JPH0399295A - Indicating device for vehicle - Google Patents

Indicating device for vehicle

Info

Publication number
JPH0399295A
JPH0399295A JP23461389A JP23461389A JPH0399295A JP H0399295 A JPH0399295 A JP H0399295A JP 23461389 A JP23461389 A JP 23461389A JP 23461389 A JP23461389 A JP 23461389A JP H0399295 A JPH0399295 A JP H0399295A
Authority
JP
Japan
Prior art keywords
light
transparent body
incident
pointer
scattered
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
JP23461389A
Other languages
Japanese (ja)
Inventor
Shigeru Okabayashi
岡林 繁
Teruhisa Matoba
的場 照久
Masayuki Hori
雅之 堀
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.)
Nissan Motor Co Ltd
Original Assignee
Nissan Motor 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 Nissan Motor Co Ltd filed Critical Nissan Motor Co Ltd
Priority to JP23461389A priority Critical patent/JPH0399295A/en
Publication of JPH0399295A publication Critical patent/JPH0399295A/en
Pending legal-status Critical Current

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  • Details Of Measuring And Other Instruments (AREA)
  • Indicating Measured Values (AREA)

Abstract

PURPOSE:To make indication of a pointer definite by a method wherein the particle diameters of numerous minute particles as light-scattering bodies which are sealed in a panel-shaped transparent body are selected to be shorter enough than the wavelength of an incident light. CONSTITUTION:A parallel light flux 10 made to enter a transparent body 2 is scattered by light-scattering bodies 1 located in the light flux, and it can be recognized in the front 19 of an instrument panel as a light-flux scattered light 11 in the directions indicated by arrows, which shines in the shape of a rod as a whole, as if there is a pointer therein. When a lateral polarized wave 21 of which the direction of polarization is the same with the direction of the X-axis of the transparent body 2 is applied to the transparent body 2, on the occasion, it collides with the light-scattering bodies 1 located in the direction 23 of advance of the incident light (the direction of the Z-axis) and an oval pattern 24 of the scattered light is formed around the direction. This pattern 24 of the scattered light does not expand to the lateral direction to the direction of advance of the polarization wave, and therefore it can be recognized definitely as the light-flux scattered light 11 of the light flux in the shape of the rod in the front 19 of the instrument panel.

Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) この発明は、車両速度などの現況が運転者等に確認でき
る目的で装着されている無指針式アナログメータ表示装
置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Field of Application) The present invention relates to a pointer-less analog meter display device that is installed for the purpose of allowing a driver or the like to check current conditions such as vehicle speed.

(従来の技術) 従来の車両などに装着されているポインタレスいわゆる
無指針式アナログメータ表示装置、例えば、車両のスピ
ードメータ(速度計)としては第5図及び第6図に示す
ようなものがある。
(Prior Art) Conventional pointerless analog meter display devices installed in vehicles, such as vehicle speedometers, are shown in Figures 5 and 6. be.

このように速度計は、多数の光の散乱体1が封入された
アクリル樹脂製の平板パネル状の透明体2と、その上に
設けられた文字盤3と指針変換部4とから構成されてい
る。
In this way, the speedometer is composed of a flat panel-shaped transparent body 2 made of acrylic resin in which a large number of light scatterers 1 are sealed, and a dial 3 and a pointer converter 4 provided thereon. There is.

第6図に指針変換部4の基本構造を示す。FIG. 6 shows the basic structure of the pointer converter 4.

この指針変換部4は、車両の速度に応じて回転するモー
タ5と、これと連結軸6で結ばれ回転運動する回転鏡7
とコリメータレンズA9と、レーザダイオード8とから
構成されている。
This pointer conversion unit 4 includes a motor 5 that rotates according to the speed of the vehicle, and a rotating mirror 7 that is connected to the motor 5 by a connecting shaft 6 and rotates.
, a collimator lens A9, and a laser diode 8.

つぎに、作用について説明する。Next, the effect will be explained.

このように構成された速度計において、レーザダイオー
ド8から発光されるレーザ丸線は、コリメータレンズA
9で平行な光線のビームすなわち平行光束10に交換さ
れ、回転鏡7に照射される。
In the speedometer configured in this way, the laser round wire emitted from the laser diode 8 is connected to the collimator lens A.
At 9, the light is exchanged into a parallel beam of light, that is, a parallel light beam 10, and is irradiated onto the rotating mirror 7.

