JPH07111448B2 - Microwave radiometer - Google Patents
Microwave radiometerInfo
- Publication number
- JPH07111448B2 JPH07111448B2 JP63133662A JP13366288A JPH07111448B2 JP H07111448 B2 JPH07111448 B2 JP H07111448B2 JP 63133662 A JP63133662 A JP 63133662A JP 13366288 A JP13366288 A JP 13366288A JP H07111448 B2 JPH07111448 B2 JP H07111448B2
- Authority
- JP
- Japan
- Prior art keywords
- primary radiator
- microwave radiometer
- divided
- radiometer
- array
- Prior art date
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- Expired - Lifetime
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Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は例えば人工衛星等に搭載するマイクロ波放射
計に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention relates to a microwave radiometer mounted on, for example, an artificial satellite.
第2図は,従来のマイクロ波放射計の構成を示す図であ
り,図において(1)は反射鏡,(4)はRF回路部,
(5)は受信部,(6)は信号処理部,(7)はスカイ
ホーンと呼ばれるホーンアンテナ,(8)は標準雑音
源,(9)は一次放射器である。FIG. 2 is a diagram showing a configuration of a conventional microwave radiometer, in which (1) is a reflecting mirror, (4) is an RF circuit section,
(5) is a receiving unit, (6) is a signal processing unit, (7) is a horn antenna called a sky horn, (8) is a standard noise source, and (9) is a primary radiator.
次に動作について説明する。反射鏡(1)を介して一次
放射器(9)より受信した入力雑音電波は,RF回路部
(4)を経由して,受信部(5)にて増幅,周波数変
換,検波されて入力雑音電波の雑音温度TMに対応した電
圧VMが得られる。この関係を第(1)式に示す。Next, the operation will be described. The input noise radio wave received from the primary radiator (9) via the reflecting mirror (1) is amplified, frequency-converted and detected by the receiving unit (5) via the RF circuit unit (4), and the input noise is received. A voltage V M corresponding to the noise temperature T M of the radio wave is obtained. This relationship is shown in equation (1).
VM=K・B・G・Cd・TM (1) ここでK:比例定数 B:帯域 G:受信機利得 Cd:検波感度 TM:入力雑音温度 第(1)式において,測定した雑音温度TMのかわりに既
知の雑音温度の雑音電波を与えて電圧VMを校正する事に
より,任意のVMに対応した入力雑音温度TMを求める事が
できる。したがつて通常の校正として雑音温度が既知の
スカイホーン(7)と,常温ダミーを用いた標準雑音源
(8)を,RF回路部(4)にて切り換える事によつて2
点校正を行つている。そして,得られた観測及び校正電
圧は信号処理部(6)にてA/D変換され地上に送信され
る。V M = K ・ B ・ G ・ C d・ T M (1) where K: proportional constant B: band G: receiver gain C d : detection sensitivity T M : input noise temperature Measured in equation (1) by calibrating the voltage V M giving noise electric wave of known noise temperature instead of the noise temperature T M that, it is possible to determine the input noise temperature T M corresponding to an arbitrary V M. Therefore, as a normal calibration, the sky horn (7) whose noise temperature is known and the standard noise source (8) using a room temperature dummy are switched by the RF circuit section (4).
Doing point calibration. Then, the obtained observation and calibration voltage is A / D converted by the signal processing unit (6) and transmitted to the ground.
ところで実際の放射計においては地上を走査する必要が
ある為,走査方法の一つとして第3図に示した様に,反
射鏡(1)に対向して,ビーム方向の異なる複数(図中
では8素子)の一次放射器のアレイ(10)を配置し各々
の一次放射器に接続されているスイツチ(3)によりRF
回路部(4)に接続する一次放射器を切り換える事によ
りビーム方向を変え地上を走査するスイツチングアンテ
ナを用いる場合がある。By the way, since it is necessary to scan the ground in an actual radiometer, as shown in FIG. 3 as one of the scanning methods, a plurality of different beam directions (in the figure, facing the reflecting mirror (1)) are used. An array (10) of primary radiators (8 elements) is placed and RF is provided by switches (3) connected to each primary radiator.
There is a case where a switching antenna for scanning the ground by changing the beam direction by switching the primary radiator connected to the circuit unit (4).
また一般にマイクロ波放射計の温度分解能△Tは第
(2)式にて表される。Further, the temperature resolution ΔT of the microwave radiometer is generally expressed by the equation (2).
