JPH0465657A - Device for detecting adhesion density of salt component - Google Patents
Device for detecting adhesion density of salt componentInfo
- Publication number
- JPH0465657A JPH0465657A JP2177581A JP17758190A JPH0465657A JP H0465657 A JPH0465657 A JP H0465657A JP 2177581 A JP2177581 A JP 2177581A JP 17758190 A JP17758190 A JP 17758190A JP H0465657 A JPH0465657 A JP H0465657A
- Authority
- JP
- Japan
- Prior art keywords
- optical
- salt
- adhesion
- amount
- salt component
- 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.)
- Granted
Links
- 150000003839 salts Chemical class 0.000 title claims abstract description 55
- 230000003287 optical effect Effects 0.000 claims abstract description 61
- 238000001514 detection method Methods 0.000 claims description 24
- FAPWRFPIFSIZLT-UHFFFAOYSA-M Sodium chloride Chemical compound [Na+].[Cl-] FAPWRFPIFSIZLT-UHFFFAOYSA-M 0.000 claims description 16
- 239000011780 sodium chloride Substances 0.000 claims description 8
- 239000012212 insulator Substances 0.000 abstract description 38
- 239000000356 contaminant Substances 0.000 abstract description 30
- 239000000428 dust Substances 0.000 abstract description 20
- OSGAYBCDTDRGGQ-UHFFFAOYSA-L calcium sulfate Chemical compound [Ca+2].[O-]S([O-])(=O)=O OSGAYBCDTDRGGQ-UHFFFAOYSA-L 0.000 abstract description 10
- NLYAJNPCOHFWQQ-UHFFFAOYSA-N kaolin Chemical compound O.O.O=[Al]O[Si](=O)O[Si](=O)O[Al]=O NLYAJNPCOHFWQQ-UHFFFAOYSA-N 0.000 abstract description 10
- 229910052622 kaolinite Inorganic materials 0.000 abstract description 9
- 239000013307 optical fiber Substances 0.000 abstract description 9
- 239000000463 material Substances 0.000 abstract description 5
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 26
- 235000012239 silicon dioxide Nutrition 0.000 description 22
- 239000010453 quartz Substances 0.000 description 18
- 238000000034 method Methods 0.000 description 17
- 238000011109 contamination Methods 0.000 description 11
- 238000005259 measurement Methods 0.000 description 8
- 238000004140 cleaning Methods 0.000 description 6
- 230000000694 effects Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 239000000377 silicon dioxide Substances 0.000 description 4
- 239000000126 substance Substances 0.000 description 4
- 238000004506 ultrasonic cleaning Methods 0.000 description 4
- 238000005406 washing Methods 0.000 description 4
- 239000013078 crystal Substances 0.000 description 3
- 239000000203 mixture Substances 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- 230000005672 electromagnetic field Effects 0.000 description 2
- 238000002474 experimental method Methods 0.000 description 2
- 230000014509 gene expression Effects 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 238000000691 measurement method Methods 0.000 description 2
- 230000001902 propagating effect Effects 0.000 description 2
- 239000005995 Aluminium silicate Substances 0.000 description 1
- 239000000853 adhesive Substances 0.000 description 1
- 230000001070 adhesive effect Effects 0.000 description 1
- 235000012211 aluminium silicate Nutrition 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 238000012937 correction Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 239000012153 distilled water Substances 0.000 description 1
- -1 dust in the air Chemical class 0.000 description 1
- 238000010292 electrical insulation Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 238000010186 staining Methods 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Chemical compound O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
- 238000009736 wetting Methods 0.000 description 1
Landscapes
- Investigating Materials By The Use Of Optical Means Adapted For Particular Applications (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
- Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)
- Insulators (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は、碍子の表面に付着する塩分量を検出し、その
量を光学的手法により検出する装置に関するものである
。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to an apparatus for detecting the amount of salt adhering to the surface of an insulator and detecting the amount using an optical method.
[従来の技術]
高圧送電線と支持鉄塔との間の電気的な絶縁を確保する
ため、碍子は広く用いられているが、当該鉛量のおかれ
る環境は苛酷のものであり、例えば工業地域や臨海地域
などにあっては、碍子表面に塩分(NaCl)、その他
の無機質を主体とする塵埃が付着して汚損され易く、そ
れらが碍子の絶縁耐圧を低下せしめて閃絡事故などを引
き起こす場合がある。[Prior Art] Insulators are widely used to ensure electrical insulation between high-voltage power transmission lines and support towers, but the environments in which lead is placed are harsh, such as in industrial areas. In coastal areas and other areas, the surface of the insulator is easily contaminated by salt (NaCl) and other inorganic dust, which can lower the dielectric strength of the insulator and cause flashover accidents. There is.
