JPS6320136B2 - - Google Patents
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- Publication number
- JPS6320136B2 JPS6320136B2 JP54001110A JP111079A JPS6320136B2 JP S6320136 B2 JPS6320136 B2 JP S6320136B2 JP 54001110 A JP54001110 A JP 54001110A JP 111079 A JP111079 A JP 111079A JP S6320136 B2 JPS6320136 B2 JP S6320136B2
- Authority
- JP
- Japan
- Prior art keywords
- graph
- piezoelectric element
- container
- weight
- output
- 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
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- Measuring And Recording Apparatus For Diagnosis (AREA)
Description
【発明の詳細な説明】
本発明は人体、たたみ、ふとん、航空機の機
体、その他の物体の表面を、急激に増減する力で
加圧し、各力に対応する物体表面のくぼみの深さ
を圧力−ひずみ図として求める装置に関するもの
である。以下、実施例にしたがい説明する。Detailed Description of the Invention The present invention applies pressure to the surface of a human body, folding mattress, futon, aircraft body, or other object with a force that rapidly increases or decreases, and adjusts the depth of the depression on the object surface corresponding to each force. -Relates to a device for obtaining strain diagrams. Examples will be explained below.
第1〜2図は本発明を実施した圧力−ひずみ図
記録装置の加動部を示めし、1は上下端の閉じた
プラスチツク製の円筒形容器で、その内空の上下
長は20cmある。2は容器1の外面の下半部にかぶ
せた高周波変成器で、上下長10cmの範囲に巻れた
第3図示の高周波コイル2aと、その外に重ね巻
きされた高周波コイル2bとを内蔵している。3
は容器1の内径より、わずかに小さな外径を持
つ、上下長10cmの鉄製の円柱形の重り。4は容器
1の下面に取りつけた円盤状の電池内蔵の電子回
路ボツクス。5はその下面に取りつけた小円盤形
のチタン酸バリウム等から成る圧電素子。6はそ
の下面に取りつけた突起状の硬質プラスチツク製
接触子である。 Figures 1 and 2 show the moving part of the pressure-strain diagram recording apparatus according to the present invention, and 1 is a cylindrical container made of plastic with closed upper and lower ends, and the vertical length of the interior thereof is 20 cm. Reference numeral 2 denotes a high frequency transformer placed over the lower half of the outer surface of the container 1, which incorporates a high frequency coil 2a shown in Figure 3 wound over a vertical length of 10 cm, and a high frequency coil 2b wound overlappingly on the outside. ing. 3
is an iron cylindrical weight with an outer diameter slightly smaller than the inner diameter of container 1 and a vertical length of 10 cm. 4 is a disc-shaped electronic circuit box with a built-in battery attached to the bottom of the container 1. 5 is a small disk-shaped piezoelectric element made of barium titanate or the like attached to its lower surface. 6 is a protruding hard plastic contact attached to the bottom surface.
第3図はこの可動部の電気回路図で、以下その
他の図も用い、可動部の作用を説明する。 FIG. 3 is an electrical circuit diagram of this movable part, and the operation of the movable part will be explained below using other figures as well.
容器1の上部を手でにぎり、人体、その他の測
定対象の水平表面に対し、垂直に振りおろし、接
触子を表面に押しつけ、すばやく引きあげて一回
の測定を終了する。この所要時間は0.1s程度であ
る。 Grasp the top of the container 1 with your hands, shake it down perpendicularly to the horizontal surface of the human body or other object to be measured, press the contact against the surface, and quickly pull it up to complete one measurement. The time required for this is approximately 0.1s.
今、被測定物体表面の高さを基準高度0cmと
し、接触子6の下端が上方5cmの高さから出発
し、0.04sを要して物体表面にたつし、しだいに
減速しつつ、0.01sを要して、物体表面を2cmの
深さまでくぼませ、以後逆の経過をたどり、元の
高さに帰えつたとすれば、第4図のグラフAのよ
うな、時間に対応する変位曲線を描く事に成る。 Now, the height of the surface of the object to be measured is set as a reference altitude of 0 cm, and the lower end of the contact 6 starts from a height of 5 cm above, takes 0.04 s to reach the object surface, and gradually decelerates to 0.01 s. If we indent the surface of the object to a depth of 2 cm, and then reverse the process and return to the original height, we can form a displacement curve corresponding to time, as shown in graph A in Figure 4. I'll end up drawing it.
