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JPH06103238B2 - Pressure pulsation analyzer - Google Patents
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JPH06103238B2 - Pressure pulsation analyzer - Google Patents

Pressure pulsation analyzer

Info

Publication number
JPH06103238B2
JPH06103238B2 JP17426490A JP17426490A JPH06103238B2 JP H06103238 B2 JPH06103238 B2 JP H06103238B2 JP 17426490 A JP17426490 A JP 17426490A JP 17426490 A JP17426490 A JP 17426490A JP H06103238 B2 JPH06103238 B2 JP H06103238B2
Authority
JP
Japan
Prior art keywords
pipe
fluid
pressure pulsation
pressure
impedance
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 - Lifetime
Application number
JP17426490A
Other languages
Japanese (ja)
Other versions
JPH0462446A (en
Inventor
猛 藤川
稔 加藤
栄子 廣岡
喜雄 井上
道也 黒橋
謙介 村井
重俊 佐藤
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.)
Kobe Steel Ltd
Original Assignee
Kobe Steel 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 Kobe Steel Ltd filed Critical Kobe Steel Ltd
Priority to JP17426490A priority Critical patent/JPH06103238B2/en
Publication of JPH0462446A publication Critical patent/JPH0462446A/en
Publication of JPH06103238B2 publication Critical patent/JPH06103238B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Measuring Fluid Pressure (AREA)
  • Control Of Positive-Displacement Pumps (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は,往復圧縮機,ポンプ等の加圧源による圧力変
動に基づく配管内の圧力の脈動を解析する圧力脈動解析
装置に関するものである。
Description: TECHNICAL FIELD The present invention relates to a pressure pulsation analyzer for analyzing pressure pulsations in a pipe based on pressure fluctuations caused by a pressure source such as a reciprocating compressor and a pump. .

〔従来技術〕[Prior art]

上記のような往復圧縮機,ポンプ等の加圧源から間欠的
に吸い込み/吐出される流体が脈動の加振源となって配
管内の流体が振動する。この流体の振動が加圧源の加振
周期と共振して大きくなった場合は配管を振動させて破
損させたり,圧縮機,ポンプ等の加圧源の性能低下をも
たらす場合がある。そのため,圧縮機,ポンプ等の加圧
源のシリンダ内の流体と配管の流体との連成を考慮して
上記加圧源による加振と配管内の圧力変動とが共振しな
いような配管の寸法デザインを決定するために,上記流
体連成を考慮した配管内の圧力脈動を解析する必要があ
る。
The fluid that is intermittently sucked in / discharged from the pressure source such as the reciprocating compressor or pump described above serves as a pulsating vibration source, and the fluid in the pipe vibrates. If the vibration of the fluid becomes large due to resonance with the vibration cycle of the pressure source, the piping may be vibrated and damaged, or the performance of the pressure source such as the compressor or pump may be deteriorated. Therefore, considering the coupling between the fluid in the cylinder of the pressure source such as the compressor and pump and the fluid in the pipe, the dimensions of the pipe so that the vibration due to the above-mentioned pressure source and the pressure fluctuation in the pipe do not resonate. In order to determine the design, it is necessary to analyze the pressure pulsation in the pipe that considers the above fluid coupling.

上記のような流体連成を考慮しない圧力脈動解析法は、
既に(往復圧縮機配管系の圧力脈動解析,神戸製鋼技報
vol.37No.1)等の文献で知られるように長い歴史と実績
があり,周知である。
The pressure pulsation analysis method that does not consider fluid coupling as described above is
Already (pressure pulsation analysis of reciprocating compressor piping system, Kobe Steel Engineering Reports
Vol.37 No.1) has a long history and track record, and is well known.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

しかしながら,上記のような従来の圧力脈動解析方法で
は,流体連成が考慮されておらず、脈動解析の精度にお
いて充分なものではなかった。
However, in the conventional pressure pulsation analysis method as described above, fluid coupling is not taken into consideration, and the accuracy of pulsation analysis is not sufficient.

又,圧力脈動解析法としては,上記文献に開示された如
く周波数領域で行うものと,時刻歴で行うものとに大別
されるが,上記時刻歴で行うものは周波数領域における
計算方法と比べて膨大な計算時間がかかり,計算費用等
の点で問題があった。
Further, the pressure pulsation analysis method is roughly classified into a method performed in the frequency domain and a method performed in the time history as disclosed in the above document. The method performed in the time history is compared with the calculation method in the frequency domain. Therefore, there was a problem in terms of calculation cost, etc.