こうした事態を未然に防止するため、碍子表面を付着す
る汚損物質を定期的に定量分析し、碍子汚損量を求める
ことが従来から行われている。In order to prevent such a situation from occurring, it has been conventional practice to periodically quantitatively analyze the contaminants adhering to the surface of the insulator to determine the amount of contamination of the insulator.
ところで碍子に付着する汚損物質としては、塩分の他、
子種類程度の無11物質があると言われているが、その
中でも特に塩分は碍子の絶縁耐圧を大きく劣化させる要
因となっている。そこで、碍子汚損量を表示するにあた
り、汚損物質が全て塩分からなると仮定した場合の単位
面積当たりの塩分量(等価塩分付着量)を用いいること
が便宜上なされている。By the way, in addition to salt, other contaminants that adhere to insulators include
It is said that there are 11 different substances, of which there are only 11 types, and among these, salt is a factor that significantly deteriorates the dielectric strength of insulators. Therefore, when displaying the amount of insulator fouling, it is convenient to use the amount of salt per unit area (equivalent salt adhesion amount) assuming that all of the fouling substances are made of salt.
従来性われている具体的手法を列記すれば以下の通りで
ある。Specific conventional methods are listed below.
(1)筆洗い法・・・実運用中の碍子と素材、形状など
が同一のパイロット碍子を、汚損量を測定したい場所に
設置しておき、所定期間経過後これを取り外し、筆によ
り付着した汚損物質を洗浄して、その洗浄液の電気伝導
度を測定することにより、等価塩分付着量を求め−る。(1) Brush washing method: A pilot insulator, which is made of the same material and shape as the insulator in actual use, is installed at the location where you want to measure the amount of contamination, and after a predetermined period of time, it is removed and the insulator is cleaned using a brush. The equivalent amount of salt deposited is determined by cleaning the contaminated material and measuring the electrical conductivity of the cleaning solution.
(2)露点式汚損量測定法・・・パイロット碍子に電子
冷却素子を組み入れ、これを露点温度以下に冷却せしめ
て空気中の水分を集め、碍子に付着している汚損物質を
強制的に充分湿潤させた状態にして漏れ抵抗を測定する
0次いで、別に求めておいた漏れ抵抗を等価塩分付着量
との関係から換算して求める。(2) Dew point type contamination measurement method: An electronic cooling element is incorporated into the pilot insulator, which is cooled to below the dew point temperature to collect moisture in the air and forcibly remove contaminants adhering to the insulator. The leakage resistance is measured in a wet state.Next, the leakage resistance obtained separately is calculated from the relationship with the equivalent salt deposition amount.
(3)超音波洗浄式汚損量測定法・・・パイロット碍子
を蒸溜水の入った洗浄槽内に入れ、碍子を回転させなが
ら超音波洗浄により汚損物質を洗い落とし、汚損物質の
溶は込んだ洗浄液の電気伝導度を測定して等価基分量を
求める。(3) Ultrasonic cleaning method for measuring the amount of contamination...The pilot insulator is placed in a cleaning tank containing distilled water, and while the insulator is rotated, the contaminants are washed away by ultrasonic cleaning, and the cleaning solution containing the contaminants is dissolved. Measure the electrical conductivity of and find the equivalent base quantity.
(4)球形模擬碍子法・・・常時、緩やかに自転する球
形の模IIi碍子を設置しておき、これに付着した汚損
物質をワイパーブラシで拭い取る。(4) Spherical simulated insulator method: A spherical simulated IIi insulator that slowly rotates on its own axis is always installed, and any contaminants adhering to it are wiped off with a wiper brush.
ワイパーブラシに付着した汚損物質は循環する洗浄液で
洗い落とされる。この洗浄液の電気伝導度を測定して、
積算された等価塩分付着量を求める。Contaminants adhering to the wiper brush are washed away by the circulating cleaning fluid. Measuring the electrical conductivity of this cleaning solution,
Find the accumulated equivalent salt adhesion amount.
[発明が解決しようとする課題] 従来技術の問題点として、(1)の筆洗い法。[Problem to be solved by the invention] The problem with the conventional technology is (1) the brush washing method.
(2)の露点式汚損量測定法、C3)の超音波洗浄式汚
損量測定法は、いずれも運用中の碍子と素材。(2) Dew point method for measuring the amount of contamination and C3) Ultrasonic cleaning method for measuring the amount of contamination are both currently in use for insulators and materials.