重り3の下端の初期高度を10cmとすれば、重力
の加速度G(980cm/s↑2)により、重り3は自
由落下し、接触子下端が物体表面に接する時点
で、
10−1/2×980×0.04↑2=9.216(cm)
の高さにいたり、接触子下端が物体表面から離れ
る時点では、
10−1/2×980×0.06↑2=8.236(cm)
の高さにいたつており、容器内空の下端は高さ5
cmにあり、3.236cmの開きがあるが、まもなく重
りの下端は上昇する内空の下端にぶつかり、引き
あげられ、元の高さに帰り、第4図のグラフBの
ような変位曲線をとる。 If the initial height of the lower end of the weight 3 is 10 cm, the weight 3 will fall freely due to the acceleration of gravity G (980 cm/s↑2), and when the lower end of the contact touches the object surface, the height will be 10-1/2× It reaches a height of 980×0.04↑2=9.216 (cm), and when the bottom end of the contact leaves the object surface, it reaches a height of 10-1/2×980×0.06↑2=8.236 (cm). , the lower end of the container is at a height of 5
cm, and there is a gap of 3.236 cm, but soon the lower end of the weight collides with the lower end of the rising inner space, is pulled up, returns to its original height, and takes a displacement curve as shown in graph B in Figure 4.
また、重り3の下端と、内空下端との間隔、す
なわち、グラフCは、
C=B−(A+5)
であたえられる。(内空下端と、接触子下端との
間隔は5cm)
可動部下端が物体上5cmにある時、鉄製の重り
3が高周波変成器2中にあり、コイル2aのイン
ダクタンスは大きく、このコイルと、電子回路ボ
ツクス4中のコンデンサー7とで構成される並列
共振回路の共振周波数は最小値を示す。容器1の
運動により、重り3が相対的にコイル2aからぬ
けでて行き、
復帰する間、共振周波数は増大し、復帰し、その
変化曲線はグラフCと相関する第5図のグラフD
と成る。 Further, the distance between the lower end of the weight 3 and the lower end of the inner space, that is, the graph C is given by C=B-(A+5). (The distance between the lower end of the inner space and the lower end of the contact is 5 cm) When the movable lower end is 5 cm above the object, the iron weight 3 is in the high frequency transformer 2, the inductance of the coil 2a is large, and this coil and The resonant frequency of the parallel resonant circuit constituted by the capacitor 7 in the electronic circuit box 4 exhibits a minimum value. Due to the movement of the container 1, the weight 3 is relatively removed from the coil 2a, and while it returns, the resonant frequency increases and returns, and its change curve correlates with the graph C, as shown in the graph D in FIG.
becomes.
ボツクス4内の電池8からコイル2bをへて、
トランジスター9のコレクター回路に通電されて
おり、コイル2aの端子電圧はトランジスターの
ベース回路に加わつているため、発振回路を形成
し、トランジスター9の出力電圧はボツクス4に
内蔵されたアンテナ10に加わり、電波信号と成
つて空間に放射される。 From the battery 8 in the box 4 through the coil 2b,
Since the collector circuit of the transistor 9 is energized and the terminal voltage of the coil 2a is applied to the base circuit of the transistor, an oscillation circuit is formed, and the output voltage of the transistor 9 is applied to the antenna 10 built in the box 4. It becomes a radio wave signal and is radiated into space.
この電波信号はグラフDのように変化し、重り
3に対する容器1の相対的な変位を周波数変調で
表示したものと成る。(容器1と接触子6はほぼ
平行移動をするため、重り3に対する接触子6の
相対位置を示めしていると言う事も出来る。)
接触子6の下端が下降して物体面にたつするま
での間、増速による加速度が加わり、接触子と圧
電素子の自重による慣性力が生じ、圧電素子5は
上下方向にちじむ力を受け、素子5は出力電圧を
発生する。ただし、両者の質量は小さく、出力電
圧も小さい。 This radio wave signal changes as shown in graph D, and becomes a frequency modulated representation of the relative displacement of the container 1 with respect to the weight 3. (Since the container 1 and the contact 6 move almost in parallel, it can also be said that this indicates the relative position of the contact 6 with respect to the weight 3.) The lower end of the contact 6 descends and stands on the object surface. Until then, acceleration due to speed increase is applied, inertia force is generated due to the weight of the contact and the piezoelectric element, the piezoelectric element 5 receives a force that bends in the vertical direction, and the element 5 generates an output voltage. However, the mass of both is small and the output voltage is also small.
