JPS59214717A - Liquid-level measuring method in hollow body - Google Patents
Liquid-level measuring method in hollow bodyInfo
- Publication number
- JPS59214717A JPS59214717A JP58089610A JP8961083A JPS59214717A JP S59214717 A JPS59214717 A JP S59214717A JP 58089610 A JP58089610 A JP 58089610A JP 8961083 A JP8961083 A JP 8961083A JP S59214717 A JPS59214717 A JP S59214717A
- Authority
- JP
- Japan
- Prior art keywords
- probe
- voltage
- liquid level
- hollow body
- crt
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F23/00—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
- G01F23/22—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water
- G01F23/28—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water by measuring the variations of parameters of electromagnetic or acoustic waves applied directly to the liquid or fluent solid material
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Thermal Sciences (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は中空体内の液面レベル測定方法に関し、さらに
詳しくは化学プラント等にd3 Lプる蒸留塔、吸収塔
、反応塔、吸着塔、洗浄塔、抽出塔<yどの各種の塔状
中空体や、貯槽、泪呈イ1す、反応槽、分R1槽、混合
槽なとの各種の櫓状中空体にd−)(づる内部の液面レ
ベルを測定するのにクイ適な測定方法に関す゛る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring a liquid level in a hollow body, and more specifically, the present invention relates to a method for measuring a liquid level in a hollow body, and more particularly, it relates to a method for measuring a liquid level in a hollow body, and more particularly, a method for measuring a liquid level in a hollow body, such as a distillation column, absorption column, reaction column, adsorption column, washing column, extraction column <y d-) (for measuring the liquid level inside the tower) Regarding the most suitable measurement method.
これらの各種の塔d3よび槽にJ5い(は、その稼動中
に4ハソる内部の状態を把握することが非帛に生変で、
生産性の向」−1保安、合理化等を目的どづる改良、改
革および新設機器の没!l”Jとに得かたい資料となる
。It is impossible to grasp the internal conditions of these various towers and tanks during their operation, and
``Increased productivity''-1 Improvements, reforms, and destruction of new equipment for the purpose of security, rationalization, etc.! It will be a difficult material to obtain for l”J.
たとえば精製中における蒸留塔では、剖イルの流量に過
不足があると効率的な蒸留効果を得られず、そのために
設4通りの効率で蒸留ざ4するように最適な流量を得る
べく、その内部状rぶを把握する必要性があるも、現状
ではでのyj策づら立っていない。For example, in a distillation column during purification, if the flow rate of the distillation column is too high or too low, an efficient distillation effect cannot be obtained. Although there is a need to understand the internal situation, there is currently no plan for YJ.
本発明は叙上問題点を解消したもので、各種の塔や櫓等
の中空体内の液面を振動させ、この振動状態の液面を、
中空体外から超音波探触器の探触子で超音波探査しなが
らその反射波の変化により捕捉して、液面レベルを検知
りることを特徴とする。即ち、中空体の内部状態を、そ
の液面レベルを測定することにより把+1P TFI能
にしたもので、その中空体が棚段形式の蒸留IW tあ
る場合、多段状の各シールパンにおりる流量ずイ≧わら
ダウンカマ一部の液面レベルを測定して内部状態を把握
して、その設削通りの蒸留効率を得ることのできる測定
システムを提案するものである。The present invention solves the above-mentioned problems by vibrating the liquid level inside hollow bodies such as various towers and turrets.
It is characterized by detecting the liquid level by detecting changes in reflected waves while conducting ultrasonic probes from outside the hollow body using a probe of an ultrasonic probe. In other words, the internal state of the hollow body is determined by measuring the liquid level, and if the hollow body is a tray-type distillation IWt, the internal state of the hollow body is determined by measuring the liquid level. We propose a measurement system that can measure the liquid level in a part of the downcomer, grasp the internal state, and obtain the distillation efficiency as designed.
以上、本発明の実施例を、棚段形式の蒸留塔である中空
体くΔ)について説明する。The embodiments of the present invention will be described above with respect to a hollow body (Δ) which is a tray type distillation column.