形状が同一のパイロット碍子を別に用意し、運用中の碍
子と同一条件下に設置する必要があり、それが高所、多
地点に至る場合には、測定に多大の労力と時間を要し極
めて不経済であった。また(4)の球形模擬鉤子法では
、球形模N碕子と実際の碍子との間にどうしても付着性
の相違が出てしまうので、これを修正する必要があり汚
損量の法定に手間がかかる。It is necessary to separately prepare a pilot insulator with the same shape and install it under the same conditions as the insulator in operation, and if the insulator is installed at a high place or at multiple points, it will take a lot of effort and time to make measurements. It was uneconomical. In addition, in the spherical simulated hook method (4), there is inevitably a difference in adhesion between the spherical simulated insulator and the actual insulator, so this needs to be corrected, which takes time and effort to determine the amount of contamination. .
次に、各手法を精度の面で考察すると、(1)の筆洗い
法では、測定に熟練を要し、手間がかかる。Next, considering each method in terms of accuracy, the brush washing method (1) requires skill and time for measurement.
(2)の露点式汚損量測定法では濡れ抵抗を等価塩分付
着量に換算するための校正機が必要となるが、これを各
測定場所ごとに作成する必要がある。The dew point method for measuring the amount of contamination (2) requires a calibration device to convert the wetting resistance into the equivalent amount of salt deposited, and this needs to be created for each measurement location.
(3)の超音波洗浄式汚損量測定法では、測定の都度碍
子が更新されるため1、暴露期間の興なる実運用中の碍
子の汚損量推定方法が問題となるが、これを精度よくな
し得るものがない、(4)の球形模N′iR子法では、
降雨による雨洗い効果が積算値に誤差をもたらし易い等
の欠点があった。In (3), the ultrasonic cleaning method for measuring the amount of contamination, the insulator is updated each time the measurement is performed, so there is a problem with how to estimate the amount of contamination on the insulator during actual operation, which depends on the exposure period. In the spherical model N'iR child method of (4), there is nothing that can be done,
There were drawbacks such as the rain-washing effect caused by rainfall which easily caused errors in the integrated value.
かかる状況の下、実運用中の碍子に付着する汚損物質の
量を定期的にではなくリアルタイムで測定したり、或い
は碍子表面の汚損物質の分布を測定するといった、より
高度な測定方法の開発が望まれていた。Under these circumstances, it is necessary to develop more advanced measurement methods, such as measuring the amount of contaminants adhering to insulators during actual operation in real time rather than periodically, or measuring the distribution of contaminants on the surface of insulators. It was wanted.
このため(5)の方法として、表面に塩分が付着すると
光損失が生ずる光導波路を碍子表面に露出して装着し、
該光導波路の一端から入射されて他端から出射する透過
光を受光し、該透過光強度の変化から碍子に付着する塩
分量を求めるようにした耐量汚損量の測定方法がある。For this reason, as method (5), an optical waveguide that causes optical loss when salt adheres to the surface is exposed and mounted on the insulator surface.
There is a method for measuring a tolerable amount of contamination in which transmitted light is received from one end of the optical waveguide and exits from the other end, and the amount of salt adhering to the insulator is determined from a change in the intensity of the transmitted light.
この(5)の方法は目的に適った優れた方法であるが、
光導波路の表面に空気中の塵埃等、塩分以外の物質が付
着した場合であっても光損失が生じ、結果的に塩分付着
を過大に評価してしまう虞れがある。This method (5) is an excellent method that suits the purpose, but
Even when substances other than salt, such as dust in the air, adhere to the surface of the optical waveguide, optical loss occurs, and as a result, there is a risk that salt adhesion may be overestimated.
この点につき吟味するに、一般に空気中を浮遊している
塵埃には、主成分として二酸化珪素(SiO2)が含ま
れ、その他にも硫酸カルシウム(CaSOa H2H2
0>、カオリナイト(AJ 2 S tos (OH
) 4 )等が含まれている。Taking a closer look at this point, dust floating in the air generally contains silicon dioxide (SiO2) as a main component, as well as calcium sulfate (CaSOa H2H2).
0>, Kaolinite (AJ 2 S tos (OH
) 4) etc. are included.
硝子の汚損試験には塩分(Nacjりの他に人工的な塵
埃を模擬する物資として、との粉が一般的に用いられて
いるが、この主成分はカオリナイトである。よって、光
導波路として純粋石英(屈折率−1,46)を用いてい
る場合、二酸化珪素(屈折率−1,46)が純粋石英表
面に付着したときは、石英内部を仏様する光が付着場所
で一度二酸化珪素内部へ透過するが、二酸化珪素と空気
境界面で反射して再び石英内部に戻ってくることになる
ので、その影響はほとんど無視できるのに対し、硫酸カ
ルシウム(屈折率=1.58) 、カオリナイト(屈折
率=1.56)が付着したときは、塩分(屈折率−1,
54)と同様の原理により光損失が生じてしまう。In addition to salt (Nacj), powder is commonly used to simulate artificial dust in glass staining tests, and its main component is kaolinite. When using pure quartz (refractive index -1.46), when silicon dioxide (refractive index -1.46) adheres to the surface of the pure quartz, the light that travels inside the quartz will be reflected once at the place of attachment. Although it passes into the interior, it is reflected at the interface between silicon dioxide and air and returns to the interior of the quartz, so its effect can be almost ignored, whereas calcium sulfate (refractive index = 1.58) and kaolin When night (refractive index = 1.56) adheres, salt (refractive index -1,
Optical loss occurs due to the same principle as 54).
