CN1794513A - Method of realizing high precision phase shifting of ferr ite phase shifting device - Google Patents
Method of realizing high precision phase shifting of ferr ite phase shifting device Download PDFInfo
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- CN1794513A CN1794513A CN 200510022749 CN200510022749A CN1794513A CN 1794513 A CN1794513 A CN 1794513A CN 200510022749 CN200510022749 CN 200510022749 CN 200510022749 A CN200510022749 A CN 200510022749A CN 1794513 A CN1794513 A CN 1794513A
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Abstract
This invention relates to a method for realizing accurate phase shift by a ferrite shifter, which applies a numerical control mode combining a flux excitation and a saturated digital excitation to make the shifter to generate accurate shift including: dividing a ferrite loaded on a waveguide center along the direction of the waves into n sections and the n is greater or equals to 2, the first section of which applies a flux excitation mode, the rest n-1 sections apply a saturation digital mode then overlapping the shift values of them and the shifter carries out digital control shift according to the step volume of the flux excitation section in the sphere greater or equals to 360deg.
Description
Technical field
The invention belongs to waveguide type transmission line field, be specifically related to the method that a kind of ferrite phase shifter is realized the high accuracy phase shift, be applied to improve the phase shifting accuracy of microwave/millimeter wave waveguide ferrite phase shifter.
Technical background
For the phase shifter of patterns such as diode, MMIC, the interior phase shifter that loads the ferrite core rod of waveguide that is used for the microwave high-frequency section has absolute predominance aspect the insertion loss objective, and the latter inserts loss only the former about 1/10.The principle of ferrite digital phase shifter is as follows: with the pulse excitation electric current ferrite in the phase shifter is carried out remanent magnetization, the remanent magnetization of corresponding different directions of the pulse current of different directions or different amplitude sizes or size.And the change of the direction of ferrite remanent magnetization or size can make that the electromagnetic wave propagation constant changes in the phase shifter, thereby will produce different additional phase shifts to the electromagnetic wave by phase shifter.When controlling, thereby when the additional phase shift that phase shifter is produced electromagnetic wave is controlled, just can realize the numerical control phase shift of ferrite phase shifter with the size and Orientation of binary code paired pulses electric current.
According to above-mentioned principle as can be known, digital phase shifter phase shift size is relevant with three factors such as length of size, direction and the Ferrite Material of magnetizing current.So, press dual mode usually and realize the numerical control phase shift:
1. magnetic flux type excitation---under the certain prerequisite of ferrite length, by changing the direction and the size of magnetizing current, the magnetic flux that promptly changes externally-applied magnetic field in the ferrite produces phase shift.
2. the saturated digital excitation/digital excitation of ferrite segmentation---under the certain prerequisite of magnetizing current size, produce phase shift by direction and the ferritic length that changes magnetizing current.
In actual use, magnetic flux type excitation phase shifter generally adopts the multidigit control code that the variable quantity of magnetizing current amplitude size is controlled to degree of precision.But because its pairing ferrite longitudinal size very long (corresponding maximum phase shift should greater than 360 °), corresponding actual phase shifter generally also can only be realized 4～6 control code numerical control phase shifts.Wherein, the phase shift stepping nominal value of 4 bit code correspondences is 22.5 °; The phase shift stepping nominal value of 6 correspondences is 5.625 °.The high accuracy that is difficult to realize the stepping phase shift with the magnetic flux type incentive program.Moreover, because the long ferrite size and the increase of the necessary serial pulses electric current of magnetic flux excitation number make that also the switching time of magnetic flux type excitation phase shifter is obviously bigger than normal.
Saturated digital excitation phase shifter is divided into several sections with the ferrite in the waveguide along direction of wave travel usually, every section respectively corresponding 1 binary system control code.Concrete segments is the figure place of usually said phase shifter, as: just produce the ferrite of phase shift divide four sections be called 4-digit number formula phase shifter.
