BEAM ADJUSTING DEVICE

Abstract: A device for adjusting the beam direction of a beam radiated from a stationary array of antenna elements. The device comprises a feed line structure configured as a star with at least four line segments extending from a central source connection terminal at the centre of the star, to the respective feed connection terminals (100). The dielectric body with two different body portions, having different effective dielectric values, is displaceable between two end positions in a central, region of the device.

Description: BEAM ADJUSTING DEVICE Field of the Invention The present invention relates to a device for adjusting the beam direction at an antenna. More particularly, the device is of the kind defined in the preamble of claim 1. Related Art and Background of the Invention Such a device is previously known from the document WO 96/37922 (Allgon AB) . The known device comprises a feed line structure integrated with a stationary array of antenna elements so as to enable adjustment of the direction of the beam radiated from the array. The feed line structure includes a feed conductor line pattern disposed on a fixed carrier plate at a distance from and in parallel to a fixed ground plate, and a movable dielectric plate located therebetween. The feed line pattern is elongated in the same direction as the movement direction of the dielectric plate. The propagation velocity of the signal components is reduced by the presence of the dielectric plate between the respective feed line and the ground plate. Accordingly, by displacing the dielectric plate in the longitudinal direction, the phase difference between the various signal components may be controlled. In the previously known device, the feed line pattern is configured basically in meander-like loops with several loop portions extending back and forth in the longitudinal direction. Accordingly, the signal paths are relatively long, and the losses of microwave power being transferred in the device is relatively high. Moreover, because of the various meander-like loops extending in parallel to each other, the device is necessarily relatively wide in a transverse direction. Therefore, the overall dimensions of the device are relatively large. μ- *ϋ rt 3 3 t D μ- ι-3 Hi O μ- v CD tr T( Ω, rt Hi rt Ω CQ CQ Ω H3 CD CQ μ- > ω H- H 0 P J pi 0 ) H- P if μ- Φ O Hi μ- 0 φ 0 O μ- s; μ- Φ Φ Φ Φ φ if P 3 rt ø Q g Hi H ϋ H- l_I. rt Hl Φ V Φ CQ ? h CQ Ω, fi ri 0 ri P CQ P Hi μ- 0 Pi ii <J O i § Hi Φ rt Ω 0 Φ Hi Ω, Φ Ω, CQ rt Φ rt 3 ^ rt φ CQ 3 rt 3 Φ μ- D £ ø φ μ- § Φ ω H- i H tr H Φ H- α, μ- if ^ μ- Φ μ- Ω Hi rt μ- ri Φ ii s 0 Ω ø ø Oi H ø 0 P 0> P i Hi μ- CQ σ Φ μ- 0 P *ϋ 0 rt P P Φ ti i Φ 0 φ rt t CQ ( Φ P Φ TJ <! ) Φ Hi Hi φ μ- CQ P ft 0 P μ- ϋ ϋ i rt , tr Ω, ϋ μ- rt ^ P 3 ) CQ CQ PJ φ rt P Φ Hi CQ P φ φ CQ ii CQ O ft μ- 0 CQ H- 1 1_I. φ ii o ft H CQ ii H- rt ri φ 3 φ μ- μ- rt 3 if r CQ Hi ■ ; μ- φ i Φ ø rt 0 • H- 3 . rt Ω, <J Φ H Φ rt 3 φ Q Φ μ- if Φ Φ • Φ P Ω μ- 0 ø * i-h ΓT P> H- Φ 3 P Φ P CQ O Φ X X 0 O i i Ω rt X Ω ft Ω Ω 3 μ- μ- to H- << TJ 0 Hi H P ) rt 0 rt rt rt ft a < μ] rt > if rt 0 Ω Φ tr CQ CQ rt P Φ r Hi Hi >< rt Ω Q 4 O CQ Φ O φ μ- t μ- rt φ Φ ti μ- μ- cr Ω CQ if Φ Φ Φ £ Φ P tr Φ a Ω P μ- a φ μ- 0 P Hi 0i CQ Φ Ω rt tr Φ tr A> Hi rt r PJ O Ω rt CQ C PJ μ- a CQ CQ P P CQ Ω, μ- μ- CD tr 0 PJ 3 <! Φ P * Φ 0 • ! μ- Hi rt O i 3 μ- ft μ- α φ φ rt μ- CQ 3 I CQ Ω H H- 0> Φ H Φ P ii 0> ω P P μ- Φ 3 Φ P Ω, μ- 0 ) O i i ti P Ω μ- •ϋ ?v 0 H i fu H- rt • CQ a a CQ P, LQ 0 μ- φ CD CD ri CQ ii H if Φ ø ri CQ <! ϋ H- 3 σ H H- CQ P Φ rt Ω H) φ 0 rt Φ • μ- X if o i Φ Φ 0 ø h- 1 CQ P H3 φ cr O i CQ μ- i μ- ) Hi φ CQ P Hi Ω, φ Ti φ < 0 a CQ IQ rt ii Φ ^ if tJ- Hi CQ μ- ϋ Ω, P rt Φ Ω 3 CQ rt rt H <! Φ ri μ- 0 rt P ø Φ 0 0> 0> Φ Hi rt CQ TJ if φ H rt Φ £ 0 0 PJ Ω φ 0 φ Ω, 0 H- l- 1 r 0> w 3 Ω, Φ A ) P J 0 i 0 0 1 0 Ω, Φ ii P rt 0 3 CQ Ω Ω, CQ 0 Φ Ωα 0 pi CT l- 1 0> TJ Φ . μ- rt Ω P Ω i <: T3 Ω <τ3 3 μ- rt if rt O μ- rt a ri φ CQ Φ rt H- P ^ rt rt O CQ Φ Ti Φ TS O i rt Ω CO φ Oi O i ri Hi < CQ H- ^ Ω ϋ r Q O μ- μ- P φ o P o μ- φ O φ • ø Pi rt φ PJ rt μ- H- < Oi Hi CQ CQ rt CD Φ tr φ 3 P CQ CQ μ- ri Ω μ- Ml . H- Ω 0 rt σ Φ μ- O i P μ- μ- O i Hi 0 X 0 ) Φ H 0 rt ti rt μ- tr 3 Φ Hi H- Hi <! 0 ) P S 0 iQ P tr rt rt rt Ω Hi , ft μ- Φ C Oi CQ 0 1 0 0 O i CQ Φ Hi 0 Φ 0 Ω, P φ P IQ CQ φ O φ Φ Φ ^ φ P CD CD ϋ ri <! O i μ- Ω Hi n ft *< μ- Λ H rt P Ω P φ T3 Ω , ^ 3 O ø 3 rt Φ ΓT Ω i i Φ P φ Φ O i Ω, i Ω, rt rt μ- Ω, , CQ φ Φ Φ ) , 0 ) H- ii P J Φ H, Φ μ- w h- 1 PJ P μ- μ- μ- co μ- 3 Ω μ- < 0 φ 0 Φ Φ P 0 M Hi 0 φ Ω ft H CQ H rt <! IQ ii Φ rt Ω rt rt μ- Φ < tr Φ P H CQ CQ Φ Hi H Ω Oi μ- μ- Φ Φ φ 0 Φ Ω, Φ Φ P μ- 0 if tr Ω Hi CQ μ- Ω ft rt CQ rt Φ rt rt H 1 CQ Hi i Ω Ω Ω μ- P Ω rt < ti Φ φ 0 ) Ω φ 0 Ω, P> if 0 ii μ- i φ Hi rt O rt i . <! Φ rt ω φ ti ) Ω Φ Ω 3 H- CQ h- 1 CQ CQ • Φ O μ- P rt Φ μ- P μ- μ- μ- H μ- Φ rt Hi if rt 0 rt • 6 Φ φ ft - Φ is P Ω CQ U H ^ 0 P- 0 Hi Φ Ω, 0> 0 Φ Hi Ω φ i ≤ tr H 0 Φ Ω rt rt CQ rt Φ Φ P a μ- Φ a X φ ft φ ϋ 0 ) 0 μ- Φ 3 i Φ rt if <! P ^ 3 rt CQ J LQ H φ Ω, rt φ μ- Φ Ω, μ- Φ <! Hi Q Ω Φ P H- Φ P. 3 OJ Ω if • i •» ω Ω * 0 Φ , 0 i i ø o μ- Φ Ctrt 0> (Q 0 μ- PJ Φ Φ Φ μ- rt rt μ- H P ti CD LQ rt CQ ø rt rl H rt 0 rt Φ ^ fJ rt . H H, Pi ii a μ- Ω, Ω rt μ- if CQ CQ if tr H- H- H- CQ £ φ rt CQ P P TJ μ- rt a rt 0 rt 0 rt i Φ Φ 0 Ω Ω <! 0> 0 Φ σ % Φ i τJ O i O P-. PJ Ω 0 tr CQ P Φ Hi φ if 0 CQ O i H PJ Φ 0> Ω Φ i ii 3 rt Hi μ- ) Φ Φ P ii 0 Φ 3 Φ H H tr rt 3 Φ φ if 0 i ii < a ti 3 Φ 3 c CO rt 0 ) Hi i to So H- 0 0 H 3 su ϊ Hi μ- 0 ) μ- Ω, Φ Ω μ- r rt Hi ø 4 0 φ φ -. rt Hi P O μ- J ■ <: K φ Q μ- CQ 0 Hi o φ H c P 4 Φ Φ Ω, φ CQ 0 tr Hi CQ > <; Ω Ω ii φ P Φ Hi P Hi i b <! PJ μ- Oi P i Ω, Φ Φ Φ Φ Φ Φ r i P s; φ Ω Φ φ O μ- O μ- Ω rt TJ £ 0 CQ ϋ pi TJ Ω Φ $. tr CQ 0 i 0 CD ii 0 Ω P - rt Φ rt a ft i if rt <i 0 0 O μ- H" rt CQ ^ P μ- φ CQ Φ ^< φ P ri Φ μ- μ- 