本発明の目的は、前記した従来技術の欠点を解消し、碍
子に付着した汚損物質のうち、塩分のみを検出して、塩
分付着密度を測定できる新規な装置を提供することにあ
る。SUMMARY OF THE INVENTION An object of the present invention is to eliminate the above-mentioned drawbacks of the prior art and to provide a novel device that can detect only salt among the contaminants adhering to an insulator and measure the density of salt adhesion.
[課題を解決するための手段]
本発明の塩分付着密度検出装置は、NaCj’の屈折率
値より小なる屈折率値を有する第1の先導波路と、Na
Clの屈折率値より大なる且つAJ 2 S iOs
(OH) 4の屈折率より小なる屈折率値を有する第
2の導波路を検出部に有し、上記第1及び第2の光導波
路の一端から入射されて他端から出射する透過光を各々
受光し、該第1及び第2の光導波路から生ずる透過光強
度の変化量の差から検出部に付着する塩分の単位面積当
たりの塩分量を求める構成のものである。[Means for Solving the Problems] The salt adhesion density detecting device of the present invention includes a first leading wavepath having a refractive index value smaller than that of NaCj';
greater than the refractive index value of Cl and AJ 2 SiOs
(OH) The detection unit has a second waveguide having a refractive index value smaller than the refractive index of 4, and transmits transmitted light that is input from one end of the first and second optical waveguides and exits from the other end. The light is received by each optical waveguide, and the amount of salt per unit area adhering to the detection portion is determined from the difference in the amount of change in transmitted light intensity generated from the first and second optical waveguides.
[作用コ
第1の光導波路は塩分と塵埃(硫酸カルシウムやカオリ
ナイト等)の汚損物検出用であり、第2の光導波路は上
記塵埃の検出用であ゛る。先導波路に汚損物の付着がな
いとかは、光導波路の周囲は空気であるため、伝搬光は
損失を受けない。[Operation] The first optical waveguide is for detecting contaminants such as salt and dust (calcium sulfate, kaolinite, etc.), and the second optical waveguide is for detecting the dust. If there is no contaminant attached to the leading waveguide, there is air around the optical waveguide, so the propagating light does not suffer any loss.
今、第1及び第2の光導波路に塩分及び塵埃が混合して
付着したとする。Now, assume that a mixture of salt and dust has adhered to the first and second optical waveguides.
第1の光導波路では、その屈折率が塩分及び塵埃より小
であるため、塩分及び塵埃による光損失を生じる。これ
に対し第2の光導波路では、その屈折率が塩分より大で
且つ塵埃より小であるため、塵埃による光損失は生じる
が塩分による光損失は生じない。Since the first optical waveguide has a smaller refractive index than salt and dust, optical loss occurs due to salt and dust. On the other hand, in the second optical waveguide, since its refractive index is greater than that of salt and smaller than that of dust, optical loss due to dust occurs but no optical loss due to salt occurs.
従って、第1の光導波路から生ずる透過光強度の変化量
と第2の光導波路から生ずる透過光強度の変化量との差
を求めることにより、検出部に付着する塩分のみに関す
る付着量(塩分付着密度)を求めることができる。Therefore, by determining the difference between the amount of change in the intensity of transmitted light generated from the first optical waveguide and the amount of change in the intensity of transmitted light generated from the second optical waveguide, it is possible to determine the amount of adhesion (salt adhesion) only related to salt adhering to the detection part. Density) can be found.
[実施例] 以下、本発明を図示の実施例に基づいて説明する。[Example] Hereinafter, the present invention will be explained based on illustrated embodiments.
第1図に塩分付着密度検出装置の構成を示す。Figure 1 shows the configuration of the salt adhesion density detection device.
本装置は、光源部1.光分岐器2.検出部3.受光部4
.演算部5.光ファイバ6、信号ケーブル7から構成さ
れる。This device includes a light source section 1. Optical splitter 2. Detection unit 3. Light receiving section 4
.. Arithmetic unit 5. It is composed of an optical fiber 6 and a signal cable 7.
検出部3は2つの光導波路3a、3bから成る。The detection section 3 consists of two optical waveguides 3a and 3b.