Comparatively speaking, the great advantage of saturation activation digital phase shifter is: switching time is less relatively.Because ferritic physical length is difficult to do too for a short time in engineering reality, as at the 8mm wave band, the pairing ferrite length of per 1 ° of phase shift is about 0.13mm.Therefore, be difficult to realize high-precision phase shift stepping with saturated digital incentive program.On microwave engineering, saturated digital excitation phase shifter generally also can only be realized 4～5 figure place control phase shifts, and wherein, the phase shift stepping nominal value of 5 correspondences is 11.25 °.This phase shifter also exists structure comparatively complexity, debugging and manufacture difficulty deficiency bigger than normal.
No matter in summary, be used for the digital phase shifter of microwave high-frequency section, be to adopt saturated digital excitation, or adopt the magnetic flux type excitation, is difficult to all realize that phase shift stepping amount is no more than 1 ° high precision numerical control phase shift.
Summary of the invention
The objective of the invention is to overcome the deficiency of prior art, the method that provides a kind of ferrite phase shifter to realize the high accuracy phase shift is so that obtain the high precision numerical control phase shifter in the microwave high-frequency section.
The technical scheme that realizes the object of the invention is the digital control scheme that adopts the magnetic flux type excitation to combine with saturated digital excitation, improves the phase shifting accuracy of ferrite phase shifter.The ferrite that it will load on waveguide core is divided into the n section along direction of wave travel, n 〉=2.Its 1st section is adopted the magnetic flux type excitation, and all the other n-1 sections adopt saturated digital excitation; Then, magnetic flux type activation fragment phase-shift value and each saturated digital activation fragment phase-shift value are superposeed, make phase shifter in more than or equal to 360 ° of scopes, the stepping amount of pressing the magnetic flux type activation fragment realizes the high accuracy phase shift.
It is as follows that described magnetic flux type activation fragment and each saturated digital activation fragment phase-shift value are carried out additive process:
1) with the binary code Control current pulse of n-1 position n-1 iron leg oxysome is carried out saturated digital excitation;
2) with the binary code Control current pulse of m position the first iron leg oxysome is carried out the magnetic flux type excitation, make phase shifter by the stepping of δ stepping amount, at 0 °～
CmaxBetween produce 2
mIndividual phase shift state;
3),, can produce 2 with m+n-1 position binary code control phase shifter with above-mentioned two kinds of phase shift systems combination
M+n-1Individual phase shift state, in described phase shift state, in the 360 ° of scopes maximum stepping amount found out is no more than the phase shift state of δ , to realize the high accuracy phase shift.
Described pairing phase-shift value of each iron leg oxysome and number of fragments n determine as follows:
The phase-shift value of each iron leg oxysome correspondence and definite principle of number of fragments n are: 1. the maximal phase of the magnetic flux type activation fragment correspondence input of moving one's steps satisfies required precision; 2. the phase-shift value of each iron leg oxysome can guarantee any one phase shift state of superposeing out and satisfy maximum stepping phase shift in surpassing 360 ° of scopes; 3. under the prerequisite that guarantees phase shifting accuracy, satisfy number of fragments n 〉=2 and as much as possible little.
According to mentioned above principle, the phase-shift value of each iron leg oxysome correspondence and the concrete determining step of number of fragments n are as follows:
At first, according to the maximum stepping amount of required phase shift δ , and, set the maximum phase-shift value of the 1st section magnetic flux type excitation ferrite correspondence with reference to the working control precision of magnetic flux type excitation drive circuit (driver) to the exciting current size
CmaxThe phase-shift value that makes the 1st iron leg oxysome correspondence is at 0～
CmaxBetween change.
Secondly, by i (the phase-shift value of iron leg oxysome correspondence of 2≤i≤n)
iThe following relational expression that should satisfy is determined the phase-shift value of all the other n-1 sections and the size of n:
cmax+
2+
3+Λ+
n-1+
n≥360 (2)
n＜360 (3)
Annotate: the variable unit's degree of being in the above relational expression
At
CmaxUnder the given condition of δ , can determine the minimum value of n as follows:
By (1) Shi Kede:
i≤2
i-2(
cmax+δ)i＝2，3，4，Λ，n-1，n (4)
Can get by (4) and (2):
cmax+(2
n-1)(
cmax+δ)≥360 (5)
By (5) formula, can obtain asking for the relational expression of minimum n value:
Choose n by the minimum value that (6) formula is determined, can guarantee that phase shifter is minimum at the segments that satisfies under the phase shifting accuracy prerequisite.
