JPH03216514A - Inclination sensor - Google Patents

Inclination sensor

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Publication number
JPH03216514A
JPH03216514A JP1391790A JP1391790A JPH03216514A JP H03216514 A JPH03216514 A JP H03216514A JP 1391790 A JP1391790 A JP 1391790A JP 1391790 A JP1391790 A JP 1391790A JP H03216514 A JPH03216514 A JP H03216514A
Authority
JP
Japan
Prior art keywords
light
colored liquid
light beams
inclination
beams
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.)
Pending
Application number
JP1391790A
Other languages
Japanese (ja)
Inventor
Hideo Mihashi
秀男 三橋
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.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP1391790A priority Critical patent/JPH03216514A/en
Publication of JPH03216514A publication Critical patent/JPH03216514A/en
Pending legal-status Critical Current

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  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

PURPOSE:To obtain an inclination value without an error by dividing a light beam from one light emitting element into two light beams to irradiate a colored liquid and calculating an inclination from a difference between the attenuation quantities of the two light beams. CONSTITUTION:The intensities of two parallel light beams emitted from one laser diode (LD) 6 of a light irradiating unit 3 are adjusted by a variable beam splitter (ABS) 7 so that the intensity ratio of the two light beams after reflected by returning mirrors 8a, 8b and 8c is equal to 1:1. When a transparent container 2 is inclined by an angle theta, one of the two parallel light beams from the light irradiating unit 3 is transmitted through a colored liquid 1 by a distance corresponding to a length H1 and the other light beam is transmitted through the liquid 1 by a distance corresponding to a length H2 and received by photosensitive elements 4 and 5, respectively. The resultant photoelectric outputs of the elements 4 and 5 are measured and an inclination theta is calculated by using a prescribed equation. Thus, since two light emitting elements are not used, an accurate measured value can be obtained without a drift generated with elapse of time and a difference between characteristics.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は傾斜センサ、特に水準器や装置の傾きの検出に
適用しうる傾斜センサに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an inclination sensor, and particularly to an inclination sensor that can be applied to detecting the inclination of a spirit level or an apparatus.

〔従来の技術〕[Conventional technology]

従来、この種の傾斜センサには2個の発光素子を使用し
たものがあり、この傾斜センサは、一定の光吸収係数を
持つ均質な着色液体と、この着色液体を入れた透明な直
方体容器と、この容器の上下いづれかの面にあって、2
本の同一強度の平行な光線を対面に垂直に照射するよう
に、一定間隔離れて取付けられた2個の発光素子と、容
器の発光素子取付け面と対面側にあって、発光素子から
照射され着色液体を通過した2本の光をそれぞれ受光す
る位置に取付けられた2個の受光素子とを含んで構成さ
れる。
Conventionally, this type of tilt sensor uses two light-emitting elements, and this tilt sensor consists of a homogeneous colored liquid with a constant light absorption coefficient, a transparent rectangular parallelepiped container containing this colored liquid, and a transparent rectangular parallelepiped container containing the colored liquid. , on either the top or bottom of this container, 2
Two light-emitting elements are installed at a certain distance apart so that parallel light beams of the same intensity are irradiated perpendicularly to the facing surface of the book. It is configured to include two light-receiving elements installed at positions that respectively receive the two lights that have passed through the colored liquid.

第2図は上述の傾斜センサの一例を示す構成図である。FIG. 2 is a configuration diagram showing an example of the above-mentioned tilt sensor.

第2図に示す傾斜センサは、一定の光吸収係数を持つ均
質な着色液体1と、着色液体1を内部に入れた直方体の
透明容器2と、透明容器2の下面に、2本の同じ強度の
平行な光線を対面に対して垂直に照射するように、一定
間隔を離して取付けられた2個の発光素子としてのレー
ザダイオード(以下LDという)9およびLDIOと、
透明容器2の上面にLD9およびLDIOから照射され
、着色液体lを通過した2本の光をそれぞれ受光するよ
うに取付けられた2個の受光素子(以下PDという)4
およびPD5とを含んで構成される。
The tilt sensor shown in Fig. 2 consists of a homogeneous colored liquid 1 with a constant light absorption coefficient, a transparent rectangular parallelepiped container 2 containing the colored liquid 1, and two tubes of equal strength on the bottom surface of the transparent container 2. A laser diode (hereinafter referred to as LD) 9 and LDIO as two light emitting elements installed at a certain distance so as to irradiate parallel light beams perpendicularly to the facing surface;
Two light receiving elements (hereinafter referred to as PD) 4 are attached to the upper surface of the transparent container 2 so as to receive the two beams of light irradiated from the LD 9 and LDIO and passed through the colored liquid 1, respectively.
and PD5.