回転鏡7に入射された平行光束10は、回転鏡7が、車
両の速度に連動して回転するモータ5により、時々刻々
回転運動するようにモータ5と連結軸6により結ばれて
いるため、入射時点での角度すなわち車速に相当する角
度で入射されて、光の散乱体1の封入されている透明体
2に反射した平行光束10として照射されている。透明
体2に入射した平行光束10は、光が波長より小さい分
子や原子に衝突して方向を変える現象、つまり“散乱”
を散乱体1が分散封入された透明体2の内部で起す。こ
の散乱は、入射した平行光束10が入射された範囲内の
散乱体1と衝突して定めのない方向に向きを変える現象
を起こすため、棒状に光り輝く矢印の方向の光束散乱光
11として、あたかも指針があるかのように計器板前面
19でドライバの目25により認知できるのである。
The parallel light beam 10 incident on the rotating mirror 7 is connected to the motor 5 by the connecting shaft 6 so that the rotating mirror 7 rotates momentarily by the motor 5, which rotates in conjunction with the speed of the vehicle. The light is incident at the angle at the time of incidence, that is, at an angle corresponding to the vehicle speed, and is irradiated as a parallel light beam 10 reflected on the transparent body 2 in which the light scatterer 1 is enclosed. The parallel light beam 10 incident on the transparent body 2 is caused by a phenomenon in which the light collides with molecules or atoms smaller than the wavelength and changes its direction, that is, "scattering".
occurs inside the transparent body 2 in which the scatterer 1 is dispersed and sealed. This scattering causes a phenomenon in which the incident parallel light beam 10 collides with the scatterer 1 within the incident range and changes its direction in an undetermined direction. It can be recognized by the driver's eyes 25 on the front surface 19 of the instrument panel as if there were a pointer.

(発明が解決しようとする課題) しかしながら、このような従来の無指針式アナログメー
タ表示装置においては、既存の指針式アナログメータ表
示装置の指針と同じような認知感覚、すなわち、指針に
よる表示の明確さも要望されている。この要望に対応す
る方法として、レーザ光線の出力をあげる、すなわち、
照度を強くする方法をとれば目的は達成されるがもじれ
ないのであるが、前述したごとく、平行光束1oが散乱
体1に照射されて発生する散乱光は、方向の定めがない
ため、この光束散乱光(即ちポインタ部)11の周囲に
平行光束10の照度に応じた半明輝部となって輝き、計
器板前面19がらみると視覚的には横方向の符号12と
して示される“にじみ”いわゆるフレア現象が発生した
ものとなる。このフレア現象は、二次散乱光12が光束
散乱光11の光路内の光散乱体1から発生するためで、
光源のレーザダイオード8の照度の増減に比例し、照度
を増加させると光散乱光11の散乱光量も増加し、指針
としての明確さも強くなるがこれと同時に光束散乱光1
1の周囲の二次散乱光12も増加することとなる。した
がって、この光束散乱光11の明確さは、この二次散乱
光12が原因で光源照度の増減では解決できないという
問題がある。
(Problem to be Solved by the Invention) However, in such conventional pointer-less analog meter display devices, the same cognitive feeling as the pointer of the existing pointer-type analog meter display device, that is, the clarity of the indication by the pointer. This is also requested. As a method to meet this demand, increasing the output of the laser beam, that is,
If the method of increasing the illuminance is used, the objective can be achieved without any problems, but as mentioned above, the scattered light generated when the parallel light beam 1o is irradiated onto the scatterer 1 has no fixed direction. Around the scattered light beam (i.e., the pointer portion) 11, a semi-bright bright area corresponding to the illuminance of the parallel light beam 10 shines, and when viewed from the front surface of the instrument panel 19, it visually shows "bleeding" as a horizontal symbol 12. This means that a so-called flare phenomenon has occurred. This flare phenomenon occurs because the secondary scattered light 12 is generated from the light scatterer 1 in the optical path of the light flux scattered light 11.
It is proportional to the increase/decrease in the illuminance of the laser diode 8 as the light source, and as the illuminance increases, the amount of scattered light 11 also increases, and the clarity as a guide becomes stronger, but at the same time, the scattered light 11
The secondary scattered light 12 around 1 also increases. Therefore, there is a problem in that the clarity of this luminous flux scattered light 11 cannot be solved by increasing or decreasing the light source illuminance due to this secondary scattered light 12.