After n determines, by the definite any one group of of the requirement of (1) (2), (3) formula
iAll can guarantee the phase shift of phase shifter realization high accuracy.
Magnetic flux type of the present invention excitation and the saturated digital excitation method that the single magnetic flux type excitation of the method that improves phase shifting accuracy and common employing or saturated digital incentive program improve phase shifting accuracy that combines is compared, and has following technical characterictic:
1. compare with magnetic flux type excitation phase shifter, owing to be 0～ only to phase shift range
CmaxThe ferrite section carry out magnetic flux type excitation, for identical pulse current variable quantity, the present invention the theoretical variable quantity of corresponding phase shifter phase shift be about the of magnetic flux excitation formula phase shifter
Cmax/ 360 ° of (
CmaxThis value only is 1/16 in the time of=22.5 °).This shows that the present invention can improve phase shifting accuracy, and can more easily realize the high accuracy phase shift;
2. compare with saturated digital excitation phase shifter, though structurally increased by an iron leg oxysome, but the minimal segment ferrite length basically identical of the saturated digital excitation phase shifter of its length and n-1 position, and superpose by phase shift, length dimension to each iron leg oxysome requires obviously to relax, therefore, and can be under the prerequisite that does not increase switching time, not only reduce manufacture difficulty, and realize the unapproachable high accuracy phase shift of saturated digital incentive program;
3. the ferrite phase shifter of using method of the present invention and being obtained, numerical control phase shifting accuracy is the highest can reach for it＜and 1 °.
Description of drawings
Fig. 1: with the ferrite phase shifter structural representation of made of the present invention
Fig. 2: phase shifter digital-control circuit output block diagram
Fig. 3 (a): the remanent magnetism point on the saturated digital when excitation magnetic hysteresis loop
Fig. 3 (b): saturated digital when excitation O point correspondence electric current
Fig. 3 (c): saturated digital when excitation E point correspondence electric current
Fig. 4 (a): the remanent magnetism point during the magnetic flux type excitation on the magnetic hysteresis loop
Fig. 4 (b): the corresponding electric current of O point during the magnetic flux type excitation
Fig. 4 (c): E during the magnetic flux type excitation
1The electric current that point is corresponding
Fig. 4 (d): E during the magnetic flux type excitation
2The electric current that point is corresponding
Fig. 4 (e): E during the magnetic flux type excitation
mThe electric current that point is corresponding
Fig. 4 (f): the corresponding electric current of E point during the magnetic flux type excitation
Fig. 5: " phase-shift value reduces " schematic diagram
Embodiment
Phase shift precision of the present invention is mainly by the decision of magnetic flux excitation ferrite section, as the maximum phase-shift value of this section
CmaxAfter determining, the phase-shift value of saturated digital excitation ferrite section
iWith hop count n many group values can be arranged.The phase shifter of the value group correspondence that these are different all can satisfy the phase shift required precision.In the phase shifter of reality, n is more little for segments, and the structure of phase shifter is simple more, manufacture difficulty is low more.Therefore, under the impregnable prerequisite of phase shift precision, have only n is selected on the smallest point in the span, just can make the design of phase shifter be in the best.
Embodiment one:
The maximum stepping amount of desired phase shift δ =1 °.
Maximum phase-shift value when the 1st iron leg oxysome that adopts the magnetic flux type excitation
CmaxIn the time of=30 °, above-mentioned phase shifting accuracy requires and can be satisfied.
According to relational expression
The minimum value of determining n is 4.54, and it is 5 that n is rounded, and promptly needs five iron leg oxysomes;
Can determine the phase shift nominal value of each iron leg oxysome of all the other 4 sections saturated digital excitations according to relational expression (1), (2), (3)
iBe followed successively by 25 °, 51.3 °, 94 °, 184.5 °.