0.04s後、接触子下端が物体面にたつし、0.01s
の間に、接触子6は漸増する圧力で圧電素子5を
圧迫し、次の0.01sの間、その圧力は漸減する。
物体から接触子が離れて元の高さに帰える直前の
減速により、接触子と圧電素子の慣性がはたら
き、圧電素子はちじむ力を受ける。 After 0.04s, the lower end of the contact reaches the object surface, and 0.01s
During this period, the contact 6 presses the piezoelectric element 5 with a gradually increasing pressure, and during the next 0.01 s, the pressure gradually decreases.
Due to the deceleration just before the contact leaves the object and returns to its original height, inertia acts on the contact and the piezoelectric element, and the piezoelectric element receives a bending force.
このような圧電素子5の出力電圧変化曲線は第
6図のグラフEのように成る。 The output voltage change curve of such piezoelectric element 5 is as shown in graph E in FIG.
この電圧はボツクス4内のFM変調器11で周
波数変調され、アンテナ10から出る電波とは異
なつた周波数帯域の電波として、ボツクス4に内
蔵されたアンテナ12から外部空間へ放射され
る。その電波の周波数変化曲線は第7図のグラフ
Fのように成る。 This voltage is frequency-modulated by an FM modulator 11 inside the box 4, and is radiated to the outside space from an antenna 12 built into the box 4 as a radio wave in a frequency band different from that emitted from the antenna 10. The frequency change curve of the radio wave is as shown in graph F in FIG.
このように加動部から放射された二種類の電波
は近くに置かれた第8図示の箱状の固定部13で
受信され、測定結果としてのグラフに成る。図中
14,15は受信用アンテナである。 The two types of radio waves radiated from the active part in this way are received by the box-shaped fixed part 13 shown in FIG. 8 placed nearby, and a graph is formed as a measurement result. In the figure, 14 and 15 are receiving antennas.
第9図は固定部13内の電気回路のブロツク図
で、以下この図を用い、固定部の作用を説明す
る。 FIG. 9 is a block diagram of the electric circuit inside the fixing part 13, and the function of the fixing part will be explained below using this diagram.
アンテナ10から出た重り3に対する接触子6
の相対位置を示す電波信号はアンテナ14に入
り、FM検波器16で検波され、内蔵された結合
コンデンサーをへて、グラフCと同波形の出力電
圧が生じ、A−D変換器17により、100KHz程
度のサンプリング頻度で、デイジタル信号に変換
され、コンピユーター18のメモリーに記録され
る。 Contactor 6 for weight 3 coming out of antenna 10
A radio wave signal indicating the relative position of 2 enters the antenna 14, is detected by the FM detector 16, passes through the built-in coupling capacitor, produces an output voltage with the same waveform as graph C, and is converted to 100KHz by the A-D converter 17. The signal is converted into a digital signal and recorded in the memory of the computer 18 at a sampling frequency of approximately 100 kHz.
また、アンテナ12から出た圧電素子5の信号
電波はアンテナ15に入り、FM検波器19で検
波され、グラフEと同波形の出力電圧はA−D変
換器20により、変換器17と同頻度でデイジタ
ル信号化され、コンピユーター18のメモリーに
記録される。なお、コンピユーター18は変換器
17の出力がOVで一定時間持続している時に
は、その信号を記録する事をせず、Oから立ちあ
がつた事を検出すれば、記録を開始し、一定時間
Oレベルが持続すれば、記録を停止する。したが
つて、グラフCの曲線部分だけが記録される。そ
れと連動し、A−D変換器20の出力がコンピユ
ーター18のメモリーの、変換器17の出力が入
つている部分とは異なつた記憶場所に記録され
る。 Further, the signal radio wave of the piezoelectric element 5 output from the antenna 12 enters the antenna 15 and is detected by the FM detector 19, and the output voltage having the same waveform as graph E is output by the A-D converter 20 with the same frequency as the converter 17. The signal is converted into a digital signal and recorded in the memory of the computer 18. Note that when the output of the converter 17 remains at OV for a certain period of time, the computer 18 does not record the signal, but when it detects that it has risen from O, it starts recording and maintains the O level for a certain period of time. If this continues, recording will stop. Therefore, only the curved portion of graph C is recorded. In conjunction therewith, the output of the A/D converter 20 is recorded in a memory location of the computer 18 that is different from the portion containing the output of the converter 17.
