JPH0373813B2 - - Google Patents
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- Publication number
- JPH0373813B2 JPH0373813B2 JP57022316A JP2231682A JPH0373813B2 JP H0373813 B2 JPH0373813 B2 JP H0373813B2 JP 57022316 A JP57022316 A JP 57022316A JP 2231682 A JP2231682 A JP 2231682A JP H0373813 B2 JPH0373813 B2 JP H0373813B2
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- enthalpy
- relative humidity
- signal
- humidity
- 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
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D21/00—Measuring or testing not otherwise provided for
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Investigating Or Analyzing Materials Using Thermal Means (AREA)
- Investigating Or Analyzing Materials By The Use Of Fluid Adsorption Or Reactions (AREA)
- Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
- Testing Or Calibration Of Command Recording Devices (AREA)
Description
本発明は湿り空気の温度および相対湿度からエ
ンタルピを算出し出力するエンタルピ出力装置に
関する。
湿り空気のエンタルピを求めるには、一般の空
気調和で用いられる温度および圧力の範囲内では
一般に次の式が使用されている。
i=0.240t+(597.3+0.441t)x ……(イ)
x=0.622hs・/(P−hs・) ……(ロ)
ここでtは乾球温度〔℃〕、xは絶対湿度
〔Kg/Kg′〕Pは大気圧〔mmHg〕、hsは飽和蒸気
圧〔mmHg〕、は相対湿度〔%〕、iはエンタル
ピ〔kcal/Kg′〕である。
したがつて従来、空気のエンタルピを求めるた
めには測定項目として乾球温度の他に絶対湿度、
あるいは湿球温度、相対湿度、露点温度等を求め
る必要があつた。
ここで露点温度または絶対湿度を求める方法で
は演算は比較的容易であるが、検出素子の反応速
度が遅く、また素子が高価であるなどの欠点を有
していた。その他、湿球温度、相対湿度、を求め
る方法では演算式が複雑で、したがつてその演算
を実行する装置も複雑になるという欠点を有して
いた。
本発明は住環境の空気条件の要素として重要な
乾球温度と相対湿度とから、保健用空気調和にお
ける室内空気条件(約20℃〜30℃)および、外気
条件など広い温度範囲において、エンタルピ演算
式(ハ)を設定し、この演算式の演算を行ないエンタ
ルピを出力する装置を提供するものである。
i=(at2+bt+c)+mt+n ……(ハ)
ここにa,b,c,m,nは定数である。
本発明による演算式(ハ)式を実行する演算装置に
よつてエンタルピ値を求めれば、(イ),(ロ)式による
従来の複雑な演算を行なうことなく、またエンタ
ルピ演算を行なう実用温度範囲内では湿り空気線
図による読み取りよりも容易に、精度の高い値を
求めることができる。
次に演算式(ハ)の導き方を説明する。
湿り空気線図(i−x線図)およびエンタルピ
演算の基本式(イ),(ロ)では、エンタルピを相対湿度
と乾球温度の簡易な関係式で表わすことは難しい
が、乾球温度を一定とした時、第1図に示す如く
エンタルピiは相対湿度の一次関数で近似でき
るため(ニ)式で表し得る。
i=α+β ……(ニ)
ここでα,βは定数である。
次に各温度ごとに(ニ)で示される近似式を作成し
て各係数α,βの温度に対する変化を考察する
と、係数αは第2図のごとく温度tの二次関数(ホ)
で近似ができ、係数βは第3図のごとく温度tの
一次関数(ヘ)で近似ができることが判明した。
α=at2+bt+c ……(ホ)
β=mt+n ……(ヘ)
ここでa,b,c,m,nは定数である。
したがつて(ホ),(ヘ)式を(ニ)式に代入すると(ハ)式
が
得られる。次に示す(ト)式は温度範囲5℃〜35℃付
近を対象にして定数を求めた演算式である。
i=(1.692×10-4t2−8.140×10-4t
+0.03753)+0.2326t+0.1054 ……(ト)
次に(ト)式の求め方を説明する。基本式(イ),(ロ)に
おいて乾球温度を一定として相対湿度とエンタ
ルピiの関係を求め、相対湿度30%、および70%
の時のエンタルピ値より、一次式で近似をする。
例えば乾球温度20℃の場合にはエンタルピiと相
対湿度との関係は(チ)式で示される。
i=0.08898・+4.757 ……(チ)
同様に乾球温度10℃、15℃、25℃、30℃の場合
の関係一次式を求める。次に温度ごとの係数α,
βを最小2乗法で近似することにより、αは(リ)
式、βは(ヌ)式で表わせる。
α=1.692×10-4t2−8.140
×10-4+0.03753 ……(リ)
β=0.2326t+0.1054 ……(ヌ)
したがつて、(リ),(ヌ)式より(ト)式が求められる。
演算式(ト)と基本式(イ),(ロ)との精度比較を表1に示
すが全範囲にわたつてエンタルピ差が0.5以下と
高精度であり、実用の温度、相対湿度の範囲内で
は十分に精度の高いものである。
The present invention relates to an enthalpy output device that calculates and outputs enthalpy from the temperature and relative humidity of humid air. To find the enthalpy of humid air, the following formula is generally used within the range of temperature and pressure used in general air conditioning. i = 0.240t + (597.3 + 0.441t ) [Kg/Kg'] P is atmospheric pressure [mmHg], hs is saturated vapor pressure [mmHg], is relative humidity [%], and i is enthalpy [kcal/Kg']. Therefore, conventionally, in order to determine the enthalpy of air, in addition to the dry bulb temperature, absolute humidity,
