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JPH0511766B2 - - Google Patents
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JPH0511766B2 - - Google Patents

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Publication number
JPH0511766B2
JPH0511766B2 JP61052249A JP5224986A JPH0511766B2 JP H0511766 B2 JPH0511766 B2 JP H0511766B2 JP 61052249 A JP61052249 A JP 61052249A JP 5224986 A JP5224986 A JP 5224986A JP H0511766 B2 JPH0511766 B2 JP H0511766B2
Authority
JP
Japan
Prior art keywords
heating element
heat
thermal
amount
human body
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
JP61052249A
Other languages
Japanese (ja)
Other versions
JPS62259014A (en
Inventor
Masahiro Kobayashi
Noboru Kobayashi
Shigehiro Kamimura
Kunikazu Torigoe
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.)
Daikin Industries Ltd
Original Assignee
Daikin Industries 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 Daikin Industries Ltd filed Critical Daikin Industries Ltd
Priority to JP61052249A priority Critical patent/JPS62259014A/en
Publication of JPS62259014A publication Critical patent/JPS62259014A/en
Publication of JPH0511766B2 publication Critical patent/JPH0511766B2/ja
Granted legal-status Critical Current

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  • Testing Or Calibration Of Command Recording Devices (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、例えば空気調和装置により人体に快
適に室内環境を提供する際にその空気調和装置の
制御データとなる環境の温熱状態を検知するため
の温熱検知素子に関し、特に、人体の皮膚表面か
らの水分蒸発に伴う湿性放熱を考慮したものに関
するものである。
[Detailed Description of the Invention] (Industrial Application Field) The present invention detects the thermal state of the environment, which serves as control data for the air conditioner, for example, when an air conditioner provides a comfortable indoor environment for the human body. The present invention relates to a thermal sensing element for use in the human body, and particularly to one that takes into consideration humid heat radiation accompanying moisture evaporation from the skin surface of the human body.

(従来の技術) 一般に、空気調和装置を室内の空気温度のみに
基づいて制御して室内を人体に快適な温熱状態に
保つには限度があり、その他の温熱環境因子とし
て気流速、湿度、輻射の各物理量を合わせて実際
の居住温熱環境を評価する必要がある。そして、
このような温熱状態を検知するための温熱検知素
子には、人体の熱的平衡を拠りどころに、素子と
人体との間に熱的な相関関係が成立するように製
作すべきことが要求される。
(Prior art) In general, there is a limit to the ability to maintain a room in a thermal state that is comfortable for the human body by controlling an air conditioner based only on the indoor air temperature. It is necessary to evaluate the actual residential thermal environment by combining each physical quantity. and,
Thermal detection elements for detecting such thermal conditions are required to be manufactured in such a way that a thermal correlation is established between the element and the human body, based on the thermal equilibrium of the human body. Ru.

ところで、この種の温熱検知素子として、従
来、例えば特開昭58−218624号公報に開示されて
いるように、中空状の球殻内に電気ヒータを配置
してなる電気発熱体と、該発熱体の表面湿度を測
定する温度測定器とを備え、電気ヒータへの通電
により発熱体へ所定の熱量を供給した上でその表
面温度を測定することにより、環境の温熱状態を
輻射を加味して検知するようにしたものは知られ
ている。
By the way, as this type of thermal detection element, conventionally, as disclosed in Japanese Patent Application Laid-Open No. 58-218624, an electric heating element consisting of an electric heater arranged in a hollow spherical shell, It is equipped with a temperature measuring device that measures the surface humidity of the body, and by supplying a predetermined amount of heat to the heating element by energizing the electric heater and then measuring the surface temperature, the thermal state of the environment can be calculated by taking into account radiation. Those that have been designed to detect this are known.

(発明が解決しようとする課題) しかし、上記従来のものでは、人体からの熱損
失(熱発散)を輻射および対流による乾性放熱の
みに限定し、皮膚表面からの水分蒸発に伴つて生
じる湿性放熱については考慮されていない。その
ため、実際の居住空間内における温熱状態を人間
の体感と同程度に精度良く評価するのに難があつ
た。
(Problems to be Solved by the Invention) However, in the conventional method described above, heat loss (heat dissipation) from the human body is limited to dry heat dissipation due to radiation and convection, and humid heat dissipation that occurs as moisture evaporates from the skin surface. is not considered. Therefore, it has been difficult to evaluate the thermal state in an actual living space as accurately as human sensation.

そこで、本発明は斯かる点に鑑みてなされたも
ので、その目的とするところは、上記の如く単一
の球殻等の殻体よりなる発熱体を備えた温熱検知
素子において、人体の皮膚表面からの水分蒸発に
よる湿性放熱を考慮し、その条件を満たすために
発熱体の寸法および供給熱量を最適範囲に特定す
ることにより、温熱検知素子を人間の実際の体感
により一層近似させるようにし、よつて実際の室
内の温熱環境を極めて精度よく検知し得るように
することにある。
Therefore, the present invention has been made in view of the above, and an object of the present invention is to provide a heat detecting element equipped with a heating element made of a single shell such as a spherical shell as described above. By taking into account humid heat dissipation due to moisture evaporation from the surface and specifying the dimensions of the heating element and the amount of heat supplied to the optimal range to satisfy the conditions, the temperature sensing element is made to more closely approximate the actual human sensation. Therefore, the object is to be able to detect the actual indoor thermal environment with extremely high accuracy.