ついでコンピユーター18は変換器17の出
力、すなわち、グラフCを元に、容器1およびそ
れに連動する接触子6の下端の、時間に対応する
変位、すなわち、下降開始時点の高さを0cmとし
た高度変化曲線aを求める動作をする。 Then, based on the output of the converter 17, that is, the graph C, the computer 18 calculates the displacement corresponding to time of the lower end of the container 1 and the contactor 6 linked thereto, that is, the height when the height at the start of descent is 0 cm. An operation is performed to obtain the change curve a.
その際、重り3の自由落下開始時点における下
端の高度を0cmとした変位曲線bをもパラメータ
ーとして用いる。 At that time, a displacement curve b in which the height of the lower end at the start of free fall of the weight 3 is 0 cm is also used as a parameter.
その関係式は、C=b−a∴a=b−Cと成
る。 The relational expression is C=b-a∴a=b-C.
このうち、Cは電波信号として固定部に送られ
て来た値であり、bは、b=−1/2×980×t
↑2(ただしtは時間s)で、コンピユーター1
8内で計算しうる値である。 Among these, C is the value sent to the fixed part as a radio wave signal, and b is b=-1/2×980×t
↑2 (where t is time s), computer 1
This is a value that can be calculated within 8.
したがつて、aを求める事は可能である。第1
0図にこの三者の関係を示すグラフを記す。 Therefore, it is possible to find a. 1st
Figure 0 shows a graph showing the relationship between these three.
ついで、コンピユーター18は圧電素子5の出
力信号のグラフE中の急激な立ちあがり開始点、
すなわち、接触子6が物体面に接触した時点を、
微分値(微係数)の急増する部分として検出し、
接触子6の下端が物体中にもつとも深くめりこん
だ時点を、微分値が0に成る部分として検出し、
両時点間の各時間に対応するaの値をX座標と
し、Eの値をY座標としてプロツトし、コンピユ
ーター18に付属のプリンター21で打ちだせば
(XYプロツター等を用いてもよい)第11図の
グラフGのような、最終的な測定結果がえられる
事に成る。 Then, the computer 18 detects the abrupt rising start point in the graph E of the output signal of the piezoelectric element 5,
In other words, the time when the contactor 6 contacts the object surface is
Detected as a part where the differential value (differential coefficient) increases rapidly,
Detecting the point at which the lower end of the contactor 6 is deeply embedded into the object as the point where the differential value becomes 0,
By plotting the value of a corresponding to each time between the two points as the X coordinate and the value of E as the Y coordinate, and printing it out with the printer 21 attached to the computer 18 (an XY plotter or the like may be used), the 11th The final measurement result as shown in graph G in the figure will be obtained.
可動部をゆつくり移動させ、次の測定部の上に
持つて来て、前述と同用の操作を行なえば、次の
グラフがとれる。 By slowly moving the movable part, bringing it to the next measurement part, and performing the same operations as above, the following graph can be obtained.
このようにして、短時間の間に多数の部位のグ
ラフがとれる。 In this way, graphs of many parts can be drawn in a short period of time.
上記実施例は種々の設計変更が可能である。以
下その概要を記す。 Various design changes can be made to the above embodiment. The outline is described below.
可動部を構成する各部の材質、形、構造、サイ
ズ等を任意に選ぶ事が出来る。たとえば、高周波
変成器2を容器1の壁内に埋めこんでもよい。電
子回路ボツクス4を、容器1の底壁中に埋めこむ
か、上壁上に取りつけ、容気1の底面に圧電素子
5を直結してもよい。 The material, shape, structure, size, etc. of each part constituting the movable part can be arbitrarily selected. For example, the high frequency transformer 2 may be embedded within the wall of the container 1. The electronic circuit box 4 may be embedded in the bottom wall of the container 1 or mounted on the top wall, and the piezoelectric element 5 may be directly connected to the bottom surface of the container 1.
圧電素子5は圧電体のほか、感圧ダイオード、
ストレインゲージ、その他を用いてもよい。 The piezoelectric element 5 includes not only a piezoelectric body but also a pressure-sensitive diode,
Strain gauges and others may also be used.