Alternatively, it was necessary to obtain wet bulb temperature, relative humidity, dew point temperature, etc. Although the method of determining dew point temperature or absolute humidity is relatively easy to calculate, it has drawbacks such as slow reaction speed of the detection element and expensive element. In addition, methods for determining wet bulb temperature and relative humidity have the disadvantage that the calculation formulas are complicated, and therefore the equipment that executes the calculations is also complicated. The present invention uses dry bulb temperature and relative humidity, which are important elements of air conditions in living environments, to calculate enthalpy in a wide temperature range such as indoor air conditions (approximately 20°C to 30°C) in health air conditioning and outside air conditions. The present invention provides a device that sets the equation (c), performs calculations on this equation, and outputs enthalpy. i=(at 2 +bt+c)+mt+n...(c) Here, a, b, c, m, and n are constants. If the enthalpy value is determined by the arithmetic device that executes the calculation formula (c) according to the present invention, there is no need to perform the conventional complicated calculations using the formulas (a) and (b), and the practical temperature range in which the enthalpy calculation can be performed is achieved. It is easier to obtain more accurate values than reading from a psychrometric chart. Next, we will explain how to derive the arithmetic expression (c). In the hygrodynamic diagram (i-x diagram) and basic formulas (a) and (b) for enthalpy calculation, it is difficult to express enthalpy as a simple relational formula between relative humidity and dry bulb temperature, but dry bulb temperature can be expressed as When it is held constant, enthalpy i can be approximated by a linear function of relative humidity as shown in FIG. 1, so it can be expressed by equation (2). i=α+β...(d) Here, α and β are constants. Next, if we create an approximation equation (D) for each temperature and consider the changes in each coefficient α and β with respect to temperature, the coefficient α is a quadratic function (H) of the temperature t, as shown in Figure 2.
It was found that the coefficient β can be approximated by a linear function (F) of the temperature t as shown in Figure 3. α=at 2 +bt+c...(e) β=mt+n...(f) Here, a, b, c, m, and n are constants. Therefore, by substituting equations (e) and (f) into equation (d), equation (c) is obtained. Equation (g) shown below is an arithmetic expression in which constants are determined over a temperature range of 5°C to 35°C. i=(1.692×10 −4 t 2 −8.140×10 −4 t +0.03753)+0.2326t+0.1054 (G) Next, how to obtain equation (G) will be explained. In the basic formulas (a) and (b), the relationship between relative humidity and enthalpy i is determined with the dry bulb temperature constant, and the relative humidity is 30% and 70%.
