JPH0560142B2 - - Google Patents
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- Publication number
- JPH0560142B2 JPH0560142B2 JP4562083A JP4562083A JPH0560142B2 JP H0560142 B2 JPH0560142 B2 JP H0560142B2 JP 4562083 A JP4562083 A JP 4562083A JP 4562083 A JP4562083 A JP 4562083A JP H0560142 B2 JPH0560142 B2 JP H0560142B2
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- Prior art keywords
- specific weight
- flow rate
- calculating
- approximate
- weight
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- G—PHYSICS
- G06—COMPUTING OR CALCULATING; COUNTING
- G06F—ELECTRIC DIGITAL DATA PROCESSING
- G06F17/00—Digital computing or data processing equipment or methods, specially adapted for specific functions
- G06F17/10—Complex mathematical operations
- G06F17/17—Function evaluation by approximation methods, e.g. inter- or extrapolation, smoothing, least mean square method
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- Engineering & Computer Science (AREA)
- General Physics & Mathematics (AREA)
- Mathematical Analysis (AREA)
- Mathematical Optimization (AREA)
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- Computational Mathematics (AREA)
- Data Mining & Analysis (AREA)
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- Algebra (AREA)
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- General Engineering & Computer Science (AREA)
- Complex Calculations (AREA)
Description
本発明は、流量測定等に用いる演算器に関する
ものである。
流量測定に用いる演算器には、天然ガス、一般
ガス、スチーム、および液等の種々の流体に対応
して各種の演算機能が要求されるため、最近はマ
イクロコンピユータを用いて構成されている。と
ころで、流量測定における演算には、例えばスチ
ームの温度、圧力に基づく比重量の演算のように
演算式が非常に複雑なものがある。複雑な演算式
をマイクロコンピユータで精度よく求めるには、
計算に多くのメモリ容量を必要とし、しかも演算
に時間がかかる。このため温度と圧力に対する比
重量のテーブルを備えておき、テーブル補間演算
により比重量を求めることも行われている。しか
しこの場合も比重量が温度、圧力に対して大きく
曲がつているので、精度よく求めるにはテーブル
の区分をこまかくしなければならず、多くのメモ
リ容量を必要とする。
本発明の目的は、複雑な演算を少ないメモリで
高速かつ精度よくできる演算器を実現するにあ
る。
本発明は、温度検出器によりスチームの温度が
温度信号に変換され圧力検出器により先のスチー
ムの圧力が圧力信号に変換されてそれぞれ入力さ
れこれ等の信号を基づいて先のスチームの実用国
際状態式に基づいた比重量に近似する近似比重量
の演算をする近似式演算手段と、先の比重量と先
の近似比重量の先の温度と圧力に対する比重量差
が格納されたテーブルと、先の温度信号と先の圧
力信号と先の比重量差とを用いて補正演算式を求
めこれから比重量補正値を算出する補正値演算手
段と、先の近似比重量と先の比重量補正値とを代
数加算して加算比重量を求める加算演算手段と、
先のスチームの流量が流量検出器により変換され
た流量信号に加算比重量を乗算して重量流量を算
出する重量流量演算手段とを設けることによつ
て、上述の目的を達成したものである。
第1図は本発明演算器の一実施例を機能的に示
すブロツク線図で、スチームの重量流量を求める
場合が例示してある。図において、1は流量検出
器(図示せず)よりのスチームの流量信号Q(m3)
が加わる端子、2は温度検出器(図示せず)より
のスチームの温度信号T(〓)が加わる端子、3
は圧力検出器(図示せず)よりの圧力信号P(Kg
f/m2)が加わる端子、4は近似式演算手段で、
温度信号Tと圧力信号Pに基づいて次式の近似演
算を行い比重量の近似値γ′(Kgf/m3)を算出す
る。
1/γ′=47.06T/P−0.668/(T/100
)3−437+6.31x10-3P/(T/100)8(1)
5は実用国際状態式に基づいた比重量γと近似値
γ′との差(γ−γ′)の温度と圧力に対するテーブ
ルで、あらかじめパソコン等でスチームに関する
国際状態式に基づいた実用国際状態式に基づいた
比重量γと(1)式の近似式による比重量の近似値
γ′とを計算し、その差(γ−γ′)を求めて作成さ
れる。
ここで、スチームに関する実用国際状態式に基
づいて算出される比重量γついて説明する。この
詳細については、1980年 日本機械学会蒸気表
(、発行所:日本機械学会、発行日:昭和56年2
月20日)に掲載されているが、その概要を以下に
説明する。
この比重量γは比容積vの逆数として与えら
れ、比容積vは、圧力−温度線図のスチーム領域
において、換算比容積X=v/vC1(但し、vC1=
0.00317m3/Kg)として、次の(1A)式により求
めることができる。
但し、θは換算温度T/TC1(TC1=647.3K)、
βは換算圧力P/PC1(PC1=22120000N/m2)、I1
は換算理想気体定数でありI1=4.260321148×100
である。
ここで、
