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JPH0335607B2 - - Google Patents
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JPH0335607B2 - - Google Patents

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Publication number
JPH0335607B2
JPH0335607B2 JP2792586A JP2792586A JPH0335607B2 JP H0335607 B2 JPH0335607 B2 JP H0335607B2 JP 2792586 A JP2792586 A JP 2792586A JP 2792586 A JP2792586 A JP 2792586A JP H0335607 B2 JPH0335607 B2 JP H0335607B2
Authority
JP
Japan
Prior art keywords
light
probe
liquid level
output
incident light
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.)
Expired
Application number
JP2792586A
Other languages
Japanese (ja)
Other versions
JPS62187222A (en
Inventor
Nobuyuki Sasaki
Iwao Asahi
Satoshi Oka
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.)
Ohkura Electric Co Ltd
Original Assignee
Ohkura Electric Co Ltd
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 Ohkura Electric Co Ltd filed Critical Ohkura Electric Co Ltd
Priority to JP2792586A priority Critical patent/JPS62187222A/en
Publication of JPS62187222A publication Critical patent/JPS62187222A/en
Publication of JPH0335607B2 publication Critical patent/JPH0335607B2/ja
Granted legal-status Critical Current

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  • Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、液面の光学的検出器に関し、とくに
簡単な構造の光源監視手段を有する光学的液面検
出器に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to an optical liquid level detector, and more particularly to an optical liquid level detector with light source monitoring means of simple construction.

従来の技術 液面の検出手段として電気的センサーは便利で
あるが、被検出液の性質によつては、電極汚染、
気泡による誤動作、センサーの腐食などの問題が
あるので、光学的手段がかえつて有利となる場合
がある。
Conventional technology Electric sensors are convenient as a means of detecting the liquid level, but depending on the nature of the liquid to be detected, they may cause electrode contamination,
Since there are problems such as malfunction due to air bubbles and corrosion of the sensor, optical means may be more advantageous.

第2図を参照して従来の光学的液面検出法を説
明する。絶対屈折率n1の媒質M1と絶対屈折率n2
の媒質M2との境界面Sを入射角θ1で入射光Iが
入ると、その入射角θ1が臨界角θ1より小であれ
ば、入射光Iの一部は反射角θ1で反射して反射光
Rとなり他の一部は屈折角θ2をもつて媒体M2
進入し透過光Dとなる。入射角が臨界角θcに等し
い場合には、入射光Icは矢印Tで示される境界面
Sに平行な光線となり、入射角が臨界角θcより大
である場合には、入射光は全反射して反射光とな
る。臨界角θcは次式で与えられる。
A conventional optical liquid level detection method will be explained with reference to FIG. Medium M 1 with absolute refractive index n 1 and absolute refractive index n 2
When incident light I enters the interface S with the medium M 2 at an incident angle θ 1 , if the incident angle θ 1 is smaller than the critical angle θ 1 , a part of the incident light I enters at the reflection angle θ 1. It is reflected and becomes reflected light R, and the other part enters the medium M 2 with a refraction angle θ 2 and becomes transmitted light D. When the angle of incidence is equal to the critical angle θc, the incident light Ic becomes a ray parallel to the boundary surface S indicated by the arrow T, and when the angle of incidence is greater than the critical angle θc, the incident light is totally reflected. It becomes reflected light. The critical angle θc is given by the following equation.

sinθc=(n1/n2) ガラスから空気へ進行する入射光に対する臨界
角は約42°であり、ガラスから水へ進行する入射
光に対する臨界角は約60°であることが知られて
いる。
sinθc=(n 1 / n 2 ) It is known that the critical angle for incident light traveling from glass to air is approximately 42°, and the critical angle for incident light traveling from glass to water is approximately 60°. .