従って,本発明は流体連成を考慮した精度の高い圧力脈
動解析を周波数領域において能率良く行うことができる
圧力脈動解析装置を提供することである。
Therefore, the present invention is to provide a pressure pulsation analysis device capable of efficiently performing highly accurate pressure pulsation analysis in consideration of fluid coupling in the frequency domain.

〔課題を解決するための手段〕[Means for Solving the Problems]

上記目的を達成するために第1の発明は,配管のインピ
ーダンスZnに基づく周波数領域での配管内の圧力脈動Δ
Pと,加圧源の周波数領域でのシリンダ内の圧力変動Δ
Pcとより,上記シリンダ内へ流出入する流体の体積のn
次成分複素振幅Xnを求める手段と,上記Xnを用いて流体
の連成を考慮した配管内流体の加振流量Qnを求める手段
と,上記Qnを用いて周波数領域における流体の連成を考
慮した配管内の圧力脈動ΔPを求める手段と,を具備し
てなる圧力脈動解析装置として構成されている。
In order to achieve the above object, the first invention is a pressure pulsation Δ in a pipe in a frequency region based on the impedance Z n of the pipe.
P and pressure fluctuation in the cylinder in the frequency domain of the pressure source Δ
From P c , n of the volume of fluid flowing into and out of the cylinder
A means for obtaining the complex amplitude X n of the next component, a means for obtaining the vibration flow rate Q n of the fluid in the pipe considering the fluid coupling using the above X n, and a fluid coupling in the frequency domain using the above Q n. And a means for determining pressure pulsation ΔP in the pipe in consideration of the formation of the pressure pulsation analyzer.

また第2の発明は,仮定された配管のインピーダンスZn
に基づく周波数領域での配管内の圧力脈動ΔPと,加圧
源の周波数領域でのシリンダ内の圧力変動ΔPcとより,
上記シリンダ内へ流出入する流体の体積のn次成分複素
振幅Xnを求める手段と,上記Xnを用いて流体の連成を考
慮した配管内流体の加振流量Qnを求める手段と,上記Qn
を用いて周波数領域における流体の連成を考慮した配管
内の圧力脈動ΔPを求める手段と,上記修正された圧力
脈動ΔPから修正された配管のインピーダンZn′を求
め,該Zn′と修正前のインピーダンスZnとを比較し,そ
の差が所定範囲内となるまで上記各手段の実行を繰り返
し,所定範囲内となった時点における修正された配管内
の圧力脈動ΔPを求める手段と,を具備してなる圧力脈
動解析装置として構成されている。
The second invention is the assumed impedance Z n of the pipe.
And pressure pulsation [Delta] P in the pipe in the frequency domain based on, more and the pressure variation [Delta] P c in the cylinder in the frequency domain of the pressure source,
Means for determining the n-th order components complex amplitude X n of the volume of fluid flowing into and out into the cylinder, means for determining the vibration rate Q n of the pipe the fluid in consideration of coupling fluid with the X n, Above Q n
Means for obtaining the pressure pulsation ΔP in the pipe in consideration of fluid coupling in the frequency domain, and the corrected pressure pulsation ΔP for the corrected pipe impedance Z n ′, and the correction with Z n ′. Means for comparing the previous impedance Z n , repeating the above-mentioned means until the difference is within a predetermined range, and obtaining the corrected pressure pulsation ΔP in the pipe at the time when the difference is within the predetermined range. It is configured as a pressure pulsation analysis device provided.

〔実施例〕〔Example〕

続いて,第1図に示した計算手順を表すフローチャート
を参照して本発明を具体化した実施例につき説明する。
Next, an embodiment embodying the present invention will be described with reference to the flowchart showing the calculation procedure shown in FIG.

尚,ここで流体連成を考慮しない周波数領域における圧
力脈動の解析手法については前記文献及びその他により
周知であるのその詳しい説明を省略する。
Incidentally, the method of analyzing the pressure pulsation in the frequency domain which does not take fluid coupling into consideration is well known from the above-mentioned literatures and others, but its detailed description is omitted.