X=exp{b(1−θ)} ……(1B)
βL=βL(θ)
=L0+L1θ+L2θ2 ……(1C)
である。ただし、
誘導定数L0,L1,L2は、L0=1.574373327×
101,L1=−3.417061978×101,L2=1.931380707
×101で与えられる。
また、μに対するn(μ)および1(μ)の数、
或いは指数z(μ,ν)およびx(μ,λ)の値は
第1表の通りである。
TECHNICAL FIELD The present invention relates to a computing unit used for flow measurement and the like. Computing units used for flow rate measurement are required to have various computing functions in response to various fluids such as natural gas, general gas, steam, and liquids, so recently they have been constructed using microcomputers. By the way, some calculations in flow rate measurement include very complicated calculation formulas, such as the calculation of specific weight based on the temperature and pressure of steam. To accurately calculate complex arithmetic expressions using a microcomputer,
Calculations require a large amount of memory and take a long time. For this reason, a table of specific weight with respect to temperature and pressure is provided, and the specific weight is determined by table interpolation calculation. However, in this case as well, the specific weight is largely curved with respect to temperature and pressure, so in order to obtain it with high accuracy, the table must be divided carefully, and a large amount of memory capacity is required. An object of the present invention is to realize an arithmetic unit that can perform complex operations at high speed and with high precision using a small amount of memory. In the present invention, the temperature of the steam is converted into a temperature signal by a temperature sensor, and the pressure of the steam is converted into a pressure signal by a pressure detector, which are inputted respectively, and based on these signals, the practical international state of the steam is determined. an approximate formula calculating means for calculating an approximate specific weight that approximates the specific weight based on the formula; a table storing the specific weight difference between the previous specific weight and the previous approximate specific weight with respect to the previous temperature and pressure; a correction value calculation means for calculating a correction calculation formula using the temperature signal, the pressure signal, and the specific weight difference, and calculating the specific weight correction value therefrom; an addition calculation means for calculating the addition ratio weight by algebraically adding the
The above object is achieved by providing a weight flow rate calculation means for calculating a weight flow rate by multiplying a flow rate signal obtained by converting the steam flow rate by a flow rate detector by an addition specific weight. FIG. 1 is a block diagram functionally illustrating an embodiment of the computing device of the present invention, illustrating the case where the weight flow rate of steam is determined. In the figure, 1 is the steam flow rate signal Q (m 3 ) from the flow rate detector (not shown).
