JPS6253054B2 - - Google Patents
Info
- Publication number
- JPS6253054B2 JPS6253054B2 JP57187087A JP18708782A JPS6253054B2 JP S6253054 B2 JPS6253054 B2 JP S6253054B2 JP 57187087 A JP57187087 A JP 57187087A JP 18708782 A JP18708782 A JP 18708782A JP S6253054 B2 JPS6253054 B2 JP S6253054B2
- Authority
- JP
- Japan
- Prior art keywords
- excitation
- magnetostrictive wire
- ultrasonic signal
- arithmetic
- receiving means
- 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
- 230000005284 excitation Effects 0.000 claims description 32
- 238000005259 measurement Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 2
- 238000010291 electrical method Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B17/00—Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B5/00—Measuring for diagnostic purposes; Identification of persons
- A61B5/103—Measuring devices for testing the shape, pattern, colour, size or movement of the body or parts thereof, for diagnostic purposes
- A61B5/107—Measuring physical dimensions, e.g. size of the entire body or parts thereof
- A61B5/1072—Measuring physical dimensions, e.g. size of the entire body or parts thereof measuring distances on the body, e.g. measuring length, height or thickness
Landscapes
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Physics & Mathematics (AREA)
- Heart & Thoracic Surgery (AREA)
- Molecular Biology (AREA)
- Dentistry (AREA)
- Biophysics (AREA)
- Pathology (AREA)
- Engineering & Computer Science (AREA)
- Biomedical Technology (AREA)
- General Physics & Mathematics (AREA)
- Medical Informatics (AREA)
- Oral & Maxillofacial Surgery (AREA)
- Surgery (AREA)
- Animal Behavior & Ethology (AREA)
- General Health & Medical Sciences (AREA)
- Public Health (AREA)
- Veterinary Medicine (AREA)
- Transmission And Conversion Of Sensor Element Output (AREA)
- Measurement Of The Respiration, Hearing Ability, Form, And Blood Characteristics Of Living Organisms (AREA)
- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
- Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)
Description
【発明の詳細な説明】
本発明は、電気的な手法によつて身長を測定す
るようにした身長測定器に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a height measuring device that measures height using an electrical method.
従来公知の身長計は、目盛を設けた支柱と、こ
の支柱に沿つて移動可能な頭上板とで構成されて
おり、被測定者を支柱を背にして直立させ、頭上
板を被測定者の頭頂に接触させその目盛を目測す
るものである。 Conventionally known height meters are composed of a column with a scale and an overhead board that can be moved along the column. The scale is measured by touching the top of the head.
このような従来公知の身長計においては、目盛
を目測するものであるために、計測誤差が伴うう
えに、精度の高い身長測定を行なうことができな
い欠点があつた。 Since such conventionally known height meters measure the scale, they suffer from measurement errors and have the disadvantage that highly accurate height measurements cannot be performed.
本発明は、これらの欠点のない身長測定器を実
現しようとするものである。 The present invention seeks to realize a height measuring instrument that does not have these drawbacks.
第1図は本発明の一実施例を示す外形図、第2
図は要部の構成斜視図、第3図は電気的なブロツ
ク図である。これらの図において、1は基台、2
は支柱、3は支柱に沿つて移動する頭上板、4は
支柱2と平行に張つた磁歪線で、その両端41,
42は機械的振動が伝わらないように軽く支持さ
れるとともに、この磁歪線内で発生した超音波信
号が反射するように構成されている。5は頭上板
3とともに移動し、磁歪線4に結合する励振及び
受信手段で、磁歪線4内に超音波信号を発生させ
るとともに、この磁歪線の両端41,42で反射
してきた超音波信号を受信する。なお、ここで
は、励振と受信とをひとつのコイルで行なう例を
示してあるが、これらは別々であつてもよい。 Fig. 1 is an outline drawing showing one embodiment of the present invention, Fig. 2 is an outline drawing showing an embodiment of the present invention;
The figure is a perspective view of the main part, and FIG. 3 is an electrical block diagram. In these figures, 1 is the base, 2
is a column, 3 is an overhead board that moves along the column, 4 is a magnetostrictive wire stretched parallel to the column 2, and its ends 41,
42 is lightly supported so that mechanical vibrations are not transmitted, and is configured so that the ultrasonic signal generated within the magnetostrictive wire is reflected. Reference numeral 5 denotes an excitation and reception means that moves together with the overhead plate 3 and couples to the magnetostrictive wire 4, which generates an ultrasonic signal within the magnetostrictive wire 4 and also receives the ultrasonic signal reflected at both ends 41 and 42 of the magnetostrictive wire. Receive. Note that although an example is shown here in which excitation and reception are performed by one coil, these may be performed separately.