The structure of present embodiment phase shifter as shown in Figure 1.The maximum phase-shift value of 1 expression wherein is 30 ° a ferrite core rod, and this section ring rod magnetizes by the magnetic flux type energisation mode.2,3,4,5 is the ferrite core rod that is uneven in length, and is used for producing 25 °, 51.3 °, 94 °, 184.5 ° four phase-shift value respectively.Five iron leg oxysome ring rods are vertical along waveguide, i.e. after the direction of ripple propagation closely links to each other successively, load on the lateral mid-point of rectangular waveguide 6.7,8,9,10,11 represent to pass the thin wire that encircles rod 1,2,3,4,5 respectively among the figure, the two ends of these thin wires pass outside the waveguide by the lead-in wire groove of the ferrite core plane rod end that passed separately and the fairlead of waveguide sidewalls, link to each other with drive circuit corresponding output end shown in Figure 2 respectively.Among Fig. 16 represents metal waveguide, and 12 expressions load on the dielectric material between jayrator transmission line and the standard waveguide mouth.These dielectric materials constitute impedance transformer network with the waveguide that it loaded, to realize the impedance matching of phase shifter transmission line and external transmission line.
According to the method that magnetic flux type excitation of the present invention combines with saturated digital excitation, the phase shift process of each iron leg oxysome ring rod is as follows:
At first, the phase shift system with ferrite core rod 2,3,4,5 is set at saturated digital excitation.These four sections ring rods are magnetized respectively by the pulse current that flows through in four section leads 8,9,10,11.When the negative-going pulse electric current that flows through in the lead shown in Fig. 3 (b), the remanent magnetization of ferrite core rod can be considered the reference point or the zero point of phase shift state corresponding to the O point (the negative sense remanent magnetism point of saturation magnetization attitude correspondence) on the magnetic hysteresis loop among Fig. 3 (a).When the direct impulse electric current that flows through in the ferrite core rod shown in Fig. 3 (c), corresponding remanent magnetization is corresponding to the point of the E among the figure (the forward remanent magnetism point of saturation magnetization attitude correspondence), and this point can be considered the phase shift point of phase shift state.If with the pulse of binary code " 0 " control negative current,, control the phase shift state of above-mentioned four iron leg oxysome ring rods with regard to available tetrad sign indicating number with the pulse of " 1 " control forward current.
Secondly, will encircle excellent 1 and carry out phase shift by the magnetic flux type energisation mode.When in encircling rod, flowing through the negative-going pulse electric current shown in Fig. 4 (b), the remanent magnetization of ferrite core rod is corresponding to the O point (the negative sense remanent magnetism point of saturation magnetization attitude correspondence) on the magnetic hysteresis loop among Fig. 4 (a), this point still is regarded as phase shift zero point, and corresponding electric current is commonly referred to as resetting current.When ring flow through in the rod shown in Fig. 4 (c), (d), (e), (f) the negative sense resetting current is arranged earlier, when again the direct impulse electric current that amplitude constantly increases being arranged, corresponding remanent magnetism point corresponds respectively to the E among Fig. 4 (a)
1, E
2..., E
m, a plurality of remanent magnetism points such as E.The forward current that these amplitudes do not wait is commonly referred to as set current.If control these different remanent magnetism attitudes with 7 binary codes, will produce 2 phase shift states.The phase-shift value of these phase shift state correspondences changes in 0～30 ° of scope.
With above two kinds of phase shift systems combination, control whole phase shifter with 7+4=11 position binary code.The corresponding relation of control code and phase-shift value is as follows:
As seen from the above, the phase-shift value of determining according to previous methods can make phase shift " phase-shift value reduces " phenomenon occur in ascending stepping process.The starting point of this phenomenon is not that " 0 " and magnetic flux type excitation ferrite segment control code occur during for " 0 " at saturated digital excitation ferrite segment control code all.As shown in Figure 5, can be in order to make phase-shift value by the normal stepping of required precision, must give up some state of a controls that have " phase-shift value reduces " phenomenon in phase shifter uses need not.When aforementioned (1), (2), when (3) relational expression is equation, " phase-shift value reduces " phenomenon then can not appear.
Table 1 is that the phase shift state verification result of gained took passages after two kinds of energisation modes combined among the embodiment one.Can find out that from table 1 embodiment one has realized the high accuracy of phase shift stepping amount＜1 °.