2 is the terminal to which the steam temperature signal T(〓) from the temperature detector (not shown) is applied, 3
is the pressure signal P (Kg) from the pressure detector (not shown)
f/m 2 ) is added, 4 is an approximate expression calculation means,
Based on the temperature signal T and pressure signal P, an approximation calculation of the following equation is performed to calculate an approximate value γ' (Kgf/m 3 ) of specific weight. 1/γ'=47.06T/P-0.668/(T/100
) 3 −437 + 6.31x10 -3 P/(T/100) 8 (1) 5 is the difference (γ − γ′) between the specific weight γ and the approximate value γ′ based on the practical international equation of state as a function of temperature and pressure. On a table, calculate in advance on a computer, etc., the specific weight γ based on the practical international equation of state based on the international equation of state for steam and the approximate value γ′ of the specific weight based on the approximation formula of equation (1), and calculate the difference (γ −γ′). Here, the specific weight γ calculated based on the practical international equation of state regarding steam will be explained. For details, see the 1980 Japan Society of Mechanical Engineers Steam Table (Publisher: Japan Society of Mechanical Engineers, Publication date: February 1980)
The following is an overview of the publication. This specific weight γ is given as the reciprocal of the specific volume v, and the specific volume v is the converted specific volume X=v/v C1 (however, v C1 =
0.00317m 3 /Kg), it can be calculated using the following formula (1A). However, θ is the converted temperature T/T C1 (T C1 = 647.3K),
β is the converted pressure P/P C1 (P C1 = 22120000N/m 2 ), I 1
is the reduced ideal gas constant and I 1 = 4.260321148×10 0
It is. Here, X=exp{b(1-θ)} ...(1B) β L =β L (θ) = L 0 +L 1 θ+L 2 θ 2 ...(1C). However, the induction constants L 0 , L 1 , L 2 are L 0 = 1.574373327×
10 1 , L 1 = −3.417061978×10 1 , L 2 = 1.931380707
It is given by ×10 1 . Also, the number of n(μ) and 1(μ) for μ,
Alternatively, the values of the indexes z (μ, ν) and x (μ, λ) are as shown in Table 1.
【表】【table】
【表】
さらに、(1A)式におけるμ、νをパラメータ
とする定数Bは第2表で与えられる。[Table] Furthermore, the constant B in which μ and ν are parameters in equation (1A) is given in Table 2.
【表】
なお、テーブル5の格子点(データのある点)
は通常等間隔に選ばれるが、本実施例ではスチー
ムが第2図に示すように飽和蒸気圧曲線によつて
定義される範囲に限定されているので、飽和蒸気
圧曲線上にテーブルの温度T、圧力Pの格子点を
とるために、温度T、圧力Pのいずれか一方のみ
等間隔に選んである。第2図イが温度Tを等間隔
に選んだ場合であり、第2図ロが圧力Pを等間隔
に選んだ場合である。なお図にはスチームの実用
範囲を考慮してTは100〜400℃、Pは1〜100Kg
