Classifications

• • H—ELECTRICITY
  • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
  • H05B—ELECTRIC HEATING; ELECTRIC LIGHT SOURCES NOT OTHERWISE PROVIDED FOR; CIRCUIT ARRANGEMENTS FOR ELECTRIC LIGHT SOURCES, IN GENERAL
  • H05B6/00—Heating by electric, magnetic or electromagnetic fields
  • H05B6/64—Heating using microwaves
  • H05B6/74—Mode transformers or mode stirrers
• • H—ELECTRICITY
  • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
  • H05B—ELECTRIC HEATING; ELECTRIC LIGHT SOURCES NOT OTHERWISE PROVIDED FOR; CIRCUIT ARRANGEMENTS FOR ELECTRIC LIGHT SOURCES, IN GENERAL
  • H05B6/00—Heating by electric, magnetic or electromagnetic fields
  • H05B6/64—Heating using microwaves
  • H05B6/70—Feed lines
  • H05B6/707—Feed lines using waveguides
  • H05B6/708—Feed lines using waveguides in particular slotted waveguides

Definitions

• the present invention relates to an electric cooking oven comprising at least one microwave energy source for delivering microwave cooking to a cooking chamber, by means of a waveguide.
• a problem generally encountered in cooking in microwave mode lies in obtaining a good distribution of microwave energy in the cooking chamber. Indeed, it is known that a steady wave regime is established in the cooking chamber during the operation of the oven. It follows that the electric fields of the modes excited in the enclosure have bellies and tension nodes which correspond respectively to so-called hot points and to so-called cold points at different locations in the enclosure.
• a first type of solution consists in providing, in the cooking enclosure, a wave agitator so as to constantly modify the standing wave regime established in the enclosure, and thus to move the hot spots and cold spots. .
• Another very widely used method today is to place the product to be reheated or cooked on a turntable.
• the relative displacement of the product and the hot spots thus makes it possible to standardize the cooking.
• FIGS 1 and 2 schematically illustrate the internal parts of a known oven operating according to this principle: in these figures, there is shown a cooking chamber 1 delimited by a bottom wall 10, a vault wall 11, a wall sole 12 and two side walls 13 and 14.
• the side wall 13 has two horizontal openings 130 and 131 superimposed along the vertical of the wall 13, for the introduction of microwave energy.
• the waves are generated by the antenna of an agnetron (not shown), and transmitted to the cooking chamber via a wave guide 2.
• the wave guide 2 has the general form of a rectangular parallelepiped whose longitudinal axis is vertical.
• the guide is delimited transversely by two rectangular flat surfaces 20 and 21, perpendicular to the longitudinal axis of the guide and separated by a predetermined distance d defining the length 1 of the guide. These two surfaces define reference planes on which the guided waves are reflected.
• the two surfaces 20 and 21 are connected to each other at a right angle by two rectangular surfaces 22, 23, parallel to the side wall 13, each surface having two edges ⁇ , b2, b 3 , b 4 of length d.
• the surface 22 furthest from the side wall 13 has a lateral extension 24 provided with an access 25 for receiving the waves generated by the magnetron's antenna.
• the surface 23 constitutes the outlet plane of the guided waves and for this purpose comprises two openings 230 and 231 placed opposite the openings 130 and 131.
• the outlet plane of the waveguide is directly constituted by a part of the side wall of the enclosure.
• the present invention relates to an improvement to the structure as described above, making it possible to obtain a better distribution of the energy inside the cooking enclosure.
• the subject of the present invention is an electric cooking oven comprising a cooking enclosure, a source of microwave energy and a waveguide of substantially parallelepiped shape delimited transversely by two substantially rectangular surfaces situated in two parallel planes. separated by a predefined distance, the exit of the guided waves being effected by at least two zones situated in an exit plane perpendicular to the two surfaces and delimited by two parallel borders connecting the two surfaces, characterized in that said borders have a length greater than the distance separating the two surfaces, so as to optimize the number of transverse electric and / or magnetic modes excited inside the cooking chamber in excitation planes parallel to the exit plane.
• FIG. 1 is a schematic perspective view of the association of a cooking chamber and a waveguide according to the prior art
• FIG. 2 is a sectional view along a vertical plane passing through the middle of the waveguide of Figure 1;
• FIG. 3 is a schematic perspective view of the association of a cooking chamber and a waveguide according to a preferred embodiment of one invention
• FIG. 4 is an elevational view of the wall side of the enclosure of Figure 3 carrying the guide;
• FIGS. 5a and 5b schematically show the number of transverse electric and / or magnetic fields excited respectively in the case of a waveguide according to the prior art and in the case of the waveguide according to the invention ;