(課題を解決するための手段) 上記の目的を達成するために、本発明の解決手
段は、第1図に示すように、中空状の殻体3内に
電気ヒータ4が配置されているとともに該殻体3
の外表面に人体に基づく分光輻射率と略合致する
輻射率を有する輻射材料層8が形成されてなる発
熱体1と、該発熱体1の表面湿度Tgを測定する
温度測定器7とを備え、上記発熱体1に所定の熱
量を供給した上でその表面湿度Tgに基づいて室
内環境の温熱状態を検知する温熱検知素子を前提
とする。そして、上記発熱体1の殻体3の寸法お
よび発熱体1への供給熱量Mを、発熱体1の対流
熱伝達率を人体の蒸発を伴つた対流熱伝達率とほ
ぼ合致させるとともに上記発熱体1への供給熱量
を人体の衣服の熱抵抗を考慮した皮膚表面からの
放散熱量とほぼ合致させて発熱体1の熱的平衡特
性が湿性放熱まで考慮した人体の熱的平衡特性と
等価になるように設定した構成としている。
(Means for Solving the Problems) In order to achieve the above object, the solving means of the present invention is as shown in FIG. The shell body 3
A heating element 1 in which a radiant material layer 8 having an emissivity substantially matching the spectral emissivity based on the human body is formed on the outer surface of the heating element 1, and a temperature measuring device 7 for measuring the surface humidity Tg of the heating element 1. , assumes a thermal detection element that supplies a predetermined amount of heat to the heating element 1 and then detects the thermal state of the indoor environment based on the surface humidity Tg. Then, the dimensions of the shell 3 of the heating element 1 and the amount of heat M supplied to the heating element 1 are adjusted so that the convective heat transfer coefficient of the heating element 1 almost matches the convective heat transfer coefficient with evaporation of the human body, and the heating element By making the amount of heat supplied to the heating element 1 almost match the amount of heat dissipated from the skin surface taking into account the thermal resistance of human clothing, the thermal equilibrium characteristics of the heating element 1 become equivalent to the thermal equilibrium characteristics of the human body, taking into account moisture heat radiation. The configuration is set as follows.

ここで、上記発熱体1の殻体3の寸法および発
熱体1への供給熱量Mの限定方法について以下に
詳細に説明する。
Here, the dimensions of the shell 3 of the heating element 1 and the method for limiting the amount of heat M supplied to the heating element 1 will be explained in detail below.

すなわち、第1図に示す温熱検知素子における
熱的平衡式は、 M=h gr(Tg−Tr)+h gc(Tg−Ta)
…(1) (但し、Tg:発熱体の表面温度、Tr:室内環
境の平均輻射温度、Ta:気温、h gr:発熱体
の輻射熱伝達率、h gc:発熱体の対流熱伝達
率) となる。一方、任意の非等温度環境下での人体の
皮膚表面からの放散熱量Hskを求めると、人体か
らの輻射、対流および蒸発による熱損失をそれぞ
れR,C,Eとして、 Hsk=R+C+E …(2) となり、上記各熱損失R,C,Eは次式で示され
る。
That is, the thermal equilibrium equation for the thermal sensing element shown in Figure 1 is: M=h gr (Tg - Tr) + h gc (Tg - Ta)
...(1) (Tg: surface temperature of the heating element, Tr: average radiant temperature of the indoor environment, Ta: air temperature, h gr: radiant heat transfer coefficient of the heating element, h gc: convective heat transfer coefficient of the heating element) Become. On the other hand, when calculating the amount of heat dissipated from the skin surface of the human body under any non-isothermal environment, Hsk=R+C+E...(2 ), and the above heat losses R, C, and E are expressed by the following equations.

R=hr・Fcl・(Tsk−Tr) …(3) C=hc・Fcl・(Tsk−Ta) …(4) E=w・k・hc・Fpcl・(Psk−φa・Pa)
…(5) (但し、hr:人体の輻射伝達率、hc:人体の
対流熱伝達率、Tsk:平均皮膚温度、φa:相対
湿度、Psk:平均皮膚温度Tskでの飽和蒸気圧、
Pa:気温Taでの飽和蒸気圧、w:皮膚の濡れ面
積率、Fcl:衣服の熱抵抗を示す係数、Fpcl:皮
膚表面から周囲に蒸発する水蒸気に対する衣服の
透過率、k:Lewisの関係で海面では2.2) ここで、米国の空中衛生学会ASHRAEで設定
され、人間の温冷感、快適感と密接な関係がある
新標準有効温度SET*を導入して室内での温熱快
適性を評価する場合、その理論に基づいて算出さ
れる放散熱量が上記(2)式でのHskと等しくなるよ
うにSET*を決定すると、 Hsk=hs・Fcls(Tsk−SET*)+w・k・hcs・
Fpcls(Psk−0.5PSET *) …(6) (ただし、hcs:標準気流での人体の対流熱伝
達率、hs:人体の輻射熱伝達率hrに標準気流での
人体の対流熱伝達率hcsを加えた熱伝達率、PSET
:SET*での飽和水蒸気圧、Fcls:着衣量0.6clo
における衣服の熱抵抗係数、Fpcls:着衣量
0.6cloにおける蒸発水蒸気に対する衣服の透過
率) となる。すなわち、SET*は、(2)式で与えられる
Hskと等しい熱量を、標準状態(着衣量0.6clo、
気流速0.1〜0.15m/s、湿度50%、Tr=Ta)で
かつ等しい生理状態(Tsk,wが等しい)で放散
できるような等温環境と定義した温度であつて、
気温Ta、平均輻射温度Tr、気流速に依存し、例
えば着衣量0.6clo、湿度50%、産熱量1Met(=
58.2W/m2)の標準状態で気流速が0.1〜0.15m/
sのとき、SET*がSET*=22.2〜25.6℃であれば
80%以上の人間が温熱的に快適であると
ASHRAEで認められているものである。
R=hr・Fcl・(Tsk−Tr) …(3) C=hc・Fcl・(Tsk−Ta) …(4) E=w・k・hc・Fpcl・(Psk−φa・Pa)
...(5) (However, hr: radiation transfer coefficient of the human body, hc: convective heat transfer coefficient of the human body, Tsk: average skin temperature, φa: relative humidity, Psk: saturated vapor pressure at average skin temperature Tsk,
Pa: saturated vapor pressure at temperature Ta, w: skin wet area ratio, Fcl: coefficient indicating thermal resistance of clothing, Fpcl: permeability of clothing to water vapor evaporating from the skin surface to the surroundings, k: Lewis relationship 2.2 at sea level) Here, we will evaluate indoor thermal comfort by introducing a new standard effective temperature SET * , which has been set by the American Air Hygiene Society ASHRAE and is closely related to human thermal sensation and comfort. In this case, if SET * is determined so that the amount of dissipated heat calculated based on the theory is equal to Hsk in equation (2) above, Hsk = hs・Fcls (Tsk − SET * ) + w・k・hcs・
Fpcls (Psk−0.5P SET * ) …(6) (where, hcs: convective heat transfer coefficient of the human body in standard airflow, hs: radiant heat transfer coefficient of the human body, hcs) Added heat transfer coefficient, P SET
* : Saturated water vapor pressure at SET * , Fcls: Clothing amount 0.6clo
Thermal resistance coefficient of clothing, Fpcls: amount of clothing
Transmittance of clothing to evaporated water vapor at 0.6clo). In other words, SET * is given by equation (2)
The amount of heat equal to Hsk in the standard state (clothing amount 0.6clo,
The temperature is defined as an isothermal environment where airflow velocity is 0.1 to 0.15 m/s, humidity is 50%, Tr = Ta) and can be dissipated under equal physiological conditions (Tsk, w are equal),
Depends on the air temperature Ta, average radiant temperature Tr, and airflow velocity.For example, amount of clothing is 0.6clo, humidity is 50%, heat production is 1Met (=
58.2W/m 2 ) air flow velocity is 0.1-0.15m/
When s, if SET * is SET * = 22.2 to 25.6℃
More than 80% of people are thermally comfortable
It is approved by ASHRAE.