3 3 n P Hi 0 rt φ , 0 Ω t- 1 f P J ^ p- P P μ- - 1 ii Φ <! Ω ø CQ φ > rt rt μ- rt Φ CQ μ- if φ Φ Φ H- rt rt Φ 3 σ Φ 0 ) P 0 tr P> 0 ft ) 0J Hi rt μ- <i Φ 0 Hi a ct μ- ø μ- 0 H- CQ P P μ- O if rt Φ P Ω, μ- o Q, P rt CQ rt α, 0> if CQ CQ c P P φ ϋ φ ^ CQ Φ μ- a rt >< D CD ■ : p ) CQ rt extending in a transverse direction from the respective line segments to the ground plane. Advantageously, the feed line structure may comprise strip line segments located between top and bottom walls of a closed elongated housing, the top and bottom walls serving as a ground plane. Then, each body portion may comprise upper and lower parts located above and below the strip line segments, respectively. These and other features of the invention will become apparent from the detailed description below. The invention will be explained more fully below with reference to the appended drawings illustrating some preferred embodiments. Brief Description of the Drawings Fig. 1 shows the device according to the invention in a perspective view; Fig. 2 shows the device of fig. 1 in an end view; Fig. 3 shows a longitudinal central section through the device of fig. 1; Fig. 4 shows a planar view of the device of fig. 1 with a top wall of the housing being taken away; Fig. 5 shows a cross section through the device of fig. 1; Fig. 6 shows a cross section through a modified version of the device of fig. 1, and Fig. 7 shows a second embodiment of the device, including a different feed line structure. Detailed Description of Preferred Embodiments The device shown in figs. 1 and 2 comprises an elongated boxlike housing 10 consisting of an upper part 20, a lower part 30, end pieces 40, 50 and a feed line structure, generally denoted 100, inside the housing 10. The housing 10 is of the general kind described in the separate Swedish patent application entitled "Shielded Housing" filed simultaneously by the same applicant. The disclosure of the "Shielded Housing" application is included herein by reference. The upper part 20 of the housing includes a substantially planar top wall 21 and, integral therewith, two downwardly directed, longitudinally extending outer side flanges 22, 23. The lower part 30 of the housing includes a substantially planar bottom wall 31 and, integral with the longitudinal edge portions of the bottom wall 31, inner side flanges 32 and 33. These inner side flanges 32, 33 are dimensioned to make contact, substantially over the entire external surface thereof, with the inside surfaces of the outer side flanges 22, 23. As explained in the separate "Shielded Housing" application, such a surface contact is obtained irrespective of the exact dimensions of the upper and lower parts within certain limits maintained during manufacture of the device. The top and bottom walls 21 and 31 of the housing are held at a pre-determined, well-defined mutual distance defined by the respective end piece 