中空体(△〉づなわら蒸留塔はシールパン(A1)・・
・を多段状に備えていて、稼動中はA・イルを上旬から
下位のシートパン(A1)に、各タウンカマ一部(A2
)にて流ト圧をもって気′a混合を行ない且つその液面
(C+)を汲置た1!ながら流下させ−(蒸留しでいる
。この蒸留jMに対して、イ゛の塔外壁面に沿い超音波
探触器([3)の探触子〈B1 )を上下に動かして超
音波探査し、CRT (B2 )に現われた反則波のパ
ターンを識別して、各ダウンカマ一部(A2)k: C
3りる液面レベルを検知する。Hollow body (△〉Zunawara distillation column is a seal pan (A1)...
・It is equipped with multiple tiers of ・During operation, A・Ile is placed on the lower seat pan (A1) from the beginning, and a portion of each town pan (A2) is placed on the lower seat pan (A1).
), the air was mixed with a flow pressure, and the liquid level (C+) was pumped up 1! The distilled water is allowed to flow down (distilled). This distillation jM is probed by ultrasonic waves by moving the probe (B1) of [3] up and down along the outer wall of the column A. , identify the pattern of foul waves appearing on the CRT (B2), and select each downcomer part (A2) k: C
3.Detects the liquid level.
ぞの具体例を第2図により説明すると、測定個所■では
CRT(B2)に現われる反則波のパターンは次の特徴
がある。A specific example of this will be explained with reference to FIG. 2. At the measurement point (3), the pattern of the foul wave appearing on the CRT (B2) has the following characteristics.
1) 反射波の動きはほとんどない。1) There is almost no movement of the reflected waves.
■) 反射波の本数が少く、輝麿が高い。■) The number of reflected waves is small and Terumaro is high.
これを解析すると、■)は超音波の部間的減衰が無いこ
とを示し、I ) C3よひ■)は塔外壁内表面におけ
る音圧反射率の変化が無いことど、内部よりの反射波が
無いことを示し、これにJ:り塔外壁内表面での81工
反射率は100%であり、■内部は気相<03 )であ
ることが分かる。Analyzing this, ■) indicates that there is no local attenuation of ultrasonic waves, and ■) indicates that there is no local attenuation of ultrasonic waves, and ■) indicates that there is no change in the sound pressure reflectance on the inner surface of the outer wall of the tower, indicating that the waves reflected from inside the tower. In addition, J: The reflectance on the inner surface of the outer wall of the tower is 100%, and (2) the gas phase is <03) inside.
測定個所■ III) I)とほぼ同じ yl> 反則波にわずかの撮動が見られる。Measurement point ■ III) Almost the same as I) yl> Slight imaging can be seen in the foul wave.
これを解析すると、m)N)はI)II>の状態に近く
、■内部は気相(C3)Tあることが分かる。またll
2)のわずかな撮動は塔外壁内面がはじ(プる気泡で繻
れていることを示していて、下側に気液相が近いことが
分かる。Analyzing this, it can be seen that m)N) is close to the state of I)II>, and (2) there is a gas phase (C3)T inside. Also ll
The slight photograph in 2) shows that the inner surface of the outer wall of the tower is covered with bubbles, and it can be seen that the gas-liquid phase is close to the bottom.
測定個所■
M) CRT (B2 >下方にI)と同様のパター
ンが現われるが、音圧レベルとしてはかなり低い。Measurement location ■ M) CRT (B2 > Below I) a similar pattern appears, but the sound pressure level is quite low.
■) CRI’(B2)上方に非常に不安定な反射波
(激しい振動を伴いながら上下に大きく変化りる)が現
われる。■) A very unstable reflected wave (which changes greatly up and down with violent vibrations) appears above CRI' (B2).