上記(2)式で示される人体の熱平衡式において、
湿性放熱分を考慮し、快適域付近(気温22〜26
℃)を考えて調節発汗の無い状態(w=0.06)と
するとともに、相対湿度φaをφa=0.5とした条件
を設定することにより、右辺のC+Eを近似的に C+E=hc′・Fcl(Tsk−Ta) …(7) (ただし、hc′:蒸発を伴つた対流熱伝達率) とまとめると、上記(2)式は、 Hsk/Fcl=hr(Tsk−Tr)+ hc′(Tsk−Ta) …(8) に書き代えられる。
In the thermal equilibrium equation of the human body shown by equation (2) above,
Considering the moisture heat dissipation, the temperature is around the comfortable range (temperature 22-26
C+E on the right side can be approximated by C+E=hc′・Fcl(Tsk −Ta) …(7) (where hc′: convective heat transfer coefficient with evaporation), the above equation (2) is: Hsk/Fcl=hr(Tsk−Tr)+hc′(Tsk−Ta ) ...(8) can be rewritten.

そして、上記(1)式と(8)式とを比較したとき、 h gr=hr …(9) h gc=hc′ …(10) M=Hsk/Fcl …(11) の関係が成立すれば、発熱体の表面温度Tgが人
体の平均皮膚温度Tskと等しくなつて、 Tg=Tsk …(12) となる(以下、(9)〜(11)式を満たすような特性を有
する発熱体表面温度TgをKET*と表示する)。
When comparing equations (1) and (8) above, if the following relationships hold: h gr=hr...(9) h gc=hc'...(10) M=Hsk/Fcl...(11) , when the surface temperature Tg of the heating element becomes equal to the average skin temperature Tsk of the human body, Tg=Tsk...(12) Display Tg as KET * ).

一方、上記したSET*においても湿性放熱を対
流熱損失に組み入れると、上記(6)式は、 Hsk=hs′・Fcls(Tsk−SET*) …(13) (ただし、hs′:標準気流での対流、蒸発およ
び輻射による総合熱伝達率) となる。上記(12)と(13)式とにより、 SET*=KET*−Hsk/(Fcls・hs′) …(14) となり、快適域付近を考えると、(14)式の右辺第2
項は定数と近似できる。
On the other hand, when moisture heat radiation is incorporated into convective heat loss in SET * mentioned above, the above equation (6) becomes The total heat transfer coefficient due to convection, evaporation, and radiation is From equations (12) and (13) above, SET * = KET * −Hsk/(Fcls・hs′) …(14), and considering the vicinity of the comfort zone, the second right-hand side of equation (14)
The term can be approximated as a constant.

したがつて、上記(9)〜(11)式の条件を満足するよ
うな伝達特性を有する発熱体表面温度KET*を測
定することにより、SET*を近似的に求めること
ができ、温熱検知素子による実際の居住環境下で
の温熱評価を厳密に行い得ることになる。
Therefore, by measuring the heating element surface temperature KET * that has a transfer characteristic that satisfies the conditions of equations (9) to (11) above, SET * can be approximately determined, and the thermal sensing element This means that thermal evaluation can be performed strictly under the actual living environment.