容器1を電動機や空気圧を用いた駆動装置に取
りつけ、被測定物体に打ちつけ、かつ引きはなす
動作を行つてもよい。 The container 1 may be attached to a drive device using an electric motor or air pressure, and the container 1 may be struck against an object to be measured and then pulled and released.
アンテナ10と14の間、およひ圧電素子5の
出力端子と固定部内のA−D変換器20の入力端
子とを柔軟なコードでつないでもよい。 A flexible cord may be used to connect the antennas 10 and 14, as well as the output terminal of the piezoelectric element 5 and the input terminal of the A-D converter 20 in the fixed part.
容器1の内面にスライド抵抗を埋めこみ、その
つまみを重り3に結合し、重りの慣性によりスラ
イド抵抗を駆動し、抵抗値変化により生ずる電圧
変化をA−D変換し、電波にのせて送信してもよ
い。 A slide resistor is embedded in the inner surface of the container 1, its knob is connected to the weight 3, the slide resistor is driven by the inertia of the weight, the voltage change caused by the change in resistance is converted from analog to digital, and it is transmitted on radio waves. Good too.
高周波変成器2を省略し、容器1の内空の底面
上に加速度測定用圧電素子をはりつけ、その上に
重り3をはりつけ、コンデンサーを通して、この
圧電素子の電圧変化成分出力を取りだし、ボツク
ス4内でA−D変換し、さらに電波にのせ
(PCM変調)アンテナ10から送信し、アンテナ
14で受信し、復調器をへて、圧電素子の出力と
同波形の電圧を得、その電圧をA−D変換器17
でデイジタル化し、コンピユーター18内で、リ
アルタイムで積分し、速度情報に変換し、さらに
積分して変位情報に変換し、前述のグラフaを得
てもよい。(加速度情報を二重積分すれば変位情
報に成る事は周知である。)
この場合、コンデンサーを通つた圧電素子の出
力は、容器1の下方への増速時(座標系における
負の加速時)素子は引きのばされ、負電圧出力を
生じ、減速時(正の加速時)素子はちぢみ、正電
圧出力を生じ、上方への増速時(正の加速時)素
子はちぢみ、正電圧出力を生じ、減速時(負の加
速時)素子は引きのばされ、負電圧出力を生じ、
いずれの方向でも、等速運動時(無加速時)素子
は元の長さをたもち、0電圧出力と成る。 The high frequency transformer 2 is omitted, a piezoelectric element for acceleration measurement is attached to the bottom of the inner space of the container 1, a weight 3 is attached on top of the piezoelectric element, and the voltage change component output of this piezoelectric element is taken out through a capacitor. A-D conversion is carried out at A-D, and then it is transmitted from the antenna 10 on a radio wave (PCM modulation), received by the antenna 14, passed through a demodulator, obtains a voltage with the same waveform as the output of the piezoelectric element, and converts that voltage into A-D. D converter 17
The above-mentioned graph a may be obtained by digitizing the data, integrating it in real time in the computer 18, converting it into velocity information, and further integrating and converting it into displacement information. (It is well known that double integration of acceleration information yields displacement information.) In this case, the output of the piezoelectric element passing through the capacitor is ) The element is stretched, producing a negative voltage output; during deceleration (positive acceleration) the element contracts, producing a positive voltage output; when increasing speed upward (positive acceleration) the element contracts, producing a positive voltage During deceleration (negative acceleration) the element is stretched, producing a negative voltage output,
In either direction, the element retains its original length during uniform motion (no acceleration) and provides zero voltage output.
A−D変換器17からは100KHz程度のサンプ
リング頻度で変換された加速度デイジタル情報が
出るが、コンピユーター18内で、容器1の始動
時0sからの電圧値を順次積算(加算、減算を含
む)し、すなわち、積分し、各時間に対応する速
度値を求め、同時に、この速度情報を容器1の始
動時から積算(積分)して行き、各時間に対応す
る高度、すなわち、変位情報であるグラフaを求
める。 The A-D converter 17 outputs acceleration digital information converted at a sampling frequency of about 100 KHz, and the computer 18 sequentially integrates (including addition and subtraction) the voltage values from 0s when the container 1 starts. That is, the velocity value corresponding to each time is obtained by integrating, and at the same time, this velocity information is integrated (integrated) from the start of the container 1, and the altitude corresponding to each time, that is, the graph which is displacement information is obtained. Find a.