ここでTA:入力雑音温度 TR:アンテナ給電系を含めた放射計総合雑音温度 B:周波数帯域 τ:受信機内部の積分器による積分時間 K:受信機方式により決る係数(デイツケ型の場合) 〔発明が解決しようとする課題〕 放射計の温度分解能は小さい程望ましい。しかし第
(2)式中でTRは受信機に使用する半導体素子の雑音指
数などの制約があり、またBは使用周波数によつて定め
られたガードバンドの制約がある。その為温度分解能を
改善するには積分時間τを長くする必要がある。 Where T A is the input noise temperature T R is the total noise temperature of the radiometer including the antenna feed system B is the frequency band τ is the integration time by the integrator inside the receiver K is the coefficient determined by the receiver method (in the case of the Daisuke type) [Problems to be solved by the invention] The smaller the temperature resolution of the radiometer, the more desirable. However, in the equation (2), T R has a constraint such as a noise figure of a semiconductor element used for the receiver, and B has a constraint of a guard band determined by the used frequency. Therefore, in order to improve the temperature resolution, it is necessary to lengthen the integration time τ.
ところが例えば人工衛星搭載用マイクロ波放射計におい
ては軌道条件により対地速度Vgが一定となる為第4図に
示すようにアンテナビームの地上におけるフツトプリン
ト(走査方向の長さx(13)X進行方向の長さy(1
2))に対して進行方向の重なり△y(14)を取るとす
ると,走査範囲l(11)が一定の場合走査周期Tが一定
となり,次式にて表される。However, for example, in a microwave radiometer mounted on an artificial satellite, the ground velocity V g is constant depending on the orbital conditions, so as shown in Fig. 4, the footprint of the antenna beam on the ground (scanning length x (13) X Direction length y (1
Assuming that the overlap Δy (14) in the traveling direction is taken with respect to 2)), the scanning period T becomes constant when the scanning range l (11) is constant, and is represented by the following equation.
ここでA:進行方向ビーム中心間距離(16) y:ビームスポツトの進行方向の長さ(12) △y:ビームスポツトの進行方向の重り(14) Vg:衛星対地速度 またこの時積分時間τは次の第(4)式にて表される。 Where A: distance between beam centers in the direction of travel (16) y: length in the direction of travel of the beam spot (12) △ y: weight in the direction of travel of the beam spot (14) V g : satellite ground speed Also, the integration time at this time τ is expressed by the following equation (4).
ここでB:走査方向ビーム中心間距離(17) x:ビームスポツトの走査方向の長さ(13) △x:ビームスポツトの走査方向の重り(15) l:走査範囲(11) T:走査周期 ここで走査範囲l(11)及び走査周期Tが一定である
為,積分時間τを長くすると走査方向のビーム中心距離
B(17)が長くなり最終的にはビームスポツトのアンダ
ーラツプが発生し放射計の距離分解能が劣化する。 Where B: distance between beam centers in scanning direction (17) x: length of beam spot in scanning direction (13) Δx: weight of beam spot in scanning direction (15) l: scanning range (11) T: scanning period Since the scanning range 1 (11) and the scanning period T are constant, if the integration time τ is lengthened, the beam center distance B (17) in the scanning direction becomes longer, and eventually an underlap of the beam spot occurs and the radiometer The distance resolution of is degraded.
この為,温度分解能と距離分解能が相反する問題点があ
つた。Therefore, there is a problem that the temperature resolution and the distance resolution conflict with each other.
この発明は前述の問題点を解消する為になされたもので
距離分解能(走査方向ビーム中心間距離B(17)を一定
に保つたまま温度分解能(積分時間)を改善できるマイ
クロ波放射計を得る事を目的とする。The present invention has been made in order to solve the above-mentioned problems, and provides a microwave radiometer capable of improving temperature resolution (integration time) while keeping the distance B (17) between beam centers in the scanning direction constant. To aim for things.
この発明に係るマイクロ波放射計は,複数の一次放射器
で構成されるアレイ(2)を数組に分割し,その1組ず
つ各々にRF回路部(4),受信部(5)及び校正源を設
けたものである。In the microwave radiometer according to the present invention, an array (2) composed of a plurality of primary radiators is divided into several sets, and an RF circuit section (4), a receiving section (5) and a calibration are provided for each set. It has a source.
この発明のマイクロ波放射計においては,例えば一次放
射器アレイ(2)をn組に等分割した場合,対地速度そ
の他が分割前と同一とする。1組のアレイが走査する走
査範囲はもとの走査範囲の1/nとなる。その結果同一の
ビームスポツトを受信機が積分する時間はn倍となり温
度分解能△Tは だけ改善される。In the microwave radiometer of the present invention, for example, when the primary radiator array (2) is equally divided into n sets, the ground speed and the like are the same as before the division. The scanning range scanned by one set of arrays is 1 / n of the original scanning range. As a result, the time required for the receiver to integrate the same beam spot is n times, and the temperature resolution ΔT is Only improved.