そこで、本発明では、上記(9)〜(11)式の条件を満
足させるために、標準状態および快適域付近で湿
性放熱を考慮したSET*の気流速、平均輻射温度
に関する特性と上記発熱体表面温度KET*の同特
性とを合致させるように発熱体(1)への供給熱量M
とその寸法とを決定する。
Therefore, in the present invention, in order to satisfy the conditions of equations (9) to (11) above, we have developed the characteristics regarding the air flow velocity and average radiant temperature of SET * considering humid heat radiation in the standard state and near the comfort zone, and the above heating element. The amount of heat M supplied to the heating element (1) is adjusted to match the same characteristics of the surface temperature KET * .
and its dimensions.

すなわち、気流速0.1m/sの状態を基準状態
とし、その基準状態から気流速が1m/sまでの
範囲に亘つて変化したときに、その気流速変化に
伴うSET*およびKET*の各変化量△SET*、△
KET*間の差の2乗の平均値S S=(△*−△*2 …(15) を算出し、発熱体(1)の殻体(3)の寸法を種々の値に
設定した上でその各寸法に関して上記平均値Sが
最小となるような供給熱量Mを求め、そのときの
最小平均値Sを各寸法についてプロツトすると、
例えば殻体(3)が球殻の場合、横軸に直径Dを取る
と第2図に示すような特性を得られる。尚、発熱
体(1)の表面温度Tgを(1)式をもとに算出し、発熱
体(1)の対流熱伝達率h gcは下記の(16)に示す球
体の強制対流熱伝達に関する実験式を用いる。
In other words, when the air velocity is 0.1 m/s as the reference state, and the air velocity changes from the reference state to 1 m/s, each change in SET * and KET * due to the change in air velocity Amount △SET * , △
The average value of the square of the difference between KET * S S = (△ * −△ * ) 2 ...(15) was calculated, and the dimensions of the shell (3) of the heating element (1) were set to various values. If we calculate the amount of heat M to be supplied such that the average value S is the minimum for each dimension above, and plot the minimum average value S for each dimension, we get
For example, if the shell (3) is a spherical shell, the characteristics shown in FIG. 2 can be obtained by taking the diameter D on the horizontal axis. In addition, the surface temperature Tg of the heating element (1) is calculated based on equation (1), and the convective heat transfer coefficient h gc of the heating element (1) is related to the forced convection heat transfer of the sphere shown in (16) below. Use an empirical formula.

Nu=2+0.645Re0.505 …(16) (ただし、Nu:ヌセルト数、Re:レイノルズ
数) また、第3図は、球殻の直径Dが100mmの場合
において、供給熱量M(Met=58.2W/m2)を変
化させたときの2乗平均値Sの変化を示し、直径
Dが決まれば、そのときの2乗平均値Sが最小と
なる最適供給熱量Mが定まる。そして、第4図
に、球殻の直径Dが変化したときの最適供給熱量
Mの変化を示す。よつて、これら第2図〜第4図
より、2乗平均値Sを小さくし精度の良い温熱検
知素子とするためには、供給熱量Mと球殻直径D
とを特定する必要があることが判る。
Nu=2+0.645Re 0.505 ...(16) (Nu: Nusselt number, Re: Reynolds number) In addition, Fig. 3 shows the amount of heat supplied M (Met=58.2W/ m 2 ) is shown, and once the diameter D is determined, the optimum amount of heat to be supplied M that minimizes the root mean square value S at that time is determined. FIG. 4 shows changes in the optimum amount of heat M to be supplied when the diameter D of the spherical shell changes. Therefore, from these figures 2 to 4, in order to reduce the root mean square value S and obtain a highly accurate thermal sensing element, the amount of heat supplied M and the spherical shell diameter D
It turns out that it is necessary to specify.

また、上記と同様にして、平均輻射温度Trと
気温Taとが等しい(Tr=Ta)状態を基準状態
とし、Tr−Taが−5℃から+5℃まで変化した
ときに、そのTr−Taの増減変化に伴うSET*
よびKET*の各変化量△SET*および△KET*
関する上記2乗平均値Sを各直径Dについてプロ
ツトすれば第5図に示すような特性が得られる。
尚、発熱体(1)への供給熱量Mは上記気流速変化に
関する特性を求める際に決定した値を用いる(第
4図に各直径Dに対する最適供給熱量Mを示す)。
In addition, in the same way as above, the state where the average radiant temperature Tr and the air temperature Ta are equal (Tr = Ta) is set as the reference state, and when Tr-Ta changes from -5℃ to +5℃, that Tr-Ta changes. If the above-mentioned root mean square value S regarding the amount of change ΔSET * and ΔKET * in SET * and KET * due to the increase/decrease change is plotted for each diameter D, the characteristics shown in FIG. 5 are obtained.
The amount of heat M to be supplied to the heating element (1) is the value determined when determining the characteristics related to the change in air flow velocity (Fig. 4 shows the optimum amount of heat M to be supplied for each diameter D).

よつて、本発明では、球殻の場合、第2図およ
び第5図に示される特性に基づき、気流速および
平均輻射温度Trと気温Taとの差の各変化に対し
て△SET*と△KET*との間に極めて密接な相関
関係が成立するよう、発熱体(1)の直径DをD=60
〜150mmの範囲に特定し、かつ、この直径Dの範
囲について発熱体(1)への供給熱量MをM=76〜
105W/m2の範囲に特定することができる。
Therefore, in the present invention, in the case of a spherical shell, △SET * and △ are calculated based on the characteristics shown in FIGS. 2 and 5 for each change in air velocity and the difference between the average radiant temperature Tr and the air temperature Ta. In order to establish an extremely close correlation with KET * , the diameter D of the heating element (1) is set to D = 60.
Specify the range of ~150 mm, and calculate the amount of heat M supplied to the heating element (1) for this diameter D range from M=76 to
It can be specified in the range of 105W/ m2 .