40, 50 as explained in detail in the "Shielded Housing" application. The housing 10 accommodates a feed line structure 100 and a movable dielectric body 111 serving as a device for adjusting the beam direction radiated from a stationary array of antenna elements (not shown) , coupled to the device. In the illustrated embodiment, the feed line structure 100 is configured like the letter "H" with a central source connection terminal 101, first and second straight line segments 102, 103 extending in a first direction along the main direction A of the device and third and fourth straight line segments 104, 105 extending in a second direction being > ω DO D M t- 1 cπ o in O en o LΠ Hi ii 0 3 rt if Φ CQ 0 0 H, Ω Φ Ω 0 0 0 Φ Ω rt μ- O 0 rt Φ ϋ 3 μ- ø Oi H O H» rt 0 rt tr φ Hi 0 0 H Hi Φ Φ Ωα connection terminals 102a, 103a, 104a, 105a. Thanks to the dielectric elements 109, 110, the impedance matching can be achieved without making the feed conductor 106 extremely wide adjacent to the source connection terminal 101. Therefore, the width of the housing 10 can be relatively small so as to reduce the overall dimensions of the device. These dimensions will be reduced for other reasons as well, as will be explained further below. The feed conductor 106 and the feed line segments 102, 103, 104, 105 are embodied as strip lines between the top and bottom walls 21 and 31, the latter walls serving as ground planes. See also figs. 5 and 6. As compared to microstrip embodiments, the strip line structure has a number of advantages. First, the device can be made shorter and less wide. The reduced width is obtained because the strip lines are generally narrower than corresponding microstrip lines (with the same impedance and ground plane distance) , and the parallel line segments can be positioned closer to each other without mutual coupling, since the double ground plane configuration limits the coupling between neighbouring parallel conductors more effectively. Also, dielectric material can be disposed above and below each strip, so virtually all of the electrical field is influenced by the dielectric material. Therefore, for a given phase angle difference, the length in the longitudinal direction can be reduced. Secondly, there will be no problems with spurious radiation, since the total structure is confined within a shielded box or housing 10. Thirdly, the dielectric material above and below the strip can serve as spacing elements so as to keep the strip line in position. In accordance with the present invention, a unitary body 111 of dielectric material is arranged between the housing walls 21,31 and the feed line segments 102, 103, 104, 105 so as to ω ) t to 1 μ> Lπ o LΠ o LΠ o LΠ μ, rt H DO rt ø μ> φ rt- LQ rt 3 TJ ti 0 Oi Ω μ- rt- rt- to TJ ι-3 μ> Φ i to to μ- Φ £ tr μ> tr TJ μ> j3 tr μ- 0 tr O i 0 o Φ TJ 0 0 to tr φ tr φ μ- 0 if μ 1 μ- ø ro μ- ø Ω 0 φ φ TJ *>. O" 1 Oi Φ μ- φ ι_ι. ii CQ TJ Ωα 0 to ro ø ro LQ ri i Φ H LQ P. 0 LQ LQ φ φ Oi 0 0 H 1 ø 0 rt rt TJ 0 0 0 i 0 LQ 3 CQ rt • 0 3 ø CQ H 1 ω Hi ii Ωα φ LQ ri tr μ- Φ CD μ> φ "• Ωα rt- CQ Φ rt- μ- Ωα TJ LQ ro 0 ) 0 to μ- 0 μ 1 Φ μ- μ- Ω μ- Φ O Ω μ- 1 Ω £ μ- tr ro ø 0 μ- CQ ^ 0 ø Φ Φ Φ ø Φ 0> 0 ) 3 ø rt tr H TJ ø rt rt rt O i rt- CQ Ω rt tr ø φ 0 CD ti ¬ rt 0 CQ LQ Ωα ø 0 Φ H 0 to 0 ) μ- CO μ- Φ μ- ^ tr rt 0 0 to 0 CQ 3 Oi μ- er to Ω Ω φ μ- Ωα ø rt μ- rt H < ~. 0 CQ ro PJ ø P. φ Φ 0 rt ro « 0 Φ μ> Ω rt rt tr Ω Φ rt μ> Φ ^ ø ø μ > Ω Ω £ μ- 3 μ> rt ø μ- > 0 ) ^ φ CQ tr 0 μ> μ > Ω rt- o 0 rt if 0 μ] TJ rt en ii 0 0 3 0 0 to ω *< Φ H ti ¬ 0 μ- Φ tr PJ t TJ 0 ii 01 rt- ø 0 if 0 if μ- μ- Φ 3 Φ O i μ> - X . ro Ω 3 φ ø - 0 0 μ- rt tr CQ ø ro 0 Φ Ω ø φ 0 PJ μ- rt H < ri ti ¬ a ri PJ ro tr ii ro Ω φ LQ Φ μ> Oi to ri S Ω ii Φ LΠ r 0 1 μ> > ro •> 3 ti ¬ ø φ H rt Ω rt μ- ø TJ H tr Φ Φ if CQ ri - TJ tr rt μ> Ω ø μ- ro to rt μ- O μ- rt- tr 0 0 0 rt μ- rt i 0 LQ TJ ii ti ¬ μ- 0 φ Φ ^ Ω ii ø μ- £ ro 0 ιl> 0 ro 0 rt- 0 ø ro to 0 P. φ 3 0 1 tr i to ii 0 μ- Φ i 0 Φ 0 0 p. rt tr φ TJ 0> ^ 0 Φ ii TJ 0 er μ- 1 0 rt CD tr ri ø CQ μ- ø Φ ro ii i * er φ μ- ro tr J 0 ø rt PJ 0 μ- φ φ oi Ωα LQ TJ ø CQ 0 o ti ¬ 0 tr φ i 0 ø Ω φ LQ TJ rt to ri • ; Ωα μ- rt 0 Ω 3 <! μ- Φ H rt er μ> ; μ > Oi rt μ- i 0 TJ to rt ^ CQ tr 0 o tj 1 φ ø H 1 Ω o PJ PI rt ii ω μ> ii tr ii ø rt tr ri 0 Oi TJ 0 ) 0 0 LQ μ- rt μ> ii tr μ- 0 i 0 ) H μ- ro S μ- CQ μ- 0 rt ri 0 ) μ> 0 Tj LQ rt μ> Ωα ø μ- •« ro Φ Ω μ- LQ μ- if P. Ω O -> μ- rt ø CQ μ> M 0 H μ> μ- μ- rt φ <! 0 ø CQ 0 rt μ- if ø μ- μ- rt ø φ O μ- o ω rt ii φ rt ω tr 3 0 φ CQ 0 CQ Φ r ro Φ Ω H ø rt LQ Ω ii tr H CQ ø 0 tr μ- rt 1 ø- 0 φ CQ 0 LQ ø ø o Ω OJ J Ω • tr φ 0 Oi < to 0 rt CQ 0 μ- rt Φ μ- Ωα ø φ rt φ ^ μ- Ω CQ 0 ti ¬ ø μ- 1 rt- Ω ø Φ μ> to tr Φ 0 0 Φ CD • : rt H if CQ rt rt tr ■ <! ro 0 ro CQ ø tr μ- rt *< CQ -> μ > μ 1 Φ li μ> ø H ii Φ Φ 3 tr 0 TJ LQ < Ωα ro Q μ- 0 co μ> μ 1 <! μ> μ 1 Φ TJ TJ 0 Φ Oi 0 i rt- 0 3 Φ φ 0 Φ Ω ~ ω H ø φ Φ H H μ- rt u 0 rt ti ¬ μ- ø ri rt μ- tr CQ μ> φ tr 0 ) ii D 0 rt- 0 H i μ- ~. > TJ tr u> μ> ø 01 0 i if ø rt Φ ø Oi μ- μ> ø o CD ø tr H ii rt μ> - TJ O i - to ii < rt μ- ro < CQ μ- 0 i rt M o ro rt Φ φ φ * μ> μ > Φ CQ ii • rt μ- μ- Q Φ CD rt μ- > ø £ μ- LO μ> ii Φ H tr μ- Ωα 0 ø μ> μ- CQ ro 0 μ- LQ tr 0 μ- 0 to OJ - φ μ> CQ CQ M H Φ ø φ 0 μ- Φ rt o rt ii Pi 0 CD μ> TJ 0 ø ø OJ ø μ 1 Oi TJ TJ φ. 0 LQ CQ Ω μ- to ø ro ro Ω to o 0 ti ¬ H O i ω 0 O i Φ CQ > rt 0 ø CQ tr CQ ω li er o μ- rt- μ- 0 Φ H * Ω Ω tr rt φ Φ => μ> O i μ- rt Ωα μ- μ- O rt ro ø Ω < tr ø 0 CQ Φ μ- rt O i if Ω μ- Ω < H Φ 0 tr ø 3 0 ) μ- TJ LQ Pi φ Φ LQ er TJ ø μ- CD φ 0 rt tr Φ O TJ 0 0 Ωα ro 0 0 0 μ- ti ¬ & J Φ Φ TJ I- 1 o LQ < 0 φ tr μ- μ- rt 0 Ωα μ- £ ø μ- i rt ro ii ii ti ¬ Ω ii H S Φ O i μ- Ω to Φ Ωα tr i ri Ω *< Ω if H rt ø P. 