以下に述べる実施例における圧力脈動解析方法は次のよ
うに要約される。即ち,前記流体の連成は流体の比重,
粘性,体積等に関連し,これは配管のインピーダンスZn
を考慮することにより達成される。このような配管のイ
ンピーダンスZnが既知の場合,このZnに基づく周波数領
域での配管内の圧力脈動ΔPと,加圧源の周波数領域で
のシリンダ内の圧力変動ΔPcとより,上記シリンダ内へ
流出入する流体の体積のn次成分複素振幅Xnがまず求め
られる。続いて,上記Xnを用いて配管内流体の加振流量
Qnを求める。この加振流量Qnは前記配管のインピーダン
スZn基づくものであるから,当然流体の連成が考慮され
ている。
The pressure pulsation analysis method in the embodiment described below is summarized as follows. That is, the fluid coupling is the specific gravity of the fluid,
Related to viscosity, volume, etc., which is the impedance of the pipe Z n
It is achieved by considering When the impedance Z n of such a pipe is known, the pressure pulsation ΔP in the pipe in the frequency region based on this Z n and the pressure fluctuation ΔP c in the cylinder in the frequency region of the pressurization source are used to determine the cylinder First, the complex amplitude X n of the n-th component of the volume of the fluid flowing in and out is obtained. Then, using the above X n , the vibration flow rate of the fluid in the pipe
Find Q n . Since this vibration flow rate Q n is based on the impedance Z n of the pipe, fluid coupling is naturally taken into consideration.

次に,上記加振流量Qnを用いて周波数領域における流体
の連成の考慮された配管内の圧力脈ΔPが求められる。
Next, the pressure pulse ΔP in the pipe in which the fluid coupling in the frequency domain is taken into consideration is obtained by using the above-mentioned vibration flow rate Q n .

このように,加圧源が単一である等,比較的簡素な系に
おいては,前記配管のインピーダンスZnを精度良く推定
することができるので計算手法としては比較的簡単であ
る。
As described above, in a relatively simple system such as a single pressurizing source, the impedance Z n of the pipe can be accurately estimated, so that the calculation method is relatively simple.

しかしながら,例えば加圧源が複数である場合や,前記
インピーダンスZnが加振流量Qnの関数になっているよう
な場合等には,インピーダンスZnが既知でないので,こ
れをまず仮定した値として与えた上で修正を繰り返す必
要がある。即ち,この場合,適当に仮定された配管のイ
ンピーダンZnに基づく周波数領域での配管内の圧力脈動
ΔPと,加圧源の周波数領域でのシリンダ内の圧力変動
ΔPcとより,上記シリンダ内へ流出入する流体の体積の
n次成分複素振幅Xnを求める。次に,上記Xnを用いて前
記同様流体の連成を考慮した配管内の流体の加振流量Qn
を求める。続いて,上記加振流量Qnを用いて周波数領域
における流体の連成を考慮して修正された配管内の圧力
脈動ΔPを求める。更に,上記修正された圧力脈動ΔP
から修正された配管のインピーダンスZn′を求め,この
Zn′と修正前のインピーダンスZnとを比較し,その差が
所定範囲内となるまで上記計算手順を繰り返して実行
し,上記インピーダンスの差が所定範囲内となった時点
における配管内の圧力脈動ΔPを修正された圧力脈動と
して採用する。
However, for example, if the pressure source is a plurality, the impedance when such as is a function of the Z n is vibrating flow Q n, the impedance Z n is not known, it is first assumed value It is necessary to repeat the correction after giving it as. That is, in this case, from the pressure pulsation ΔP in the pipe in the frequency region based on the appropriately assumed pipe impedance Z n , and the pressure fluctuation ΔP c in the cylinder in the frequency region of the pressurization source, The complex amplitude X n of the n-th component of the volume of fluid flowing in and out of is calculated. Next, using the above X n , the fluid flow rate Q n
Ask for. Subsequently, the pressure pulsation ΔP in the pipe corrected by taking into account the fluid coupling in the frequency domain is obtained by using the above-mentioned vibration flow rate Q n . Further, the corrected pressure pulsation ΔP
The corrected impedance Z n ′ of the pipe is calculated from
Z n ′ is compared with the uncorrected impedance Z n, and the above calculation procedure is repeated until the difference is within the predetermined range. The pressure in the pipe at the time when the impedance difference is within the predetermined range Adopt pulsation ΔP as the corrected pressure pulsation.

上記の手順を詳細に説明すると以下の通りである。The above procedure will be described in detail below.