OSは押しボタンPBによつて作動する励振パル
ス発生器で、その出力パルスはダイオードDOを
介して励振受信手段5に印加されている。FF
1,FF2はいずれもフリツプフロツプ回路で、
励振パルス発生器OSからの出力パルスがそれぞ
れ比較器を介してセツト端子Sにそれぞれ印加さ
れている。また、励振受信手段5からの受信信号
が、それぞれ比較器OP1,OP2及びプリセツトカ
ウンタPC1,PC2を介してリセツト端子Rに印加
されている。CKはフリツプフロツプ回路FF1,
FF2からの時間幅信号が印加される演算回路、
INは演算回路CKの演算結果がアナログまたはデ
イジタル表示される指示計である。各フリツプフ
ロツプ回路FF1,FF2、演算回路CK及び指示
計INは、いずれも頭上板3に搭載されている。 OS is an excitation pulse generator operated by a push button PB, and its output pulse is applied to the excitation receiving means 5 via a diode DO. FF
Both 1 and FF2 are flip-flop circuits,
Output pulses from the excitation pulse generators OS are respectively applied to the set terminals S via comparators. Further, the received signal from the excitation receiving means 5 is applied to the reset terminal R via comparators OP 1 and OP 2 and preset counters PC 1 and PC 2 , respectively. CK is flip-flop circuit FF1,
an arithmetic circuit to which the time width signal from FF2 is applied;
IN is an indicator that displays the calculation results of the calculation circuit CK in analog or digital form. Each flip-flop circuit FF1, FF2, arithmetic circuit CK, and indicator IN are all mounted on the overhead board 3.
このように構成した装置の動作を次に説明す
る。 The operation of the apparatus configured in this way will be described next.
被測定者MHを基台1上に直立させ頭上板3を
被測定者の頭頂に接触させる。この操作は従来公
知の身長計の測定手法と同様である。この状態に
おいて、押しボタンスイツチPBによつて、励振
パルス発生器OSを作動させ、ここから励振パル
スを一定周期で出力する。励振受信手段5に励振
パルスが印加されると、所謂ジユール(Joule)
効果によつて励振手段5の位置であつて磁歪線4
の内部に超音波信号が発生する。このような超音
波信号発生の動作は、励振受信手段5が磁歪線4
のどの位置にあつても同一条件で行なわれる。励
振パルス発生器OSからのパルスは、磁歪線4に
沿つて移動可能な励振受信手段5を介して、磁歪
線4内であつて、励振受信手段5の位置で超音波
信号を発生させるとともに、各フリツプフロツプ
回路FF1,FF2を比較器を介してセツト状態に
する。 The person to be measured MH is made to stand upright on the base 1, and the overhead board 3 is brought into contact with the top of the head of the person to be measured. This operation is similar to the measuring method of a conventionally known height meter. In this state, the push button switch PB is used to operate the excitation pulse generator OS, which outputs excitation pulses at regular intervals. When an excitation pulse is applied to the excitation receiving means 5, a so-called Joule
Due to the effect, the position of the excitation means 5 and the magnetostrictive wire 4
Ultrasonic signals are generated inside the In such an operation of generating an ultrasonic signal, the excitation receiving means 5 receives the magnetostrictive wire 4.