以下この発明の一実施例を図について説明を行う。 An embodiment of the present invention will be described below with reference to the drawings.
ここでは例として第3図に示したスイツチングアンテナ
方式の放射計において,一次放射器アレイ(10)(8素
子)を,4素子ずつ2等分したものを第1図に示す。As an example, FIG. 1 shows, as an example, the switching antenna type radiometer shown in FIG. 3 in which the primary radiator array (10) (8 elements) is divided into four equal parts.
第1図において,(1)は反射鏡,(2)は分割した一
次放射器アレイ,(3)は切り換えスイツチ,(4)は
RF回路部,(5)は受信部,(6)は信号処理部,
(7)はスカイホーン,(8)は標準雑音源である。In FIG. 1, (1) is a reflecting mirror, (2) is a divided primary radiator array, (3) is a switching switch, and (4) is
RF circuit section, (5) receiver section, (6) signal processing section,
(7) is a sky horn, and (8) is a standard noise source.
その他の衛星対地速度Vgアンテナビーム幅,走査範囲l
等の条件はこの発明による放射計も従来の放射計も全て
同一とする。この時,この発明のマイクロ波放射計にお
いては一次放射器アレイ(8素子)が2分割されて4素
子ずつとなつている為,各アレイに対応する地上のビー
ムスポツトは第4図における右4つ及び左4つに分割さ
れる。衛星対地速度Vg及びビーム幅が一定である為,本
放射計を用いた場合走査周期は従来と同様となる。一方
走査範囲は分割した一次放射器アレイ1つに対し従来の
走査範囲l(11)の1/2となる。この発明の放射計の構
成では分割した一次放射器アレイ1つに対し一つ受信部
(積分器)(5)が接続されている為それぞれの受信部
(積分器)(5)の積分時間τ′は次の式で表される。Other satellite ground speed V g Antenna beam width, scanning range l
The same conditions apply to the radiometer according to the present invention and the conventional radiometer. At this time, in the microwave radiometer of the present invention, since the primary radiator array (8 elements) is divided into two to form four elements, the beam spot on the ground corresponding to each array is the right 4 in FIG. And left four. Since the satellite ground speed V g and the beam width are constant, the scanning cycle is the same as before when this radiometer is used. On the other hand, the scanning range is 1/2 of the conventional scanning range l (11) for one divided primary radiator array. In the structure of the radiometer of the present invention, since one receiving unit (integrator) (5) is connected to one divided primary radiator array, the integration time τ of each receiving unit (integrator) (5) is ′ Is expressed by the following equation.
これにより分割した場合の一つのビームスポツトに対す
る積分時間は従来のものの2倍となる。これよりこの発
明による温度分解能△T′は第(2)式より次のように
なる。 As a result, the integration time for one beam spot when divided is twice as long as the conventional one. From this, the temperature resolution ΔT 'according to the present invention is as follows from the equation (2).
この結果,この発明を用いる事により,温度分解能△T
は従来の放射計に比べ だけ改善される。 As a result, by using the present invention, the temperature resolution ΔT
Compared to conventional radiometers Only improved.
なお本実施例では2等分の場合を示したが,同様にアレ
イをn等分し,n系統の受信部(積分器)を用いた場合も
温度分解能は従来の 倍だけ改善される。In the present embodiment, the case where the array is divided into two equal parts is shown. Similarly, when the array is equally divided into n parts and n system receivers (integrators) are used, the temperature resolution is the same as that of the conventional one. Only doubled.
またアレイを等分割せずに適当な比率で分割した場合も
総合ではそれに対応した温度分解能の改善効果が得られ
る。Further, when the array is not divided into equal parts but divided into an appropriate ratio, the effect of improving the temperature resolution corresponding to the total is obtained.
またアンテナはスイツチングアンテナでなくとも同様の
構成で走査範囲の分割が可能であれば分解したアンテナ
の各々に受信部(積分器)を接続する事により,同様の
改善効果が得られる。Even if the antenna is not a switching antenna, the same improvement effect can be obtained by connecting a receiving unit (integrator) to each of the disassembled antennas if the scanning range can be divided with the same configuration.
以上の様に,この発明によれば,マイクロ波放射計のス
イツチングアンテナの一次放射器アレイを分割し,その
各々に受信部(積分器)を設ける事によつて一定の距離
分解能を確保した上で,温度分解能が改善できる効果が
ある。As described above, according to the present invention, the primary radiator array of the switching antenna of the microwave radiometer is divided, and the receiving portion (integrator) is provided in each of them, so that a certain range resolution is secured. Above, there is an effect that the temperature resolution can be improved.