まず,第1図におけるステップS1において,計算に必要
な定数が入力される。計算に必要な因子は, (1)流体特性に関する因子 音速,密度,平均圧力,粘性係数, 体積弾性率,状態変化の指数等 (2)配管特性に関する因子 配管長さ,配管直径等 (3)圧縮機等加圧源の特性に関する因子 ピストンの動き,ピストンの直径, 回転数等 定数の入力が終わると加圧源ノシリンダ内に流出入する
流体の体積のn次成分複素振幅Xnを求める(S2)。上記
複素振幅Xnは次の計算方法に基づき計算される。
First, in step S1 in FIG. 1, constants required for calculation are input. Factors required for calculation are (1) factors related to fluid characteristics: sound velocity, density, average pressure, viscosity coefficient, bulk modulus, index of state change, etc. (2) factors related to piping characteristics, pipe length, pipe diameter, etc. (3) Factors related to characteristics of pressure source such as compressor When the piston movement, piston diameter, rotation speed and other constants are input, the complex amplitude X n of the nth component of the volume of fluid flowing into and out of the pressure source cylinder is calculated ( S2). The complex amplitude Xn is calculated based on the following calculation method.

圧縮機,ポンプ等の加圧源のシリンダ内の圧力変動ΔPc
は, で表される。
Pressure fluctuation in the cylinder of the pressure source such as compressor, pump ΔP c
Is It is represented by.

ここで,γ…流体の状態変化を表す指数 Po…配管内流体の平均圧力 V…シリンダ室内の体積 x…シリンダ室内の流出入する 流体の体積 y…ピストンの体積変位 である。Here, γ is an index representing a change in the state of the fluid, P o is the average pressure of the fluid in the pipe, V is the volume in the cylinder chamber, x is the volume of fluid flowing in and out of the cylinder chamber, y is the volume displacement of the piston.

一方,配管内の圧力変動ΔPのフーリエ展開の式は, ΔP=ΣjnωZn ejnωt …(2) で表される。On the other hand, expression of the Fourier expansion of the pressure variation [Delta] P in the pipe is expressed by ΔP = ΣjnωZ n e jnωt ... ( 2).

ここで,j…虚数 n…フーリエ展開の次数 ω…圧縮機等加圧源の回転数 Zn…配管のインピーダンス Xn…シリンダ内へ流入する流体の体積の n次成分複素振幅 t…時刻 である。Where j ... Imaginary number n ... Order of Fourier expansion ω ... Rotation speed of pressure source such as compressor Z n ... Impedance of piping X n ... Complex amplitude of n-th order component of fluid flowing into cylinder t ... At time is there.

ここで,上記のような配管と加圧源とが連通状態になっ
ている時はΔPc=ΔPであり,xをフーリエ展開で表す
と, x=ΣXn ejnωt であるから,下記の(3)式が得られる。
Here, ΔP c = ΔP when the pipe and the pressure source are in communication with each other as described above, and when x is represented by Fourier expansion, x = ΣX n e jnωt. Equation 3) is obtained.

上記(1),(2),(3)の各式において用いられ配
管のインピーダンスZnは単純な系やZnがQnの関数になっ
ていないような場合等には,既知として扱うことができ
るが,加圧源が複数あるような場合やZnがQnの関数にな
っているような場合等には一該に決定できない。
The impedance Z n of the pipe used in the above equations (1), (2), and (3) should be treated as known in a simple system or when Z n is not a function of Q n. However, if there are multiple pressure sources or if Z n is a function of Q n , it cannot be completely determined.

そのため,この実施例では前記(2)式及び(3)式に
用いたインピーダンスZnは当初適当に仮定した値が採用
される。尚,その他の数値y,V,ωは加圧機の仕様に応じ
て決定され,γ,Poは配管,流体,運転条件が決まれば
一義的に決定される。
Therefore, in this embodiment, the impedance Z n used in the equations (2) and (3) has a value that is initially assumed to be appropriate. The other values y, V, and ω are determined according to the specifications of the pressurizer, and γ and P o are uniquely determined if the piping, fluid, and operating conditions are determined.

上記(3)式が得られると,これより上記シリンダ内へ
流出入する流体の体積のn次成分複素振幅Xnが求まる。
この手順が前記ステップS2である。
When the (3) is obtained, than this volume of fluid flowing into and out into the cylinder n th component complex amplitude X n is obtained.
This procedure is step S2.

