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JPS5831339Y2 - Specific gravity detector for storage batteries - Google Patents

Specific gravity detector for storage batteries

Info

Publication number
JPS5831339Y2
JPS5831339Y2 JP5555077U JP5555077U JPS5831339Y2 JP S5831339 Y2 JPS5831339 Y2 JP S5831339Y2 JP 5555077 U JP5555077 U JP 5555077U JP 5555077 U JP5555077 U JP 5555077U JP S5831339 Y2 JPS5831339 Y2 JP S5831339Y2
Authority
JP
Japan
Prior art keywords
light
specific gravity
refractive index
receiving element
angle
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
JP5555077U
Other languages
Japanese (ja)
Other versions
JPS53149821U (en
Inventor
一樹 谷
Original Assignee
日本電池株式会社
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 日本電池株式会社 filed Critical 日本電池株式会社
Priority to JP5555077U priority Critical patent/JPS5831339Y2/en
Publication of JPS53149821U publication Critical patent/JPS53149821U/ja
Application granted granted Critical
Publication of JPS5831339Y2 publication Critical patent/JPS5831339Y2/en
Expired legal-status Critical Current

Links

Classifications

    • Y02E60/12

Landscapes

  • Secondary Cells (AREA)

Description

【考案の詳細な説明】 本考案は蓄電池の電解液の比重を計る比重検出器に関す
るものである。
[Detailed Description of the Invention] The present invention relates to a specific gravity detector that measures the specific gravity of an electrolyte in a storage battery.

一般に蓄電池の電解液の比重は、電池の状態と密接な関
係があり、特に鉛電池においては、残存容量を知るため
には比重を計測すれば良い。
In general, the specific gravity of the electrolyte in a storage battery has a close relationship with the battery condition, and in lead batteries in particular, the remaining capacity can be determined by measuring the specific gravity.

そのため従来より、簡便に比重を計るために種々の装置
が考案されている。
Therefore, various devices have been devised to easily measure specific gravity.

電解液濃度即ち比重の変化により、電解液の屈折率が変
化するのに着目して、発光部と受光部を併用し、光量変
化を電気信号として取り出す方法もその一つであるが、
屈折率の変化が極めて微少であるため未だに実用化され
ていないのが現状である。
One method is to take note of the fact that the refractive index of the electrolyte changes with changes in the electrolyte concentration, that is, the specific gravity, and use a light emitting part and a light receiving part together to extract changes in the amount of light as an electrical signal.
At present, it has not yet been put into practical use because the change in refractive index is extremely small.

この屈折率の変化を検出する方式のものは、浮子の浮力
を検出する方式のものに比べて、電解液液面の変化、動
揺等の影響を全く受けないという利点を有することが考
えられる。
It is thought that the method of detecting changes in the refractive index has an advantage over the method of detecting the buoyancy of the float in that it is completely unaffected by changes in the electrolyte level, fluctuations, etc.

また、光電変換によって極めて簡単に遠隔操作で比重の
表示ができるという利点がある。
Another advantage is that the specific gravity can be displayed extremely easily by remote control using photoelectric conversion.

本考案の目的は簡単な構造で、しかも簡便に電解液の比
重を屈折率の変化として検出する比重計を得ることにあ
る。
The purpose of the present invention is to obtain a hydrometer that has a simple structure and that can easily detect the specific gravity of an electrolytic solution as a change in refractive index.

前記の目的を達成するための本考案の要旨とするところ
は次のとおりである。
The gist of the present invention to achieve the above object is as follows.