上記の方式以外の、加速度をリアルタイムで電
圧に変換するセンサーを、容器1に取りつけても
よい。 A sensor other than the above-mentioned method that converts acceleration into voltage in real time may be attached to the container 1.
被測定物体の側面や傾斜面を測定する場合、容
器1を水平位または傾斜位にしなければならない
が、容器1の上面に傾斜測定用の圧電素子をはり
つけ、その上に傾斜測定用の重りをはりつけ、容
器1が鉛直方向から傾斜すれば、その圧電素子の
出力が減少するようにしておき、その出力電圧を
電波で送信し、固定部の専用アンテナで受信し、
検波とA−D変換を行ない、コンピユーター18
で電圧値から傾斜角を算出し、重り3に加わる重
力の加速度の、容器1の長軸方向成分を求め、b
を求める計算式を補正し、容器1内における、重
り3の、容器1の長軸方向の落下による変位を算
出し、aを計算するようにしてもよい。 When measuring a side surface or an inclined surface of an object to be measured, the container 1 must be placed in a horizontal or inclined position.A piezoelectric element for measuring the inclination is attached to the top surface of the container 1, and a weight for measuring the inclination is placed on top of the piezoelectric element. If the container 1 is tilted from the vertical direction during crucifixion, the output of the piezoelectric element is made to decrease, and the output voltage is transmitted by radio waves and received by a dedicated antenna on the fixed part.
The computer 18 performs wave detection and A-D conversion.
Calculate the inclination angle from the voltage value in , find the long axis direction component of the container 1 of the acceleration of gravity applied to the weight 3, and b
The calculation formula for calculating a may be corrected, and the displacement of the weight 3 within the container 1 due to the fall in the longitudinal direction of the container 1 may be calculated, and a may be calculated.
この場合、圧電素子と重りの上下長は小さいも
のを用いる。被測定物体に向つて動きはじめる前
の、容器1が鉛直方向を向いている時の圧電素子
の出力を1とすれば、鉛直線に対する傾斜角のコ
サインに比例した出力電圧が生ずる。従つてその
信号を受けたコンピユーター18はG(980cm/s
↑2)にその値をかけbを計算する事が出来る。
(駆動時情報も用いうる)
測定結果のグラフの形式を種々に変えたり、数
表で表示したりする事は容易に出来る。 In this case, the vertical length of the piezoelectric element and the weight are small. If the output of the piezoelectric element is 1 when the container 1 is oriented vertically before it starts moving toward the object to be measured, an output voltage proportional to the cosine of the inclination angle with respect to the vertical line is generated. Therefore, the computer 18 that received the signal is G (980 cm/s
You can calculate b by multiplying ↑2) by that value.
(Information during driving can also be used.) It is easy to change the graph format of the measurement results in various ways or to display them in a numerical table.
重り3の材質をヘライトその他に代えてもよ
い。 The material of the weight 3 may be replaced with helite or other materials.
その他種々の設計変更が可能である。 Various other design changes are possible.
なお、測定対象が人体の腹部、部厚いゴム板等
のように、柔軟な部厚い物体である場合、時間に
対するくぼみの深さの曲線、グラフaは深くな
り、同時に得られる圧力曲線、グラフEとから求
められる圧力−歪図のグラフGはゆるやかな傾斜
と成る。 Note that when the object to be measured is a flexible and thick object, such as the abdomen of a human body or a thick rubber plate, the curve of the depth of the indentation versus time, graph a, becomes deeper, and the pressure curve obtained at the same time, graph E. Graph G of the pressure-strain diagram obtained from , has a gentle slope.
測定対象が強固に固定された部厚い鋼鉄板のよ
うな場合、グラフaは深さが0に近い、近似的な
直線と成り、グラフEの立ち上がりの所要時間は
ごく短く、急傾斜に成り、近似的な方形波を描
く。 If the object to be measured is a strongly fixed thick steel plate, graph a will be an approximate straight line with a depth close to 0, and graph E will take a very short time to rise and will have a steep slope. Draw an approximate square wave.
しかし、この短時間の間にも、わずかながら、
接触子6の下端は対象表面を押し下げて行き、圧
電素子5からは出力電圧が漸増的に発生している
から圧力−歪図は得られる事に成る。 However, even during this short period of time,
The lower end of the contactor 6 presses down on the target surface, and since the output voltage is gradually generated from the piezoelectric element 5, a pressure-strain diagram can be obtained.