次に配管内流体の加振流量Qnは前記xの微分値であるか
ら, =ΣjnωXn ejnωt であり,Qn=jnωXn …(4) より加振流量Qnが求められる(S3)。
Since then vibrating flow Q n of the pipe the fluid is a differential value of the x, = a ΣjnωX n e jnωt, vibrating flow Q n are obtained from the Q n = jnωX n ... (4 ) (S3) .

こうして求められた加振流量Qnは流体連成に基づくもの
であり,これを周知の周波数領域における配管内の圧力
脈動値の計算手法に代入することにより,上記配管の連
成を考慮した配管内の圧力脈動値ΔPが演算される(S
4)。
The vibration flow rate Q n obtained in this way is based on fluid coupling, and by substituting this into the calculation method of the pressure pulsation value in the piping in the well-known frequency range, the piping considering the above-mentioned piping coupling is considered. The pressure pulsation value ΔP inside is calculated (S
Four).

ここで,前記仮定されたZnが適正な値であれば,上記S4
で求めた圧力脈動Δ等を(2)式に代入して得られる修
正されたインピーダンスZn′(S5)と修正される前のイ
ンピーダンスZnとが等しいか近似するはずである。
Here, if the assumed Z n is a proper value, the above S4
The corrected impedance Z n ′ (S5) obtained by substituting the pressure pulsation Δ and the like obtained in step (2) into the equation (2) should be equal or approximate to the uncorrected impedance Z n .

従って,配管系の簡単な場合や,ZnがQnの関数になって
いないような場合等には,上記S4で求めた圧力脈動値Δ
Pを最終結果として出力してもよい。
Therefore, when the piping system is simple or when Z n is not a function of Q n , the pressure pulsation value Δ
P may be output as the final result.

しかしながら,上記Znが既知でない場合には,上記最初
に仮定したZnが適性な値とは限らないので,上記ステッ
プS5で得られたインピーダンスZn′と修正前のZnとを比
較し(S6),両者の差が所定範囲よりも大きい場合に
は,修正されたZn′を新たに仮定された配管インピーダ
ンスとして前記S2〜S6の手順を繰り返す。こうして仮定
された配管のインピーダンスZnが徐々に修正され,系に
適したものとなった時に修正前後のZnが一致する。この
時の圧力脈動値ΔPが最終結果として出力される。
However, the if Z n is not known, since the first assumed Z n is not necessarily the proper value, by comparing the Z n before modification and impedance Z n 'obtained in step S5 (S6) If the difference between the two is larger than the predetermined range, the procedure from S2 to S6 is repeated using the corrected Z n ′ as the newly assumed pipe impedance. The impedance Z n of the pipe thus assumed is gradually corrected, and when it becomes suitable for the system, the Z n before and after the correction match. The pressure pulsation value ΔP at this time is output as the final result.

こうして計算の結果,上記圧力脈動値ΔPが所定の基準
よりも大きい場合には例えば配管のレイアウト(配管内
径,配管長さ等)の変更を行ったり,減衰機能(アキュ
ムレーター,オリフィス等)を付与することにより脈動
の減衰が図られる。
When the pressure pulsation value ΔP is larger than the predetermined standard as a result of the calculation in this way, for example, the layout of the pipe (pipe inner diameter, pipe length, etc.) is changed, or a damping function (accumulator, orifice, etc.) is added. By doing so, pulsation can be attenuated.

〔発明の効果〕〔The invention's effect〕

本発明は,以上述べたように構成されているので,周波
数領域において連成を考慮した能率の良い高精度の解析
を行うことができる。
Since the present invention is configured as described above, it is possible to perform efficient and highly accurate analysis in consideration of coupling in the frequency domain.

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

第1図は本発明の一実施例に係る圧力脈動解析装置の処
理手順を示すフローチャートである。 〔符号の説明〕 Zn…配管インピーダンス ΔP…配管内の圧力脈動 ΔPc…シリンダ内の圧力変動 Xn…シリンダ内へ吸入する流体の体積のn次成分複素振
幅 Qn…配管内の流体の加振流量 Zn′…修正された配管のインピーダンス
FIG. 1 is a flow chart showing a processing procedure of a pressure pulsation analyzer according to an embodiment of the present invention. [Explanation of symbols] Z n … Piping impedance ΔP… Pressure pulsation in the pipe ΔP c … Pressure fluctuation in the cylinder X n … Nth-order component of the volume of fluid sucked into the cylinder Complex amplitude Q n … of the fluid in the pipe Excitation flow rate Z n ′… Impedance of modified pipe