即ち、電解液の屈折率よりも大きな屈折率を有する透明
で一様な物質によって形成された円柱又は平行な面を有
する角柱の軸方向の一端に受光部を設け、相対する一端
には前記円柱又は角柱の軸と不平行になる方向へ、ある
立体角で光を出す発光素子を設けて、電解液の屈折率が
変化すれば発光部から出て、円柱又は角柱の側面で反射
し、受光部に達する光の量が変化することを検出する比
重検出器である。
That is, a light-receiving portion is provided at one end in the axial direction of a cylinder or a prism having parallel surfaces formed of a transparent and uniform substance having a refractive index greater than that of the electrolytic solution, and the light-receiving portion is provided at one end in the axial direction of the cylinder formed of a transparent and uniform substance having a refractive index greater than that of the electrolytic solution. Alternatively, a light emitting element that emits light at a certain solid angle in a direction that is non-parallel to the axis of the prism is provided, and when the refractive index of the electrolyte changes, the light is emitted from the light emitting part, reflected on the side of the cylinder or prism, and received. This is a specific gravity detector that detects changes in the amount of light reaching the area.

次に図面に示した一実施例で鉛電池用比重検出器につい
て具体的に説明する。
Next, a specific gravity detector for a lead-acid battery will be specifically explained using an example shown in the drawings.

第1図は本考案の原理説明図であり、屈折率n1の物質
Iから屈折率n2(nl>n2)の物質IIに光が入射
した場合を示している。
FIG. 1 is a diagram explaining the principle of the present invention, and shows a case where light is incident from a substance I having a refractive index n1 to a substance II having a refractive index n2 (nl>n2).

光線Aの場合、光の反射・屈折の法則によす、一部は入
射角iに等しい反射角でA′として反射し、また一部は
次式に従ってA//として屈折角γで屈折する。
In the case of a ray A, according to the law of reflection and refraction of light, part of it is reflected as A' at a reflection angle equal to the angle of incidence i, and part of it is refracted at a refraction angle γ as A// according to the following formula: .

即ちn 、sin i = n 2sinγ・・・・・
・(1)光が屈折率の大きいものから小さいものに入る
時には屈折角は入射角より必ず大きいから、入射角を次
第に増していくと屈折角が90°になるときか′ある。
That is, n, sin i = n 2 sin γ...
(1) When light enters an object with a large refractive index and a small one, the angle of refraction is always greater than the angle of incidence, so if the angle of incidence is gradually increased, the angle of refraction will sometimes reach 90°.

これが光線Bの場合で、式(2)が成り立つ。即ちn1
sinθ=n2Sin90°= n 2−・・・−(2
)いわゆる全反射という現象であり、θを臨界角といい
、θより入射角の大きな光線は全て反射されることにな
る。
This is the case of ray B, and equation (2) holds true. That is, n1
sinθ=n2Sin90°=n 2−...−(2
) This is a phenomenon called total internal reflection, where θ is called the critical angle, and all light rays with an incident angle greater than θ are reflected.

ところで、硫酸の屈折率は20℃において、各濃度に対
し次表の如くなっている。
Incidentally, the refractive index of sulfuric acid at 20° C. is as shown in the following table for each concentration.

また屈折率が上記硫酸の屈折率)り大きい透明な物質の
1つにアクリル樹脂があるが、その屈1折率は゛メチル
エステル□で1.4032であ衣。
Acrylic resin is one of the transparent substances whose refractive index is higher than that of sulfuric acid, and its refractive index is 1.4032 for methyl ester.

l’(2)式からアクリル樹脂と水及び50%□硫酸と
の間め臨界::角を求めれば、水の場谷で71.8°、
50%硫酸では83゜8°となる′。
If we calculate the intermediate critical angle between the acrylic resin, water and 50%□sulfuric acid from equation l'(2), we find that the angle at the water point is 71.8°,
In 50% sulfuric acid, it becomes 83°8°'.

□ □ ・ ・1 − 第′2図は本考案の二実施例である比重検出器を淡い硫
酸中は入れ・た場合の光線の状況を示し:であ□
・ 1 1.1 □ 。
□ □ ・ ・1 - Figure '2 shows the state of the light beam when the specific gravity detector, which is the second embodiment of the present invention, is placed in dilute sulfuric acid.
・1 1.1 □.

る。Ru.