Table 1: embodiment one phase shifter phase shift state verification result (extracts)
| The numerical control binary code | Phase-shift value | The numerical control binary code | Phase-shift value | The numerical control binary code | Phase-shift value |
| 0000 0000000 | 0° | 0000 0011001 | 1 | 0000 0011010 | 1.1 |
| 0000 0011011 | 1.2 | 0000 0011100 | 1.3 | 0000 0011101 | 1.4 |
| 0000 0011110 | 1.4 | 0000 0011111 | 1.5 | 0000 0100000 | 1.6 |
| 0000 0100001 | 1.8 | 0000 0100010 | 2 | 0000 0100011 | 2.2 |
| 0000 0100100 | 2.4 | 0000 0100101 | 2.6 | 0000 0100110 | 2.8 |
| 0000 0100111 | 3 | 0000 0101000 | 3.2 | 0000 0101001 | 3.5 |
| 0000 0101010 | 4 | 0000 0101011 | 4.2 | 0000 0101100 | 4.5 |
| 0000 0101101 | 4.7 | 0000 0101110 | 5 | 0000 0101111 | 5.5 |
| 0000 0110000 | 5.7 | 0000 0110001 | 6 | 0000 0110010 | 6.5 |
| 0000 0110011 | 6.8 | 0000 0110100 | 7.1 | 0000 0110101 | 7.4 |
| 0000 0110110 | 8 | 0000 0110111 | 8.3 | 0000 0111000 | 8.6 |
| 0000 0111001 | 9 | 0000 0111010 | 9.5 | 0000 0111011 | 10 |
| 0000 0111100 | 10.5 | 0000 0111101 | 11 | 0000 0111110 | 11.5 |
| 0000 0111111 | 12 | 0000 1000000 | 12.6 | 0000 1000001 | 12.7 |
| 0000 1000010 | 13 | 0000 1000011 | 13.5 | 0000 1000100 | 14 |
| 0000 1000101 | 14.6 | 0000 1000110 | 15.5 | 0000 1000111 | 15.9 |
| 0000 1001000 | 16.6 | 0000 1001001 | 17 | 0000 1001010 | 17.9 |
| 0000 1001011 | 18.5 | 0000 1001100 | 19 | 0000 1001101 | 19.5 |
| 0000 1001110 | 20 | 0000 1001111 | 20.5 | 0000 1010000 | 21.2 |
| 0000 1010001 | 21.8 | 0000 1010010 | 22.2 | 0000 1010011 | 22.5 |
| 0000 1010100 | 23 | 0000 1010101 | 23.5 | 0000 1010110 | 23.8 |
| 0000 1010111 | 24.3 | 0000 1011000 | 24.7 | 0000 1011001 | 25 |
| 0000 1011010 | 25.4 | 0000 1011011 | 25.8 | 0000 1011100 | 26.2 |
| 0000 1011101 | 27 | 0000 1011110 | 27.3 | 0000 1011111 | 27.5 |
| 0000 1100000 | 28 | 0000 1100001 | 28.2 | … | … |
| 0000 1110001 | 29 | … | … | 0000 1111111 | 30 |
| 0001 0000000 * | 25 * | … | … | 0001 1100000 | 53 |
| … | … | 0010 0000000 * | 51.3 * | … | … |
| 0010 1100000 | 79 | … | … | 0100 0000000 * | 94 * |
| … | … | 0100 1100000 | 122 | … | … |
| 1000 0000000 * | 184.5 * | … | … | 1000 1100000 | 212.5 |
| … | … | 1111 1100000 | 382.8 |
Annotate: the state of band " * " is the starting point of " phase-shift value reduces " phenomenon in the table
The lateral dimension of phase shifter transmission line of the present invention, longitudinal size comprise that each segment length, drive circuit and impedance transformer network all adopt ripe already method to design.The characteristic parameter of the phase shifter of embodiment one is as follows:
Frequency range: 25～27GHz
Jayrator waveguide lateral dimension: 4 * 2.2mm
2
Ferrite core rod lateral dimension: 1.5 * 2.2mm
2
Encircle excellent centre bore lateral dimension: 0.2 * 0.8mm
2
Ferrite saturation magnetization: 4500Gs
4.5,4,6.5,13,25.5mm 5 iron leg oxysome length are respectively:
Maximum surge current: 4A
The maximum phase-shift value of 5 iron leg oxysomes is respectively:
30°、25°、51.3°、94°、184.5°
Binary system control code figure place: 11 (7 magnetic fluxs)
Phase shift stepping amount (phase shifting accuracy):＜1 °
Embodiment two:
The maximum stepping amount of desired phase shift δ =4 °.
