials in form of sheets or bands, such as
papers, adhesive tapes, or cinematographic films. In the art a
rectangular wave-guide having a longitudinal slot is generally
used, said wave-guide being excited on a mode TE 01 by a magnetron
placed at one of the ends of the guide, and the sheet or band to be
treated is moved transversely with respect to the slot, i.e. with
respect to the axis of the wave propagation inside the resonant
cavity of the wave-guide furnaces. In such furnaces, the
attenuation of energy is not linear relative to the material being
treated, because the propagation direction of the energy is
perpendicular to the travel of the material whereby one side of the
latter is heated more than the other side.
This disadvantage is not too serious when the energy applied to the
band or sheet to be treated is not important, or when the sheet or
band is not wide, as is the case in cinematographic films. On the
contrary, however, it prevents the treatment of wide bands or
sheets having a width of for example several meters, and also of
sheets having a thickness greater than 1 millimeter, or sheets
having a high energy absorption coefficient, because then only one
portion of the width of the sheet is properly heated.
To cope with this problem, the wave-guide may be folded in
serpentine manner in a meander furnace so that the resonant cavity
of such wave-guide furnaces delimits several successive windings.
However, even in such a case it has not been possible, up to now,
to obtain uniform heating over the whole width of the bands or
sheets to be treated.
The invention solves the above problem in a simple way and makes
possible the treatment of sheets or bands of great width and which
travel continuously through the microwave furnace.
According to the invention, there is provided a device for
adjusting the microwave energy transmitted to a sheet or band
travelling transversely to the axis of propagation of microwave
energy in a resonant cavity furnace. The resonant cavity furnace is
provided in one of the walls thereof with at least one slot in
front of which the sheet or band is made to travel, and the slot
area increases in direction of microwave energy attenuation along
the axis of propagation of the microwave energy.
Other characteristics of the invention are shown in the following
detailed description.
Embodiments of the invention are shown by way of none restrictive
examples in the accompanying drawings, in which
FIG. 1 is a sectional perspective view of a microwave furnace
according to the invention;
FIG. 2 is a diagrammatic plan view of FIG. 1;
FIGS. 3, 4 and 5 each are plan views similar to FIG. 2 and
illustrating miscellaneous modifications;
FIG. 6 is a sectional perspective view similar to FIG. 1 but of the
embodiment of FIG. 5;
FIG. 7 is a sectional view showing a further embodiment of the
invention; and
FIG. 8 is a diagram of an additional adjusting device.
In the drawings, the microwave furnace comprises a wave-guide
excited according to the mode TE; this wave-guide is designated in
the following description as a "resonant cavity." In the resonant
cavity 1 is located the antenna 2 of a microwave generator 3, a
magnetron for example, supplied with electric energy by a source 4.
An adjustment or matching device 5 constituted, for example, by one
or several rings made of polytetrafluorethylene is placed between
antenna 2 and the resonant cavity.
Moreover, an additional absorption load 6 is provided near the end
of the resonant cavity to absorb such energy as is not applied to
the material to be treated. Said material is shown as a plate or
sheet 7 which is continuously moved in the direction indicated by
arrow f.sub.1 by means of a driving device which may be constituted
by a pair of cylinders 8 or by any other suitable conveyor.
The magneto-electric energy transmitted from the antenna 2 is
applied to sheet 7 through one of the walls of the resonant cavity
1, i.e., in the example shown in the drawings, through the upper
wall wherein openings are provided.
According to the invention and as particularly shown in FIGS. 2-5,
the openings can have various shapes. In fact, it has been noticed
that in a resonant cavity of the above described type and of
rectangular cross-section, which is excited according to mode TE
01, the attenuation of the energy transmitted through a
longitudinal slot is not linear since the direction of energy
propagation is perpendicular to the travel direction of the
material, that is the direction of advancement of sheet 7. To
prevent this disadvantage, FIG. 2 shows that the slot 9, whose
length is equal to the width of sheet 7, has an increasing width in
the direction of propagation of the waves passing through the
resonant cavity 1, that is following the direction of arrow
f.sub.2.
Because the energy attenuation in the sheet 7 to be treated varies
according to an exponential law, the slot 9 is advantageously so
configurated that its width increases inversely to the attenuation.
A first embodiment is shown in FIG. 2, for use when the sheets 7 to
be treated are always of the same nature and consequently have a
known absorption coefficient and also an invariable thickness.
The opening of slot 9 need, however, not be continuous, as is shown
in FIG. 3. FIG. 3 shows longitudinal slots 9a arranged in
succession, the number or extent thereof increasing in the
direction of the microwave energy transmission. It is advantageous,
as shown in FIG. 3 that successive slots 9a are alternated or
staggered to ensure that the material of sheet 7 will receive
energy in all the portions thereof.