ただし、硬質の対象を精度良く測定するには、
容器1、電子回路ボツクス4、圧電素子5、接触
子6等を硬質材料で造り、急変する圧電素子5の
出力電圧変化を忠実に再現し得る、応答速度の速
い周波数変調器、復調器、A−D変換器、D−A
変換器等を用いなければならない。 However, in order to accurately measure hard objects,
A frequency modulator and demodulator with a fast response speed, in which the container 1, electronic circuit box 4, piezoelectric element 5, contactor 6, etc. are made of hard materials, and can faithfully reproduce sudden changes in the output voltage of the piezoelectric element 5. -D converter, D-A
A converter etc. must be used.
通常の測定対象はその中間にあり、対象の硬度
に応じて適当に設計された装置を用いれば良い。 Normal objects to be measured fall somewhere in between, and it is sufficient to use an appropriately designed device depending on the hardness of the object.
人体の腹部等では数Kgの加圧で数cmくぼむが、
たたみ等では数mmしかくぼまない。小型飛行機の
布ばりの機体部分では大きくくぼむし、大型機の
フレームの外側に取りつけられた外装板の外面で
は、ほとんどくぼまない等、あらゆる物体の色々
な場所を本装置で測定した場合、さまざまな傾斜
のグラフGが得られる事に成る。 In the abdomen of the human body, pressure of several kilograms causes a depression of several centimeters.
When folded, etc., it only dents a few mm. When measuring various locations on various objects using this device, there are various problems such as large dents in the fabric fuselage of a small airplane, and almost no dents in the outer surface of the exterior panel attached to the outside of the frame of a large airplane. This results in a graph G with a slope of .
浅い部に骨がある人体の足背部、前頭部、ある
いはコンクリートの床上に敷かれたじゆうたん等
について測定した場合には、グラフGは始めゆる
やかに上昇し、すぐ急傾斜と成り、ピークにたつ
する。 When measuring the dorsal part of the human body, which has bones in shallow parts, the front of the head, or a carpet placed on a concrete floor, graph G starts out gradually rising, then quickly becomes steep, and reaches the peak. To stand.
このような場合、ゆるやかな傾斜の部分のグラ
フは読みとりやすいが、急傾斜部は読みとりにく
くなるので、プリンター21で横軸方向(深さ)
を引きのばしたグラフを打ちだせば、見やすく成
る。 In such a case, it is easy to read the graph in the gently sloped part, but it is difficult to read the steeply sloped part, so the printer 21 prints the graph in the horizontal direction (depth).
If you draw out a graph that stretches out the graph, it will be easier to see.
グラフGでは時間要素は現われないが、袋につ
めた粘土等、塑性変形の可能な物では、接触子6
がめりこむ際、圧電素子5から電圧が出るが、引
き上げる時には電圧がほとんど出ない。弾性ゴム
等ではこのような事はない。従つて引き上げる際
の情報も利用すれば、コンピユーター18に対象
の弾性、塑性の度合を判定させる事も出来る。 Although the time element does not appear in graph G, for objects that can be plastically deformed, such as clay packed in a bag, contact 6
When the piezoelectric element 5 sinks in, a voltage is generated from the piezoelectric element 5, but when it is pulled up, almost no voltage is generated. This does not happen with elastic rubber, etc. Therefore, if the information obtained during pulling is also used, the computer 18 can determine the degree of elasticity and plasticity of the object.
グラフGはグラフaとグラフEから求めるが、
パラメーターは圧力と深さ変化だけで、時間は入
つていない。そこで、時間要素も加える必要があ
る場合には、一つのグラフ上に横軸を共通な時間
軸として、グラフaとグラフEを同時に記入した
物をプリンター21で打ちだせば良い。 Graph G is found from graph a and graph E, but
The only parameters are pressure and depth change, and time is not included. Therefore, if it is necessary to add a time element, the printer 21 can print out a graph in which graphs a and E are simultaneously drawn on one graph, with the horizontal axis as a common time axis.