It is performed under the same conditions no matter where it is placed in the throat. The pulses from the excitation pulse generator OS generate ultrasonic signals within the magnetostrictive line 4 at the position of the excitation receiving means 5 via an excitation receiving means 5 movable along the magnetostrictive line 4, and Each flip-flop circuit FF1, FF2 is set to a set state via a comparator.
磁歪線4内であつて、励振受信手段5の位置で
発生した超音波信号は、この磁歪線4を伝播経路
としてその両端に向けて伝播し、両端41,42
で反射し、磁歪線4を再び伝播して励振受信手段
5でそれぞれ検出される。この実施例では励振受
信手段としてコイルが用いられているので、この
コイルに近接する磁歪線4内を超音波信号が通過
するとき、所謂ビラリ(Villari)効果によつてパ
ルス状の電圧e1,e2が発生する。比較器OP1,
OP2は、励振パルス発生器OSからの励振パルス
と、励振受信手段5からの受信パルスとを区別
(励振パルスと受信パルスとは、極性、振幅が異
なる)し、受信パルスだけを選択し、また、プリ
セツトカウンタPC1,PC2はそれぞれ、受信パル
スの第1発目と、第2発目とを選択する。したが
つて、フリツプフロツプ回路FF1のリセツト端
子Rには例えば第1発目の受信パルスが印加さ
れ、また、FF2のリセツト端子Rには、第2発
目の受信パルスが印加される。いま励振パルスの
印加と同時に、励振受信手段5の位置で超音波信
号が発生するものとすれば、この超音波信号が磁
歪線4を伝播し、その両端41,42で反射し、
再び励振、受信手段5の位置まで往復する伝播時
間t1、t2は(1)式、(2)式で表わすことができる。 The ultrasonic signal generated within the magnetostrictive wire 4 at the position of the excitation receiving means 5 propagates toward both ends of the magnetostrictive wire 4 as a propagation path, and reaches both ends 41 and 42.
, propagates again through the magnetostrictive line 4 and is detected by the excitation receiving means 5 . In this embodiment, a coil is used as the excitation receiving means, so when an ultrasonic signal passes through the magnetostrictive wire 4 close to this coil, a pulse-like voltage e 1 , e 2 occurs. Comparator OP 1 ,
OP 2 distinguishes between the excitation pulse from the excitation pulse generator OS and the received pulse from the excitation receiving means 5 (the excitation pulse and the received pulse are different in polarity and amplitude), selects only the received pulse, Further, preset counters PC 1 and PC 2 select the first and second received pulses, respectively. Therefore, for example, the first received pulse is applied to the reset terminal R of the flip-flop circuit FF1, and the second received pulse is applied to the reset terminal R of the flip-flop circuit FF2. Assuming that an ultrasonic signal is generated at the position of the excitation receiving means 5 at the same time as the excitation pulse is applied, this ultrasonic signal propagates through the magnetostrictive line 4 and is reflected at both ends 41 and 42 of the ultrasonic signal.
The propagation times t 1 and t 2 for excitation and reciprocation to the position of the receiving means 5 can be expressed by equations (1) and (2).