第1の光導波路3aは、NaClの屈折率値1.54よ
り小なる屈折率値を有する先導波路であり、本実施例で
は純粋石英(屈折率1.46)を用いた石英棒から構成
される。第2の光導波路3bは、NaCl2の屈折率値
より大なる且つ
AJ 2 S i Os (OH) 4の屈折率1.
56より小なる屈折率値を有する光導波路であり、本実
施例では水晶(屈折率1.55)を用いた水晶棒から構
成される。The first optical waveguide 3a is a leading waveguide having a refractive index value smaller than the refractive index value of NaCl, which is 1.54, and in this embodiment is made of a quartz rod made of pure quartz (refractive index 1.46). Ru. The second optical waveguide 3b has a refractive index value of AJ 2 S i Os (OH) 4 greater than 1.
It is an optical waveguide having a refractive index value smaller than 56, and in this embodiment, it is composed of a quartz rod using quartz crystal (refractive index 1.55).
光源部1から出射された光は、光ファイバ6を介して光
分岐器2に導かれ、該光分岐器2で二分される。光分岐
器2を用いない構成も考えられるが、その時には、光源
部1を増−設する必要があるばかりか、光出力の温度補
正等をする必要があり、コスト面で実用的でない0分岐
された各々の光は、それぞれ光ファイバ6を介して上記
検出部3に至り、その第1.第2の光導波路3a、3b
に導がれる。検出部3において塩分及び塵埃の付着によ
る光損失変化を各々経験した光は、それぞれ光ファイバ
6を介して受光部4を構成している受光器4a、4bに
導かれ、透過光強度に応じた電気的出力に変換される。Light emitted from the light source section 1 is guided to the optical splitter 2 via the optical fiber 6, and is split into two by the optical splitter 2. It is possible to consider a configuration that does not use the optical splitter 2, but in that case, not only would it be necessary to add the light source unit 1, but it would also be necessary to perform temperature correction for the optical output, making it impractical in terms of cost. Each of the detected lights reaches the detection unit 3 via the optical fiber 6, and the first . Second optical waveguide 3a, 3b
guided by. The light that has experienced optical loss changes due to the adhesion of salt and dust in the detection unit 3 is guided to the light receivers 4a and 4b that constitute the light receiving unit 4 via the optical fiber 6, respectively, and is changed depending on the intensity of the transmitted light. converted into electrical output.
尚、検出部3は、その第1.第2の光導波路、3a+
3bの入射端側及び出射端側を、それぞれ光ファイバ6
で接続しているため、検出部3が強電磁場(例えば実課
電碍子環境)に設置されている場合でも、光源部1.受
光部4.演算部5をこの強電磁場から隔離して安全に計
測することができる。Incidentally, the detection section 3 has the first. second optical waveguide, 3a+
The input end side and the output end side of 3b are connected to optical fibers 6, respectively.
Since the light source unit 1. is connected to the light source unit 1. Light receiving section 4. The calculation unit 5 can be isolated from this strong electromagnetic field to safely perform measurements.
演算部5は、信号ゲープル7.7を通して受光器4 a
+ 4 bより得られる透過光強度変化量(つまり検出
部3に付着が無い場合を基準としたときの透過光強度)
を基に、光導波路3a、3bにつき予め分かっている透
過光強度変化量と単位面積当りの汚損物付着量との間の
関係式から、塩分のみの付着量(塩分付着密度)を算出
する。この塩分付着量の演算は、本実施例では、受光器
4aで求められた単位面積当りの汚損物付着量と、受光
部4bで求められた単位面積当りの汚損物付着量との差
を求める処理による。The arithmetic unit 5 connects the light receiver 4a to the light receiver 4a through the signal gaple 7.7.
+ 4 The amount of change in transmitted light intensity obtained from b (that is, the transmitted light intensity based on the case where there is no adhesion on the detection part 3)
Based on this, the amount of salt only (salt adhesion density) is calculated from the relational expression between the amount of transmitted light intensity change known in advance for the optical waveguides 3a and 3b and the amount of contaminant adhesion per unit area. In this embodiment, the salt adhesion amount is calculated by calculating the difference between the amount of contaminant adhesion per unit area determined by the light receiver 4a and the amount of contaminant adhesion per unit area determined by the light receiving section 4b. Depends on processing.
具体的に説明しよう。Let me explain in detail.