すなわち、この特定理由について述べるに、第
5図より、球殻の直径Dが小さくなると2乗平均
値Sが著しく増大し、検知素子としての性能が低
下する。ここで、平均輻射温度Trを変化させた
場合、△KET*はこのTrと正比例関係となり、
△SET*もTrとほぼ正比例な関係となるので、
Trの増大に対して(△SET*−△KET*)も増大
する。そこで、上記平均輻射温度Trの1℃の変
化に対し、(△SET*−△KET*)を0.1℃まで許
容すると、第5図ではTrを−5℃〜+5℃まで
変化させているので、2乗平均値Sは、上記(15)式
よりS=0.1となる。そして、第5図より、この
SがS≦0.1である範囲は、球殻の直径DではD
≧60mmとなる。一方、温熱検知素子としてはその
大きさ、寸法が小さい方が使いやすいので、直径
Dの上限を150mmとした。この直径D=60〜150mm
に対応する最適供給熱量Mは、第4図より、M=
76〜105(W/m2)=1.3〜1.8(Met)となるのであ
る。
That is, to explain the specific reason, as shown in FIG. 5, as the diameter D of the spherical shell becomes smaller, the root mean square value S increases significantly, and the performance as a sensing element deteriorates. Here, when the average radiant temperature Tr is changed, △KET * is directly proportional to this Tr,
△SET * is also almost directly proportional to Tr, so
As Tr increases, (△SET * −△KET * ) also increases. Therefore, if we allow (△SET * -△KET * ) up to 0.1°C for a 1°C change in the above average radiation temperature Tr, then in Figure 5, Tr is changed from -5°C to +5°C, so The root mean square value S becomes S=0.1 from the above equation (15). From Fig. 5, the range where S≦0.1 is D for the diameter D of the spherical shell.
≧60mm. On the other hand, since it is easier to use the temperature sensing element if its size and dimensions are small, the upper limit of the diameter D was set to 150 mm. This diameter D = 60~150mm
From Fig. 4, the optimal amount of heat to be supplied M corresponding to M =
76 to 105 (W/m 2 )=1.3 to 1.8 (Met).

尚、殻体(3)の形状は上記の球形に限られず、円
柱状、回転楕円体等、種々の形状が採用可能であ
る。これらの場合も、上記と同様の方法によつ
て、発熱体(1)の寸法および発熱体(1)への供給熱量
Mを湿性放熱まで考慮した人体の熱的平衡特性と
等価となるように特定することができる。例とし
て、円柱の場合、下記の円柱の強制対流熱伝達に
関する五十嵐、平田の式を用いて、 Nu=0.373Re1/2+0.057Re2/3 …(17) 球の場合と同様に、円柱の直径Dに対して上記(15)
式で得られる2乗平均値Sの値をプロツトする
と、それぞれ気流速および平均輻射温に対する変
化特性が第6図および第7図に示すようになり、
この場合、直径Dは80mm以上が好ましいことが判
る。また、このときの最適供給熱量Mは76W/m2
以上となる。
Note that the shape of the shell (3) is not limited to the above-mentioned spherical shape, and various shapes such as a cylindrical shape and a spheroidal shape can be adopted. In these cases, the same method as above is used to make the dimensions of the heating element (1) and the amount of heat M supplied to the heating element (1) equivalent to the thermal equilibrium characteristics of the human body, taking into account the moisture heat radiation. can be specified. As an example, in the case of a cylinder, using the equation of Igarashi and Hirata regarding forced convection heat transfer of the cylinder below, Nu=0.373Re 1/2 +0.057Re 2/3 ...(17) As in the case of a sphere, (15) above for the diameter D of
When the values of the root mean square value S obtained by the formula are plotted, the change characteristics with respect to the air velocity and the average radiant temperature are shown in Figs. 6 and 7, respectively.
In this case, it is found that the diameter D is preferably 80 mm or more. In addition, the optimal amount of heat supplied at this time M is 76W/m 2
That's all.

(作用) 上記の構成により、本発明では、温熱検知素子
における発熱体(1)の殻体(3)の寸法および該発熱体
(1)への供給熱量Mが人体の湿性放熱を加味した上
で設定されているので、素子の熱的平衡は人体の
熱的平衡に対して極めて近似した相関関係とな
り、人体に快適感を与える温熱状態を単一の検知
素子で高精度に検知することができることにな
る。
(Function) With the above configuration, in the present invention, the dimensions of the shell (3) of the heating element (1) in the thermal detection element and the heating element
Since the amount of heat M supplied to (1) is set after taking into account the humid heat dissipation of the human body, the thermal equilibrium of the element has a very close correlation to the thermal equilibrium of the human body, giving a sense of comfort to the human body. This means that the applied thermal state can be detected with high precision using a single sensing element.

さらに、発熱体(1)の寸法および供給熱量Mの、
人体の熱的平衡特性との等価設定の際、湿性放熱
まで考慮したので、上記発熱体(1)の寸法を小さく
することが可能となる。すなわち、第8図は、球
形、円柱形等の殻体(3)形状の発熱体(1)を有する温
熱検知素子における該殻体(3)の直径Dに対する対
流熱伝達率hgcを示し、また人体の対流伝達率hc
および上記(7)式で定義した湿性放熱まで考慮した
対流伝達率hc′のレベルも併せて示している。同
図に示されるように、直径Dが大きくなるに従つ
てhgcが小さくなる特性を有するので、hcとhgc
とを合致させるように快定した直径DAよりも、
hc′とhgcとを合致させるように決定した直径DB
の方が小さい値となり、寸法の縮小化が図れる。
Furthermore, the dimensions of the heating element (1) and the supplied heat amount M,
When setting the equivalence with the thermal equilibrium characteristics of the human body, moisture heat radiation was also taken into consideration, making it possible to reduce the size of the heating element (1). That is, FIG. 8 shows the convective heat transfer coefficient hgc with respect to the diameter D of the shell (3) in a thermal sensing element having a heating element (1) in the shape of a shell (3) such as a sphere or a cylinder. Convection transmissibility hc of human body
It also shows the level of the convective transmissivity hc′, which takes into account the moisture heat radiation defined by equation (7) above. As shown in the figure, as the diameter D increases, hgc decreases, so hc and hgc
From the diameter D A , which was determined to match the
Diameter D B determined to match hc′ and hgc
has a smaller value, and the dimensions can be reduced.

