JPH029702B2 - - Google Patents
Info
- Publication number
- JPH029702B2 JPH029702B2 JP57182363A JP18236382A JPH029702B2 JP H029702 B2 JPH029702 B2 JP H029702B2 JP 57182363 A JP57182363 A JP 57182363A JP 18236382 A JP18236382 A JP 18236382A JP H029702 B2 JPH029702 B2 JP H029702B2
- Authority
- JP
- Japan
- Prior art keywords
- thermal expansion
- connecting shaft
- shaft
- bellows
- main 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L19/00—Details of, or accessories for, apparatus for measuring steady or quasi-steady pressure of a fluent medium insofar as such details or accessories are not special to particular types of pressure gauges
- G01L19/0007—Fluidic connecting means
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Fluid Pressure (AREA)
Description
【発明の詳細な説明】
本発明は、流体の圧力、液位等を測定するため
に使用される圧力伝送器に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a pressure transmitter used to measure fluid pressure, liquid level, etc.
従来、この種の圧力伝送器として、第1図に示
すものが知られている。図について説明すると、
符号1は本体である。この本体1は、有底円筒状
に形成された胴部2と、この胴部2の一側開口部
に嵌合されたフランジ部3とからなつている。こ
の本体1の内部には、一対の絶縁部材4a,4b
の間に、支持リング5a,5bを介してレンジス
プリング6が挟持されている。前記絶縁部材4
a,4bは胴部2の壁部2aとフランジ部3とに
よつて本体1内部に固定されている。 Conventionally, as this type of pressure transmitter, one shown in FIG. 1 is known. To explain the diagram,
Reference numeral 1 is the main body. This main body 1 consists of a body part 2 formed in a cylindrical shape with a bottom, and a flange part 3 fitted into an opening on one side of the body part 2. Inside this main body 1, a pair of insulating members 4a, 4b are provided.
A range spring 6 is held between them via support rings 5a and 5b. The insulating member 4
a and 4b are fixed inside the main body 1 by the wall 2a of the body 2 and the flange 3.
また、前記フランジ部3の外面側には、凹部3
aが形成され、この凹部3aの中央部には、円形
の貫通孔3bが穿設されている。このフランジ部
3には、その貫通孔3bを塞ぐように受圧要素と
してのベローズ7の一端が固定されている。この
ベローズ7の他端と前記レンジスプリング6の中
央部との間は、丸棒状の連結軸8によつて連結さ
れており、前記ベローズ7に加えられる圧力が連
結軸8を介してレンジスプリング6に伝達される
ようになつている。 Further, a recess 3 is provided on the outer surface side of the flange portion 3.
a is formed, and a circular through hole 3b is bored in the center of this recess 3a. One end of a bellows 7 as a pressure receiving element is fixed to this flange portion 3 so as to close the through hole 3b. The other end of the bellows 7 and the center of the range spring 6 are connected by a round rod-shaped connecting shaft 8, and the pressure applied to the bellows 7 is applied to the range spring 6 through the connecting shaft 8. It is now being transmitted to
さらに、連結軸8には、前記レンジスプリング
6を挟んで対向するように移動電極10a,10
bが固定されている。これらの移動電極10a,
10bは、前記絶縁部材4a,4bの対向面に設
けられた固定電極11a,11bとともに、前記
レンジスプリング6の変位量を出力信号に変換す
るための静電容量式の変換機構12を構成してい
る。 Further, movable electrodes 10a and 10 are disposed on the connecting shaft 8 so as to face each other with the range spring 6 in between.
b is fixed. These moving electrodes 10a,
10b constitutes a capacitive conversion mechanism 12 for converting the displacement amount of the range spring 6 into an output signal, together with fixed electrodes 11a and 11b provided on the opposing surfaces of the insulating members 4a and 4b. There is.
また、本体1の壁部2a中央部には、貫通孔2
bが穿設されており、壁部2aの外面側には温度
補償用ダイアフラム13が、その周縁部で本体1
に固定されている。そして本体1の前記ベローズ
7及び温度補償用ダイアフラム13によつて閉塞
された空間には、封入流体が充填されている。 In addition, a through hole 2 is provided in the center of the wall 2a of the main body 1.
A temperature compensating diaphragm 13 is provided on the outer surface side of the wall portion 2a, and a temperature compensating diaphragm 13 is provided on the outer surface side of the wall portion 2a.
is fixed. The space closed by the bellows 7 and the temperature compensating diaphragm 13 of the main body 1 is filled with a sealed fluid.
上記の圧力伝送器は、測定に際してベローズ7
に被測定圧力が加えられると、ベローズ7の有効
受圧面積に応じて力が連結軸8に加わり、これに
伴つてレンジスプリング6が、上記連結軸8を介
して伝達される力に応じて変位を生じる。このレ
ンジスプリング6の変位量を固定電極11a,1
1bと移動電極10a,10bとの間の静電容量
に基いて検出し、被測定圧力に対応する信号を得
ることができる。 The above pressure transmitter uses a bellows 7 when measuring.