From the enthalpy value when , approximate with a linear equation.
For example, when the dry bulb temperature is 20°C, the relationship between enthalpy i and relative humidity is expressed by equation (H). i=0.08898・+4.757...(H) Similarly, find the linear equation for the dry bulb temperatures of 10℃, 15℃, 25℃, and 30℃. Next, the coefficient α for each temperature,
By approximating β using the least squares method, α is (re)
Equation, β can be expressed as (nu) equation. α=1.692×10 -4 t 2 −8.140 ×10 -4 +0.03753 ……(li) β=0.2326t+0.1054 ……(nu) Therefore, from equations (li) and (nu), (g) A formula is required.
Table 1 shows a comparison of the accuracy between the calculation formula (g) and the basic formulas (a) and (b).The enthalpy difference is 0.5 or less over the entire range, which is highly accurate, and within the range of practical temperature and relative humidity. The accuracy is sufficiently high.
【表】
次に演算式(ト)で表わされる演算を行なうエンタ
ルピ演算装置の実施例を第4図〜第5図にもとづ
いて説明する。演算回路で演算を行なう場合には
(ハ)式を書き直した(ル)式が便利である。
i=(at2+bt+c)+mt+n
=a・{(t+p)2+q}・+mt+n
……(ル)
次に本発明の一実施例について説明する。
第4図は本発明の基本図であり、図中1は湿度
センサを備えた湿度信号出力部で、相対湿度に比
例した電圧を出力する。2および3は温度信号出
力部で温度を変数とする一次関数で表わされる抵
抗によつて増幅度を変化させる。5,6は第1及
び第2の乗算部で温度信号と相対湿度信号との乗
算を行なう。ここで乗算部5,6を直列に設置し
てあるため、乗算部6の出力は、相対湿度信号
と、温度信号の2乗との積で表わせる。7は加算
器で、乗算部6の出力信号と温度信号出力部4の
出力信号との加算を行ない、エンタルピ値を出力
部8に電圧値として出力する。
第5図は第4図に示す本発明の一実施例の具体
構成を示すもので、9は湿度変化を抵抗変化とし
て検出する湿度センサ10と直列に接続した抵抗
13とからなる湿度信号出力部である。端子11
の電圧値は端子12にかかる電圧値を湿度センサ
10の抵抗9および抵抗13の比率に分割した値
で、湿度センサ10すなわち、相対湿度に比例し
た電圧として表わすことが可能である。14,1
5,16は各温度センサ17,18,19およ
び、それぞれに接続する抵抗などの素子と協同し
て作用する抵抗で、おのおの温度の一次関数で表
わされる抵抗値を示すもので乗算器として使用す
る第1の乗算器としてのオペアンプ20の入力端
子11に相対湿度に比例した電圧を入力すると、
抵抗21および温度センサ14の抵抗17によつ
て定まる増幅度に応じた電圧が端子22に出力さ
れる。ここで温度センサの合成抵抗14を温度を
変数とする一次関数で表わすと、端子22の出力
電圧は相対湿度と、温度の一次関数の乗算で表わ
すことができる。同様に、第2の乗算器としての
オペアンプ23での乗算により、オペアンプ23
の出力端子24の電圧は相対湿度と温度の一次関
数の2乗の積で表わすことができる。ここでオペ
アンプ23の負帰還回路中に電圧出力部25を置
くことにより、演算式(ル)のβに相当する定数
補正を行なえる。オペアンプ26は加算器であつ
て、端子24の電圧と、端子27にかかる電圧を
温度センサ16の抵抗16と直列抵抗28の比率
に分割した電圧で表わされる端子29の電圧値と
の加算を行ない、端子30にエンタルピ値を電圧
値として出力する。
上述のように、演算式(ル)を実行してエンタ
ルピ値を導く方式による本発明のエンタルピ出力
装置は実施例に示すごとく、温度センサ、湿度セ
ンサと演算部でなる構成で、電子計算機を必要と
せずしかも構成素子の少ない、簡易な演算回路か
らなる安価な演算装置を作成することができる。
以上の通り、本発明のエンタルピ出力装置は、
環境指数として最も重要な乾球温度と相対湿度を
変数とする簡単な演算式から演算をする方式のn
装置であるため、乾球温度と相対湿度を検出すれ
ば、飽和蒸気圧など他の要素を近似式あるいは換
算表などで検索する必要がなく、直接演算でき
る。また本発明によるエンタルピ出力装置は、温
度信号、湿度信号の演算部をプログラム化するこ
とにより、電子計算機などで演算する場合にも容
易にしかも精度の高い値を演算することが可能で
ある。また本演算装置によれば空気調和を行なう
場合に直接対象となる温度、相対湿度から空気の
保有する熱エネルギーであるエンタルピ値を電気
信号として出力することができるため、空気調和
の自動制御に展開することが容易であることなど
利点の大なるものである。また、この装置は構成
要素が少ないので、簡単な構成のエンタルピ出力
装置の実現が可能となる。[Table] Next, an embodiment of an enthalpy calculation device that performs the calculation expressed by the calculation formula (g) will be described based on FIGS. 4 and 5. When performing calculations with an arithmetic circuit,
Equation (L), which is a rewrite of Equation (C), is convenient. i=(at 2 +bt+c)+mt+n =a・{(t+p) 2 +q}・+mt+n
...(l) Next, one embodiment of the present invention will be described. FIG. 4 is a basic diagram of the present invention. In the figure, 1 is a humidity signal output section equipped with a humidity sensor, which outputs a voltage proportional to relative humidity. Reference numerals 2 and 3 are temperature signal output sections, and the degree of amplification is changed by a resistance expressed by a linear function with temperature as a variable. Reference numerals 5 and 6 denote first and second multipliers for