JPH047456B2 - - Google Patents
Info
- Publication number
- JPH047456B2 JPH047456B2 JP6058483A JP6058483A JPH047456B2 JP H047456 B2 JPH047456 B2 JP H047456B2 JP 6058483 A JP6058483 A JP 6058483A JP 6058483 A JP6058483 A JP 6058483A JP H047456 B2 JPH047456 B2 JP H047456B2
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- time
- body temperature
- sensor
- electronic thermometer
- 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
Links
- 230000036760 body temperature Effects 0.000 claims description 18
- 238000000034 method Methods 0.000 claims description 13
- 238000001514 detection method Methods 0.000 claims description 6
- 238000005259 measurement Methods 0.000 description 10
- RRLHMJHRFMHVNM-BQVXCWBNSA-N [(2s,3r,6r)-6-[5-[5-hydroxy-3-(4-hydroxyphenyl)-4-oxochromen-7-yl]oxypentoxy]-2-methyl-3,6-dihydro-2h-pyran-3-yl] acetate Chemical compound C1=C[C@@H](OC(C)=O)[C@H](C)O[C@H]1OCCCCCOC1=CC(O)=C2C(=O)C(C=3C=CC(O)=CC=3)=COC2=C1 RRLHMJHRFMHVNM-BQVXCWBNSA-N 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 238000009529 body temperature measurement Methods 0.000 description 2
- 239000004973 liquid crystal related substance Substances 0.000 description 1
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 1
- 229910052753 mercury Inorganic materials 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01K—MEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
- G01K7/00—Measuring temperature based on the use of electric or magnetic elements directly sensitive to heat ; Power supply therefor, e.g. using thermoelectric elements
- G01K7/42—Circuits effecting compensation of thermal inertia; Circuits for predicting the stationary value of a temperature
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Temperature Or Quantity Of Heat (AREA)
Description
【発明の詳細な説明】
(イ) 発明の分野
この発明は、電子体温計特に測定開始後の早期
に被測定者の体温を測定し得る電子体温計に関す
る。DETAILED DESCRIPTION OF THE INVENTION (a) Field of the Invention The present invention relates to an electronic thermometer, and particularly to an electronic thermometer that can measure the body temperature of a subject at an early stage after starting measurement.
(ロ) 従来技術とその問題点
一般に体温を測定するのに水銀体温計やサーミ
スタ等の感温センサを用いた電子体温計が使用さ
れる。これらの体温計は測定時に検出部を腋の下
や舌下に挿入するのが通常であるが、検出部が体
温と熱平衡状に至るのに時間がかかるので、測定
終了までに長時間を要するという問題がある。そ
こでこの問題を解決し早期に体温を測定できるよ
うに従来の電子体温計では、センサ部を腋の下等
に挿入して測定開始後の一定時間経過で一定温度
(例えば0.5℃)を上乗せして、収束体温を予測す
る方法が採用されていた。しかしながら、体温測
定時における検出温度の上昇度合は個人によつて
ばらつきがあり(例えば平衡状態に達する時定数
が相違する)。上記従来の電子体温計は、このよ
うな個人的ばらつきを全く無視しているので、得
られた測定結果は精度が悪いという欠点があつ
た。(b) Prior art and its problems Generally, electronic thermometers using temperature sensors such as mercury thermometers and thermistors are used to measure body temperature. These thermometers usually have the detection part inserted under the armpit or under the tongue when taking measurements, but since it takes time for the detection part to reach thermal equilibrium with body temperature, there is a problem in that it takes a long time to complete the measurement. be. Therefore, in order to solve this problem and measure body temperature early, conventional electronic thermometers insert the sensor part into the armpit, etc., and add a certain temperature (for example, 0.5 degrees Celsius) after a certain period of time after starting the measurement. A method was used to predict body temperature. However, the degree of increase in detected temperature during body temperature measurement varies depending on the individual (for example, the time constant for reaching an equilibrium state differs). The above-mentioned conventional electronic thermometer completely ignores such individual variations, and therefore has the disadvantage that the obtained measurement results are low in accuracy.