f/cm2obsの範囲で示してある。6は補正値Δγの
演算手段で、温度信号Tと圧力信号Pに基づいて
テーブル5からテーブル補間演算により補正値
Δγを求めるものである。テーブル補間演算は、
二つの変数T,Pに対してΔγの値が決まつてい
るので、平面の方程式
Δγ=a・T+b・P+c
の係数a,b,cを求め、これによりΔγの値を
算出するものである。その演算は、まず測定点
(T,P)を取り囲むテーブル5の四つの格子点
A(TNt,PNp,ΔγNt,Np)、B(TNt+1,PNp,
ΔγNt+1,Np)、C(TNt+1,PNp+1,ΔγNt+1,Np+1)、
D
(TNt,PNp+1,ΔγNt,Np+1)を決める。次にこの四
角形ABCDの中に、三角形ABCおよび三角形
ACDの二つの三角形を考え、測定点(T,P)
がどちらの三角形に属するかを調べる。その結果
測定点(T,P)が三角形ABCに属する場合に
は格子点A,B,Cに対応する三つの平面の方程
式、
a・TNt+b・PNp+c=ΔγNt,Np
a・TNt+1+b・PNp+c=ΔγNt+1,Np
a・TNt+1+b・PNp+1+c=ΔγNt+1,Np+1 (3)
により係数a,b,cの値を求め、(2)式により
Δγを求める。なお測定点(T,P)が三角形
ACDに属する場合には、格子点A,C,Dに対
応する三つの平面の方程式により係数a,b,c
の値を求める。
7は加算手段で、近似式演算手段4からの近似
値γ′に補正値Δγ演算手段6からの補正値Δγを加
算し、近似値の誤差を補正した値(γ′+Δγ)を
比重量として求めるものである。8は重量流量演
算手段で、流量信号Qと加算手段7からの比重量
の演算値(γ′+Δγ)との乗算を行い、重量流量
Wを算出し出力するものである。そして上述の演
算手段4,6,7,8はコンピユータのプログラ
ムで実現される。
このように構成した本発明の動作を以下に説明
する。まず、温度信号Tと圧力信号Pに基づいて
近似式演算手段4で(1)式の近似演算を行い、比重
量の近似値γ′を求める。しかしこの近似式には2
%程度の誤差がある。次に実用国際状態式に基づ
いた比重量γと近似値γ′との差のテーブル5を用
いて、補正値演算手段6でテーブル補間演算によ
り、温度信号Tと圧力信号Pに応じた補正値Δγ
を求める。この補正値Δγを加算手段7に加え、
近似式演算手段4からの近似値γ′との加算を行な
い、γ′を補正した(γ′+Δγ)を比重量の演算値と
して出力する。この補正演算により誤差は±0.2
%以下となる。その後重量流量演算手段8によ
り、流量信号Qと比重量の演算値(γ′+Δγ)と
の間で、Q+(γ′+Δγ)となる演算を行い、重量
流量Wを算出する。
そして、(1)式による近似式演算はスチームに関
する国際状態式から実用国際状態式に基づいた比
重量γを求める演算に比して簡単になり、メモリ
容量が少なくてすみ、演算も高速にできる。また
補正値を求めるテーブル補間演算は、実用国際状
態式に基づいた比重量γと近似値γ′との差が実用
国際状態式に基づいた比重量γに比べて、温度、
圧力に対する曲がりが非常に小さくなり、それだ
けテーブルの区分を粗くできるため、メモリの容
量が非常に少なくてすむ。その結果近似値を求め
る近似式演算と補正値を求めるテーブル補間演算
とを組合せた本発明においては、少ないメモリ
で、精度よくかつ高速に比重量を演算できる。
なお上述では、近似式演算回路4で(1)式の演算
を行う場合を例示したが、(1)式をさらに簡略化し
た例えば次式の近似演算を行うようにしてもよ
い。
1/γ′=47.06T/P−0.668/(T/100)3 (4)
ただし、この場合(1)式の近似演算に比して誤差
が大きくなり、補正値の曲がりも大きくなるた
め、テーブルの区分を細かくする必要がある。要
する近似式とテーブルとは、少ないメモリで、精
度よくかつ高速に演算できる組合であればよい。
また上述では、スチームの比重量を演算する場合
を例示したが、これに限定されることなくその他
の複雑な演算式の演算に適用できることは言うま
でもない。
以上説明したように本発明においては、実用国
際状態式に基づいた比重量を求める複雑な演算式
を簡略化した近似式で演算を行つてまず近似値を
求め、次に実用国際状態式に基づいた比重量と近
似値との差のテーブルを用いてテーブル補間演算
により補正差を求め、この補正値で近似値を補正
しているので、複雑な演算式を少ないメモリで、
精度よくかつ高速に演算できる演算器が得られ
る。[Table] In addition, grid points in Table 5 (points with data)
are normally selected at equal intervals, but in this example, since the steam is limited to the range defined by the saturated vapor pressure curve as shown in FIG. , pressure P, only one of temperature T and pressure P is selected at equal intervals. Figure 2A shows the case where the temperature T is selected at equal intervals, and Figure 2B shows the case where the pressure P is selected at equal intervals. In addition, in the figure, considering the practical range of steam, T is 100 to 400℃ and P is 1 to 100Kg.