A further development of the arrangement shown in FIG. 3 is
illustrated in FIG. 4, according to which the successive
longitudinally extending slots 9a are completed by transversely
extending slots 9b which are separated from each other by an
interval approximately equal to .lambda. g/2, which means half of
the wave length in the resonant cavity.
Preferably, the transversely extending slots 9b are located
laterally of the longitudinal slots 9a, because the magnetic field
is at a maximum at the sides of the resonant cavity 1. Thus by
arranging the slots 9b in a diverging pattern as shown, the
attenuation is compensated according to the longitudinal energy
propagation axis, which results in an energy application that is
substantially uniform over the entire width of sheet 7 during the
advancement of the same.
FIGS. 5 and 6 illustrate another embodiment according to which the
wave-guide 1 has an extended slot 9 at the type above described in
FIG. 2, as well as transversely extending slots 9b which are
located in a divergent arrangement. In addition, a tapered plate or
ridge 10 tends in the cavity 1 in front of slot 9; it has an
inclined top face 10a, the slope of which is directed towards the
antenna 2. Preferably the tapered plate 10 can be adjusted
vertically by an adjusting device 11, thus making it possible to
concentrate the field towards the slot 9 along the field
attenuation into the resonant cavity, whereby practically all the
energy transmitted by the antenna 2 is uniformly absorbed by the
sheet 7.
When the furnace must be utilized for successive treatment of
sheets 7 of various thickness and/or with different absorption
coefficients, or also of non-uniform thickness then it is
advantageous, as shown in FIG. 7, to place on the wall of the
resonant cavity 1, provided with the slots 9 or 9a or 9b above
described, a grid 12 with apertures 9a.sub.1 9b.sub.1 similar to
said slots 9a, 9b. Said grid 12 is connected to an operating screw
or other similar device 13 for imparting an axial sliding motion to
the grid, so that the apertures 9a.sub.1, 9b.sub.1 can be brought
in front of slots 9a, 9b or be more or less shifted with respect to
said slots with a view towards reducing the amount of energy
applied to sheet 7. Also preferably a tapered plate 10 for the
concentration of the magnetic field is utilized as above described
with reference to FIGS. 5 and 6.
It is also possible for the plate 10 which is made of metal, to be
associated with a plate 14 of a material pervious to microwaves,
for example polytetrafluorethylene, in order to adapt or match the
impedance of the resonant cavity according to the adjustment of the
magnetic field concentration in said cavity, and consequently to
the concentration of the electrical field applied to the absorbing
material of sheet 7.
The arrangement of FIG. 7 and also of FIGS. 5 and 6 are
particularly suitable for the treatment of materials with a very
high absorption coefficient.
FIG. 8 illustrates an additional adjusting device including, in the
cavity 1, a detector 15, for example a neon lamp which becomes
excited if a sufficient amount of energy is applied to it and which
then lights up. A cell 16 is placed in front of the lamp 15 to
determine if the lamp is or is not lighted. The output of cell 16
is connected to an amplifier 17 whose output signal 15 is used for
the control of a power unit 18 for the magnetron 3. For example,
the output signal from amplifier 17 can directly control a
servo-motor 19 which adjusts the input voltage of a
self-transformer 20, the output voltage of the same directly
feeding the magnetron 3.
Also, the resonant cavity 1 can be provided with the additional
load 6 which constitutes a further safety device intended to
absorb, for short intervals of time, an oversupply of energy
produced by the magnetron 3.
As it is evident from the above, if some power is not absorbed by
sheet 7, then the lamp 15 lights up, which illumination is detected
by the cell 16 the output current of which, after amplification in
17, reduces the feeding voltage of the magnetron 3.
In the above description, it has been considered that detector 15
was constituted by a neon lamp. It is possible to constitute said
detector as a thermo-electric probe placed into the additional load
6. Said probe then detects any temperature rise of said load and
consequently the presence of an excessive amount of power radiated
by the magnetron 3. The output voltage from the thermoelectric
probe, after amplification in amplifier 17, operates the
servo-motor 19 or any other device for adjusting the input voltage
of magnetron 3.
It is also possible to use a ferrite element which becomes
saturated if the microwaves are not absorbed. The detection of the
saturation then can be used to adjust the magnetron power
supply.
The invention is not restricted to the embodiments shown and
described in detail, for various modifications thereof can moreover
be applied to it without departing from the scope of the invention.
Especially in case where the whole power developed by the magnetron
would not be absorbed by the wave-guide, then the energy could be
sent back into one or several other similar wave-guides through
suitable bends.
* * * * *