(ハ) 発明の目的
この発明の目的は、上記従来の電子体温計の欠
点を解消し、早期に精度の高い測定が可能な電子
体温計を提供するにある。(c) Purpose of the Invention The purpose of the present invention is to eliminate the drawbacks of the conventional electronic thermometers described above and to provide an electronic thermometer that is capable of performing early and highly accurate measurements.
(ニ) 発明の構成と効果
上記目的を達成するために、この発明の電子体
温計は、被測定体温の時間微分の対数値TLと時
間tの間に直線的な関係があり、TL=A−τ′tで
表わせることに着目し、回帰法により定数A及び
τ′を求め、これらの定数から収束体温を予測する
ようにしている。すなわちこの発明の電子体温計
は体温を検出するセンサと、このセンサの出力を
サンプリングし、n回のサンプルタイムの各々ti
に、各検出出力の時間微分の対数値TLiを算出す
る手段と、算出されたサンプルタイムt1,t
2,……ti……tn毎の検出出力の時間微分の対数
値TL1,TL2,……TLi,……TLoとに基づき直
線TL=A−τ′tの定数A及びτ′を回帰法で算出す
る手段と、算出された定数A及びτ′と検出初期温
度Toとに基づき、熱平衡後の体温Tsを予測算出
する手段とから構成されている。(d) Structure and Effects of the Invention In order to achieve the above object, the electronic thermometer of the present invention has a linear relationship between the logarithm T L of the time differential of the body temperature to be measured and time t, and T L = Focusing on the fact that it can be expressed as A-τ't, the constants A and τ' are determined by a regression method, and the convergence body temperature is predicted from these constants. That is, the electronic thermometer of the present invention includes a sensor that detects body temperature, samples the output of this sensor, and samples the output of this sensor at each of n sampling times.
In addition, means for calculating the logarithmic value T Li of the time differential of each detection output, and the calculated sample times t1, t
Based on the logarithm value T L of the time differential of the detection output for each 2 , ... ti ... tn and τ' by a regression method, and means for predicting and calculating the body temperature Ts after thermal equilibrium based on the calculated constants A and τ' and the detected initial temperature To.
この発明の電子体温計によれば、個人毎に異な
る定数を回帰法により算出して、収束体温を予測
するものであるから、個人的なばらつきに左右さ
れずに精度良く体温を早期に測定することができ
る。 According to the electronic thermometer of this invention, constants that differ for each individual are calculated by regression method to predict convergence body temperature, so body temperature can be measured quickly and accurately without being influenced by individual variations. I can do it.
ここで、この発明の電子体温計の理解を容易に
するために、その採用原理について説明する。 Here, in order to facilitate understanding of the electronic thermometer of the present invention, the principle of its adoption will be explained.
一般に、横軸に時間、縦軸に温度をとつて体温
を温度センサで測定した場合の時間経過を示すと
第1図に示すように指数関数的に変化する。 Generally, when time is plotted on the horizontal axis and temperature is plotted on the vertical axis, the passage of time when body temperature is measured by a temperature sensor changes exponentially as shown in FIG. 1.
図において、体温測定に必要な温度値は収束温
度Tsであるが、通常の方法ではこの温度に達す
るのに時間がかかる。これは人体が体温計そのも
のによつて、熱をうばわれて、元に戻るまでに時
間がかかるという生理的理由により生じる現象で
ある。 In the figure, the temperature value required for body temperature measurement is the convergence temperature Ts, but it takes time to reach this temperature using normal methods. This is a phenomenon that occurs due to the physiological reason that the human body loses heat due to the thermometer itself, and it takes time for the body to return to its original state.
この発明では、上記特性曲線を測定開始の早い
時機に予測して収束値を推定しようとするもので
ある。 The present invention attempts to estimate the convergence value by predicting the characteristic curve as soon as the measurement starts.
平衡状態の温度Tsと時間tにおける温度Tの
間には、次の熱平衡式
d(Ts−T)/dt=−1/τ(Ts−T) (1)
が成立することが知られている。 It is known that the following thermal equilibrium equation d(Ts-T)/dt=-1/τ(Ts-T) (1) holds between the temperature Ts in equilibrium and the temperature T at time t. .