さらに、発熱体(1)の球殻(3)外表面に人体に基づ
く分光輻射率と略合致した輻射率を有する輻射材
料層(8)が形成されているので、検知素子の発熱体
(1)表面の輻射熱伝達率h grを人体の輻射熱伝達
率hrに精度良く一致させることができ、温熱検知
素子によつて実際の居住環境下での温熱状態をよ
り一層精密に検知することができる。
Furthermore, since a radiant material layer (8) having an emissivity that approximately matches the spectral emissivity based on the human body is formed on the outer surface of the spherical shell (3) of the heating element (1), the heating element of the sensing element
(1) The radiant heat transfer coefficient h gr of the surface can be accurately matched to the radiant heat transfer coefficient hr of the human body, and the thermal state in the actual living environment can be detected more precisely by the thermal detection element. can.

(実施例) 次に、本発明の実施例を図面に基づいて説明す
る。
(Example) Next, an example of the present invention will be described based on the drawings.

第1図は本発明の実施例に係る空気調和装置制
御用の温熱検知素子Aを示す。同図において、1
は球状の発熱体であつて、該発熱体1は、パイプ
状の支持棒2を貫通固定した銅等の金属よりなる
中空状の球殻3内の中心部に電気ヒータ4が封入
されてなる。上記ヒータ4には支持棒2内に充填
固定した電気絶縁体5を貫通してヒータ4に電力
を供給する電力供給線6,6が接続され、この電
力供給線6,6によりヒータ4が球殻3内で固定
支持されている。
FIG. 1 shows a thermal detection element A for controlling an air conditioner according to an embodiment of the present invention. In the same figure, 1
is a spherical heating element, and the heating element 1 has an electric heater 4 sealed in the center of a hollow spherical shell 3 made of metal such as copper, which is fixed through a pipe-shaped support rod 2. . Power supply lines 6, 6 are connected to the heater 4 to supply power to the heater 4 through an electric insulator 5 filled and fixed in the support rod 2. It is fixedly supported within the shell 3.

また、上記発熱体1の球殻3内表面には発熱体
1表面(球殻3)の温度Tgを測定する温度測定
器としての熱電対7が固着されている。該熱電対
7の出力は上記絶縁体5、支持棒2内を通つて球
殻3外に導出されており、電気ヒータ4を通電に
より発熱させて発熱体1に所定の熱量を供給し、
その状態で熱電対7の出力電圧により発熱体1の
表面温度Tgを検出してそれに基づいて室内環境
の温熱状態を検知するようになされている。
Further, a thermocouple 7 is fixed to the inner surface of the spherical shell 3 of the heating element 1 as a temperature measuring device for measuring the temperature Tg of the surface of the heating element 1 (spherical shell 3). The output of the thermocouple 7 is led out of the spherical shell 3 through the insulator 5 and the support rod 2, and the electric heater 4 is energized to generate heat and supply a predetermined amount of heat to the heating element 1.
In this state, the surface temperature Tg of the heating element 1 is detected by the output voltage of the thermocouple 7, and the thermal state of the indoor environment is detected based on this.

さらに、上記発熱体1の球殻3外表面には、人
体の皮膚ないし衣服の分光輻射率と概略合致する
輻射率を有する例えば四弗化エチレン樹脂
(PTFE)等の弗素樹脂および酸化チタン(Ti
O2)等の所定顔料よりなる薄膜の輻射材料層8
が形成されている。
Further, on the outer surface of the spherical shell 3 of the heating element 1, a fluororesin such as tetrafluoroethylene resin (PTFE) and titanium oxide (Ti
A thin radiant material layer 8 made of a predetermined pigment such as O 2 )
is formed.

そして、本発明の特徴として、上記発熱体1の
球殻3の直径Dおよび発熱体1への供給熱量M
(電気ヒータ4への電気入力)は湿性放熱まで考
慮した人体の熱的平衡特性と等価になるように、
具体的にはD=60〜150mmの範囲に、M=76〜
105W/m2の範囲に設定されている。
The present invention is characterized by the diameter D of the spherical shell 3 of the heating element 1 and the amount of heat M supplied to the heating element 1.
(Electrical input to the electric heater 4) is made to be equivalent to the thermal equilibrium characteristics of the human body, taking into account moisture heat radiation.
Specifically, D=60~150mm, M=76~
It is set in the range of 105W/ m2 .

したがつて、上記実施例においては、発熱体1
の球殻3の直径Dおよび発熱体1への供給熱量M
が湿性放熱まで考慮した人体の熱的平衡特性と等
価になるように設定されているので、上記説明し
た理由により、湿熱検知素子Aの熱的バランスを
人体のそれに極めて顕著に近似させることがで
き、温熱検知素子AによるKET*の検出によつて
実際の温熱環境のSET*を精度良く検出すること
ができる。
Therefore, in the above embodiment, the heating element 1
The diameter D of the spherical shell 3 and the amount of heat M supplied to the heating element 1
is set to be equivalent to the thermal equilibrium characteristics of the human body, taking into account wet heat dissipation, so for the reasons explained above, the thermal balance of the wet heat sensing element A can be extremely closely approximated to that of the human body. By detecting KET * by thermal detection element A, it is possible to accurately detect SET * in the actual thermal environment.