It is shown in the range of f/cm 2 obs. Reference numeral 6 denotes a calculation means for calculating the correction value Δγ, which calculates the correction value Δγ from the table 5 by table interpolation calculation based on the temperature signal T and the pressure signal P. The table interpolation calculation is
Since the value of Δγ is determined for the two variables T and P, we find the coefficients a, b, and c of the plane equation Δγ=a・T+b・P+c, and use these to calculate the value of Δγ. . The calculation begins with the four grid points A (T Nt , P Np , Δγ Nt,Np ), B (T Nt+1 , P Np ,
Δγ Nt+1,Np ), C(T Nt+1 , P Np+1 , Δγ Nt+1,Np+1 ),
D
(T Nt , P Np+1 , Δγ Nt,Np+1 ) are determined. Next, inside this quadrilateral ABCD, triangle ABC and triangle
Considering two triangles of ACD, measurement points (T, P)
Find out which triangle belongs to. As a result, if the measurement point (T, P) belongs to triangle ABC, the equations of the three planes corresponding to grid points A, B, and C are a・T Nt +b・P Np +c=Δγ Nt,Np a・T Nt+1 +b・P Np +c=Δγ Nt+1,Np a・T Nt+1 +b・P Np+1 +c=Δγ Nt+1,Np+1 (3) and calculate Δγ using equation (2). Note that the measurement point (T, P) is a triangle.
If it belongs to ACD, the coefficients a, b, c are
Find the value of. 7 is an addition means which adds the correction value Δγ from the correction value Δγ calculation means 6 to the approximate value γ′ from the approximate formula calculation means 4, and calculates the value (γ′+Δγ) obtained by correcting the error of the approximate value as the specific weight. It is something to seek. Reference numeral 8 denotes a weight flow rate calculating means which multiplies the flow rate signal Q by the calculated specific weight value (γ'+Δγ) from the adding means 7 to calculate and output the weight flow rate W. The arithmetic means 4, 6, 7, and 8 described above are realized by a computer program. The operation of the present invention configured as described above will be explained below. First, based on the temperature signal T and the pressure signal P, the approximation calculation means 4 performs the approximation calculation of equation (1) to obtain an approximate value γ' of the specific weight. However, this approximate formula has 2
There is an error of about %. Next, using the table 5 of the difference between the specific weight γ and the approximate value γ' based on the practical international equation of state, the correction value calculation means 6 performs table interpolation calculation to calculate the correction value according to the temperature signal T and the pressure signal P. Δγ
seek. Adding this correction value Δγ to the addition means 7,
The approximation value γ' from the approximation formula calculation means 4 is added, and γ' is corrected (γ'+Δγ), which is output as the calculated value of the specific weight. This correction calculation results in an error of ±0.2
% or less. Thereafter, the weight flow rate calculating means 8 calculates the weight flow rate W by calculating Q+(γ'+Δγ) between the flow rate signal Q and the calculated value of specific weight (γ'+Δγ). The approximation calculation using equation (1) is simpler than the calculation of the specific weight γ based on the practical international equation of state from the international equation of state for steam, requires less memory capacity, and can be performed at high speed. . In addition, the table interpolation calculation for calculating the correction value shows that the difference between the specific weight γ based on the practical international equation of state and the approximate value γ′ is the temperature,
The bending in response to pressure becomes very small, and the table can be divided into sections that much more coarsely, so the memory capacity can be very small. According to the present invention, which combines approximate formula calculation for obtaining an approximate value and table interpolation calculation for obtaining a correction value, specific weight can be calculated accurately and at high speed with a small amount of memory. In the above description, the case where the approximation calculation circuit 4 performs the calculation of equation (1) has been exemplified, but it is also possible to further simplify equation (1), for example, to perform the approximate calculation of the following equation. 1/γ'=47.06T/P-0.668/(T/100) 3 (4) However, in this case, the error will be larger than in the approximate calculation of equation (1), and the curve of the correction value will also be larger, so It is necessary to divide the table into smaller sections. The required approximate expressions and tables may be combinations that can be calculated accurately and quickly with a small amount of memory.