この(1)式より、
Ts−T=(Ts−To)e-1/〓 t
この式より
T=Ts−(Ts−To)e-1/〓 t (2)
ただし、τ:時定数、TS:初期値(t=0の
時のTの値)。時定数τは、熱平衡状に達する速
さの度合を表わす定数で個人差があると考えられ
るものである。 From this formula (1), Ts−T=(Ts−To)e -1/ 〓 tFrom this formula, T=Ts−(Ts−To)e -1/ 〓 t (2) Where, τ: time constant, T S : Initial value (value of T when t=0). The time constant τ is a constant representing the speed at which thermal equilibrium is reached, and is thought to vary from person to person.
今ここで、τ′=1/τとおいて、上記(2)式を時
間微分すると
T′=dT/dt=τ′(Ts−To)e-〓′t (3)
となる。さらにこの(3)式の両辺の対数をとると、
logT′=logτ′(Ts−To)−τ′t (4)
となる。ここで、
TL=logT′,A=logτ′(Ts−To)
とおくと、(4)式は
TL=A−τ′t (5)
と表わせる。 Now, if we set τ′=1/τ and differentiate the above equation (2) with time, we get T′=dT/dt=τ′(Ts−To)e − 〓′ t (3). Furthermore, if we take the logarithm of both sides of equation (3), we get logT′=logτ′(Ts−To)−τ′t (4). Here, by setting T L = logT' and A = logτ' (Ts - To), equation (4) can be expressed as T L = A - τ't (5).
この(5)式は第2図に示すように、勾配が−
τ′で、縦軸とAで交わる直線となる。 As shown in Figure 2, this equation (5) has a slope of -
At τ', it becomes a straight line that intersects the vertical axis at A.
各時間tにおいて温度Tは実測されるから、
T′=dT/dtを求めることができ、さらにT=
logT′も求めることができる。したがつて測定開
始当初のn組のサンプルタイムにおける(t1,
TL1),(t2,TL2),……(tn,TLo)の値から
A,τ′を周知の回帰法で算出することができる。
すなわち
A=Σti2ΣTL−ΣtiΣtiTLi/nΣti2−(Σti)2(6)
τ′=−nΣtiTLi−ΣtiΣTLi/nΣti2−(Σti)2(7
)
一方、上記したように
logτ′(Ts−To)=A
であるから、これより、収束温度Tsは
Ts=eA/τ′+To (8)
となる。この(8)式において、初期値Toは検出さ
れ、定数A及びτ′は(6),(7)式で算出されるから
Tsを求めることができる。しかも個人的ばらつ
きを含む定数A及びτ′は測定開始の早期(t1,
……tn)に算出することにより収束温度Tsも早
期に精度よく予測することができる。 Since the temperature T is actually measured at each time t,
T'=dT/dt can be determined, and T=logT' can also be determined. Therefore, (t1,
A and τ' can be calculated from the values of T L1 ), (t2, T L2 ), . . . (tn, T Lo ) using a well-known regression method.
That is, A=Σti 2 ΣT L −ΣtiΣtiT Li /nΣti 2 −(Σti) 2 (6) τ′=−nΣtiT Li −ΣtiΣT Li /nΣti 2 −(Σti) 2 (7
) On the other hand, as mentioned above, since logτ'(Ts-To)=A, the convergence temperature Ts becomes Ts=e A /τ'+To (8). In this equation (8), the initial value To is detected, and the constants A and τ′ are calculated using equations (6) and (7).
You can find Ts. Moreover, the constants A and τ′, which include individual variations, are lost early in the measurement (t1,
...tn), it is possible to predict the convergence temperature Ts quickly and accurately.