また、発熱体1の球殻3外表面に人体の皮膚な
いし衣服の分光輻射率と略合致した輻射率を有す
る弗素樹脂を主成分とする輻射材料層8が形成さ
れているので、検知素子Aの発熱体1の表面の輻
射熱伝達率h grを人体の輻射熱伝達率hrに精度
良く一致させることができ、温熱検知素子Aによ
つて実際の居住環境下での温熱状態をより一層精
密に検知することができる。
Furthermore, since a radiant material layer 8 mainly composed of a fluororesin having an emissivity that substantially matches the spectral emissivity of human skin or clothing is formed on the outer surface of the spherical shell 3 of the heating element 1, the sensing element A The radiant heat transfer coefficient h gr of the surface of the heating element 1 can be precisely matched to the radiant heat transfer coefficient hr of the human body, and the thermal state in the actual living environment can be detected even more precisely by the thermal detection element A. can do.

さらに、人体の熱的平衡において、蒸発を伴つ
た対流熱伝達率hc′を設定し、その熱伝達率hc′を
発熱体1の対流伝達率h gcに一致させるよう
にしているので、発熱体1の周りを覆つて発熱体
1への輻射熱を透過しかつ対流を抑制させるため
の発熱体カバーを用いることなく、発熱体1の直
径Dを小さく設定することができる。
Furthermore, in the thermal equilibrium of the human body, the convective heat transfer coefficient hc' with evaporation is set, and the heat transfer coefficient hc' is made to match the convective transfer coefficient h gc of the heating element 1. The diameter D of the heating element 1 can be set small without using a heating element cover that covers the heating element 1 to transmit radiant heat to the heating element 1 and suppress convection.

(具体例) 最後に具体的な実施例について説明する。上記
した実施例の構成を有する温熱検知素子におい
て、その発熱体の直径DをD=100mmに、供給熱
量MをM=92.2W/m2(1.585Met)にそれぞれ設
定し、その検知素子について気流速を0.1〜
1.0m/sの範囲で変化させたときの基準状態
(気流速0.1m/sのとき)からのKET*の変化量
△KET*を求めたところ、第9図で実線にて示す
ような特性が得られた。図の破線は同じ条件下で
のSET*の変化量△SET*の特性を示す。
(Specific Example) Finally, a specific example will be described. In the thermal sensing element having the configuration of the above embodiment, the diameter D of the heating element is set to D = 100 mm, the amount of heat supplied M is set to M = 92.2 W/m 2 (1.585 Met), and care is taken about the sensing element. Flow rate from 0.1 to
When we calculated the amount of change △KET * in KET * from the reference state (air velocity 0.1 m/s) when changing it in the range of 1.0 m/s, we found the characteristics shown by the solid line in Figure 9. was gotten. The broken line in the figure shows the characteristics of the amount of change ΔSET * in SET * under the same conditions.

また、上記と同一の検知素子に対し、室内環境
の平均輻射温度Trと気温Taとの差Tr−Taを−
5〜+5℃の範囲で変化させたときの基準状態
(Tr=Taのとき)からの上記△KET*の特性は第
10図で実線にて示すようになつた。図中、破線
は△SET*の特性を示す。
In addition, for the same sensing element as above, the difference Tr−Ta between the average radiant temperature Tr and the air temperature Ta in the indoor environment is −
The characteristic of ΔKET * from the reference state (when Tr=Ta) when varied in the range of 5 to +5° C. is as shown by the solid line in FIG. In the figure, the broken line indicates the characteristics of △SET * .

したがつて、この第9図および第10図によ
り、本発明の温熱検知素子によると、気流速およ
び平均輻射温度Trと気温Taとの差Tr−Taのそ
れぞれの変化に対し△KET*は△SET*との間に
極めて優れた相関関係があり、実際の温熱環境に
対する検出精度を高め得ることが判る。
Therefore, according to FIGS. 9 and 10, according to the thermal detection element of the present invention, △KET * is △ for each change in the air velocity and the difference Tr−Ta between the average radiant temperature Tr and the air temperature Ta. It can be seen that there is an extremely good correlation with SET * , and that the detection accuracy in the actual thermal environment can be improved.

(発明の効果) 以上説明したように、本発明の温熱検知素子に
よれば、内部に電気ヒータを封入した中空状殻体
よりなる発熱体の寸法およびその供給熱量を人体
の湿性放熱を考慮して特定したものであるので、
温熱検知素子の熱的平衡を人体の熱的平衡に顕著
に近似させて、実際の居住空間内における温熱状
態を体感と同程度に評価することができる。ま
た、結果として湿性放熱を考慮することで発熱体
の寸法を小さくすることができ、よつて空気調和
装置の作動制御に最適な高精度でかつ小型の温熱
検知素子の提供を実現することができるものであ
る。
(Effects of the Invention) As explained above, according to the thermal detection element of the present invention, the dimensions of the heating element made of a hollow shell in which an electric heater is enclosed and the amount of heat supplied by the heating element are determined in consideration of the humid heat dissipation of the human body. Since it is specified by
The thermal equilibrium of the thermal detection element is made to closely approximate the thermal equilibrium of the human body, and the thermal state in an actual living space can be evaluated to the same degree as the bodily sensation. In addition, as a result, the size of the heating element can be reduced by considering moisture heat dissipation, and it is therefore possible to provide a highly accurate and compact thermal sensing element that is ideal for controlling the operation of air conditioners. It is something.