・・ ・ ・ 1゜1はアクリル樹脂
で出來f、= Pl’柱又は角柱であ1り一端にCdS
素子又はホトトランジスタ等の受光素子2″を:取付け
くもう−1一端にはランブゴを□取付↓すである。
・・・ ・ ・ 1゜1 is made of acrylic resin f, = Pl' is a pillar or prismatic pillar, and one end is CdS
Attach a light-receiving element 2'' such as an element or a phototransistor, and attach a lambgo to one end.

ランプ3の光線は遮光器 (三よづて、光のI中心部ち
光軸□5・に対1角度1め広′が□す;を:有する一点
鎖線範囲内の光線と、なっている□。
The light rays of lamp 3 are within the range of the dashed dot line, and have a shading device (the center of the light is the center of the light, and the optical axis □5. □.

また、□光軸は下の円柱又は角柱の軸に対し90°−傾
斜しており、ランプ3カンら出た光線が2.受光素子2
□に直接入射する量を極力抑制している。
□The optical axis is tilted at 90 degrees with respect to the axis of the lower cylinder or prism, and the light rays emitted from the three lamps are 2. Light receiving element 2
The amount directly incident on □ is suppressed as much as possible.

□ ′□第、2図(辷おい七、う・′
ンプ3:b・ら□出た光線6を1全反射の臨界とすれば
、図中α+β+δ−90°の範□囲内に出た光線は全て
受光素子2に入射する。
□ ′□Figure 2 (Touch 7, U・′
If the light rays 6 emitted from the amplifier 3: b and □ are considered as the critical point for one total reflection, all the light rays emitted within the range □ of α+β+δ−90° in the figure enter the light-receiving element 2.

界面・に対し、□臨界角以上の入射角で入射した光線は
、1.図中破線で示す光軸方向の光線の如く、反射と屈
折を操り返して進む7Si、界面で一部□が屈゛折され
る夫め、次第に減衰し七行く。
A ray incident on the interface □ at an angle of incidence greater than the critical angle is 1. As shown by the broken line in the figure, the ray of light in the optical axis direction of the 7Si, which travels by manipulating reflection and refraction, gradually attenuates as a part of the □ is refracted at the interface.

光線5′1は界面で7回反対するので、反射率をK(〈
1)・とすれば、受光素−1−□2に達した時はランプ
3゛1が:ら放射きh’#=時点での強さ1こ討しに7
ま・で減寮する□ことにな□す、実際には受光素子2で
検出されない。
Since the ray 5'1 opposes 7 times at the interface, the reflectance can be expressed as K(〈
1), then when the light-receiving element -1-□2 is reached, the lamp 3゛1 emits from: h'# = the strength at the time 1 and 7
As a result, the number of dormitories will be reduced, and the light receiving element 2 will not actually detect it.

第3図は濃い硫酸中に入れた場谷の光線の状況11□ζ
J を示す。
Figure 3 shows the situation of Batani's ray placed in concentrated sulfuric acid 11□ζ
Indicates J.

硫酸濃度力吠きくなり、屈折率が地加すると(2)式に
より臨界角も大きくなる。
When the sulfuric acid concentration increases and the refractive index increases, the critical angle also increases according to equation (2).

光線7を全反射の臨界とすれば、第3′図においてα十
β+δ90°の範囲内に出た光線は全て受光素子2に入
射するカモα′〈α□であるため、淡い硫酸に比べて濃
い硫酸中では受光素子2に入射する光線量は少ないこと
になる。
If the light ray 7 is considered to be the critical point for total internal reflection, all the light rays that come out within the range of α10β+δ90° in Fig. 3' are rays α'〈α□ that are incident on the light-receiving element 2, so compared to the light sulfuric acid, In concentrated sulfuric acid, the amount of light incident on the light receiving element 2 is small.

また、淡い硫酸中と同様に臨界角以上の入射角の光線は
減衰する。
Furthermore, as in dilute sulfuric acid, light rays with an incident angle greater than the critical angle are attenuated.