第1図はこの発明の一実施例によるマイクロ波放射計を
示すブロツク図,第2図は従来のマイクロ波放射計のブ
ロツク図,第3図はスイツチングアンテナ方式のマイク
ロ波放射計のブロツク図,第4図はマイクロ波放射計の
地上のフツトプリントの説明図である。 図中(1)は反射鏡,(2)は分割した一次放射器アレ
イ,(3)は切り換えスイツチ,(4)はRF回路部,
(5)は受信部,(6)は信号処理部,(7)はスカイ
ホーン,(8)は標準雑音源,(9)は一次放射器,
(10)は一次放射器アレイ,(11)は走査範囲l,(12)
はビームスポツトの進行方向の長さy,(13)はビームス
ポツトの走査方向の長さx,(14)はビームスポツトの進
行方向重り△y,(15)はビームスポツトの走査方向の重
り△x,(16)は進行方向のビームスポツト中心間距離A,
(17)は走査方向のブームスポツト中心間距離Bを示
す。 なお図中,同一符号は同一又は相当部分を示す。1 is a block diagram showing a microwave radiometer according to an embodiment of the present invention, FIG. 2 is a block diagram of a conventional microwave radiometer, and FIG. 3 is a block diagram of a microwave radiometer of a switching antenna system. , Fig. 4 is an illustration of the ground print of the microwave radiometer. In the figure, (1) is a reflecting mirror, (2) is a divided primary radiator array, (3) is a switching switch, (4) is an RF circuit section,
(5) is a receiving unit, (6) is a signal processing unit, (7) is a sky horn, (8) is a standard noise source, (9) is a primary radiator,
(10) is the primary radiator array, (11) is the scanning range l, (12)
Is the length y in the direction of travel of the beam spot, (13) is the length x in the direction of scan of the beam spot, (14) is the weight in the direction of travel of the beam spot Δy, (15) is the weight in the direction of scan of the beam spot Δ x, (16) is the beam spot center distance A,
(17) shows the distance B between the boom spot centers in the scanning direction. In the drawings, the same reference numerals indicate the same or corresponding parts.
Claims (1)
た複数の一次放射器アレイと,上記一次放射器に接続さ
れ上記一次放射器を切り換えてアンテナビーム走査を行
うためのスイツチと,上記スイツチの出力端に接続され
たRF回路部と,上記RF回路部を経由して取得した雑音電
波の雑音温度に対応した電圧値を得る受信部と,上記受
信部の出力電圧をA/D変換,データ処理する信号処理部
とを具備したマイクロ波放射計において,上記一次放射
器アレイ及びスイツチを数組に分割し,その一組毎,各
々に上記RF回路部及び受信部を設けた事を特徴とするマ
イクロ波放射計。1. A reflector, a plurality of primary radiator arrays installed facing the reflector, and a switch connected to the primary radiator for switching the primary radiator to perform antenna beam scanning. , An RF circuit connected to the output terminal of the switch, a receiver for obtaining a voltage value corresponding to the noise temperature of the noise radio wave acquired via the RF circuit, and an output voltage of the receiver for A / In a microwave radiometer equipped with a signal processing unit for D conversion and data processing, the primary radiator array and switches are divided into several sets, and each set is provided with the RF circuit unit and the receiving unit. A microwave radiometer that features things.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63133662A JPH07111448B2 (en) | 1988-05-31 | 1988-05-31 | Microwave radiometer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63133662A JPH07111448B2 (en) | 1988-05-31 | 1988-05-31 | Microwave radiometer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01302178A JPH01302178A (en) | 1989-12-06 |
| JPH07111448B2 true JPH07111448B2 (en) | 1995-11-29 |
Family
ID=15109996
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63133662A Expired - Lifetime JPH07111448B2 (en) | 1988-05-31 | 1988-05-31 | Microwave radiometer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH07111448B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| ES2353104B2 (en) * | 2010-12-29 | 2011-07-11 | Universidad Politécnica de Madrid | ANTENNA FOR MONITORING OF THE ENVIRONMENTAL ELECTROMAGNETIC FIELD IN REAL TIME. |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63124926A (en) * | 1986-11-14 | 1988-05-28 | Nec Corp | High-accuracy microwave radiometer |
-
1988
- 1988-05-31 JP JP63133662A patent/JPH07111448B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01302178A (en) | 1989-12-06 |
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