multiplying the temperature signal and the relative humidity signal. Here, since the multipliers 5 and 6 are installed in series, the output of the multiplier 6 can be expressed as the product of the relative humidity signal and the square of the temperature signal. An adder 7 adds the output signal of the multiplication section 6 and the output signal of the temperature signal output section 4, and outputs an enthalpy value to the output section 8 as a voltage value. FIG. 5 shows a specific configuration of one embodiment of the present invention shown in FIG. 4, in which reference numeral 9 denotes a humidity signal output section consisting of a humidity sensor 10 that detects humidity changes as resistance changes and a resistor 13 connected in series. It is. Terminal 11
The voltage value is a value obtained by dividing the voltage value applied to the terminal 12 by the ratio of the resistance 9 and the resistance 13 of the humidity sensor 10, and can be expressed as a voltage proportional to the humidity sensor 10, that is, relative humidity. 14,1
5 and 16 are resistors that act in cooperation with the temperature sensors 17, 18, and 19 and elements such as resistors connected to each, and are used as multipliers, each representing a resistance value expressed as a linear function of temperature. When a voltage proportional to the relative humidity is input to the input terminal 11 of the operational amplifier 20 as the first multiplier,
A voltage corresponding to the amplification determined by the resistor 21 and the resistor 17 of the temperature sensor 14 is output to the terminal 22 . Here, if the combined resistance 14 of the temperature sensor is expressed as a linear function with temperature as a variable, the output voltage of the terminal 22 can be expressed as the product of the relative humidity and the linear function of temperature. Similarly, the multiplication by the operational amplifier 23 as the second multiplier causes the operational amplifier 23 to
The voltage at the output terminal 24 of can be expressed as the product of the square of a linear function of relative humidity and temperature. By placing the voltage output unit 25 in the negative feedback circuit of the operational amplifier 23, constant correction corresponding to β in the arithmetic expression (L) can be performed. The operational amplifier 26 is an adder, and adds the voltage at the terminal 24 and the voltage value at the terminal 29, which is represented by the voltage obtained by dividing the voltage applied to the terminal 27 by the ratio of the resistor 16 of the temperature sensor 16 and the series resistor 28. , outputs the enthalpy value to the terminal 30 as a voltage value. As mentioned above, the enthalpy output device of the present invention, which uses the method of deriving the enthalpy value by executing the arithmetic expression (R), is composed of a temperature sensor, a humidity sensor, and a calculation section, as shown in the embodiment, and does not require an electronic computer. In addition, it is possible to create an inexpensive arithmetic device consisting of a simple arithmetic circuit with a small number of constituent elements. As mentioned above, the enthalpy output device of the present invention is
n, a method that calculates from a simple formula using dry bulb temperature and relative humidity, which are the most important environmental indices, as variables.