以上、実施例につい:で述べたが、角柱の長さ40m/
m、β=45°、 δ==40°とし、受光素子2D、
:CdS素子を用いでミ□微少定電流を流し、硫酸濃度
を重化□させで実験したところ□、CdSに発生ずる電
圧は水の場合で0.5〜.比重1.4め硫酸で1.3□
Vを得、その間比重の変化に従って電圧値も変化した。
Above, as described in the example, the length of the prism is 40 m/
m, β=45°, δ==40°, light receiving element 2D,
: When we conducted an experiment using a CdS element by passing a small constant current and increasing the sulfuric acid concentration, we found that the voltage generated in CdS was 0.5 to 0.5 in the case of water. Specific gravity 1.4, 1.3□ with sulfuric acid
V was obtained, and the voltage value also changed in accordance with the change in specific gravity.

−また、実施例で゛は、6光素子と七て一般の小型
ランプを用いて説明したが発光ダ不オニ゛:L′を使用
する□ことも可能である。
Although the embodiment has been described using six light elements and a general small lamp, it is also possible to use a light emitting diode: L'.

□・本考案は以上に説明した構成を有するもめで次
のような効果を得ることができる。
□・The present invention can obtain the following effects with the structure described above.

即ち、従来の比重:計測素子に比べて、電解液の動揺、
液面の変化による影響を受けず、極めて簡便に比重計測
を行なうことが七゛きる。
That is, compared to the conventional specific gravity: measurement element, the fluctuation of the electrolyte,
Specific gravity can be measured extremely easily without being affected by changes in liquid level.

□ ・□・

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

第1図は本考案の原理図を示し、第2′図は本考案の一
実施例を示すと共(ご、淡い電解液中に浸漬した場合の
光線の状態を示す。 第3図は、同じ:く濃い電解液中に浸漬じた場合を示す
。 ・ □1・・・・・・アクリル樹脂の円柱又・は角
柱、2・=・・・・受光素子、3・・・・・・ランプ、
4・・・・・・遮光器。
Fig. 1 shows the principle of the present invention, and Fig. 2' shows an embodiment of the invention, and also shows the state of the light beam when immersed in a dilute electrolyte. Same: Shows the case of being immersed in a thick electrolyte. ・ □1... Acrylic resin cylinder or/prismatic column, 2 =... Light receiving element, 3... lamp,
4... Light shield.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 蓄電池の電解液の屈折率よりも大きな屈折率を有する透
明で一様な物質によって形成された円柱又は平行な面を
持つ角柱の軸方向の一端に受光素子を設け、相対する一
端には、前記円柱又は角柱の軸と不平行になる方向へ、
ある立体角で光を出す発光素子を設けた蓄電池用比重検
出器。
A light-receiving element is provided at one end in the axial direction of a cylinder or a prism with parallel surfaces formed of a transparent and uniform substance having a refractive index larger than that of the electrolyte of the storage battery, and a light-receiving element is provided at one end in the opposite direction. in a direction that is non-parallel to the axis of the cylinder or prism,
A specific gravity detector for storage batteries equipped with a light emitting element that emits light at a certain solid angle.
JP5555077U 1977-04-30 1977-04-30 Specific gravity detector for storage batteries Expired JPS5831339Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5555077U JPS5831339Y2 (en) 1977-04-30 1977-04-30 Specific gravity detector for storage batteries

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5555077U JPS5831339Y2 (en) 1977-04-30 1977-04-30 Specific gravity detector for storage batteries

Publications (2)

Publication Number Publication Date
JPS53149821U JPS53149821U (en) 1978-11-25
JPS5831339Y2 true JPS5831339Y2 (en) 1983-07-11

Family

ID=28951513

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5555077U Expired JPS5831339Y2 (en) 1977-04-30 1977-04-30 Specific gravity detector for storage batteries

Country Status (1)

Country Link
JP (1) JPS5831339Y2 (en)

Also Published As

Publication number Publication date
JPS53149821U (en) 1978-11-25

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