[go: up one dir, main page]

CN212967601U - Quasi-optical transmission device capable of adjusting microwave incident angle - Google Patents

Quasi-optical transmission device capable of adjusting microwave incident angle Download PDF

Info

Publication number
CN212967601U
CN212967601U CN202021462405.4U CN202021462405U CN212967601U CN 212967601 U CN212967601 U CN 212967601U CN 202021462405 U CN202021462405 U CN 202021462405U CN 212967601 U CN212967601 U CN 212967601U
Authority
CN
China
Prior art keywords
vacuum chamber
flange
quasi
transmission device
optical transmission
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn - After Issue
Application number
CN202021462405.4U
Other languages
Chinese (zh)
Inventor
施培万
钟武律
石中兵
杨曾辰
闻杰
佟瑞海
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Southwestern Institute of Physics
Original Assignee
Southwestern Institute of Physics
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Southwestern Institute of Physics filed Critical Southwestern Institute of Physics
Priority to CN202021462405.4U priority Critical patent/CN212967601U/en
Application granted granted Critical
Publication of CN212967601U publication Critical patent/CN212967601U/en
Withdrawn - After Issue legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Aerials With Secondary Devices (AREA)

Abstract

本实用新型属于受控核聚变等离子体诊断技术领域,具体涉及一种可调节微波入射角度的准光学传输装置,包括:高斯透镜、真空腔、椭球镜、法兰A、法兰B、盲板、金属杆、平面镜、密封法兰、螺杆和步进电机;本装置通过高斯透镜调节微波束腰以减少微波传输损耗;通过调整平面镜倾斜度从而实现不同角度的微波入射。

Figure 202021462405

The utility model belongs to the technical field of controlled nuclear fusion plasma diagnosis, in particular to a quasi-optical transmission device capable of adjusting the incident angle of microwaves, comprising: a Gaussian lens, a vacuum cavity, an ellipsoid mirror, a flange A, a flange B, a blind Plate, metal rod, plane mirror, sealing flange, screw and stepping motor; the device adjusts the microwave beam waist through Gaussian lens to reduce microwave transmission loss; adjusts the inclination of the plane mirror to achieve microwave incidence at different angles.