本発明の実施により、接触子先端の被測定物体
中への陥入の深さを求めるための、可動部の変位
検出器の主要部分を、可動部中に納める事が出
来、機能のわりに小型であり、ワンタツチで一箇
所の測定が出来るため、短時間に多数の部位の測
定をし得る、人体、たたみ、ふとん、いすのシー
ト、自動車や飛行機の外装、その他の物体表面に
おける、硬度にも関連する、連続的に強さが変化
する加圧に対応する、くぼみの深さを、グラフに
描く測定装置がえられる利点がある。 By implementing the present invention, the main parts of the displacement detector of the movable part for determining the depth of penetration of the tip of the contact into the object to be measured can be housed within the movable part, and the size is small compared to the function. Since it is possible to measure one place with one touch, it is possible to measure many parts in a short time.It is also suitable for hardness of the human body, folds, futons, chair seats, the exterior of cars and airplanes, and other object surfaces. It is advantageous to have a measuring device that graphs the depth of the indentation in response to an associated pressure of continuously varying intensity.
第1図は本発明を実施した圧力−歪図記録装置
の可動部の平面図。第2図はその縦断面図。第3
図はその電気回路図。第4図は可動部の運動に関
するグラフ。第5図はグラフCの電圧をFM変調
した電波のグラフ。第6図は圧電素子5の出力電
圧のグラフ。第7図はそのFM変調電波のグラ
フ。第8図は固定部の平面図。第9図は固定部の
電気回路のブロツク図。第10図はコンピユータ
ー18内で活動する、可動部の運動に関するグラ
フ。第11図は測定結果のグラフである。
FIG. 1 is a plan view of a movable part of a pressure-strain diagram recording device embodying the present invention. Figure 2 is a longitudinal cross-sectional view. Third
The figure shows the electrical circuit diagram. FIG. 4 is a graph regarding the motion of the movable part. Figure 5 is a graph of radio waves obtained by FM modulating the voltage in graph C. FIG. 6 is a graph of the output voltage of the piezoelectric element 5. Figure 7 is a graph of the FM modulated radio waves. FIG. 8 is a plan view of the fixing part. FIG. 9 is a block diagram of the electric circuit of the fixed part. FIG. 10 is a graph relating to the motion of movable parts active within the computer 18. FIG. 11 is a graph of the measurement results.
Claims (1)
器中に、円筒軸の方向にスライド可能な重りを入
れ、容器の運動にともなう、重りに対する容器の
変位を、電気信号に変換して送信する電気回路を
取りつけ、下端に圧電素子を介して、被測定物体
に接触するための接触子を取りつけ、圧電素子の
出力を電気信号に変換して送信する電気回路を取
りつけて成る可動部と、可動部の変位に関する信
号を受信する電気回路と、圧電素子の出力信号を
受信する電気回路と、両回路の出力の対応関係を
グラフ化する装置とを有する固定部とより成る、
物体表面の加圧に対応するくぼみの深さをグラフ
化して表示する装置。1. A weight that can be slid in the direction of the cylindrical axis is placed in a small container with a cylindrical interior space with the axial direction facing up and down, and as the container moves, the displacement of the container relative to the weight is converted into an electrical signal and transmitted. a movable part having an electric circuit attached thereto, a contact element for contacting the object to be measured via a piezoelectric element attached to the lower end, and an electric circuit attached thereto that converts the output of the piezoelectric element into an electric signal and transmits it; consisting of a fixed part having an electric circuit for receiving a signal regarding the displacement of the movable part, an electric circuit for receiving an output signal of the piezoelectric element, and a device for graphing the correspondence of the outputs of both circuits;
A device that graphs and displays the depth of depressions corresponding to pressurization on the surface of an object.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP111079A JPS5594238A (en) | 1979-01-08 | 1979-01-08 | Stresssstrain diagram recorder of human body |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP111079A JPS5594238A (en) | 1979-01-08 | 1979-01-08 | Stresssstrain diagram recorder of human body |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5594238A JPS5594238A (en) | 1980-07-17 |
| JPS6320136B2 true JPS6320136B2 (en) | 1988-04-26 |
Family
ID=11492319
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP111079A Granted JPS5594238A (en) | 1979-01-08 | 1979-01-08 | Stresssstrain diagram recorder of human body |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5594238A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4517149B2 (en) * | 2005-03-09 | 2010-08-04 | 国立大学法人高知大学 | Hardness measuring instrument, hardness measuring apparatus, and hardness evaluation method |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5184684A (en) * | 1975-01-22 | 1976-07-24 | Toitsu Kogyo Kk | KODOSOKUTEIHOSHIKI |
-
1979
- 1979-01-08 JP JP111079A patent/JPS5594238A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5594238A (en) | 1980-07-17 |
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