これを解析Jるど、■)は塔外壁内面での音圧反射率の
低下を示して内部に超音波が伝わる物質が存在リ−るこ
とを示し、■)は、内部に通過した超音波が物質の切れ
目(気泡)などにより瞬間的に反射されていることを示
し、これにより■内部には非常に不安定な気液相(C2
)の上レベルが存在づることか分かる。Analyzing this, ■) shows a decrease in the sound pressure reflectance on the inner surface of the outer wall of the tower, indicating that there is a substance inside that transmits ultrasonic waves, and ■) shows that the ultrasonic waves that passed inside the tower This shows that the gas is momentarily reflected by a break in the material (bubble), etc., and as a result, there is an extremely unstable gas-liquid phase (C2) inside.
), it can be seen that there is an upper level.
測定個所■
■) 反則波が非常に激しく振動しながら上下に大きく
変化する。Measurement location ■ ■) The foul wave vibrates very violently and changes greatly up and down.
これを解析すると、■)は塔外壁内面での音)):反射
率がさらに低Fして叙上■)の現象が顕著になったこと
を示し、■内部には非常に不安定な気液相(C2)が存
在4ることが分かる。Analyzing this, ■) indicates that the sound reflection rate on the inner surface of the outer wall of the tower has become even lower, and the phenomenon described in ■) has become more pronounced. It can be seen that a liquid phase (C2) exists4.
測定個所■ i) 反則波が細く現われ月つ激しく撮動づる。Measurement point ■ i) The foul wave appears thinly and shoots violently.
但し、上下方向の大きな変化はない。However, there is no major change in the vertical direction.
■) 反射波の本数が多い。■) There are many reflected waves.
これを解析づ−ると、■)は超音波の内部への通過率が
かなり安定していることを/]くし、■)は内部に無数
の反射体か右ることを示し、これににす■内部には比較
的安定した気液相(C2)が存在していることか分かる
。Analyzing this, ■) indicates that the passage rate of ultrasonic waves into the interior is quite stable, and ■) indicates that there are countless reflectors inside. It can be seen that a relatively stable gas-liquid phase (C2) exists inside the chamber.
測定個所■
X) 反射波にやや振動が認められるが比較的安定して
おり、且つ反射波の本数か■)よりも少い。Measurement location ■X) Slight vibration is observed in the reflected waves, but it is relatively stable and the number of reflected waves is smaller than ■).
これを解析づると、X〉は超音波の内部への通過率がか
なり安定しくいて、内部には反射体があまり存在しない
ことを示し、これにより■内部には比較的安定した液相
(C)が存在していることが分かる。Analyzing this, it shows that the passage rate of ultrasonic waves into the interior of ) is found to exist.
斯くして、蒸留塔における各段の流ωを把握し得、且つ
気液相(C2)の存在およびレベルまでをも把握し得る
。In this way, the flow ω of each stage in the distillation column can be grasped, and the presence and level of the gas-liquid phase (C2) can also be grasped.
本発明の測定に用いる超音波探触器(B)は公シ、11
のしの(、高電圧の電気パルスを生成して探触j’ <
13. +、 )に流す送信部<133)と、電気パ
ルスを振動子により超音波に変換し、またその反CfJ
波を電圧に変換する探触子(B1)と、反射波により振
動子に発生りる電F〔を増幅する増幅部(85)J’i
、J:ひ受波電圧をCRT(B2.)に通11な人ぎさ
に変換づ−る減衰器(感度調整器)<136)からなる
受信部(Ba)と、受信部<13.+)からの電圧を垂
直軸に、後i!Isの時間11ql+部(B7)からの
電圧を水平軸に表示づるC R1(B>)ど、CRT(
[32)の輝点(スボツ1へ)を水平に等速度で動かづ
電圧を発する面間軸部(+:37)とて構成されている
。The ultrasonic probe (B) used in the measurement of the present invention is public, 11
Noshino(, generate high voltage electric pulse and probe j'<
13. +,
A probe (B1) that converts waves into voltage, and an amplification section (85) J'i that amplifies the electric current F generated in the vibrator by the reflected waves.
, J: A receiving section (Ba) consisting of an attenuator (sensitivity adjuster) <136) that converts the received wave voltage to a CRT (B2.) into a 11-level signal, and a receiving section <13. +) on the vertical axis, after i! The voltage from the time 11ql+ part (B7) of Is is displayed on the horizontal axis.