t1=2x/vs (1)
t2=2(L−x)/vs (2)
ただし、
vs:磁歪線4内を超音波信号が伝播する速度
x:被測定身長(励振受信手段5と反射端41と
の距離)
L:磁歪線4の長さで、ここではL−xはxより
常に大きくなるように選ばれるものとする。 t 1 = 2x/v s (1) t 2 = 2(L-x)/v s (2) where, v s : Speed at which the ultrasonic signal propagates within the magnetostrictive wire 4 x : Measured height (excitation reception (distance between the means 5 and the reflective end 41) L: length of the magnetostrictive line 4; here L-x is chosen so that it is always larger than x;
各フリツプフロツプ回路FF1,FF2は、励振
パルスによつてセツトされ、受信パルスによつて
それぞれリセツトされるもので、ここからは、前
記した往復の伝播時間t1、t2に対応する時間幅を
もつパルス幅信号が得られ、これらの信号が演算
回路CKに印加される。演算回路CKは、この2つ
の時間幅信号t1,t2を入力し、例えば(3)式の演算
を行なうことによつて身長xを求める。 Each of the flip-flop circuits FF1 and FF2 is set by an excitation pulse and reset by a received pulse, and from this point on, the flip-flop circuits have a time width corresponding to the round-trip propagation times t 1 and t 2 described above. Pulse width signals are obtained and these signals are applied to the arithmetic circuit CK. The arithmetic circuit CK inputs these two time width signals t 1 and t 2 and calculates the height x by calculating, for example, equation (3).
t1−t2/t1+t2=2x−L/L
x=L/2(t1−t2/t1+t2+1) (3)
このような演算を行なうことによる特長は、超
音波信号の伝播速度vs(この伝播速度vsは周囲
温度等の変化によつて変わる)に影響されない
で、身長xを測定することができるところにあ
る。そして、指示計INはこの演算結果を指示す
る。この表示は、頭上板3においてなされること
から、頭上板3の頭頂への接触、測定指示および
指示値の読みとり操作を従来のものと同様に簡単
に行なうことができる。 t 1 −t 2 /t 1 +t 2 =2x−L/L x=L/2(t 1 −t 2 /t 1 +t 2 +1) (3) The advantage of performing such calculation is that The height x can be measured without being affected by the signal propagation velocity v s (this propagation velocity v s changes due to changes in ambient temperature, etc.). Then, the indicator IN indicates the result of this calculation. Since this display is made on the overhead board 3, touching the overhead board 3 to the top of the head, giving measurement instructions, and reading the indicated value can be easily performed as in the conventional case.
なお、上記の実施例では、励振手段、受信手段
を共用し、これを磁歪線に巻回するコイルとした
ものであるが、他の構造でもよく、また、これら
の手段の近くに永久磁石を配置させ、これによつ
て磁歪線にバイアスを与え励振あるいは受信効率
を増大させるようにしてもよい。また、ここでは
身長を測定する場合を例にとつて説明したが、座
高、その他の長さ測定にも適用できることは勿論
である。 In the above embodiment, the excitation means and the reception means are shared, and are made of a coil wound around the magnetostrictive wire, but other structures may be used, and permanent magnets may be placed near these means. The magnetostrictive wires may be arranged so as to bias the magnetostrictive wires and increase the excitation or reception efficiency. Moreover, although the case of measuring height has been described here as an example, it is of course applicable to measuring sitting height and other lengths.
以上説明したように、本発明によれば、測定値
をデイジタル表示することが容易であり、計測誤
差がなく、しかも周囲温度等の影響を受けないの
で測定精度の高い身長測定装置が実現できる。 As described above, according to the present invention, it is easy to digitally display measured values, there is no measurement error, and there is no influence of ambient temperature, etc., so it is possible to realize a height measuring device with high measurement accuracy.
第1図は本発明の一実施例を示す外形図、第2
図は要部の構成斜視図、第3図はその電気的なブ
ロツク図である。
1……基台、2……支柱、3……頭上板、4…
…磁歪線、5……励振受信手段、FF1,FF2…
…フリツプフロツプ回路、CK……演算回路、OS
……パルス発生器、IN……指示計。
Fig. 1 is an outline drawing showing one embodiment of the present invention, Fig. 2 is an outline drawing showing an embodiment of the present invention;
The figure is a perspective view of the main part, and FIG. 3 is its electrical block diagram. 1... Base, 2... Support, 3... Overhead board, 4...
...Magnetostrictive wire, 5...Excitation receiving means, FF1, FF2...
...Flip-flop circuit, CK... Arithmetic circuit, OS
...Pulse generator, IN...Indicator.