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Pi Φ rt ti ¬ Hi to μ- ø Φ ø 4 Φ < Oi ti ¬ ii μ- P. φ ø if er 0 0 i i rr φ H 1 er μ- μ- ø rt φ 0 0 CQ φ Q Ω Pi o 4 CQ illustrated in figure 6, where the second body portion 214a, 214b is much thinner than the first body portion 213a, 213b. The illustrated embodiment with holes 115 in one of the body portions is advantageous for the reason that the two body portions 113, 114 have the same overall thickness and serve as effective spacing elements between the feed line segments and the housing walls. Of course, other kinds of irregularities may be used instead of holes, such as recesses extending only partially through the material in a transverse direction. Longitudinal slots or the like are also possible. Preferably, the dielectric material has a high dielectric constant. A suitable material is IXEF 1032 (manufactured by SOLVAY, Belgium) which has a dielectric constant of 4.5. Preferably, the dielectric constant of the dielectric material should be in the interval between 2 and 6. Generally, low dielectric constant values make the whole structure longer, as the difference in electrical length is less between an air line and a line with dielectric material beneath and above. A too high dielectric constant value, on the other hand, makes the impedance difference so great that multiple transformation sections 113 ',113", etc might be necessary to achieve a good impedance match, with associated increased length. A higher dielectric constant value also makes the design more sensitive to thickness tolerance induced air gaps between the strip line and the dielectric material . The central source connection terminal may itself serve as a feed connection terminal for direct connection to an antenna element. Moreover, there may be more than four feed line segments extending in a star configuration from the central source connection terminal, e.g. three feed line segments in each opposite direction with associated dielectric body portions having mutually different effective dielectric values . A modified embodiment of the feed line structure is shown in fig. 7, where corresponding parts are denoted with numerals 201, etc instead of 101, etc. (fig.3 and 4) . The displaceable dielectric body 211, with side portions 213,214, covers (partially) only the four line segments 202, 203, 204, 205, whereas the feed conductor 206 and a fifth line segment 207 extend freely inside the housing with air gaps to the top and bottom walls 21,31 (fig. 2). The fifth line segment 207 is connected to a centrally located antenna element . The phase angle of the signal component reaching this centrally located antenna element (not shown) or sub-array is independent of the particular position of the displaceable dielectric body 211. The line segments 202,203 are connected, e.g. via coaxial cables, to two antenna elements or sub-arrays on one side of the central element, and the line segments 204,205 are connected to two antenna elements or sub-arrays on the other side of the central element.