Maximum phase-shift value when the 1st iron leg oxysome that adopts the magnetic flux type excitation
CmaxIn the time of=57 °, above-mentioned phase shifting accuracy requires and can be satisfied.
According to relational expression
The minimum value of determining n is 3.58, and it is 4 that n is rounded, and promptly needs four iron leg oxysomes;
Can determine the phase shift nominal value of each iron leg oxysome of all the other 3 sections saturated digital excitations according to relational expression (1), (2), (3)
iBe followed successively by 51 °, 96.4 °, 187.2 °.
Each iron leg oxysome phase shift stacked system of present embodiment is with embodiment one.Table 2 is that present embodiment phase shift state verification result takes passages, and shows phase shift stepping amount≤4 ° from table 2 data.
Table 2: embodiment two phase shifter phase shift state verification results (extracts)
| The numerical control binary code | Phase-shift value | The numerical control binary code | Phase-shift value | The numerical control binary code | Phase-shift value |
| 000 00100 | 1.8 | 000 00101 | 2.8 | 000 00110 | 4.6 |
| 000 00111 | 6.4 | 000 01000 | 8 | 000 01001 | 10.5 |
| 000 01010 | 13.5 | 000 01011 | 16 | 000 01100 | 19 |
| 000 01101 | 23 | 000 01110 | 26.5 | 000 01111 | 30 |
| 000 10000 | 33.5 | 000 10001 | 36 | 000 10010 | 39.5 |
| 000 10011 | 42 | 000 10100 | 44 | 000 10101 | 46 |
| 000 10110 | 48 | 000 10111 | 49.8 | 000 11000 | 51 |
| 000 11001 | 52 | 000 11010 | 53 | 000 11011 | 55 |
| 000 11100 | 55.6 | 000 11101 | 56.1 | 000 11110 | 56.7 |
| 000 11111 | 57 | 001 00000 * | 51 * | … | … |
| 001 00111 | 57.5 | … | … | 001 11111 | 107.3 |
| 010 00000 * | 96.4 * | … | … | 011 11111 | 204 |
| 100 00000 * | 187.2 * | … | … | 111 11111 | 391.4 |
Annotate: the state of band " * " is the starting point of " phase-shift value reduces " phenomenon in the table
The high accuracy phase shifter characteristic parameter that embodiment two makes at millimeter wave frequency band is as follows:
Frequency range: 33～35GHz
Jayrator waveguide lateral dimension: 3.4 * 1.8mm
2
Ferrite core rod lateral dimension: 1.2 * 1.8mm
2
Encircle excellent centre bore lateral dimension: 0.2 * 0.8mm
2
Ferrite saturation magnetization: 4500Gs
7.5,7.0,14,27mm 4 iron leg oxysome length are respectively:
Maximum surge current: 4A
The maximum phase-shift value of 4 iron leg oxysomes is respectively:
57°、51°、96.4°、187.2°
Binary system control code figure place: 8 (5 magnetic fluxs)
Phase shift stepping amount (phase shifting accuracy) :≤4 °
Embodiment three:
The maximum stepping amount of desired phase shift δ =1 °.
Maximum phase-shift value when the 1st iron leg oxysome that adopts the magnetic flux type excitation
CmaxIn the time of=30 °, above-mentioned phase shifting accuracy requires and can be satisfied.
According to relational expression
The minimum value of determining n is 4.54, and it is 5 that n is rounded, and promptly needs five iron leg oxysomes;
Can determine the phase shift nominal value of each iron leg oxysome of all the other 4 sections saturated digital excitations according to relational expression (1), (2), (3)
iBe followed successively by 30 °, 60 °, 110 °, 160 °.