以上の構成において、透明容器2が水平に対し角度θ傾
斜したとき、LD9から照射された光線が着色液体1を
通る長さをH1、LDIOから照射された光線が着色液
体1を通る長さをH2とし、LD9とLDIOとの距離
をDとする。また、LD9とLDIOとから照射される
光線の強度を共にφ。、PD4で受光する光線の強度を
φいPD5で受光する光線の強度をφ2とし、着色液体
1の光吸収係数をμとする。このとき、一定の光吸収係
数を持つ物質を通過した光の強度は、物質の厚さに指数
的に減衰していく性質がある(ランバートの法則)。そ
こで(1)式および(2)式が成立する。
In the above configuration, when the transparent container 2 is tilted at an angle θ with respect to the horizontal, H1 is the length of the light beam emitted from the LD9 passing through the colored liquid 1, and H1 is the length of the light beam emitted from the LDIO passing through the colored liquid 1. Let H2 be the distance between LD9 and LDIO. Also, both the intensities of the light beams emitted from LD9 and LDIO are set to φ. , the intensity of the light beam received by PD4 is φ2, the intensity of the light beam received by PD5 is φ2, and the light absorption coefficient of the colored liquid 1 is μ. At this time, the intensity of light passing through a material with a constant light absorption coefficient has the property of attenuating exponentially with the thickness of the material (Lambert's law). Therefore, equations (1) and (2) hold true.

φ,=φ。e−1・            ・・・・
・・(1)φ2=φ。e1H″           
  ・・・・・・(2)また、幾何学的に(3)式が成
立する。
φ,=φ. e-1...
...(1)φ2=φ. e1H''
(2) Also, equation (3) holds true geometrically.

l tanθ=   (H2Hl) D よって、(1)〜(3)式より、(4)式が導かれる。l tanθ= (H2Hl) D Therefore, formula (4) is derived from formulas (1) to (3).

・・・・・・(3) ここで、PD4の出力aの値を工、、PD5の出力bの
値を■2とすると、工、および工,はそれぞれφ1およ
びφ2に比例した値なので、(4)式はとなり、■,お
よびI2を測定することで、角度θを求めることができ
る。
......(3) Here, if the value of the output a of PD4 is , and the value of the output b of PD5 is 2, then , and , are values proportional to φ1 and φ2, respectively, so Equation (4) becomes, and by measuring ■ and I2, the angle θ can be determined.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上述した従来の傾斜センサは、着色液体を通過する2本
の光の減衰量の違いにより傾斜の角度を検出するが、2
本の光の照射源が別々の発光素子となっているので、発
光素子の経時ドリフトや特性の違いにより、発光時の光
強度が2本の光で異なってしまい、減衰量が正しく計算
されないために、検出した傾斜の角度に誤差が生じるこ
とがあるという欠点がある。
The conventional tilt sensor described above detects the tilt angle based on the difference in the amount of attenuation of two beams of light passing through the colored liquid.
Since the irradiation source of the book's light is a separate light emitting element, due to the drift over time and differences in the characteristics of the light emitting elements, the light intensity when emitted will differ between the two lights, and the amount of attenuation will not be calculated correctly. However, there is a drawback that an error may occur in the detected angle of inclination.