第5図は、このフレア現象すなわち二次散乱光12の現
況を示した例である。
FIG. 5 is an example showing the current state of this flare phenomenon, that is, the secondary scattered light 12.

さらに、夜間やトンネル等の環境下での車両等の運転の
際、計器板前面19の全体が、この二次散乱光12によ
り半明輝状態となり、光束散乱光11や数値の認知が不
明確となり表示品質の低下を招くという問題点もあった
。そこで、この発明は二次散乱光によりぼける事のない
明確な光束による表示の得られる車両用表示装置を提供
し、もって前記問題を解決する事を目的とする。
Furthermore, when driving a vehicle at night or in an environment such as a tunnel, the entire front surface of the instrument panel 19 becomes semi-bright due to the secondary scattered light 12, making it unclear to recognize the luminous flux scattered light 11 and numerical values. There was also the problem that display quality deteriorated. SUMMARY OF THE INVENTION An object of the present invention is to provide a display device for a vehicle that can display a clear luminous flux that is not blurred by secondary scattered light, thereby solving the above problem.

[発明の構成] (課題を解決するための手段) この発明は、前記目的を達成するため、車両等に積載さ
れる無指針式アナログメータ表示装置においてパネル状
の透明体に封入される多数の光の散乱体としての微小粒
体の粒子直径を、入射光波長より十分に短かい長さに選
定し、かつ、前記入射光が前記透明体の側面から入射さ
れる散乱手段と、前記散乱手段への入射光が透明体の表
面に平行な偏光方向を持つ光線として入射される偏光手
段を有する構成としたものである。
[Structure of the Invention] (Means for Solving the Problems) In order to achieve the above-mentioned object, the present invention provides a method for achieving the above-mentioned object by incorporating a large number of points enclosed in a panel-shaped transparent body in a pointer-less analog meter display device mounted on a vehicle or the like. a scattering means in which the diameter of the microparticles as a light scatterer is selected to be sufficiently shorter than the wavelength of the incident light, and the incident light enters from a side surface of the transparent body; and the scattering means The structure includes a polarizing means so that the incident light is incident as a light beam having a polarization direction parallel to the surface of the transparent body.

(作用) 散乱手段への入射光が透明体表面に平行な偏光方向を持
っており、かつ、前記入射光は透明ていの側面から入射
される。更に透明体内封入の散乱体の粒子直径が入射光
波長に比して格段と短かい長さに選定されているため、
入射光が衝突して生ずる散乱光は偏光方向での散乱の幅
が小さいもの、即ち、入射光が横に広がらないものとな
る為、その表示は明確なポインタ部としてドライバの目
に達する。
(Function) The incident light to the scattering means has a polarization direction parallel to the surface of the transparent body, and the incident light is incident from the side surface of the transparent body. Furthermore, since the particle diameter of the scatterer enclosed in the transparent body is selected to be much shorter than the wavelength of the incident light,
The scattered light generated by the collision of the incident light has a small scattering width in the polarization direction, that is, the incident light does not spread laterally, so the display reaches the driver's eyes as a clear pointer.

(実施例) 以下、この発明の一実施例を第1図〜第3図に基づいて
説明する。
(Example) Hereinafter, an example of the present invention will be described based on FIGS. 1 to 3.

まず、構成を説明すると、車両の速度に応じて回転する
モータ5とこれと連結軸6で結ばれ回転運動する偏光板
13の付設された回転鏡14とコリメータレンズA9、
レーザダイオード8、透明体2から構成されており、こ
の透明体2中にTiO2等の光散乱体1が多数閉じこめ
られている。
First, to explain the configuration, there is a motor 5 that rotates according to the speed of the vehicle, a rotating mirror 14 connected to the motor 5 by a connecting shaft 6 and equipped with a polarizing plate 13 that rotates, and a collimator lens A9.
It is composed of a laser diode 8 and a transparent body 2, and a large number of light scatterers 1 such as TiO2 are confined in this transparent body 2.