Each iron leg oxysome phase shift stacked system of present embodiment is with embodiment one.
Present embodiment phase shifting accuracy test result is: phase shift stepping amount＜1 °
On the phase shifter engineering, when the saturated digital energisation mode of independent use, for four saturated digital phase shifters, the theoretical nominal value of each section is necessary for 22.5 °, 45 °, 90 °, 180 °, in order to reach phase shifting accuracy preferably, this device has strict requirement to the phase-shift value of each iron leg oxysome---with the deviation of theoretical nominal value on average in ± 5 °.This makes that saturated digital phase shifter needs the length of each ferrite section is carried out meticulous adjusting in manufacturing process.By contrast, the phase shifter that the present invention forms then allows the length dimension of each iron leg oxysome to change in a big way, thereby manufacture difficulty is reduced.By embodiment one and embodiment three as can be seen, each section phase-shift value of determining by technical solution of the present invention allows to have bigger excursion.That is: 5 nominal values are respectively the phase shifter that 30 °, 25 °, 51.3 °, 94 °, 184.5 ° phase shifter and 5 nominal values be respectively 30 °, 30 °, 60 °, 110 °, 160 ° and all can realize high-precision numerical control phase shift function.
Claims (3)
1. a ferrite phase shifter is realized the method for high accuracy phase shift, the digital control scheme that adopts the magnetic flux type excitation to combine with saturated digital excitation, satisfy microwave high-frequency phase shifter high accuracy phase shift requirement, the ferrite that it will load on waveguide core is divided into the n section along direction of wave travel, n 〉=2; Its 1st section is adopted the magnetic flux type excitation, and all the other n-1 sections adopt saturated digital excitation; Then, magnetic flux type activation fragment phase-shift value and each saturation activation section phase-shift value are superposeed, make phase shifter in, realized the high accuracy phase shift by the phase shift stepping amount of magnetic flux type activation fragment more than or equal to 360 ° of scopes.
2. realize the method for high accuracy phase shift according to the described ferrite phase shifter of claim, it is characterized in that: pairing phase-shift value of each iron leg oxysome and number of fragments n determine as follows:
1), sets the maximum phase-shift value of the 1st section magnetic flux type excitation ferrite according to the maximum stepping amount of required phase shift δ
Cmax, the phase-shift value that makes the 1st iron leg oxysome correspondence is at 0～
CmaxBetween change by stepping amount δ ;
2) at
CmaxUnder the given condition of δ , by as shown in the formula the minimum value of determining n:
N 〉=2 also round
3) at the maximum phase-shift value of magnetic flux type excitation ferrite section
CmaxAfter determining, the phase shift nominal value of saturated digital each section of excitation ferrite
iDetermine in the following relationship:
i≤
i-1+
i-2+Λ+
2+
cmax+δ i＝2，3，4，Λ，n-1，n
cmax+
2+
3+Λ+
n-1+
n≥360
n＜360
3. realize the method for high accuracy phase shift according to claim 1,2 described ferrite phase shifters, it is characterized in that: described magnetic flux type activation fragment and each saturated digital activation fragment phase-shift value superpose according to the following procedure:
1) with the binary code Control current pulse of n-1 position n-1 iron leg oxysome is carried out saturated digital excitation;
2) with the binary code Control current pulse of m position the first iron leg oxysome is carried out the magnetic flux type excitation, make phase shifter by the stepping amount stepping that is no more than δ , at 0 °～
CmaxBetween produce 2
mIndividual phase shift state;
3),, can produce 2 with m+n-1 position binary code control phase shifter with above-mentioned two kinds of phase shift systems combination
M+n-1Individual phase shift state, in described phase shift state, in the 360 ° of scopes maximum stepping amount found out is no more than the phase shift state of δ , to realize the high accuracy phase shift.