Claims (1)
で構成された身長測定装置において、前記支柱に
ほぼ平行に張られその両端において超音波信号が
反射するように構成された磁歪線と、前記頭上板
とともに移動し前記磁歪線に結合してこの磁歪線
内に超音波信号を発生させるとともに磁歪線の両
端で反射してきた超音波信号を受信する励振及び
受信手段と、前記励振手段によつて磁歪線内に発
生した超音波信号が磁歪線の両端で反射し前記受
信手段に到達するまでの往復の伝播時間t1、t2を
得る回路手段と、前記往復の伝播時間t1、t2に関
連する信号を入力し、少なくともt1−t2/t1+t
2なる演算 を含む演算を行ない身長を求めるための演算回路
と、この演算回路での演算結果を表示する指示計
とを設け、前記回路手段、演算回路及び指示計を
前記頭上板に搭載させたことを特徴とする身長測
定装置。[Scope of Claims] 1. A height measuring device consisting of a support and an overhead plate movable along the support, which is extended approximately parallel to the support and configured to reflect ultrasonic signals at both ends thereof. a magnetostrictive wire, and an excitation and receiving means that moves with the head plate and couples to the magnetostrictive wire to generate an ultrasonic signal within the magnetostrictive wire and receives the ultrasonic signal reflected at both ends of the magnetostrictive wire; circuit means for obtaining round-trip propagation times t 1 and t 2 for the ultrasonic signal generated in the magnetostrictive wire by the excitation means to reflect at both ends of the magnetostrictive wire and reach the receiving means; and the round-trip propagation. Input signals related to times t 1 , t 2 , at least t 1 −t 2 /t 1 +t
An arithmetic circuit for performing arithmetic operations including the second arithmetic operation to determine the height, and an indicator for displaying the arithmetic results of the arithmetic circuit are provided, and the circuit means, the arithmetic circuit, and the indicator are mounted on the overhead board. A height measuring device characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57187087A JPS5882110A (en) | 1982-10-25 | 1982-10-25 | Stature measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57187087A JPS5882110A (en) | 1982-10-25 | 1982-10-25 | Stature measuring device |
Related Parent Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14062078A Division JPS5566702A (en) | 1978-11-15 | 1978-11-15 | Height measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5882110A JPS5882110A (en) | 1983-05-17 |
| JPS6253054B2 true JPS6253054B2 (en) | 1987-11-09 |
Family
ID=16199883
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57187087A Granted JPS5882110A (en) | 1982-10-25 | 1982-10-25 | Stature measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5882110A (en) |
Families Citing this family (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60127511U (en) * | 1984-02-07 | 1985-08-27 | 横河電機株式会社 | Rotating magnetostrictive potentiometer |
| JPS6197523A (en) * | 1984-10-18 | 1986-05-16 | Yokogawa Hokushin Electric Corp | Position detecting circuit for reflection type magnetostrictive potentiometer |
| JPS63150612A (en) * | 1986-12-16 | 1988-06-23 | Yaskawa Electric Mfg Co Ltd | Absolute displacement sensor using magnetostrictive delay line |
| DE212007000087U1 (en) * | 2006-12-22 | 2009-09-03 | Zhongshan Transtek Electronics Co., Ltd., Zhongshan | Body size measuring device |
| DE102012220468B3 (en) * | 2012-11-09 | 2014-03-27 | Seca Ag | length measuring instrument |
| DE102012220412B3 (en) * | 2012-11-28 | 2014-03-27 | Seca Ag | length measuring instrument |
| CN104757997A (en) * | 2015-03-13 | 2015-07-08 | 东莞捷荣技术股份有限公司 | Height measuring instrument |
| CN106767581A (en) * | 2016-12-12 | 2017-05-31 | 山东登海种业股份有限公司 | A kind of corn plants height measurement device |
-
1982
- 1982-10-25 JP JP57187087A patent/JPS5882110A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5882110A (en) | 1983-05-17 |
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