Claims: CLAIMS 1. A device for adjusting the beam direction of a beam radiated from a stationary array of antenna elements, wherein at least four antenna element feed points are coupled to a common signal source via a planar feed line structure having a source connection terminal (101) to be connected to said source and at least four feed connection terminals (102a, 103a, 104a, 105a) to be connected to said antenna element feed points, said feed line structure being elongated in a main direction (A) at a distance from and in parallel to a fixed ground plane on at least one side of said feed line structure, wherein a movable dielectric body (111) is located between said feed line structure and said ground plane so as to change the exciting phase of signal components being transferred between said source connection terminal and the respective feed connection terminals, said dielectric body being movable in said main direction for effecting a controlled phase shift of said signal components so as to adjust said beam direction, c h a r a c t e r i z e d in that said feed line structure is configured as a star with at least four line segments (102,103,104,105) extending from said source connection terminal (101) , at the centre of said star, to said feed connection terminals, at least a first line segment (102) and a second line segment (103) extending generally in a first direction along said main direction (A) , at least a third line segment (104) and a fourth line segment (105) extending generally in a second direction being opposite to said first direction, said dielectric body (111) having a first body portion (113) located adjacent to said first and third line segments and having a first effective dielectric value, and a second body portion (114) located adjacent to said second and fourth line segments and having a second effective dielectric value being different from said first effective dielectric value, and said dielectric body (111) being linearly displaceable between two end positions while keeping said first and second body portions (113,114) in proximity to the respective pair of oppositely extending line segments (102,104 and 103,105) . 2. The device as defined in claim 1, wherein - said dielectric body (111) is elongated and has a length exceeding the distance between said two end positions. 3. The device as defined in claim 1 or 2 , wherein said feed line structure is configured as the letter "H" with four line segments (102,103,104,105) of substantially equal length. 4. The device as defined in any one of claims 1-3, wherein a feed conductor (106) extends from a feed terminal (106a) at one end of the device along two (104,105) of said four line segments to said source connection terminal (101) . 5. The device as defined in any one of claims 1-4, wherein said first and second body portions (113,114) of said dielectric body have different geometrical cross-sections along at least a major part of their respective length. 6. The device as defined in any one of claims 1-5, wherein said first and second body portions (113,114) of said dielectric body have mutually different geometrical irregularities making the effective dielectric values different . 7. The device as defined in claim 6, wherein - said irregularities comprise holes (115) . 8. The device as defined in claim 7, wherein said holes (115) extend in a transverse direction from said line segment to said ground plane. 9. The device as defined in any one of claims 1-8, wherein said first and second body portions of said dielectric body are made of different materials having two different dielectric constants. 10. The device as defined in any one of claims 1-9, wherein said planar feed line structure comprises strip line segments (102,103,104,105) located between mutually parallel top and bottom walls (21,31) of a closed elongated housing (10) , said top and bottom walls serving as said ground plane . 11. The device as defined in claim 10, wherein each of said body portions (113,114) of said dielectric body comprises an upper part (113a, 114a) and a lower part (113b, 114b), said upper part being located between said strip line segment and said top wall and said lower part being located between said strip line segment and said bottom wall . 12. The device as defined in any one of claims 1-11, wherein said dielectric body is movable by means of a movement transfer member (120) secured on said dielectric body (111) , said movement transfer member extending through a longitudinal slot (121) in said elongated (housing) and being mechanically displaceable from the outside of said housing.

Inventors: JONSSON STEFAN, LILJEVIK TORD, LINDMARK BJOERN, JONSSON, STEFAN, LILJEVIK, TORD, LINDMARK, BJOERN
Applicants: ALLGON AB, JONSSON STEFAN, KARLSSON DAN, LILJEVIK TORD, LINDMARK BJOERN, ALLGON AB>, JONSSON, STEFAN, KARLSSON, DAN, LILJEVIK, TORD, LINDMARK, BJOERN
Application year: 2001
Main classification: H01Q3
IPC codes: H01Q1, H01Q3