(ホ) 実施例の説明
第3図はこの発明が実施される電子体温計のブ
ロツク図である。同図において1は体温を検知す
るためのサーミスタ等のセンサ、2はセンサ1か
らの出力をアナログ信号からデジタル信号の変換
するA/D変換器、3はCPUであつてA/D変
換器2よりの検出温度信号を受け、ROM4に記
憶されるプログラムにしたがい、後述する収束温
度Ts予測のための制御を行なう。5は制御の過
程で種々のデータを記憶するRAMである。6は
測定体温を表示する表示器である。この表示器6
の表示体としては、液晶、発光ダイオード、螢光
表示管等周知のものが使用される。7は測定開始
を指示するスイツチである。(E) Description of Embodiments FIG. 3 is a block diagram of an electronic thermometer in which the present invention is implemented. In the figure, 1 is a sensor such as a thermistor for detecting body temperature, 2 is an A/D converter that converts the output from sensor 1 from an analog signal to a digital signal, and 3 is a CPU, which is the A/D converter 2. After receiving the detected temperature signal from the ROM 4, it performs control for predicting the convergence temperature Ts, which will be described later, according to a program stored in the ROM 4. 5 is a RAM that stores various data during the control process. 6 is a display that displays the measured body temperature. This display 6
As the display body, well-known ones such as liquid crystal, light emitting diode, fluorescent display tube, etc. are used. 7 is a switch for instructing the start of measurement.
次に、第4図に示すフロー図を参照して上記実
施例電子体温計の動作を説明する。 Next, the operation of the electronic thermometer of the above embodiment will be explained with reference to the flowchart shown in FIG.
スイツチ7がオンして動作がスタートすると、
先ずステツプST1で初期温度値Toが、A/D変
換器2を経てCPU3に取り込まれる。続いて、
サンプルタイムが到来しているか否かステツプ
ST2で判定する。サンプルタイムが到来すると、
A/D変換器2を経て取り込まれるその時の検出
温度T1をRAM5に記憶する(ST3)。次に、
検出温度T1の時間微分値dT1/dtを算出し
(ST4)、さらにこの時間微分値の対数値TL1=
logdT1/dtを求める(ST5)。そして算出した、
TL1と、その時のサンプルタイムt1をRAM5
に記憶する(ST6)。次にサンプルタイム回数i
が予め設定するnに達しているか否か判定し
(ST7)、達していない場合にはステツプST2に
リターンし、以後サンプル回数iがnに達するま
でサンプルタイムの到来毎にステツプST3,ST
4,……ST6の処理を繰り返す。この処理によ
り各サンプルタイムt1,t2,……tnとそのサ
ンプルタイム毎の検出温度の時間微分値の対数値
TL1,TL2,……TLoがRAM5に記憶される。 When switch 7 is turned on and operation starts,
First, in step ST1, the initial temperature value To is taken into the CPU 3 via the A/D converter 2. continue,
Step to see if sample time has arrived
Determine in ST2. When sample time arrives,
The detected temperature T1 at that time taken in through the A/D converter 2 is stored in the RAM 5 (ST3). next,
Calculate the time differential value dT1/dt of the detected temperature T1 (ST4), and further calculate the logarithm value of this time differential value T L1 =
Find logdT1/dt (ST5). Then, calculate T L1 and the sample time t1 at that time in RAM 5.
(ST6). Next, the number of sample times i
It is determined whether or not n has reached a preset value (ST7). If it has not reached n, the process returns to step ST2. From then on, steps ST3 and ST are performed every time a sample time arrives until the number of samples i reaches n.
4,...Repeat the process of ST6. Through this processing, each sample time t1, t2,...tn and the logarithm of the time differential value of the detected temperature for each sample time are
T L1 , T L2 , . . . T Lo are stored in the RAM 5.
サンプルタイム回数iがnに達するとステツプ
ST7の判定がYESとなり続いて記憶しているデ
ータt1,t2,……tn及びTL1,TL2,……TLo
をもとに上記(6)式により定数Aを算出する(ST
8)とともに、さらに上記(7)式により、定数τ′を
算出する(ST9)。これにより、被測定者個有の
特性曲線が特定されるので、続いて上記(8)式によ
り収束温度Tsを算出する(ST10)そして、こ
の温度Tsが表示器6に体温として表示される
(ST11)。 When the sample time count i reaches n, step
When the judgment in ST7 is YES, the stored data t1, t2, ... tn and T L1 , T L2 , ... T Lo
Calculate the constant A using equation (6) above based on (ST
In addition to 8), the constant τ' is further calculated using the above equation (7) (ST9). As a result, the characteristic curve unique to the person to be measured is specified, so the convergence temperature Ts is then calculated using the above equation (8) (ST10), and this temperature Ts is displayed as the body temperature on the display 6 ( ST11).