まず、NaClとAJ2 S i Os (OH)
4とを1:1の割合で混合した汚損物を検出部3に付着
し、受光部4で検゛出される光強度から求められる透過
光強度変化量と、検出部3近傍に置いた試料板(単一面
積板)に付着した汚損物付着量(汚損物重量を試料面積
で除算したもの)との関係を調べた。この実験結果を第
2図に示す。第2図(a)は石英棒から成る第1の光導
波路3aにおける透過光強度□変化量と汚損物付着量の
関係を、第2図(b)は水晶棒から成る第2の光導波i
3bにおける透過光強度変化量と汚損物付着量と間係を
示している0次に、汚損物の上記混合割合を変化させて
みたが、今回用いた光源部1が波長0.85μmのレー
ザダイオードLEDの場合、汚損物の混合割合を変化さ
せたときも透過光強度変化量と汚損物質量の関係は第2
図とほぼ同一となった。First, NaCl and AJ2SiOs(OH)
The amount of change in transmitted light intensity determined from the light intensity detected by the light receiving part 4 and the sample plate placed near the detecting part 3 are determined by the amount of change in transmitted light intensity determined from the light intensity detected by the light receiving part 4. The relationship between the amount of contaminants adhering to (single area plate) (the weight of contaminants divided by the sample area) was investigated. The results of this experiment are shown in FIG. FIG. 2(a) shows the relationship between the amount of change in transmitted light intensity □ and the amount of contaminants attached in the first optical waveguide 3a made of a quartz rod, and FIG.
3b shows the relationship between the amount of change in transmitted light intensity and the amount of contaminants attached Next, we tried changing the above mixing ratio of contaminants, but the light source 1 used this time was a laser diode with a wavelength of 0.85 μm. In the case of LEDs, even when the mixing ratio of contaminants is changed, the relationship between the amount of change in transmitted light intensity and the amount of contaminants is
It is almost the same as the figure.
上記前捉の下で、塩分のみを検出する作用につき説明す
る。既に述べたように、第1の光導波路3aには石英棒
(屈折率1.46)が、第2の先導波路3bには水晶(
屈折率1.55>が用いられているものとする。The function of detecting only salinity under the above-mentioned pre-trapping will be explained. As already mentioned, the first optical waveguide 3a includes a quartz rod (refractive index 1.46), and the second leading waveguide 3b includes a quartz rod (refractive index: 1.46).
It is assumed that a refractive index of 1.55> is used.
今、検出部3に、塩分NaCj’(屈折率値1.54)
と共に、塵埃としてカオリナイトAj2SiO。Now, in the detection unit 3, the salt content NaCj' (refractive index value 1.54)
Also, kaolinite Aj2SiO is present as dust.
(OH)、が混合して付着した場合について考える。こ
こで、塵埃としてカオリナイト
Aj2stos (OH)、(屈折率1.56)を考
察することは、それより趨折率値の大きい硫酸カルシウ
ム(屈折率1.58)を考察することと等価である。Consider the case where (OH) is mixed and deposited. Here, considering kaolinite Aj2stos (OH) (refractive index 1.56) as dust is equivalent to considering calcium sulfate (refractive index 1.58), which has a larger trend index value. .
石英棒(3a)及び水晶棒(3b)にそれぞれの一端か
ら光を入射した場合、上記のような汚損物の付着がない
状態では両棒の周囲が空気となるのため、伝搬光はほぼ
損失なく石英棒及び水晶棒の他端に達する。しかし、゛
検出部3eこ上記塩分と共にカオリナイトが付着した場
合、NaClとAj2Sin、(OH)4より小なる屈
折率を持つ石英棒(3a)では、付着した塩分及びカオ
リナイトによる光損失を生じる。これに対し、NaCl
より大なる且うAJ x S i Os (OH)−
より小なる屈折率を持つ水晶棒(3b)では、カオリナ
イトによる光損失は生ずるが、塩分による光損失は生じ
ない。When light enters the quartz rod (3a) and the quartz rod (3b) from one end of each, the propagating light is almost lost because there is air around both rods in the absence of contaminants as described above. Without reaching the other end of the quartz rod and the crystal rod. However, if kaolinite adheres to the detection part 3e along with the above salt, the quartz rod (3a), which has a refractive index smaller than NaCl and Aj2Sin, (OH)4, will cause optical loss due to the adhered salt and kaolinite. . On the other hand, NaCl
Greater AJ x Si Os (OH)-
In the quartz crystal rod (3b) having a smaller refractive index, light loss occurs due to kaolinite, but no light loss occurs due to salt.
要するに、石英棒(3a)から得られる透過光強度には
塩分と塵埃の両者による光損失の影響が含まれているが
、水晶棒(3b)から得られる透過光強度には塵埃によ
る光損失の影響しか含まれていない、受光器4a、4b
はこれらを電気的出力に変換する。In short, the transmitted light intensity obtained from the quartz rod (3a) includes the influence of optical loss due to both salt and dust, but the transmitted light intensity obtained from the quartz rod (3b) includes the influence of optical loss due to dust. Receivers 4a and 4b that only include effects
converts these into electrical output.