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

第1図は本発明の実施例における温熱検知素子
の断面図である。第2図は球殻の場合での直径に
対する2乗平均値の気流速に対する変化特性図、
第3図は同じく直径が100mmのときの供給熱量に
対する2乗平均値の変化特性図、第4図は同じく
直径に対する最適供給熱量の変化特性図、第5図
は平均輻射温度と気温との差の増減変化に対する
2乗平均値の特性図である。第6図および第7図
はそれぞれ円柱殻の場合において直径に対して2
乗平均値の気流速および平均輻射温度に対する変
化特性図であり、第8図は殻体の直径に対する対
流熱伝達率の特性図である。第9図および第10
図はそれぞれ発熱体の直径、供給熱量を本発明範
囲内の所定値に特定したときの気流速および平均
輻射温度と気温との差に対する△KET*を△
SET*と比較して示す特性図である。 A……温熱検知素子、1……発熱体、3……球
殻、4……電気ヒータ、7……熱電対、8……輻
射材料層。
FIG. 1 is a sectional view of a thermal sensing element in an embodiment of the present invention. Figure 2 is a characteristic diagram of the change in air flow velocity of the root mean square value for the diameter in the case of a spherical shell.
Figure 3 is a characteristic diagram of the change in the root mean square value with respect to the amount of heat supplied when the diameter is 100 mm, Figure 4 is a characteristic diagram of the change in the optimum amount of heat supplied with respect to the diameter, and Figure 5 is the difference between the average radiant temperature and the air temperature. It is a characteristic diagram of the root mean square value with respect to the increase/decrease change of. Figures 6 and 7 respectively show 2 for the diameter in the case of a cylindrical shell.
FIG. 8 is a characteristic diagram of the variation of the root mean value with respect to the air velocity and the average radiant temperature, and FIG. 8 is a characteristic diagram of the convective heat transfer coefficient with respect to the diameter of the shell body. Figures 9 and 10
The figures show △KET * for the air velocity and the difference between the average radiant temperature and the air temperature when the diameter of the heating element and the amount of heat supplied are specified to predetermined values within the range of the present invention, respectively.
It is a characteristic diagram shown in comparison with SET * . A... Temperature sensing element, 1... Heating element, 3... Spherical shell, 4... Electric heater, 7... Thermocouple, 8... Radiant material layer.

Claims (1)

【特許請求の範囲】[Claims] 1 中空状の殻体3内に電気ヒータ4が配置され
ているとともに該殻体3の外表面に人体に基づく
分光輻射率と略合致する輻射率を有する輻射材料
層8が形成されてなる発熱体1と、該発熱体1の
表面温度Tgを測定する温度測定器7とを備え、
上記発熱体1に所定の熱量を供給し、その表面温
度Tgに基づいて室内環境の温熱状態を検知する
温熱検知素子であつて、上記発熱体1の殻体3の
寸法および発熱体1への供給熱量は、発熱体1の
対流熱伝達率を人体の蒸発を伴つた対流熱伝達率
とほぼ合致させるとともに上記発熱体1への供給
熱量を人体の衣服の熱抵抗を考慮した皮膚表面か
らの放散熱量とほぼ合致させて発熱体1の熱的平
衡特性が湿性放熱まで考慮した人体の熱的平衡特
性と等価になるように設定されていることを特徴
とする温熱検知素子。
1. Heat generation in which an electric heater 4 is disposed inside a hollow shell 3, and a radiant material layer 8 having an emissivity that substantially matches the spectral emissivity based on the human body is formed on the outer surface of the shell 3. body 1, and a temperature measuring device 7 for measuring the surface temperature Tg of the heating element 1,
A thermal detection element that supplies a predetermined amount of heat to the heating element 1 and detects the thermal state of the indoor environment based on the surface temperature Tg of the heating element 1. The amount of heat supplied is determined so that the convective heat transfer coefficient of the heating element 1 almost matches the convective heat transfer coefficient with evaporation of the human body, and the amount of heat supplied to the heating element 1 is determined by adjusting the amount of heat supplied to the heating element 1 from the skin surface taking into account the thermal resistance of the human body's clothing. A thermal detection element characterized in that the thermal equilibrium characteristics of the heating element 1 are set to almost match the amount of heat dissipated, and are set to be equivalent to the thermal equilibrium characteristics of the human body, taking into account even moisture heat radiation.
JP61052249A 1986-03-10 1986-03-10 Thermal detecting element Granted JPS62259014A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61052249A JPS62259014A (en) 1986-03-10 1986-03-10 Thermal detecting element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61052249A JPS62259014A (en) 1986-03-10 1986-03-10 Thermal detecting element

Publications (2)

Publication Number Publication Date
JPS62259014A JPS62259014A (en) 1987-11-11
JPH0511766B2 true JPH0511766B2 (en) 1993-02-16

Family

ID=12909459

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61052249A Granted JPS62259014A (en) 1986-03-10 1986-03-10 Thermal detecting element

Country Status (1)

Country Link
JP (1) JPS62259014A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107461860B (en) * 2016-06-17 2019-11-08 深圳安星建设集团有限公司 A kind of intelligent fresh air purification system and its control method

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56128413A (en) * 1980-12-12 1981-10-07 Showa Denko Kk Measuring instrument to thermal environment
JPS59104016U (en) * 1982-12-28 1984-07-13 トヨタ自動車株式会社 Warm detection model
JPS60219512A (en) * 1984-04-16 1985-11-02 Matsushita Electric Ind Co Ltd environmental assessment equipment

Also Published As

Publication number Publication date
JPS62259014A (en) 1987-11-11

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