〔課題を解決するための手段〕[Means to solve the problem]

本発明の傾斜センサは、一定の光吸収係数を持つ均質な
着色液体と、この着色液体を入れた透明な直方体容器と
、1個の発光素子からの光を同一強度の2本の光に分割
し、その2本の光を一定間隔離して前記直方体容器の上
下いづれかの面から対面に垂直に照射する光照射部と、
前記直方体容器の前記光照射部と対面側にあってこの光
照射部から照射され前記着色液体を通過した2本の光を
それぞれ受光する位置に取付けられた2個の受光素子と
を含むことにより構成される。
The tilt sensor of the present invention consists of a homogeneous colored liquid with a constant light absorption coefficient, a transparent rectangular parallelepiped container containing the colored liquid, and a light emitting element that splits light into two beams of the same intensity. and a light irradiation unit that separates the two lights for a certain period of time and irradiates the rectangular parallelepiped container vertically from either the upper or lower surface to the opposite side;
and two light receiving elements installed at positions facing the light irradiation part of the rectangular parallelepiped container and respectively receiving two lights irradiated from the light irradiation part and passed through the colored liquid. configured.

〔実旅例〕[Actual travel example]

次に、本発明の実施例について図面を参照して詳細に説
明する。
Next, embodiments of the present invention will be described in detail with reference to the drawings.

第1図は本発明の一実施例を示す構成図である。FIG. 1 is a block diagram showing an embodiment of the present invention.

第1図に示す傾斜センサは、一定の光吸収係数を持つ均
質な着色液体1と、着色液体1を内部に入れた直方体の
透明容器2と、透明容器2の下面に取付けられ、同一強
度の平行な2本の光線を対面に垂直に照射する光照射部
3と、透明容器2の上面にあって、光照射部3から照射
され着色液体1を通過した2本の光を、それぞれ受光す
る位置に取付けられた2個のPD4およびPD5とを含
んで構成される。光照射部3は、発光素子としての1個
のLD6と、LD6から照射された光を2本の光に分割
し、その2本の光の強度の割合を調整できる可変ビーム
スプリッタ(以下A B .Sという)7と、ABS7
で分割された2本の光を折返して、透明容器2の上面に
対し垂直な2本の平行光線とする3枚の折返しミラー8
a,8bおよび8cとで構成される。
The tilt sensor shown in FIG. 1 includes a homogeneous colored liquid 1 having a constant light absorption coefficient, a rectangular transparent container 2 containing the colored liquid 1, and a rectangular parallelepiped transparent container 2 that is attached to the bottom surface of the transparent container 2. A light irradiation unit 3 that irradiates two parallel light beams perpendicularly to each other facing each other, and a light irradiation unit 3 that is located on the top surface of the transparent container 2 and receives two rays of light that have been irradiated from the light irradiation unit 3 and passed through the colored liquid 1, respectively. It is configured to include two PD4 and PD5 attached to the position. The light irradiation unit 3 includes one LD 6 as a light emitting element and a variable beam splitter (hereinafter referred to as A B .S)7 and ABS7
three folding mirrors 8 which fold back the two beams of light split by
a, 8b and 8c.

以上の構成において、光照射部3から照射される2本の
平行光線の強度は、ABS7を調整することにより、折
返しミラー8a,8bおよび8Cで反射された後、着色
液体1を通過する前の時点で1:1になるようにする。
In the above configuration, by adjusting the ABS 7, the intensity of the two parallel light beams irradiated from the light irradiation unit 3 can be adjusted by adjusting the intensity of the two parallel light beams after being reflected by the folding mirrors 8a, 8b and 8C and before passing through the colored liquid 1. Make it 1:1 at this point.