第1図に示すプローブ1の検出面2に対し入射
角45°で入射光を与えると、検出面2が水中にあ
る場合には入射角が臨界角より小であるから入射
光の大部分が透過光Dとなる。他方、検出面2が
空気中にある場合には入射角が臨界角より大であ
るから入射光の大部分が同図に点線で示される様
に全反射を2回行ない入射光Iと平行な反射光R
となる。従つて、反射光Rの有無を検出すれば、
この場合水面である液面Lを検出することができ
る。
When incident light is applied to the detection surface 2 of the probe 1 shown in Fig. 1 at an incident angle of 45°, when the detection surface 2 is underwater, most of the incident light is smaller than the critical angle. This becomes transmitted light D. On the other hand, when the detection surface 2 is in the air, the incident angle is larger than the critical angle, so most of the incident light undergoes total reflection twice as shown by the dotted line in the same figure, and becomes parallel to the incident light I. Reflected light R
becomes. Therefore, if the presence or absence of reflected light R is detected,
In this case, the liquid level L, which is the water surface, can be detected.

しかし、上記の従来法では、第1図の光源3に
障害が発生し入射光Iが消滅又は著しく減少した
場合に特に対策を施さない限り反射光Rが検出さ
れなくなるから、現実の液面の存否とは無関係に
液面が検出される不都合が生ずる。例えば、液面
検出器を満水位検出に適用した場合に現実の水位
が満水位以下である場合にも満水と判断され不都
合である。この不都合を解決するため、第3図に
示される様に光源3の脇に監視用検出素子7を設
け、光源3の劣化を監視することが考えられる。
この解決法には、本来の検出素子以外に余分の監
視用検出素子7及びそのハウジング7aが必要と
なり、構造の複雑化とコスト増を招く欠点があ
る。
However, in the conventional method described above, if a failure occurs in the light source 3 in Fig. 1 and the incident light I disappears or significantly decreases, the reflected light R will not be detected unless special measures are taken. A problem arises in that the liquid level is detected regardless of its presence or absence. For example, when a liquid level detector is applied to detect the full water level, even if the actual water level is below the full water level, it is judged as full, which is inconvenient. In order to solve this problem, it is conceivable to provide a monitoring detection element 7 beside the light source 3 to monitor the deterioration of the light source 3, as shown in FIG.
This solution requires an extra monitoring detection element 7 and its housing 7a in addition to the original detection element, which has the disadvantage of complicating the structure and increasing costs.

発明が解決しようとする問題点 従つて、本発明が解決しようとする問題点は、
光学的液面検出器における光源3の劣化監視の簡
易化にある。
Problems to be solved by the invention Therefore, the problems to be solved by the invention are as follows:
The objective is to simplify the deterioration monitoring of the light source 3 in the optical liquid level detector.

問題点を解決するための手段 第1図を参照するに、本発明の好ましい実施例
においては、プローブ1の入射光Iの光源側光路
41にプローブの入射端に接する空隙9を設け、
プローブ入射端の端面を一部反射面10とし、入
射光Iの一部pをその一部反射面10で反射させ
て一部反射光qとしこれを検出面2からの反射光
Rの光路51へ向け反射光Rとともに光路51内
を進光させ、単一の光検出素子5により反射光R
と一部の反射光qとの和を検出する。上記の一部
反射面10は、必ずしも空隙9によつて構成する
必要はなく、ハーフミラーその他の手段によつて
形成してもよい。
Means for Solving the Problems Referring to FIG. 1, in a preferred embodiment of the present invention, a gap 9 is provided in the light source side optical path 41 of the incident light I of the probe 1 in contact with the input end of the probe.
The end face of the probe entrance end is made into a partially reflecting surface 10, and a portion p of the incident light I is reflected by the partially reflecting surface 10 to become partially reflected light q, which is then reflected onto the optical path 51 of the reflected light R from the detection surface 2. The reflected light R is caused to travel along the optical path 51 along with the reflected light R toward the
The sum of the reflected light q and a part of the reflected light q is detected. The partially reflective surface 10 described above does not necessarily need to be formed by the void 9, and may be formed by a half mirror or other means.

なお、第1図の光源側光フアイバ4を単にプロ
ーブ1に直接に結合するだけでは、一部反射面1
0を形成することはできない。
Note that simply connecting the light source side optical fiber 4 shown in FIG.
It is not possible to form a 0.