• FIG. 6 illustrates an elevational view of the input side of a waveguide according to a possible embodiment according to the invention
• - Figure 7 illustrates an elevational view of the outlet plane of the guide of Figure 6;
• FIG. 8 is a section along line C-C of Figure 6;
• FIG. 9 is a section of the guide along line A-A of FIG. 6,
• FIG. 10 is a section of the guide along line B-B in FIG. 6.
• the waveguide 2 ′ is of substantially parallelepipedal shape delimited transversely by two surfaces 20 ′, 21 ′ of substantially rectangular shape, and longitudinally by two surfaces 22 'and 23' forming, like the surfaces 22 and 23 of FIG. 1, the inlet and outlet surfaces of the waveguide.
• the borders b' ⁇ , b ' 4 and b' 2 , b ' 3 respectively delimiting the entry planes 23 'and outlet 22' of the guide, by connecting the surfaces 20 'and 21', have a length 1 greater than the distance d separating said surfaces 20 ', 21'.
• the waveguide 2 ′ therefore no longer has the shape of a straight parallelepiped, but of an oblique parallelepiped whose longitudinal axis, parallel to said edges, is inclined relative to an axis orthogonal to the end surfaces 20 'and 21'. It follows that, for the same distance d separating the two surfaces 20 ′ and 21 ′, the waveguide 2 ′ according to the invention has a length 1 greater than that of the waveguide 2 in FIG. 1, this which will optimize, as will now be explained, the number of transverse electric and / or magnetic modes excited inside the cooking chamber 1, in excitation planes parallel to the outlet plane 23 'of the guide.
• the dimensions of the cooking chamber are fixed at 33 cm for the width, 34.4 cm for the depth, and 21.2 cm for the height. Given these dimensions, there are in theory 205 possible excitation modes in the cooking chamber. In reality, a mode in a cavity behaves like a bandpass filter whose bandwidth is around 140 MHz under load for a central frequency of 2450 MHz. It can be shown in these conditions that only fifteen modes can be activated in the cooking chamber. If we note TE mn p and TM mn p the transverse electric and magnetic modes respectively with m oscillations on the width of the enclosure, n oscillations on the height and p oscillations on the depth, these fifteen modes are the following:
• the exit zones of the guide are distributed over the height.
• a mode of the enclosure located in the excitation planes parallel to the exit plane must have one of its tension bellies facing an exit zone of the waveguide. Consequently, all the modes of the form EmQp or TM m 0 p 1 ! do not have bellies on the height, can not be excited.
• the modes whose central frequency is too far from the 2450 MHz frequency will be very weakly coupled.
• the ultimately dominant modes, which should be excited are the modes TE 033 , TE 215 , TM 215 , TE 232 , TM 232 , TE 422 , TM 422 .
• FIGS. 5a and 5b allow a comparison to be made between the number of transverse electrical and / or magnetic modes excited using respectively a waveguide structure of the prior art and a waveguide structure according to the present invention.
• the reference P indicates an excitation plane of the modes parallel to the plane of exit of the waveguides. This excitation plane has the same dimensions as the side wall 13 of the cooking enclosure.
• the position of the tension bellies has been indicated for the various transverse electrical modes which should be excited. These positions are indicated by dots for the mode TE 033 by crosses for mode E 232 , by rectangles for mode TE 422 and P by diamonds for mode TE 2 i5- In FIG.
• the output plane 23 is superimposed on the excitation plane P a waveguide of the type shown in FIG. 1 with two exit zones in the form of two rectangular openings 230 and 231, distributed along and centered on the vertical longitudinal axis. It will be recalled that the exit plane is delimited in height by the two surfaces 20 and 21, and has two lateral edges b ⁇ and b 4 connecting the two surfaces at right angles.
• the output zones 230 and 231 are opposite two tension bellies of the TE 033 mode. Consequently, only this mode will be able to be excited in the plane P with the structure of the guide according to the prior art.
• the outlet plane 23 'of the waveguide according to the invention is delimited by two borders b'i and b' 4 connecting the surfaces 20 'and 21' on a length 1 greater than the distance d separating the two surfaces.
• a third opening 232 as shown in dotted lines in FIG. 5b, this opening 232 being placed opposite a belly of the TE215 mode.
• the oblong openings 230, 231 and 232 have a longitudinal axis extending parallel to the end surfaces 20 'and 21' of the guide. Due to the inclination of the longitudinal axis of the guide, a wave which leaves the antenna of the magnetron does not travel the same distance to reach one or the other end of the same opening. This results in a phase difference between the ends of an opening.
• the non-coherence in phase of the waves at the ends of an opening has the consequence that the electric field radiated towards the enclosure through this opening is not maximum.