It consists of an interplane shaft part (+: 37) that moves the bright spot (towards the slot 1) horizontally at a constant speed and emits a voltage.
しlこがって本発明によれば次の利点がある。In summary, the present invention has the following advantages.
■ 中空体内部の液面1ノベルを外部から測定して把握
することができる。■ The liquid level inside the hollow body can be measured and understood from the outside.
■ 流量の把握を必須とする蒸留塔等では、その内部状
態すなわち副機状態を、液面レベル11JII定し−て
正確に把握することかできるものであり、その蒸留効率
を最適の状態に外部から監ン只することができる。■ In distillation columns, etc., where it is essential to know the flow rate, the internal state, that is, the state of the auxiliary equipment, can be accurately determined by determining the liquid level. Can only be supervised from
■ 従来まで把握不可能てあ引こ蒸留塔なとの中空体の
内部状態を把握できて、その蒸留効率のみなら一す゛、
蒸留塔そのものの設面に員(pなデーターを提供し得る
ものである。■ It is now possible to understand the internal state of a hollow body such as a distillation column, which was previously impossible to understand, and its distillation efficiency alone is excellent.
It can provide important data on the design of the distillation column itself.
第1図は本発明測定方法を蒸留塔に用い−(実施した例
を示す断面図。第2図はモの部分拡大断面図。第3図は
本発明測定方法に使用した超音波探触器のブロック図で
ある。
図中
(△〉は中空体
(13)は超音波探触器
(1B+)は探触子
(C1)は液面Figure 1 is a cross-sectional view showing an example in which the measuring method of the present invention is applied to a distillation column. Figure 2 is a partially enlarged cross-sectional view of the measuring method of the present invention. Figure 3 is an ultrasonic probe used in the measuring method of the present invention. This is a block diagram. In the figure (△>), the hollow body (13) is the ultrasonic probe (1B+), and the probe (C1) is the liquid level.
Claims (1)
中空体外から超音波探触器の探触子で超音波探査しなが
らその反射波の変化により捕捉()て、液面レベルを検
知るすることを特徴とりる中空イホ内の液面レベル測定
方法。The liquid level inside the body and the inside of the body is vibrated, and the liquid level in this vibrating state is
A method for measuring the liquid level inside a hollow body, which is characterized by detecting the liquid level by detecting changes in the reflected waves while performing ultrasonic exploration with a probe of an ultrasonic probe from outside the hollow body. .
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58089610A JPS59214717A (en) | 1983-05-21 | 1983-05-21 | Liquid-level measuring method in hollow body |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58089610A JPS59214717A (en) | 1983-05-21 | 1983-05-21 | Liquid-level measuring method in hollow body |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59214717A true JPS59214717A (en) | 1984-12-04 |
Family
ID=13975514
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP58089610A Pending JPS59214717A (en) | 1983-05-21 | 1983-05-21 | Liquid-level measuring method in hollow body |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59214717A (en) |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS51124954A (en) * | 1975-04-25 | 1976-10-30 | Texaco Development Corp | Liquid level variation detector for detecting minute change in liquid level caused by leakage |
JPS539150A (en) * | 1976-07-12 | 1978-01-27 | Vni I K I Tsubetometoafutomach | Method of and apparatus for inspecting boundaries between gas and liquid or between liquid and liquid in single molecule layer storing tank |
JPS5522177A (en) * | 1978-08-04 | 1980-02-16 | Baumooru Jiyosefu | Ultrasonic liquid level detector |
-
1983
- 1983-05-21 JP JP58089610A patent/JPS59214717A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS51124954A (en) * | 1975-04-25 | 1976-10-30 | Texaco Development Corp | Liquid level variation detector for detecting minute change in liquid level caused by leakage |
JPS539150A (en) * | 1976-07-12 | 1978-01-27 | Vni I K I Tsubetometoafutomach | Method of and apparatus for inspecting boundaries between gas and liquid or between liquid and liquid in single molecule layer storing tank |
JPS5522177A (en) * | 1978-08-04 | 1980-02-16 | Baumooru Jiyosefu | Ultrasonic liquid level detector |
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