フロントページの続き (72)発明者 村井 謙介 大阪府箕面市箕面8―16―8 (72)発明者 佐藤 重俊 兵庫県神戸市灘区篠原伯母野山町2―3― 1Front Page Continuation (72) Inventor Kensuke Murai 8-16-8 Minoh, Minoh City, Osaka Prefecture (72) Inventor Shigetoshi Sato 2-3-1 Shinohara Aki Nonomachi, Nada-ku, Kobe City, Hyogo Prefecture

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】配管のインピーダンスZnに基づく周波数領
域での配管内の圧力脈動ΔPと,加圧源の周波数領域で
のシリンダ内の圧力変動ΔPcとより,上記シリンダ内へ
流出入する流体の体積のn次成分複素振幅Xnを求める手
段と, 上記Xnを用いて流体の連成を考慮した配管内流体の加振
流量Qnを求める手段と, 上記Qnを用いて周波数領域における流体の連成を考慮し
た配管内の圧力脈動ΔPを求める手段と, を具備してなる圧力脈動解析装置。
1. A fluid flowing in and out of the cylinder based on pressure pulsation ΔP in the pipe in the frequency region based on the impedance Z n of the pipe and pressure fluctuation ΔP c in the cylinder in the frequency region of the pressure source. means for determining the volume of n-th order components complex amplitude X n, means for determining the vibration rate Q n of the fluid in the pipe in consideration of coupling fluid with the X n, the frequency domain using the Q n A pressure pulsation analysis device comprising: means for determining pressure pulsation ΔP in a pipe in consideration of fluid coupling in
【請求項2】仮定された配管のインピーダンスZnに基づ
く周波数領域での配管内の圧力脈動ΔPと,加圧源の周
波数領域でのシリンダ内の圧力変動ΔPcとより,上記シ
リンダ内へ流出入する流体の体積のn次成分複素振幅Xn
を求める手段と, 上記Xnを用いて流体の連成を考慮した配管内流体の加振
流量Qnを求める手段と, 上記Qnを用いて周波数領域における流体の連成を考慮し
た配管内の圧力脈動ΔPを求める手段と, 上記修正された圧力脈動ΔPから修正された配管のイン
ピーダンZn′を求め,該Zn′と修正前のインピーダンス
Znとを比較し,その差が所定範囲内となるまで上記各手
段の実行を繰り返し,所定範囲内となった時点における
修正された配管内の圧力脈動ΔPを求める手段と, を具備してなる圧力脈動解析装置。
2. Outflow into the cylinder due to pressure pulsation ΔP in the pipe in the frequency region based on the assumed impedance Z n of the pipe and pressure fluctuation ΔP c in the cylinder in the frequency region of the pressurization source. Nth-order component of the volume of the entering fluid complex amplitude X n
And a means for determining the vibration flow rate Q n of the fluid in the pipe considering the fluid coupling using the above X n, and a fluid in the piping considering the fluid coupling in the frequency domain using the above Q n . means for determining the pressure pulsation ΔP of 'seeking, the Z n' impedance Z n of the pipe that have been modified from the modified pressure pulsation ΔP before correction impedance
Means for comparing Z n with each other, repeating the above-mentioned means until the difference is within a predetermined range, and obtaining a corrected pressure pulsation ΔP in the pipe at the time when the difference is within the predetermined range. Pressure pulsation analyzer.
JP17426490A 1990-06-29 1990-06-29 Pressure pulsation analyzer Expired - Lifetime JPH06103238B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17426490A JPH06103238B2 (en) 1990-06-29 1990-06-29 Pressure pulsation analyzer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17426490A JPH06103238B2 (en) 1990-06-29 1990-06-29 Pressure pulsation analyzer

Publications (2)

Publication Number Publication Date
JPH0462446A JPH0462446A (en) 1992-02-27
JPH06103238B2 true JPH06103238B2 (en) 1994-12-14

Family

ID=15975603

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17426490A Expired - Lifetime JPH06103238B2 (en) 1990-06-29 1990-06-29 Pressure pulsation analyzer

Country Status (1)

Country Link
JP (1) JPH06103238B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4822745B2 (en) * 2005-06-07 2011-11-24 千代田化工建設株式会社 Pressure pulsation analyzer
JP4551875B2 (en) * 2006-02-15 2010-09-29 株式会社東芝 Main steam piping

Also Published As

Publication number Publication date
JPH0462446A (en) 1992-02-27

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