透明容器2が水平に対し角度θ傾斜したとき、光照射部
3から照射される2本の平行光線のうち一方が着色液体
1を通る長さをH1、もう一方の光線が着色液体1を通
る長さをH2とし、2本の平行光線間の距離をDとする
。また、2本の平行光線の着色液体1を通過する前の強
度をφいPD5で受光する光線の強度をφいPD6で受
光する光線の強度をφ2とし、着色液体1の光吸収係数
をμとする。またPD4の出力aの値を工、、PD5の
出力bの値を工,とすると、上述の従来の技術で説明し
たと同じに、 となり、It,I2を測定することで角度θを求めるこ
とができる。
When the transparent container 2 is tilted at an angle θ with respect to the horizontal, the length of one of the two parallel light beams emitted from the light irradiation unit 3 passing through the colored liquid 1 is H1, and the length of the other light beam passing through the colored liquid 1 is H1. Let the length be H2 and the distance between the two parallel rays be D. In addition, the intensity of the two parallel light beams before passing through the colored liquid 1 is φ, the intensity of the light beam received by the PD5 is φ, the intensity of the light beam received by the PD6 is φ2, and the light absorption coefficient of the colored liquid 1 is μ. shall be. Also, if the value of the output a of PD4 is , and the value of the output b of PD5 is , then as explained in the above conventional technology, the angle θ can be found by measuring It and I2. I can do it.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明の傾斜センサは、着色液体を
通過する2本の光の減衰量の違いから傾斜角を検出する
が、その2本の光の照射源を2個の別々な発光素子とす
る代りに、1個の発光素子の光を2本に分割して照射す
るため、発光素子の経時ドリフトや特性の違いによる光
強度のばらつきがなくなり、誤差のない傾斜値が得られ
るという効果がある。
As explained above, the inclination sensor of the present invention detects the inclination angle from the difference in the amount of attenuation of the two lights passing through the colored liquid. Instead, the light from one light emitting element is divided into two beams and irradiated, which eliminates variations in light intensity due to drift over time or differences in characteristics of the light emitting elements, and provides an error-free slope value. There is.

4

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

第1図は本発明の一実施例の構成図、第2図は従来の傾
斜センサの一例の構成図である。 1・・・・・着色液体、2・・・・・・透明容器、3・
・・・・・光照射部、4.5−・・−受光素子(P D
)、6,9.10−・・・・レーザタイオード(LD)
、7・・・・・・可変ビームスプリッタ(ABS)、8
 a, 8 b, 8 c−−折返しミラ
FIG. 1 is a block diagram of an embodiment of the present invention, and FIG. 2 is a block diagram of an example of a conventional tilt sensor. 1... Colored liquid, 2... Transparent container, 3...
・・・・Light irradiation part, 4.5-・・・Photo-receiving element (P D
), 6, 9.10-... Laser diode (LD)
, 7... variable beam splitter (ABS), 8
a, 8 b, 8 c--Folding mirror

Claims (1)

【特許請求の範囲】[Claims] 一定の光吸収係数を持つ均質な着色液体と、この着色液
体を入れた透明な直方体容器と、1個の発光素子からの
光を同一強度の2本の光に分割し、その2本の光を一定
間隔離して前記直方体容器の上下いづれかの面から対面
に垂直に照射する光照射部と、前記直方体容器の前記光
照射部と対面側にあってこの光照射部から照射され前記
着色液体を通過した2本の光をそれぞれ受光する位置に
取付けられた2個の受光素子とを含むことを特徴とする
傾斜センサ。
A homogeneous colored liquid with a constant light absorption coefficient, a transparent rectangular parallelepiped container containing this colored liquid, and a light emitting element that splits the light into two beams of the same intensity. a light irradiation section that irradiates vertically to the opposite surface from either the upper or lower surface of the rectangular parallelepiped container while separating the liquid for a certain period of time; A tilt sensor comprising: two light-receiving elements mounted at positions that respectively receive two passing beams of light.
JP1391790A 1990-01-23 1990-01-23 Inclination sensor Pending JPH03216514A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1391790A JPH03216514A (en) 1990-01-23 1990-01-23 Inclination sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1391790A JPH03216514A (en) 1990-01-23 1990-01-23 Inclination sensor

Publications (1)

Publication Number Publication Date
JPH03216514A true JPH03216514A (en) 1991-09-24

Family

ID=11846524

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1391790A Pending JPH03216514A (en) 1990-01-23 1990-01-23 Inclination sensor

Country Status (1)

Country Link
JP (1) JPH03216514A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5583867B1 (en) * 2014-03-04 2014-09-03 実 山本 Green tilt measuring instrument
JP5638719B1 (en) * 2014-07-14 2014-12-10 山本 実 Green tilt measuring instrument

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5583867B1 (en) * 2014-03-04 2014-09-03 実 山本 Green tilt measuring instrument
JP5638719B1 (en) * 2014-07-14 2014-12-10 山本 実 Green tilt measuring instrument

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