表示後、なお検出温度が変化している場合
(ST12)は、ステツプST2にリターンし上記
処理が繰り返されるが、検出温度の変化が0とな
ると続いて他の所要の測定終了処理を行なう。 After the display, if the detected temperature is still changing (ST12), the process returns to step ST2 and the above process is repeated, but when the change in the detected temperature becomes 0, other required measurement completion processes are subsequently performed.
第1図は体温計における体温の時間推移を示す
図、第2図は、時間tと温度の時間微分の対数値
TLとの関係を示す図、第3図はこの発明が実施
される電子体温計のブロツク図、第4図は同電子
体温計の動作を説明するためのフロー図である。
1……センサ、2……A/D変換器、3……
CPU、4……ROM、5……RAM、6……表示
器、7……スタートスイツチ。
Figure 1 shows the time course of body temperature in a thermometer, and Figure 2 shows the logarithm of the time differential of temperature versus time t.
FIG . 3 is a block diagram of an electronic thermometer in which the present invention is implemented, and FIG. 4 is a flow diagram for explaining the operation of the electronic thermometer. 1...Sensor, 2...A/D converter, 3...
CPU, 4...ROM, 5...RAM, 6...Display, 7...Start switch.
Claims (1)
をサンプリングし、n回のサンプルタイムの各々
tiに、各検出出力の時間微分の対数値TLiを算出
する手段と、算出されたサンプルタイムt1,…
…tn毎の検出出力の時間微分の対数値TL1,…
…TLoとに基づき直線式TL=A−τ′tの定数A及び
τ′を回帰法で算出する手段と、算出された定数A
及びτ′と検出初期温度T0とに基づき、熱平衡後の
体温Tsを予測算出する手段とよりなる電子体温
計。1. A sensor that detects body temperature, samples the output of this sensor, and samples the output of this sensor at each of n sample times.
ti, means for calculating the logarithm T Li of the time differential of each detection output, and the calculated sample times t1,...
...logarithm of the time differential of the detection output for each tn T L 1,...
...T Lo and means for calculating the constants A and τ' of the linear equation T L = A - τ't by a regression method, and the calculated constant A
An electronic thermometer comprising means for predicting and calculating body temperature Ts after thermal equilibrium based on τ' and detected initial temperature T 0 .
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6058483A JPS59187233A (en) | 1983-04-06 | 1983-04-06 | Electronic clinical thermometer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6058483A JPS59187233A (en) | 1983-04-06 | 1983-04-06 | Electronic clinical thermometer |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59187233A JPS59187233A (en) | 1984-10-24 |
JPH047456B2 true JPH047456B2 (en) | 1992-02-12 |
Family
ID=13146432
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP6058483A Granted JPS59187233A (en) | 1983-04-06 | 1983-04-06 | Electronic clinical thermometer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59187233A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2006103923A1 (en) * | 2005-03-29 | 2006-10-05 | Citizen Holdings Co., Ltd. | Electronic thermometer |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
AU607725B2 (en) * | 1986-11-19 | 1991-03-14 | Terumo Kabushiki Kaisha | Electronic thermometer |
JPH0795004B2 (en) * | 1986-12-24 | 1995-10-11 | テルモ株式会社 | Body temperature measuring device |
US5738441A (en) * | 1995-07-11 | 1998-04-14 | The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration | Electronic clinical predictive thermometer using logarithm for temperature prediction |
JP4582060B2 (en) * | 2006-06-29 | 2010-11-17 | パナソニック株式会社 | Gas shut-off device |
-
1983
- 1983-04-06 JP JP6058483A patent/JPS59187233A/en active Granted
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2006103923A1 (en) * | 2005-03-29 | 2006-10-05 | Citizen Holdings Co., Ltd. | Electronic thermometer |
JP4702781B2 (en) * | 2005-03-29 | 2011-06-15 | シチズンホールディングス株式会社 | Electronic thermometer |
Also Published As
Publication number | Publication date |
---|---|
JPS59187233A (en) | 1984-10-24 |
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