この、散乱体の直径aは使用する光の波長λに較ベて十
分に小さく構成しである。又、使用する光線は透明体2
の表面19に平行な偏光方向を持つように偏光板13に
より変換入射されるものである。例えば波長λは570
nm、直径aは30μmである。
The diameter a of this scatterer is configured to be sufficiently small compared to the wavelength λ of the light used. Also, the light beam used is transparent body 2
The incident light is converted by the polarizing plate 13 so that the polarization direction is parallel to the surface 19 of the light beam. For example, the wavelength λ is 570
nm, and the diameter a is 30 μm.

次に作用を第2図及び第3図をも参照して説明する。こ
のように構成された速度計において、レーザダイオード
8から発射されるレーザ光線は、コリロータレンズA9
で平行光束1oに変換され、回転鏡14に入射される。
Next, the operation will be explained with reference to FIGS. 2 and 3. In the speedometer configured in this way, the laser beam emitted from the laser diode 8 passes through the co-rotor lens A9.
The parallel light beam 1o is converted into a parallel light beam 1o, and is incident on the rotating mirror 14.

回転鏡14が車の速度に連動して回転するモータ5によ
り時々刻々回転運動するように、モータ5と連結軸6に
より結ばれているため、入射時点での角度すなわち車速
に相当する角度で偏光板13で反射され、そのとき、透
明体2には横波λの波長の平行光束1oとして入射され
る。透明体2に入射された平行光束1゜は、光束の範囲
内の光散乱体1により散乱され、全体として棒状に光り
輝く矢印方向の光束散乱光11として、あたかも指針が
あるがのように計器板前面19で認知できるのである。
Since the rotating mirror 14 is connected to the motor 5 by a connecting shaft 6 so as to be rotated every moment by the motor 5, which rotates in conjunction with the speed of the car, the light is polarized at the angle at the time of incidence, that is, at the angle corresponding to the speed of the car. It is reflected by the plate 13, and at that time, it enters the transparent body 2 as a parallel light beam 1o having the wavelength of the transverse wave λ. The parallel light beam 1° incident on the transparent body 2 is scattered by the light scattering body 1 within the range of the light beam, and as a whole shines in a rod shape as a light beam scattered light 11 in the direction of the arrow, it appears on the instrument panel as if there were a pointer. It can be recognized from the front 19.

その際、前述の如<TiO2等の光の散乱体1の粒子の
直径を3μm1使用するレーザ光線の波長をλnmとし
、粒子の直径aumを波長λnmに比べて2×104以
下の微粒子であるa(λとした条件のもとでは、散乱さ
れている光エネルギは、波長の4乗に逆比例し、短波長
はど強く散乱される、第2図に示すようなレーリー散乱
(Rayleigh  Scattering)となる
At that time, as described above, the diameter of the particles of the light scattering material 1 such as TiO2 is 3 μm1, the wavelength of the laser beam used is λnm, and the particle diameter aum is 2×104 or less fine particles compared to the wavelength λnm. (Under the condition of λ, the scattered light energy is inversely proportional to the fourth power of the wavelength, and short wavelengths are scattered more strongly than Rayleigh scattering as shown in Figure 2.) Become.

即ち、第2図において、(a)に示すように偏光のない
(ランダムな偏向方向を有する)標準波が散乱体1に衝
突すると散乱光は球状に全面反射するが、(b)に示す
ように偏光方向がそろった光が散乱体1に衝突すると散
乱光は断面8の字状で偏光面(表面19と平行な面)内
に幅Bを持ち、矢印方向に直径りを持つドーナツ形状(
0図参照)のようになる。直径D〉幅Bである。従って
、(d)図に示すようにパネル状透明体2の側面に偏向
方向がそろった光が投入されると散乱体1に衝突してで
きる散乱波は透明体前面19に直角な方向には直径りの
ものとして散乱するが、それと直角な方向には広がらな
いものとなる。
That is, in Fig. 2, when a standard wave without polarization (having a random polarization direction) collides with the scatterer 1 as shown in (a), the scattered light is totally reflected in a spherical shape, but as shown in (b), When light with the same polarization direction collides with the scatterer 1, the scattered light has a figure-eight cross section, a width B in the polarization plane (plane parallel to the surface 19), and a donut shape with a diameter in the direction of the arrow.
(See Figure 0). Diameter D>width B. Therefore, as shown in figure (d), when light with the same polarization direction is incident on the side surface of the panel-shaped transparent body 2, the scattered waves generated by colliding with the scatterer 1 will not be reflected in the direction perpendicular to the front surface 19 of the transparent body. It is scattered as a diameter, but it does not spread in the direction perpendicular to it.