作 用 第1図において、反射光Rの光路51にフオト
ダイオード等の光検出素子6を配置し光路51の
光量を検出する。(一部反射光qのみ)及び(一
部反射光q+検出面2からの反射光R)に対する
光検出素子5の出力をそれぞれ第5図のE0及び
E1であるとすれば、出力E0のみの存在により液
面の存在を検出し、出力E1の存在により液面の
不存在を検出することができる。光源3の劣化又
は喪失の場合には、出力E0が低下又は消滅する
ので、液面の存在とは区別できる。
Operation In FIG. 1, a photodetector element 6 such as a photodiode is arranged in the optical path 51 of the reflected light R to detect the amount of light in the optical path 51. The outputs of the photodetecting element 5 for (partially reflected light q only) and (partially reflected light q + reflected light R from the detection surface 2) are expressed as E 0 and E 0 in FIG. 5, respectively.
If E 1 , the presence of the liquid level can be detected by the presence of only the output E 0 , and the absence of the liquid level can be detected by the presence of the output E 1 . In case of deterioration or loss of the light source 3, the output E 0 decreases or disappears, so that it can be distinguished from the presence of a liquid level.

従つて、本発明によれば入射側光路41におけ
る部分反射面10の形成という極めて簡便な手段
により、光源3の劣化を監視することができる。
Therefore, according to the present invention, the deterioration of the light source 3 can be monitored by the extremely simple means of forming the partially reflecting surface 10 in the incident side optical path 41.

実施例 本発明の一実施例を第1図により説明する。発
光ダイオード等の光源3に結合された光フイバ4
の一端及びフオトダイオード等の光検出素子5に
結合された光フイバ6の一端を中空ホルダー8に
固定し、その中空ホルダー8をプローブ1の光源
側に嵌合することにより、光源側光フアイバ4と
プローブ1の受光端との間に空隙9を形成する。
光源側光フアイバ4から出る光束は必ずしも完全
な平行光線ではないから、入射光Iの一部pはプ
ローブ1の受光端端面で反射し一部反射光qとな
る。空隙9の形状寸法及び光フアイバ4,6の取
付け位置を適当に選択し、上記一部反射光qを反
射光Rの光路51へ向ける。こうしてプローブ1
の上記受光端端面は一部反射面10として作用す
る。
Embodiment An embodiment of the present invention will be described with reference to FIG. Optical fiber 4 coupled to a light source 3 such as a light emitting diode
By fixing one end of the optical fiber 6 coupled to one end and a photodetecting element 5 such as a photodiode to a hollow holder 8, and fitting the hollow holder 8 to the light source side of the probe 1, the light source side optical fiber 4 is fixed. A gap 9 is formed between the probe 1 and the light receiving end of the probe 1.
Since the light flux emitted from the light source side optical fiber 4 is not necessarily a perfectly parallel light beam, a portion p of the incident light I is reflected by the light receiving end face of the probe 1 and becomes a partially reflected light q. The shape and dimensions of the gap 9 and the mounting positions of the optical fibers 4 and 6 are appropriately selected to direct the partially reflected light q to the optical path 51 of the reflected light R. Thus probe 1
The above-mentioned light-receiving end facet partially functions as a reflecting surface 10.

図示例のプローブ1は石英ガラス製であり、円
筒形部分と円錐形先端部とが一体に形成されてい
る。先端部の頂角が適当に選ばれ、その円錐面に
よつて検出面2が形成され、円筒部の軸線と平行
に進行する入射光Iが入射角約45°で検出面2へ
入射する。空気Kと被検出液Wとの界面即ち液面
Lが検出面2の上方にある場合には、入射光Iの
大部分は被検出液W中へ屈折光Dとして進行し、
検出面2における反射光は少ない。被検出液面L
がプローブ1の下方にあつて検出面2の外側が空
気Kのみである場合には、入射光Iは第1図の点
線で示される様に検出面2で2回反射し入射光I
と平行な入射光Rとなる。
The illustrated probe 1 is made of quartz glass, and has a cylindrical portion and a conical tip portion formed integrally. The apex angle of the tip is appropriately selected, and its conical surface forms a detection surface 2, and the incident light I traveling parallel to the axis of the cylindrical portion is incident on the detection surface 2 at an incident angle of about 45°. When the interface between the air K and the liquid W to be detected, that is, the liquid level L, is above the detection surface 2, most of the incident light I travels into the liquid W to be detected as refracted light D.
There is little reflected light on the detection surface 2. Detected liquid level L
is below the probe 1 and the outside of the detection surface 2 is only air K, the incident light I is reflected twice by the detection surface 2 as shown by the dotted line in FIG.
The incident light R is parallel to .