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| CN101587988B (en) * | 2009-05-25 | 2013-03-06 | 中国兵器工业第二0六研究所 | Method for selecting 'zero phase shift remanence operating point' of magnetic flux excitation ferrite phase shifter |
| CN105356015A (en) * | 2015-08-11 | 2016-02-24 | 西北核技术研究所 | Ferrite phase shifter used for X waveband |
| CN107994881A (en) * | 2017-12-19 | 2018-05-04 | 南京国睿微波器件有限公司 | 4-digit number formula ferrite phase shifter drive circuit and control method |
| CN109379316A (en) * | 2018-10-09 | 2019-02-22 | 西安电子工程研究所 | A kind of implementation method of programmable ferrite width phase modulation control circuit |
| CN110277609A (en) * | 2019-06-03 | 2019-09-24 | 北京神舟博远科技有限公司 | A kind of plasma filled waveguide phase shifter |
| CN115498380A (en) * | 2022-08-19 | 2022-12-20 | 西南应用磁学研究所(中国电子科技集团公司第九研究所) | Independent excitation method for differential phase shift ferrite lock switch |
| CN115498381A (en) * | 2022-08-19 | 2022-12-20 | 西南应用磁学研究所(中国电子科技集团公司第九研究所) | Series excitation method for differential phase shift ferrite lock type switch |
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| FR1526056A (en) * | 1967-03-20 | 1968-05-24 | Csf | Two-way ferrite phase shifter |
| JPS5761301A (en) * | 1980-09-30 | 1982-04-13 | Nec Corp | Waveguide type phase shifter |
| US4445099A (en) * | 1981-11-20 | 1984-04-24 | Rca Corporation | Digital gyromagnetic phase shifter |
| US4564824A (en) * | 1984-03-30 | 1986-01-14 | Microwave Applications Group | Adjustable-phase-power divider apparatus |
| JPH0492501A (en) * | 1990-08-08 | 1992-03-25 | Toshiba Corp | Waveguide type ferrite phase shifter |
| JP4092501B2 (en) * | 2003-10-27 | 2008-05-28 | 株式会社Ｉｎａｘ | Thin remote control device using wireless tag switch |
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| CN101557024B (en) * | 2009-05-20 | 2012-05-30 | 电子科技大学 | Stripline-style ferrite phase shifter based on LTCC technology |
| CN101587988B (en) * | 2009-05-25 | 2013-03-06 | 中国兵器工业第二0六研究所 | Method for selecting 'zero phase shift remanence operating point' of magnetic flux excitation ferrite phase shifter |
| CN105356015A (en) * | 2015-08-11 | 2016-02-24 | 西北核技术研究所 | Ferrite phase shifter used for X waveband |
| CN105356015B (en) * | 2015-08-11 | 2019-07-19 | 西北核技术研究所 | A kind of ferrite phase shifter for X-band |
| CN107994881A (en) * | 2017-12-19 | 2018-05-04 | 南京国睿微波器件有限公司 | 4-digit number formula ferrite phase shifter drive circuit and control method |
| CN109379316A (en) * | 2018-10-09 | 2019-02-22 | 西安电子工程研究所 | A kind of implementation method of programmable ferrite width phase modulation control circuit |
| CN109379316B (en) * | 2018-10-09 | 2021-06-08 | 西安电子工程研究所 | Programmable ferrite amplitude and phase modulator control circuit implementation method |
| CN110277609A (en) * | 2019-06-03 | 2019-09-24 | 北京神舟博远科技有限公司 | A kind of plasma filled waveguide phase shifter |
| CN115498380A (en) * | 2022-08-19 | 2022-12-20 | 西南应用磁学研究所(中国电子科技集团公司第九研究所) | Independent excitation method for differential phase shift ferrite lock switch |
| CN115498381A (en) * | 2022-08-19 | 2022-12-20 | 西南应用磁学研究所(中国电子科技集团公司第九研究所) | Series excitation method for differential phase shift ferrite lock type switch |
| CN115498381B (en) * | 2022-08-19 | 2024-01-16 | 西南应用磁学研究所(中国电子科技集团公司第九研究所) | Differential phase shift ferrite lock type switch series excitation method |
| CN115498380B (en) * | 2022-08-19 | 2024-01-16 | 西南应用磁学研究所(中国电子科技集团公司第九研究所) | Differential phase shift ferrite lock type switch individual excitation method |
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