Further, in the above description, the case where the specific weight of steam is calculated has been exemplified, but it goes without saying that the present invention is not limited to this and can be applied to calculations of other complicated calculation formulas. As explained above, in the present invention, an approximate value is obtained by first calculating an approximate value by simplifying the complex calculation formula for calculating specific weight based on the practical international equation of state, and then calculating an approximate value based on the practical international equation of state. Using a table of differences between specific weights and approximate values, the correction difference is calculated by table interpolation calculation, and the approximate value is corrected using this correction value, so complex calculation formulas can be written with less memory.
An arithmetic unit that can perform calculations with high precision and high speed can be obtained.
第1図は本発明演算器の一実施例を機能的に示
すブロツク線図、第2図はテーブルの格子点を説
明するための線図である。
1……流量信号の入力端子、2……温度信号の
入力端子、3……圧力信号の入力端子、4……近
似式演算手段、5……テーブル、6……補正値演
算手段、7……加算回路、8……重量流量演算手
段。
FIG. 1 is a block diagram functionally showing an embodiment of the arithmetic unit of the present invention, and FIG. 2 is a diagram for explaining grid points of a table. DESCRIPTION OF SYMBOLS 1... Input terminal for flow rate signal, 2... Input terminal for temperature signal, 3... Input terminal for pressure signal, 4... Approximate formula calculation means, 5... Table, 6... Correction value calculation means, 7... ...addition circuit, 8...weight flow rate calculation means.
Claims (1)
に変換され圧力検出器により前記スチームの圧力
が圧力信号に変換されてそれぞれ入力されこれ等
の信号を用いて前記スチームの実用国際状態式に
基づいた比重量に近似する近似比重量の演算をす
る近似式演算手段と、前記比重量と前記近似比重
量の前記温度と圧力に対する比重量差が格納され
たテーブルと、前記温度信号と前記圧力信号と前
記比重量差とを用いて補正演算式を求めこれから
比重量補正値を算出する補正値演算手段と、前記
近似比重量と前記比重量補正値とを代数加算して
加算比重量を求める加算演算手段と、前記スチー
ムの流量が流量検出器により変換された流量信号
に加算比重量を乗算して重量流量を算出する重量
流量演算手段とを具備することを特徴とする演算
器。1 The temperature of the steam is converted into a temperature signal by a temperature sensor, the pressure of the steam is converted into a pressure signal by a pressure detector, and these signals are used to calculate the ratio based on the practical international equation of state of the steam. an approximate formula calculating means for calculating an approximate specific weight that approximates the weight; a table storing the specific weight difference between the specific weight and the approximate specific weight with respect to the temperature and pressure; a correction value calculating means for determining a correction calculation formula using the specific weight difference and calculating a specific weight correction value therefrom; and an addition calculation means for calculating an added specific weight by algebraically adding the approximate specific weight and the specific weight correction value. and weight flow rate calculation means for calculating a weight flow rate by multiplying a flow rate signal obtained by converting the steam flow rate by a flow rate detector by an addition specific weight.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4562083A JPS59172080A (en) | 1983-03-18 | 1983-03-18 | Operator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4562083A JPS59172080A (en) | 1983-03-18 | 1983-03-18 | Operator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59172080A JPS59172080A (en) | 1984-09-28 |
| JPH0560142B2 true JPH0560142B2 (en) | 1993-09-01 |
Family
ID=12724416
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4562083A Granted JPS59172080A (en) | 1983-03-18 | 1983-03-18 | Operator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59172080A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0251771A (en) * | 1988-08-15 | 1990-02-21 | Nec Corp | High-speed numerical calculation system using numerical chart and interpolation formula |
-
1983
- 1983-03-18 JP JP4562083A patent/JPS59172080A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59172080A (en) | 1984-09-28 |
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