第1図のパルス発生回路11は、発光ダイオー
ド等の光源3に駆動パルスを与え、パルス状に光
束即ち入射光Iを発生させる。
A pulse generating circuit 11 shown in FIG. 1 applies a driving pulse to a light source 3 such as a light emitting diode, and generates a light flux, that is, incident light I in a pulsed manner.

反射光Rの光路51における光、即ち上記反射
光R及び一部反射光qは光フアイバ6を介してフ
オトダイオード等の光検出素子5に加えられ電気
信号に変換される。検出回路12は、光検出素子
5の出力を解析して液面Lを検出し、検出結果を
表示器13に表示する。検出回路12が第4図の
増幅回路20のみからなる場合には、増幅器出力
端Aにおける出力は第5図の様になる。即ち、一
部反射光qのみに対する出力E0の検出により液
面Lがプローブ1の位置又はそれ以上にあること
を判断し必要に応じこれを表示する。(一部反射
光q+検出面2からの反射光R)に対する出力
E1の検出により液面Lがプローブ1より下にあ
ることを判断し必要に応じこれを表示する。一部
反射光qのみに対する出力E0の欠如の検出によ
り光源3の劣化又は損傷を判断し必要に応じこれ
をも表示することができる。
The light in the optical path 51 of the reflected light R, that is, the above-mentioned reflected light R and partially reflected light q, is applied to a photodetecting element 5 such as a photodiode via an optical fiber 6 and converted into an electric signal. The detection circuit 12 analyzes the output of the photodetection element 5 to detect the liquid level L, and displays the detection result on the display 13. When the detection circuit 12 consists only of the amplifier circuit 20 shown in FIG. 4, the output at the amplifier output terminal A becomes as shown in FIG. That is, by detecting the output E 0 for only the partially reflected light q, it is determined that the liquid level L is at or above the position of the probe 1, and this is displayed as necessary. Output for (partially reflected light q + reflected light R from detection surface 2)
By detecting E1 , it is determined that the liquid level L is below the probe 1, and this is displayed as necessary. Deterioration or damage to the light source 3 can be determined by detecting the absence of the output E 0 for only the partially reflected light q, and this can also be displayed if necessary.

上記出力E1が外乱である場合の誤動作を防止
するため、パルス状の出力E1が連続的に複数個
あることを計数した上で判断することとし、その
ためのカウンタ(図示せず)を設けた構成の検出
回路12としてもよい。
In order to prevent malfunctions when the above output E 1 is a disturbance, the presence of multiple pulse-like outputs E 1 is counted and determined, and a counter (not shown) is provided for this purpose. The detection circuit 12 may have a different configuration.

第5図を参照するに外乱E2が(一部反射光q
+検出面2からの反射光R)に対する出力E1′に
比して大きく、反射光Rの存在の検出が困難であ
る場合には、外乱光の影響を除去するため第4図
に示される様に、検出回路12にパルス発生回路
のパルスと同期した切換スイツチ21、正負変換
回路22、及び積分回路23を含めることができ
る。切換スイツチ21は、第4図に示される様に
入射光Iがない期間のみ出力を反転するので、外
乱E2のみが反転される。
Referring to Figure 5, the disturbance E 2 (partially reflected light q
+Reflected light R from the detection surface 2 Similarly, the detection circuit 12 can include a changeover switch 21 synchronized with the pulse of the pulse generation circuit, a positive/negative conversion circuit 22, and an integration circuit 23. Since the changeover switch 21 inverts the output only during the period when there is no incident light I, as shown in FIG. 4, only the disturbance E2 is inverted.