• the oblong openings 230 to 232 are inclined relative to a transverse axis of the outlet plane 23 'parallel to the end surfaces 20' and 21 ', so as to reduce the difference distance to travel for a wave from the antenna to the two ends of the same opening.
• the coherence of the incident wave on the aperture is thereby improved, as is the radiated power.
• the consistency is perfect in the case where the openings are inclined so as to present a longitudinal axis orthogonal to the longitudinal axis of the guide.
• the angle of inclination will be chosen in an angular sector delimited by a transverse axis of the plane 23 ', parallel to the surfaces 20', 21 ', and by a transverse axis of the plane 23', perpendicular to the longitudinal axis of the guide.
• the oblong openings of the guide exit plane made either directly in the wall of the enclosure, or in a wall of the guide, have the shape of an ellipse (see FIG. 7) .
• U Ep (1)
• the voltage U evolves like a sinusoid arch along the length of the opening.
• the width a is constant over the entire length of the opening. Consequently, according to equation (1), the radiated field Ep follows exactly the same law as the voltage.
• the width a is almost zero at the ends of the opening and increases towards the center.
• the field Ep remains substantially constant over the length of the opening. The radiated energy is therefore greater in the case of an elliptical opening.
• a waveguide structure in accordance with the present invention and particularly suitable for an electric oven capable of receiving products to be heated on two distinct levels, one level lower corresponding, for example, substantially at the level of the hearth of the oven, and a so-called higher level corresponding, for example, to the mid-height of the cooking chamber.
• the outlet plane 23 'of the waveguide is directly in the side wall 13 of the cooking chamber, so that FIG. 7 only illustrates the delimitations of the outlet plane 23' by compared to openings 230, 231 and 232.
• the guide surfaces 20 ′ and 21 ′ are spaced apart by a distance d substantially equal to 165 mm, while the edges b'2 b ' 3 or b l 4, b' 1 , separated by a distance substantially equal to 86 mm, have a length 1 of approximately 178 mm.
• the longitudinal axis of the guide is therefore inclined about 22 degrees relative to the vertical.
• the center of the opening 25 for the entry of the waves into the guide is located substantially at a distance of 94.5 mm, in orthogonal projection, from the end surface 20 '.
• the opening 25 has a circular section with a diameter substantially equal to 30.6 mm.
• the distance from the outlet plane 23 'to the inlet plane 22' is approximately 21 mm.
• the distance from the outlet plane 23 'to the end of the extension 24 is approximately 41 mm. The previous dimensions allow obtaining a non-resonant waveguide.
• the waves exit takes place at three elliptical openings 230 to 232 ( Figure 7).
• the intermediate opening 232 is advantageously located near the upper cooking level. In this way, the intermediate opening 232 makes it possible to create, on the one hand with the upper opening 230 and on the other hand with the lower opening 231, two interference zones that are fairly well uncorrelated from each other. , and therefore less sensitive to the charges placed on each of the two cooking levels.
• the longitudinal axis of the openings 230 to 232 is for example inclined 11.5 degrees relative to an axis transverse to the outlet plane 23 'and parallel to the surfaces 20' and 21 '. This choice makes it possible to obtain a good compromise between a good restored power and a good temperature balancing on the two plates.
• the height positioning of the openings is preferably also chosen according to the position of the tension bellies of the modes of the form E mn p or TM- mn p, the integer n, corresponding to the oscillations on the height, being equal to 1 , 2 or 3.
• openings 230, 231 and 232 shown in FIG. 7 have different sizes. This advantageously makes it possible to maximize the total power restored while respecting the constraints of impedance matching.

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• Physics & Mathematics (AREA)
• Electromagnetism (AREA)
• Engineering & Computer Science (AREA)
• Power Engineering (AREA)
• Constitution Of High-Frequency Heating (AREA)
• Electric Ovens (AREA)

Applications Claiming Priority (3)

Publications (2)

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• 1996
  • 1996-07-15 FR FR9608825A patent/FR2751055B1/fr not_active Expired - Fee Related
• 1997
  • 1997-07-11 KR KR10-1999-7000257A patent/KR100458670B1/ko not_active IP Right Cessation
  • 1997-07-11 ES ES97933715T patent/ES2155257T3/es not_active Expired - Lifetime
  • 1997-07-11 US US09/214,902 patent/US6057535A/en not_active Expired - Fee Related
  • 1997-07-11 WO PCT/FR1997/001283 patent/WO1998003041A1/fr active IP Right Grant
  • 1997-07-11 EP EP97933715A patent/EP0913070B1/de not_active Expired - Lifetime
  • 1997-07-11 DE DE69703801T patent/DE69703801T2/de not_active Expired - Fee Related
  • 1997-07-11 CN CN97197640A patent/CN1132506C/zh not_active Expired - Fee Related

Non-Patent Citations (1)

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