かくして第3図に示すように、入射光の偏光方向が透明
体2のX軸の方向と同方向の波長である横偏光波21が
透明体2に照射されると、入射光の進行方向23(Z軸
方向)の光の散乱体1と衝突し、その周囲にy軸押ち計
器板面前19の面に向く方向の8の字状に強く輝き全体
としてやや偏平楕円状の散乱光模様24が生ずる。この
散乱模様24は偏光波の進行方向の横方向には拡がらな
いものであるため、計器板前面19に棒状の光束の光束
散乱11として明確に認知できるものとなるものである
Thus, as shown in FIG. 3, when the transparent body 2 is irradiated with a horizontally polarized light wave 21 whose polarization direction is the same wavelength as the X-axis direction of the transparent body 2, the traveling direction 23 of the incident light is irradiated onto the transparent body 2. The light collides with the light scatterer 1 (in the Z-axis direction), and a scattered light pattern 24 that shines strongly in the shape of a figure 8 in the direction facing the front 19 of the Y-axis instrument panel is generated around it, with a slightly oblate elliptical shape as a whole. occurs. Since this scattering pattern 24 does not spread in the lateral direction of the polarized wave traveling direction, it can be clearly recognized as a bar-shaped light flux scattering 11 on the front surface of the instrument panel 19.

第4図には、他の実施例を示す。FIG. 4 shows another embodiment.

この実施例の構成を説明すると、車両の速度に応じて回
転するモータ5とこれと連結軸6で結ばれ回転運動する
偏光面保存光ファイババンドル15が装着された回転板
16、コリメータレンズA9、レーザダイオード8、透
明体2の側面に設けられた溝18の内に収納されている
コリメータレンズB17および透明体2から構成されて
いる。
To explain the configuration of this embodiment, a motor 5 that rotates according to the speed of the vehicle, a rotary plate 16 connected to the motor 5 by a connecting shaft 6 and equipped with a polarization preserving optical fiber bundle 15 that rotates, a collimator lens A9, It is composed of a laser diode 8, a collimator lens B17 housed in a groove 18 provided on the side surface of the transparent body 2, and the transparent body 2.

散乱体1の直径及び入射光波長との関係及び入射光の偏
光方向は前実施例と同じである。この実施例では光フア
イババンドル15が透明体2の溝18内に入っているの
で光の洩れが少なく光の結合率を向上させることができ
る効果がある他、前実施例と同様の作用効果を奏する。
The relationship between the diameter of the scatterer 1 and the wavelength of the incident light and the polarization direction of the incident light are the same as in the previous embodiment. In this embodiment, since the optical fiber bundle 15 is placed in the groove 18 of the transparent body 2, the light leakage is reduced and the light coupling rate can be improved, and the same effects as in the previous embodiment are achieved. play.

[発明の効果] 以上、説明してきたように、この発明によれば、その構
成を車両等に積載される無指針式アナログメータ表示装
置において、パネル状の透明体に封入される多数の光の
散乱体としての微小粒体の粒子直径を、入射光波長より
十分に短かい長さに選定し、かつ、前記入射光が前記透
明体の側面がら入射される散乱手段と、前記散乱手段へ
の入射光が透明体の表面に平行な偏光方向を持つ光線と
して入射される偏光手段を有する構成としたため、指針
表示が明確になり、従来の無指針式アナログメータ表示
装置に見られた二次以上の散乱に起因する指針部相当の
光束散乱光の不鮮明さや夜間などの環境での計器のパネ
ル全面が薄明るく輝くときの表示数値の読み取りにくさ
、また、全体的な表示品質の低下を防止することができ
るという効果が得られる。
[Effects of the Invention] As described above, according to the present invention, the configuration of a pointerless analog meter display device mounted on a vehicle etc. is such that a large number of lights enclosed in a panel-shaped transparent body can be used. The particle diameter of the microparticles as a scatterer is selected to be sufficiently shorter than the wavelength of the incident light, and the incident light is incident on a side surface of the transparent body, and a scattering means is provided. Since the structure has a polarizing means in which the incident light is incident as a light beam with a polarization direction parallel to the surface of the transparent body, the pointer display becomes clearer, and the second order or higher order seen in conventional pointerless analog meter display devices is used. Prevents the blurring of the scattered light equivalent to the pointer section due to scattering of light, the difficulty in reading displayed values when the entire surface of the instrument panel shines dimly brightly in environments such as nighttime, and the deterioration of the overall display quality. You can get the effect that you can.