Since it is a device, once dry bulb temperature and relative humidity are detected, other factors such as saturated vapor pressure can be calculated directly without the need to search for approximations or conversion tables. Further, the enthalpy output device according to the present invention can easily calculate values with high precision even when calculating with an electronic computer etc. by programming the calculation section of the temperature signal and humidity signal. In addition, this computing device can output the enthalpy value, which is the thermal energy held by the air, as an electrical signal from the temperature and relative humidity that are directly targeted when performing air conditioning, so it can be used for automatic control of air conditioning. It has great advantages such as being easy to do. Furthermore, since this device has fewer components, it is possible to realize an enthalpy output device with a simple configuration.
第1図は相対湿度とエンタルピとの関係を示す
グラフ、第2図は乾球温度と係数を示すグラフ、
第3図は乾球温度と係数βとの関係を示すグラ
フ、第4図は本発明実施例の基本構成図、第5図
は同実施例の電気回路図である。
10……湿度センサ、17,18,19……温
度センサ、20,21,26……オペアンプ。
Figure 1 is a graph showing the relationship between relative humidity and enthalpy, Figure 2 is a graph showing dry bulb temperature and coefficient,
FIG. 3 is a graph showing the relationship between dry bulb temperature and coefficient β, FIG. 4 is a basic configuration diagram of an embodiment of the present invention, and FIG. 5 is an electric circuit diagram of the embodiment. 10... Humidity sensor, 17, 18, 19... Temperature sensor, 20, 21, 26... Operational amplifier.
Claims (1)
と、温度を温度信号に変換する温度センサと、前
記温度信号を入力とし、温度信号の二次関数を導
く第1の演算手段と、前記第1の演算手段の出力
と前記湿度信号との積信号を導く第2の演算手段
と、前記温度信号の一次関数も導く第3の演算手
段と前記第2の演算手段の出力と前記第3の演算
手段の出力とを加算し、その結果をエンタルピ値
として出力をする第4の演算手段よりなる演算部
を有するエンタルピ出力装置。1. A humidity sensor that converts relative humidity into a humidity signal, a temperature sensor that converts temperature into a temperature signal, a first calculation means that receives the temperature signal as input and derives a quadratic function of the temperature signal, and the first a second calculation means that derives a product signal of the output of the calculation means and the humidity signal; a third calculation means that also derives a linear function of the temperature signal; and an output of the second calculation means and the third calculation means. An enthalpy output device having an arithmetic unit including a fourth arithmetic means that adds the outputs of the two and outputs the result as an enthalpy value.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57022316A JPS58139018A (en) | 1982-02-15 | 1982-02-15 | Enthalpy output device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57022316A JPS58139018A (en) | 1982-02-15 | 1982-02-15 | Enthalpy output device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58139018A JPS58139018A (en) | 1983-08-18 |
| JPH0373813B2 true JPH0373813B2 (en) | 1991-11-25 |
Family
ID=12079320
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57022316A Granted JPS58139018A (en) | 1982-02-15 | 1982-02-15 | Enthalpy output device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58139018A (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5723846A (en) * | 1980-07-21 | 1982-02-08 | Kazuhiro Miyamoto | Measuring device for a thermodynamic function |
-
1982
- 1982-02-15 JP JP57022316A patent/JPS58139018A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58139018A (en) | 1983-08-18 |
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