従つて、反射光Rが存在するとき即ち液面Lが
プローブ1より下方にあるときには、検出回路1
2が適当な積分時間Tiの後に第7図に示される
様な有限出力Viを発生する。他方、反射光Rが
存在しないとき即ち液面Lがプローブ1の位置又
はそれ以上にあるときには、検出回路12は適当
な積分時間Tiの後にも第8図に示される様に有
意の出力を発生しない。これにより、外乱が大き
い場合にも正確な液面検出をすることができる。
Therefore, when the reflected light R exists, that is, when the liquid level L is below the probe 1, the detection circuit 1
2 produces a finite output Vi as shown in FIG. 7 after a suitable integration time Ti. On the other hand, when there is no reflected light R, that is, when the liquid level L is at or above the position of the probe 1, the detection circuit 12 generates a significant output as shown in FIG. 8 even after an appropriate integration time Ti. do not. This makes it possible to accurately detect the liquid level even when the disturbance is large.

発明の効果 以上説明した如く、本発明の光学的液面検出器
はプローブの入射光光路に部分的反射面を設ける
ので、次の効果を奏する。
Effects of the Invention As explained above, since the optical liquid level detector of the present invention provides a partial reflection surface in the optical path of the incident light of the probe, it has the following effects.

(イ) 光源劣化監視用の光検出素子及びそのハウジ
ングを省略することができる。
(a) A photodetector element for monitoring light source deterioration and its housing can be omitted.

(ロ) 光源と共に光伝送路の劣化も監視することが
できる。
(b) Deterioration of the optical transmission line as well as the light source can be monitored.

(ハ) 正負変換回路及び積分回路を組込むことによ
り外乱が検出に及ぼす影響を除去することがで
きる。
(c) By incorporating a positive/negative conversion circuit and an integration circuit, the influence of disturbances on detection can be removed.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明による光学的液面検出器の図式
的説明図、第2図は臨界角の説明図、第3図は従
来の光学的液面検出器の図式的説明図、第4図は
検出回路の回路図、第5図ないし第8図は検出回
路の動作説明図である。 I……入射光、R……反射光、p……入射光の
一部、q……一部反射光、K……空気、L……液
面、W……被検出液、1……プローブ、2……検
出面、3……光源、4,6……光フアイバ、5…
…光検出素子、7……監視用検出素子、8……ホ
ルダー、9……空隙、10……一部反射面、11
……パルス発生回路、12……検出回路、13…
…表示器、20……増幅回路、21……切換スイ
ツチ、22……正負変換回路、23……積分回
路、41……光源側光路、51……反射光の光
路。
FIG. 1 is a schematic illustration of an optical liquid level detector according to the present invention, FIG. 2 is an illustration of a critical angle, FIG. 3 is a schematic illustration of a conventional optical liquid level detector, and FIG. 4 is a schematic illustration of a conventional optical liquid level detector. is a circuit diagram of the detection circuit, and FIGS. 5 to 8 are diagrams explaining the operation of the detection circuit. I...Incoming light, R...Reflected light, p...Part of incident light, q...Partially reflected light, K...Air, L...Liquid surface, W...Liquid to be detected, 1... Probe, 2...Detection surface, 3...Light source, 4, 6...Optical fiber, 5...
...Photodetection element, 7...Detection element for monitoring, 8...Holder, 9...Gap, 10...Partially reflective surface, 11
...Pulse generation circuit, 12...Detection circuit, 13...
. . . Display device, 20 . . . Amplification circuit, 21 . . . Changeover switch, 22 .