演算部5は、まず、第2図(a)(b)の特性曲線を表
す関係式により、上記電気的出力たる透過光強度の変化
量を、単位面積当りの汚損物付着量に換算する。既に明
らかなように、第2図(a)の特性曲線より求められる
汚損物質付着量は、NaClIとAJ x S i O
s (OH) 4の混合したものであり、第2図(b
)の特性曲線より求められる汚損物質付着量は、AJ
2S i Os (OH)−のものである。The calculation unit 5 first converts the amount of change in the transmitted light intensity, which is the electrical output, into the amount of contaminant adhesion per unit area using the relational expressions representing the characteristic curves shown in FIGS. 2(a) and 2(b). As is already clear, the amount of contaminant adhesion determined from the characteristic curve of FIG. 2(a) is
It is a mixture of s (OH) 4, and is shown in Figure 2 (b).
) The amount of contaminant adhesion determined from the characteristic curve of AJ
2S i Os (OH)-.
次いで、演算部5は、上記のようにして求められたNa
Cl及びAj 2sios (OH)、を混合したも
のの汚損物付着量と、
AN 2 S i Os ’(OH) 4の汚損物付着
量との差を求める。かくして、NaClのみの単位面積
当りの付着量が求められる。Next, the calculation unit 5 calculates the Na
The difference between the amount of contaminants attached to the mixture of Cl and Aj 2sios (OH) and the amount of contaminants attached to AN 2 S i Os '(OH) 4 is determined. In this way, the amount of NaCl attached per unit area is determined.
次に、上記検出部3の具体的構成例を示す。Next, a specific example of the configuration of the detection section 3 will be shown.
上記光導波路3a、3bは基本的には、(1)薄膜上に
露出して装着する、(2)11子表面に接着して設置す
る、或いは(3)碍子表面に設置された治具で固定する
等の構成がとれる。The optical waveguides 3a and 3b are basically (1) mounted exposed on a thin film, (2) installed by adhering to the surface of the insulator, or (3) installed with a jig installed on the surface of the insulator. It can be configured to be fixed.
第3図は、棒状の光導波路3a、3bの両端をL字状の
スタンド形治具8で固定した実施例である。検出部3は
このようなスタンド形治具8を用いないで、測定面(例
えば碍子の表面)に直接接着することもできるが、この
場合の接着剤としては、その屈折率値が第1の光導波路
(NaCオの屈折率値より小なる屈折率値を持つもの)
より小さいものが望ましい。FIG. 3 shows an embodiment in which both ends of rod-shaped optical waveguides 3a and 3b are fixed with an L-shaped stand-shaped jig 8. The detection unit 3 can be directly bonded to the measurement surface (for example, the surface of an insulator) without using such a stand-type jig 8, but in this case, the adhesive should have a refractive index value that is Optical waveguide (having a refractive index value smaller than that of NaC)
A smaller one is preferable.
第4図(a)は、光導波路3a、3bを円状のものとし
て、碍子9の下面のひだの円状溝10内に設置し、ひだ
内での塩分量を求める構成例を示す。FIG. 4(a) shows an example of a configuration in which the optical waveguides 3a and 3b are circular and installed in circular grooves 10 of the folds on the lower surface of the insulator 9, and the amount of salt in the folds is determined.
検出部3の機械的強度を保つために、光導波路3a、3
bはその周囲をリング形治具81で固定支持することが
好ましい。In order to maintain the mechanical strength of the detection unit 3, the optical waveguides 3a, 3
It is preferable that the periphery of b is fixedly supported by a ring-shaped jig 81.
第4図(b)は硝子9の下面に基板11を設置し、この
基板上に検出部3を設置し、下面全体に付着する塩分量
を求める構成例を示す、光導波路3a。FIG. 4(b) shows an optical waveguide 3a in which a substrate 11 is installed on the lower surface of the glass 9, a detection unit 3 is installed on this substrate, and the amount of salt adhering to the entire lower surface is determined.
3bの長さを変化させることにより測定範囲の拡大を図
ることができ、同図(b)のように光導波路3a、3b
を同心円状にすれば、検出部3の設置位置の影響を受け
ないでII定を行うことできる。The measurement range can be expanded by changing the length of the optical waveguides 3a and 3b, as shown in FIG.
If they are made concentric, II determination can be performed without being affected by the installation position of the detection unit 3.
この場合も、検出部3の機械的強度を保つため、光導波
路3a、3bはその周囲をリング形治具82で固定支持
することが好ましい。In this case as well, in order to maintain the mechanical strength of the detection section 3, it is preferable that the optical waveguides 3a, 3b are fixedly supported around the circumference by a ring-shaped jig 82.
尚、第3図及び第4図のいずれの構成例においても、治
具8.81.82の光導波路と接する面には、光導波路
の屈折率値よりも小さな屈折率値を持つ樹脂(シリコー
ン等)を塗布しておくことが望ましい。In both of the configuration examples shown in FIG. 3 and FIG. etc.) is desirable.