Figure 202021462405

Description

Quasi-optical transmission device capable of adjusting microwave incident angle
Technical Field
The utility model belongs to the technical field of the controlled nuclear fusion plasma diagnosis, concretely relates to quasi-optical transmission device of adjustable microwave incident angle.
Background
Controlled nuclear fusion is very likely to be one of the ultimate approaches to thoroughly solve the human energy problem. However, there are macroscopic and microscopic instabilities in magnetically confined plasmas, which are a great challenge for tokomak devices to maintain long-term steady state operation. In order to deeply analyze the basic characteristics of the magnetofluid instability and the relevant excitation dependent parameters thereof, the microwave reflectometer becomes an important diagnosis for carrying out magnetofluid instability measurement on a great logarithm Tokamak device due to the sensitivity and the characteristic of no disturbance to plasma. Generally, microwave reflectometers can be classified into conventional reflectometers and doppler reflectometers according to the microwave angle of the incident plasma. The two reflectometers are the biggest difference in that the microwave is incident on the plasma at different angles; the microwave emitted by the conventional reflectometer is vertical to the incidence of the plasma, namely the incidence angle is 0; the Doppler reflectometer is injected into the plasma at a certain angle delta, and the relation between the incident angle and the turbulent wave number and incident wave number satisfies kt=kisin (δ), it follows that the ability of doppler to measure turbulence is limited by the angle of incidence when the frequency of the microwaves is fixed. To achieve a beam with angular incidence, a common approach is to mount the doppler reflectometer at a position offset from the midplane. Conventional reflectometers are more sensitive to macroscopic instabilities, such as high energy particle modes, while doppler is more used for measurement of micro-turbulence. The two types of reflectometers are installed at different positions to meet the physical measurement requirements, but in the existing and future tokamak devices, the diagnosis window is extremely limited, so that effective measures must be taken to enable microwaves to enter plasma at different angles and to maximize the measurement capability of the reflectometers for turbulence of different characteristic dimensions.
Therefore, it is necessary to design a quasi-optical transmission device capable of adjusting the microwave incidence angle, so as to realize free switching between a conventional reflectometer and a doppler system by adjusting the microwave incidence angle, and realize turbulence measurement of different wave numbers.
SUMMERY OF THE UTILITY MODEL
The utility model aims at designing an adjustable microwave incident angle's quasi-optical transmission device, realize the free switching of conventional reflectometer and Doppler system through adjusting microwave incident angle for it is limited because of the diagnosis window in current and future tokamak device to solve, and inconvenient two kinds of reflectometers of installing simultaneously carry out the problem that magnetic current body instability measures diagnosis.
The technical scheme of the utility model:
a quasi-optical transmission device capable of adjusting the incident angle of microwave comprises a Gaussian lens, a vacuum cavity, an ellipsoidal mirror, a flange A, a flange B, a blind plate, a metal rod, a plane mirror, a sealing flange, a screw rod and a stepping motor;
a Gaussian lens is arranged at one end outside the vacuum cavity; a blind plate is fixed at the other end outside the vacuum cavity through a flange B;
the vacuum cavity is also provided with a screw rod, one end of the screw rod is arranged inside the vacuum cavity and connected with the plane mirror, and the other end of the screw rod is arranged outside the vacuum cavity and sequentially connected with a sealing flange and a stepping motor in series;
the metal rod is arranged in the vacuum cavity, and one end of the metal rod is connected with the plane mirror; the other end of the metal rod is connected with a blind plate;
the ellipsoidal mirror is fixed in the vacuum cavity;
the flange A is arranged outside the vacuum cavity and connected with the Tokamak vacuum chamber.
The vacuum cavity is integrally of a hollow L-shaped structure, and microwaves are emitted into the vacuum cavity through the Gaussian lens and then are emitted onto the ellipsoidal mirror.
The ellipsoidal mirror is fixed at the right-angle corner position in the vacuum cavity and can receive the microwave injected through the Gaussian lens;
the ellipsoidal mirror is also arranged in parallel with the plane mirror in the vacuum cavity, and the microwave reflected by the ellipsoidal mirror can be vertically emitted onto the plane mirror.
The flange A is arranged outside the vacuum cavity, the height of the flange A is the same as that of the position of the plane mirror arranged inside the vacuum cavity, and the microwave energy reflected by the plane mirror can be emitted into the Tokamak vacuum chamber through the flange A.
The integral structure of the flange A is an elliptical ring-shaped structure.
The whole vacuum cavity is made of stainless steel with low magnetic conductivity, one end of the sealing flange is fixed on the outer wall of the vacuum cavity, and the other end of the sealing flange is fixedly connected with the stepping motor.
The utility model has the advantages that:
the device designed by the utility model adjusts the microwave beam waist through the Gaussian lens to reduce the microwave transmission loss; microwave incidence at different angles is realized by adjusting the inclination of the second reflecting surface; the microwave device is protected by directly connecting the transmission device with the vacuum chamber; the utility model discloses still have following advantage: the device can flexibly adjust the incident angle of the microwave by controlling the parameters of the stepping motor; the quasi-optical transmission device is integrally connected with the vacuum chamber through a runway-type flange, the flange of the device is not sealed by a lens, and the sealed lens is at the rear end and cannot be polluted by plasma. The incident angle of the microwave is adjusted, so that the free switching between a conventional reflectometer and a Doppler system can be realized, and turbulence measurement on different wave numbers can be realized.
Drawings
Fig. 1 is a schematic structural view of a quasi-optical transmission device capable of adjusting an incident angle of microwave according to the present invention;
wherein: 1-gauss lens, 2-vacuum cavity, 3-ellipsoidal mirror, 4-flange A, 5-flange B, 6-blind plate, 7-metal rod, 8-plane mirror, 9-sealing flange, 10-screw rod and 11-stepping motor
Detailed Description
The invention will be further described with reference to the following drawings and examples:
the device adjusts the microwave beam waist through the Gaussian lens to reduce the microwave transmission loss; microwave incidence at different angles is realized by adjusting the inclination of the second reflecting surface, namely the plane mirror; the microwave device is protected by connecting the transmission device directly to the tokamak vacuum chamber.
The specific embodiment is as follows: a quasi-optical transmission device capable of adjusting the incident angle of microwave comprises a Gaussian lens 1, a vacuum cavity 2, an ellipsoidal mirror 3, a flange A4, a flange B5, a blind plate 6, a metal rod 7, a plane mirror 8, a sealing flange 9, a screw rod 10 and a stepping motor 11;
wherein, a Gaussian lens 1 is arranged at one end outside the vacuum cavity 2; a blind flange 6 is fixed at the other end outside the vacuum cavity 2 through a flange B5; the vacuum cavity 2 is also provided with a screw rod 10, one end of the screw rod 10 is arranged inside the vacuum cavity 2 and is connected with the plane mirror 8, and the other end of the screw rod 10 is arranged outside the vacuum cavity 2 and is sequentially connected with a sealing flange 9 and a stepping motor 11 in series; the metal rod 7 is arranged in the vacuum cavity 2, and one end of the metal rod 7 is connected with the plane mirror 8; the other end of the metal rod 7 is connected with the blind plate 6;
the whole vacuum cavity 2 is of a hollow L-shaped structure, the whole vacuum cavity 2 is made of stainless steel with low magnetic conductivity, and microwaves are emitted into the vacuum cavity 2 through the Gaussian lens 1 and then are emitted onto the ellipsoidal mirror 3.
The ellipsoidal mirror 3 is fixed at the right-angle corner position inside the vacuum cavity 2 and can receive the microwave injected through the Gaussian lens 1; the ellipsoidal mirror 3 is also arranged in parallel with the plane mirror 8 in the vacuum chamber 2, and the microwave reflected by the ellipsoidal mirror 3 can be vertically incident on the plane mirror 8.
The flange A4 overall structure is oval ring shape structure, and flange A4 sets up in the outside of vacuum chamber 2, is connected with the tokamak vacuum chamber, and flange A4 sets up the position in the outside of vacuum chamber 2 and the position height that level mirror 8 set up in the inside of vacuum chamber 2 is the same, and the microwave energy after passing through level mirror 8 reflection penetrates into the tokamak vacuum chamber through flange A4.
One end of the sealing flange 9 is fixed on the outer wall of the vacuum cavity 2, and the other end of the sealing flange 9 is fixedly connected with the stepping motor 11.
The method for adjusting the angle of the quasi-optical transmission device capable of adjusting the microwave incidence angle comprises the following steps:
the method comprises the following steps: the microwave is emitted into the vacuum cavity 2 through the Gaussian lens 1, and is emitted into the ellipsoidal mirror 3 after being converged in the vacuum cavity 2;
step two: the microwave is reflected by the ellipsoidal mirror 3 and is emitted onto a plane mirror 8 supported by a metal rod 7, at the moment, a stepping motor 11 is switched on, and a screw 10 moves left and right in the horizontal direction of the vacuum cavity 2 through the movement of the stepping motor 11;
step three: the screw 10 moves left and right and simultaneously drives the plane mirror 8 to rotate slightly at the same frequency in the vacuum chamber 2, so that the microwave reflected to the plane mirror 8 is incident into the plasma in the tokamak vacuum chamber through the flange A4 at a certain angle.
The utility model discloses the device is passed through flange A4 and is directly connected with the real empty room of ask mark device, and thereby it is kept away from and is avoided being plated the chemical contamination by plasma as sealed lens, gauss lens 1.
The method for adjusting the incident reflection angle of the microwave designed by the device can be used in the existing and future magnetic confinement nuclear fusion experiments and engineering, and has important application value.
Wherein flange a4 is not lensed and not sealed, and is directly pierced; flange B5 is sealed without a lens and is directly sealed using blind plate 6.
The present invention has been described in detail with reference to the accompanying drawings and examples, but the present invention is not limited to the above examples, and various changes can be made without departing from the spirit of the present invention within the knowledge of those skilled in the art. The present invention can adopt the prior art for the content which is not described in detail in the present invention.