Claims (1)

【特許請求の範囲】 1 プローブ内からその検出面への入射光の入射
角がプローブ材質と空気との間の臨界角より大き
くプローブ材質と被検出液との間の臨界角より小
である光学系を有する液面検出器において、上記
入射光の一部を上記検出面からの反射光の光路上
へ反射する如く上記プローブ入射側光路に設けた
一部反射面、及び上記検出面からの反射光と上記
一部反射面からの反射光との和を受光する単一の
光検出素子を備えてなる光学的液面検出器。 2 特許請求の範囲第1項記載の光学的液面検出
器において、上記入射光の光源側光路に上記プロ
ーブの入射端に接する空〓を設け、上記プローブ
の入射端の端面を上記一部反斜面としてなる光学
的液面検出器。 3 プローブ内から検出面への入射光の入射角が
プローブ材質と空気との間の臨界角より大きくプ
ローブ材質と被検出液との間の臨界角より小であ
る光学系、上記入射光を間欠的に上記プローブへ
投射する光源、上記プローブの上記入射光の光路
に適当に設けられて上記入射光の一部を上記検出
面からの反射光の光路上へ反射させる一部反射
面、上記反射光の光路に適当に設けられ上記検出
面からの反射光と上記一部反射面からの反射光と
の和に比例した電気出力を発生する光検出素子、
上記光源の間欠的投射に同期された反転スイツチ
を介して上記光検出素子の出力に適当に接続され
て上記入射光の投射時に上記光検出素子出力と同
一極性出力を発生し且つ上記入射光の非投射時に
上記光検出素子出力の反転出力を発生する反転回
路、及び上記反転回路の出力に接続された積分回
路を備えてなる光学的液面検出器。
[Claims] 1. An optical system in which the angle of incidence of light from inside the probe to its detection surface is greater than the critical angle between the probe material and air and smaller than the critical angle between the probe material and the liquid to be detected. In the liquid level detector having a system, a partial reflection surface provided in the optical path on the probe entrance side so as to reflect a part of the incident light onto the optical path of the reflected light from the detection surface, and a part of the reflection surface from the detection surface. An optical liquid level detector comprising a single photodetecting element that receives the sum of light and reflected light from the partially reflecting surface. 2. In the optical liquid level detector according to claim 1, an optical path of the incident light on the light source side is provided with an air space that is in contact with the input end of the probe, and the end surface of the input end of the probe is arranged so that the end surface of the input end of the probe is Optical liquid level detector that acts as a slope. 3 An optical system in which the angle of incidence of the incident light from inside the probe to the detection surface is larger than the critical angle between the probe material and air and smaller than the critical angle between the probe material and the liquid to be detected, and the above incident light is intermittently transmitted. a light source that projects the light onto the probe; a partial reflection surface that is appropriately provided in the optical path of the incident light on the probe and reflects a part of the incident light onto the optical path of the reflected light from the detection surface; a photodetecting element that is appropriately provided in the optical path of the light and generates an electrical output proportional to the sum of the reflected light from the detection surface and the reflected light from the partially reflective surface;
Suitably connected to the output of the photodetector element via a reversing switch synchronized with the intermittent projection of the light source to generate an output of the same polarity as the output of the photodetector element when the incident light is projected, and An optical liquid level detector comprising: an inverting circuit that generates an inverted output of the output of the photodetecting element during non-projection; and an integrating circuit connected to the output of the inverting circuit.
JP2792586A 1986-02-13 1986-02-13 Optical liquid level indicator Granted JPS62187222A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2792586A JPS62187222A (en) 1986-02-13 1986-02-13 Optical liquid level indicator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2792586A JPS62187222A (en) 1986-02-13 1986-02-13 Optical liquid level indicator

Publications (2)

Publication Number Publication Date
JPS62187222A JPS62187222A (en) 1987-08-15
JPH0335607B2 true JPH0335607B2 (en) 1991-05-28

Family

ID=12234458

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2792586A Granted JPS62187222A (en) 1986-02-13 1986-02-13 Optical liquid level indicator

Country Status (1)

Country Link
JP (1) JPS62187222A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003042828A (en) * 2001-07-30 2003-02-13 Hitachi Medical Corp Rejected container expulsion confirmation apparatus and liquid level inspection apparatus

Also Published As

Publication number Publication date
JPS62187222A (en) 1987-08-15

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