[発明の効果〕
以上述べたように、本発明によれば、次のような優れた
効果を発揮する。\
(1)碍子表面等に付着する汚損物質のうち、殻の塵埃
成分を除いた塩分量だけを区別して求めることができる
。[Effects of the Invention] As described above, according to the present invention, the following excellent effects are exhibited. \ (1) Among the contaminating substances adhering to the insulator surface, only the amount of salt can be determined separately, excluding the dust component of the shell.
(2)高電磁場環境での測定が行える。(2) Measurements can be made in a high electromagnetic field environment.
第1図は本発明の塩分付着密度検出装置の実施例を示す
構成図、第2図は実験により得られた検出部の透過光損
失変化量と汚損物付着量との関係を示す図、第3図は検
出部の具体的構成例を示す模式図、第4図は検出部の他
の構成例′を示す模式図である。
図中、1は光源部、2は光分岐器、3は検出部、3aは
第1の光導波路、3bは第2の光導波路、4は受光部、
4a、4bは受光器、5は演算部、6は光ファイバ、7
は信号ゲーブル、8.81゜82は治具、9は碍子、1
0は清、11は基板を示す。
特許出願人 日立電線株式会社
代理人弁理士 絹 谷 信 雄
(a)
(b)
第2図Fig. 1 is a configuration diagram showing an embodiment of the salt adhesion density detecting device of the present invention, Fig. 2 is a diagram showing the relationship between the amount of change in transmitted light loss of the detection part and the amount of contaminant adhesion obtained by experiment. FIG. 3 is a schematic diagram showing a specific example of the configuration of the detection section, and FIG. 4 is a schematic diagram showing another example of the configuration of the detection section. In the figure, 1 is a light source section, 2 is an optical splitter, 3 is a detection section, 3a is a first optical waveguide, 3b is a second optical waveguide, 4 is a light receiving section,
4a, 4b are light receivers, 5 is a calculation unit, 6 is an optical fiber, 7
is a signal cable, 8.81°82 is a jig, 9 is an insulator, 1
0 indicates clear and 11 indicates substrate. Patent applicant: Hitachi Cable Co., Ltd. Representative Patent Attorney Nobuo Kinutani (a) (b) Figure 2
Claims (1)
1の光導波路と、NaClの屈折率値より大なる且つA
l_2SiO_5(OH)_4の屈折率より小なる屈折
率値を有する第2の導波路を検出部に有し、上記第1及
び第2の光導波路の一端から入射されて他端から出射す
る透過光を各々受光し、該第1及び第2の光導波路から
生ずる透過光強度の変化量の差から検出部に付着する塩
分の単位面積当たりの塩分量を求めることを特徴とする
塩分付着密度検出装置。1. A first optical waveguide having a refractive index value smaller than the refractive index value of NaCl, and a first optical waveguide having a refractive index value larger than the refractive index value of NaCl;
The detection unit has a second waveguide having a refractive index value smaller than the refractive index of l_2SiO_5(OH)_4, and transmitted light enters from one end of the first and second optical waveguides and exits from the other end. A salt adhesion density detecting device, characterized in that the salt adhesion density detecting device receives each light and determines the amount of salt per unit area of the salt adhering to the detection part from the difference in the amount of change in transmitted light intensity generated from the first and second optical waveguides. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2177581A JPH0687041B2 (en) | 1990-07-06 | 1990-07-06 | Salt attachment density detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2177581A JPH0687041B2 (en) | 1990-07-06 | 1990-07-06 | Salt attachment density detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0465657A true JPH0465657A (en) | 1992-03-02 |
| JPH0687041B2 JPH0687041B2 (en) | 1994-11-02 |
Family
ID=16033479
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2177581A Expired - Lifetime JPH0687041B2 (en) | 1990-07-06 | 1990-07-06 | Salt attachment density detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0687041B2 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04258747A (en) * | 1991-02-12 | 1992-09-14 | Hitachi Cable Ltd | Optical salinity pollution quantity detecting device |
| CN104730036A (en) * | 2015-03-13 | 2015-06-24 | 华北电力大学(保定) | Dust density detection device and dust density detection method on power transmission line |
-
1990
- 1990-07-06 JP JP2177581A patent/JPH0687041B2/en not_active Expired - Lifetime
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04258747A (en) * | 1991-02-12 | 1992-09-14 | Hitachi Cable Ltd | Optical salinity pollution quantity detecting device |
| CN104730036A (en) * | 2015-03-13 | 2015-06-24 | 华北电力大学(保定) | Dust density detection device and dust density detection method on power transmission line |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0687041B2 (en) | 1994-11-02 |
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