Claims (7)

1.一种可调节微波入射角度的准光学传输装置,其特征在于,包括:高斯透镜(1)、真空腔(2)、椭球镜(3)、法兰A(4)、法兰B(5)、盲板(6)、金属杆(7)、平面镜(8)、密封法兰(9)、螺杆(10)和步进电机(11);1. a quasi-optical transmission device with adjustable microwave incident angle, is characterized in that, comprises: Gaussian lens (1), vacuum cavity (2), ellipsoid mirror (3), flange A (4), flange B (5), a blind plate (6), a metal rod (7), a plane mirror (8), a sealing flange (9), a screw (10) and a stepping motor (11); 所述真空腔(2)外部一端安装高斯透镜(1);真空腔(2)外部的另一端通过法兰B(5)固定有盲板(6);A Gaussian lens (1) is installed at one end outside the vacuum chamber (2); a blind plate (6) is fixed at the other end outside the vacuum chamber (2) through a flange B (5); 所述真空腔(2)上还设置有螺杆(10),螺杆(10)的一端设置在真空腔(2)内部并连接平面镜(8),螺杆(10)的另一端设置在真空腔(2)外部并依次串接有密封法兰(9)和步进电机(11);The vacuum chamber (2) is also provided with a screw (10), one end of the screw (10) is arranged inside the vacuum chamber (2) and connected to the plane mirror (8), and the other end of the screw (10) is arranged in the vacuum chamber (2) ) are connected in series with a sealing flange (9) and a stepping motor (11) in sequence; 所述金属杆(7)设置在真空腔(2)内部,金属杆(7)的一端与平面镜(8)连接;金属杆(7)的另一端连接盲板(6);The metal rod (7) is arranged inside the vacuum chamber (2), and one end of the metal rod (7) is connected with the plane mirror (8); the other end of the metal rod (7) is connected with the blind plate (6); 所述椭球镜(3)固定在真空腔(2)内部;The ellipsoid mirror (3) is fixed inside the vacuum chamber (2); 所述法兰A(4)设置在真空腔(2)的外部,与托卡马克真空室相连接。The flange A (4) is arranged outside the vacuum chamber (2) and is connected with the tokamak vacuum chamber. 2.如权利要求1所述的一种可调节微波入射角度的准光学传输装置,其特征在于,所述真空腔(2)整体呈中空L型结构,微波通过高斯透镜(1)射入至真空腔(2)内部后,射入椭球镜(3)上。2. A quasi-optical transmission device capable of adjusting the incident angle of microwaves as claimed in claim 1, characterized in that the vacuum cavity (2) has a hollow L-shaped structure as a whole, and microwaves are injected into the vacuum chamber through a Gaussian lens (1). After the inside of the vacuum chamber (2), it is injected into the ellipsoid mirror (3). 3.如权利要求2所述的一种可调节微波入射角度的准光学传输装置,其特征在于:所述椭球镜(3)固定在真空腔(2)内部直角转角位置处,且可接收到通过高斯透镜(1)射入的微波。3. A quasi-optical transmission device with adjustable microwave incident angle as claimed in claim 2, characterized in that: the ellipsoid mirror (3) is fixed at a right-angle corner position inside the vacuum cavity (2), and can receive to the microwaves incident through the Gaussian lens (1). 4.如权利要求3所述的一种可调节微波入射角度的准光学传输装置,其特征在于:所述椭球镜(3)还与真空腔(2)内的平面镜(8)平行设置,且椭球镜(3)反射后的微波可垂直射入至平面镜(8)上。4. The quasi-optical transmission device with adjustable microwave incident angle as claimed in claim 3, characterized in that: the ellipsoid mirror (3) is also arranged in parallel with the plane mirror (8) in the vacuum cavity (2), And the microwave reflected by the ellipsoid mirror (3) can be vertically incident on the plane mirror (8). 5.如权利要求4所述的一种可调节微波入射角度的准光学传输装置,其特征在于:所述法兰A(4)设置在真空腔(2)外部,其在真空腔(2)外部设置位置与平面镜(8)设置在真空腔(2)内部的位置高度相同,且经过平面镜(8)反射后的微波能通过法兰A(4)射入托卡马克真空室内。5. A quasi-optical transmission device with adjustable microwave incident angle as claimed in claim 4, characterized in that: the flange A (4) is arranged outside the vacuum chamber (2), which is inside the vacuum chamber (2) The external setting position is at the same height as the plane mirror (8) inside the vacuum chamber (2), and the microwave energy reflected by the plane mirror (8) is injected into the tokamak vacuum chamber through the flange A (4). 6.如权利要求5所述的一种可调节微波入射角度的准光学传输装置,其特征在于:所述法兰A(4)整体结构呈椭圆圆环形结构。6 . The quasi-optical transmission device capable of adjusting the incident angle of microwaves according to claim 5 , wherein the overall structure of the flange A ( 4 ) is an elliptical annular structure. 7 . 7.如权利要求6所述的一种可调节微波入射角度的准光学传输装置,其特征在于:所述真空腔(2)整体为低磁导率不锈钢材质,所述密封法兰(9)的一端固定在真空腔(2)的外壁上,密封法兰(9)的另一端与步进电机(11)固定连接。7. The quasi-optical transmission device with adjustable microwave incident angle according to claim 6, characterized in that: the vacuum chamber (2) is made of stainless steel with low magnetic permeability as a whole, and the sealing flange (9) One end of the sealing flange (9) is fixed on the outer wall of the vacuum chamber (2), and the other end of the sealing flange (9) is fixedly connected with the stepping motor (11).
CN202021462405.4U 2020-07-23 2020-07-23 Quasi-optical transmission device capable of adjusting microwave incident angle Withdrawn - After Issue CN212967601U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202021462405.4U CN212967601U (en) 2020-07-23 2020-07-23 Quasi-optical transmission device capable of adjusting microwave incident angle