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

第1図は、本発明による無指針式アナログメータ表示装
置の一実施例の基本構成斜視図、第2図は、本発明によ
るレーり散乱の原理説明図、第3図は第1図の作用を示
す散乱光模様説明図、第4図は、本発明による他の実施
例の構成斜視図、第5図は、従来の無指針式アナログメ
ータ表示装置の一例である速度計の正面図、第6図は、
従来の無指針式アナログメータ表示装置の一例で、指針
変換部の基本構成斜視図である。 1・・・散乱体    2・・・透明体3・・・文字盤
    4・・・指針変換部5・・・モータ    6
・・・連結軸7・・・回転鏡    8・・・レーザダ
イオード9・・・コリメータレンズA 10・・・平行光束   12・・・二次散乱光13・
・・偏光板 14・・・偏光板の付設された回転鏡 15・・・偏光面保存光ファイバ
FIG. 1 is a perspective view of the basic configuration of an embodiment of a pointer-less analog meter display device according to the present invention, FIG. 2 is a diagram illustrating the principle of Ray scattering according to the present invention, and FIG. 3 is the effect of FIG. 1. 4 is a perspective view of the configuration of another embodiment of the present invention, and FIG. 5 is a front view of a speedometer, which is an example of a conventional pointerless analog meter display device. Figure 6 is
FIG. 2 is a perspective view of the basic configuration of a pointer converter, which is an example of a conventional pointerless type analog meter display device. 1...Scatterer 2...Transparent body 3...Dial 4...Pointer converter 5...Motor 6
...Connection shaft 7...Rotating mirror 8...Laser diode 9...Collimator lens A 10...Parallel light flux 12...Secondary scattered light 13.
...Polarizing plate 14...Rotating mirror 15 attached with a polarizing plate...Polarization plane preserving optical fiber

Claims (1)

【特許請求の範囲】[Claims] (1)車両等に積載される無指針式アナログメータ表示
装置において、パネル状の透明体に封入される多数の光
の散乱体としての微小粒体の粒子直径を、入射光波長よ
り十分に短かい長さに選定し、かつ、前記入射光が前記
透明体の側面から入射される散乱手段と前記散乱手段へ
の入射光が透明体の表面に平行な偏光方向を持つ光線と
して入射される偏光手段を有することを特徴とする車両
用表示装置。
(1) In pointer-less analog meter display devices installed on vehicles, etc., the particle diameter of the many microscopic particles that act as light scatterers enclosed in a panel-shaped transparent body is set to be sufficiently shorter than the wavelength of the incident light. a scattering means for making the incident light enter from a side surface of the transparent body; and polarization for making the incident light incident on the scattering means as a light beam having a polarization direction parallel to the surface of the transparent body. A display device for a vehicle, characterized in that it has a means.
JP23461389A 1989-09-12 1989-09-12 Indicating device for vehicle Pending JPH0399295A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23461389A JPH0399295A (en) 1989-09-12 1989-09-12 Indicating device for vehicle

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23461389A JPH0399295A (en) 1989-09-12 1989-09-12 Indicating device for vehicle

Publications (1)

Publication Number Publication Date
JPH0399295A true JPH0399295A (en) 1991-04-24

Family

ID=16973790

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23461389A Pending JPH0399295A (en) 1989-09-12 1989-09-12 Indicating device for vehicle

Country Status (1)

Country Link
JP (1) JPH0399295A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008051342A (en) * 2007-10-29 2008-03-06 Smc Corp Pipe coupling
JP2010071907A (en) * 2008-09-22 2010-04-02 Nippon Seiki Co Ltd Display device for vehicle

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008051342A (en) * 2007-10-29 2008-03-06 Smc Corp Pipe coupling
JP2010071907A (en) * 2008-09-22 2010-04-02 Nippon Seiki Co Ltd Display device for vehicle

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