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202021462405.4U CN212967601U (en) 2020-07-23 2020-07-23 Quasi-optical transmission device capable of adjusting microwave incident angle

Publications (1)

Publication Number Publication Date
CN212967601U true CN212967601U (en) 2021-04-13

Family

ID=75396413

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202021462405.4U Withdrawn - After Issue CN212967601U (en) 2020-07-23 2020-07-23 Quasi-optical transmission device capable of adjusting microwave incident angle

Country Status (1)

Country Link
CN (1) CN212967601U (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111785606A (en) * 2020-07-23 2020-10-16 核工业西南物理研究院 A quasi-optical transmission device with adjustable microwave incident angle and its angle adjustment method

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111785606A (en) * 2020-07-23 2020-10-16 核工业西南物理研究院 A quasi-optical transmission device with adjustable microwave incident angle and its angle adjustment method
CN111785606B (en) * 2020-07-23 2024-07-16 核工业西南物理研究院 Quasi-optical transmission device capable of adjusting microwave incidence angle and angle modulation method thereof

Similar Documents

Publication Publication Date Title
CN212967601U (en) Quasi-optical transmission device capable of adjusting microwave incident angle
CN203672702U (en) Sample pond for solid ablation with laser
CN108093550A (en) A kind of new quick rotation high power electronic cyclotron wave transmitting antenna
CN109729633A (en) Linear Magnetic Confinement Plasma Device
CN111785606B (en) Quasi-optical transmission device capable of adjusting microwave incidence angle and angle modulation method thereof
CN111664816A (en) QTT antenna main reflection surface deformation detection method, correction method and detection device
CN108956360B (en) Magnetic suspension thermobalance based on photo-thermal rapid heating
Wang et al. Potential application of using vortex ring for personalized ventilation
CN206341469U (en) A kind of new quick rotation high power electronic cyclotron wave transmitting antenna
CN112903950A (en) Device suitable for high-temperature in-situ nondestructive testing of liquid metal battery
CN208589548U (en) A kind of circular waveguide leaky wave slot antenna based on TM01 mould
CN205657179U (en) Arrange microwave diagnostics antenna system in real empty room in
Kolemen et al. Real-time mirror steering for improved closed loop neoclassical tearing mode suppression by electron cyclotron current drive in DIII-D
CN114397085A (en) A vertical flow coupled gust generation system
CN114415312A (en) A lens barrel structure suitable for imaging with bright background
CN110052606A (en) Laser powder feeding additive manufacturing device and powder flow control method
Liu et al. Upgrade and application of the gas puff imaging system in EAST
CN115691837A (en) Tokamak plasma current profile on-line feedback control system and method
CN205726637U (en) The micro-burnt target of a kind of scanning
Yoshimura et al. Construction of 106G Hz ECH System on CHS
CN117393183A (en) A method for controlling the backflow of fuel particles at the plasma boundary using powder feedback injection
CN116631655B (en) Megawatt steady-state high-power conical water load
CN215004019U (en) Conical flow guiding device
CN106847652B (en) A kind of coaxial continuous wave Terahertz of gradual change tiltedly notes pipe
Yano et al. Improvement of field accuracy and plasma performance in the RT-1 device

Legal Events

Date Code Title Description
GR01 Patent grant
GR01 Patent grant
AV01 Patent right actively abandoned

Granted publication date: 20210413

Effective date of abandoning: 20240716

AV01 Patent right actively abandoned

Granted publication date: 20210413

Effective date of abandoning: 20240716

AV01 Patent right actively abandoned
AV01 Patent right actively abandoned