When a pressure to be measured is applied to the bellows 7, a force is applied to the connecting shaft 8 according to the effective pressure receiving area of the bellows 7, and the range spring 6 is accordingly displaced according to the force transmitted through the connecting shaft 8. occurs. The amount of displacement of this range spring 6 is determined by the fixed electrodes 11a, 1
1b and the moving electrodes 10a, 10b, it is possible to obtain a signal corresponding to the pressure to be measured.
ところで、従来のこの種の圧力伝送器は、温度
変化が生じて各構成要素に膨張(または収縮)が
起きた場合に、受圧要素としてのベローズ7とレ
ンジスプリング6との剛性の比に関係して、変換
機構12の移動電極10a,10bと固定電極1
1a,11bとの相対位置に温度依存性の変位を
生じ、出力のゼロ点変動を起こすという問題があ
つた。これは、ベローズ7の先端部7aと変換機
構12を構成する移動電極10a,10bとを連
結している連結軸8の熱膨張率の温度特性と、ベ
ローズ7及びこのベローズ7と変換機構12の固
定電極11a,11bとの間に介在する本体1や
絶縁部材4a等の部材の集合体の実効的な熱膨張
率の温度特性との間に差があることに起因するも
のである。この問題を解消するための対策とし
て、従来は電気的な処理によりゼロ点変動の温度
補償を行なつていた。しかるに、上記のような各
部材が異なつた材料(例えば本体1はSUS430、
ベローズ7はSUS316等)を用いて構成されてい
る場合の集合体の実効的な熱膨張特性は、温度変
化に対して線形の変化を示さず、複雑な特性を有
するため、これに対応し得る電気的な温度補償手
段がコスト高となるという新たな問題を生じてい
た。 By the way, in this type of conventional pressure transmitter, when expansion (or contraction) occurs in each component due to a temperature change, the rigidity ratio of the bellows 7 as a pressure receiving element and the range spring 6 is affected. The movable electrodes 10a, 10b and the fixed electrode 1 of the conversion mechanism 12
There was a problem in that a temperature-dependent displacement occurred in the relative position with respect to 1a and 11b, causing a zero point fluctuation of the output. This is due to the temperature characteristics of the thermal expansion coefficient of the connecting shaft 8 that connects the tip 7a of the bellows 7 and the moving electrodes 10a, 10b that constitute the conversion mechanism 12, and the temperature characteristics of the bellows 7 and the conversion mechanism 12. This is due to the fact that there is a difference between the temperature characteristics of the effective coefficient of thermal expansion of the assembly of members such as the main body 1 and the insulating member 4a interposed between the fixed electrodes 11a and 11b. Conventionally, as a measure to solve this problem, temperature compensation for zero point fluctuations has been performed by electrical processing. However, each member as mentioned above is made of different materials (for example, the main body 1 is made of SUS430,
When the bellows 7 is constructed using SUS316, etc., the effective thermal expansion characteristics of the assembly do not change linearly with temperature changes and have complex characteristics, so this can be accommodated. A new problem has arisen in that electrical temperature compensation means are expensive.
本発明は、上記事情に鑑みてなされたもので、
電気的な温度補償手段を必要とせずに温度変化に
よるゼロ点変動を防止できる圧力伝送器を提供す
ることを目的とするものである。 The present invention was made in view of the above circumstances, and
It is an object of the present invention to provide a pressure transmitter that can prevent zero point fluctuations due to temperature changes without requiring electrical temperature compensation means.
この目的を達成するために、本発明は、伝送器
本体の一側部に受圧要素を備えると共に本体の内
部に前記受圧要素の変位量を出力信号に変換する
ための変位変換機構が設けられ、少なくとも前記
受圧要素と変位変換機構との間で連結軸により連
結されてなる圧力伝送器において、前記連結軸を
2種以上の材料の組び合わせて構成し、もつて前
記連結軸の熱膨張率の温度特性と、前記変位変換
機構の本体に支持された部分と前記受圧要素との
間に介在する複数の部材の実効的な熱膨張率の温
度特性とを一致させ得るようにしたものである。 In order to achieve this object, the present invention includes a pressure receiving element on one side of a transmitter main body, and a displacement conversion mechanism for converting the amount of displacement of the pressure receiving element into an output signal inside the main body. In a pressure transmitter in which at least the pressure receiving element and the displacement conversion mechanism are connected by a connecting shaft, the connecting shaft is configured by a combination of two or more types of materials, and the thermal expansion coefficient of the connecting shaft is The temperature characteristics of the effective thermal expansion coefficients of the plurality of members interposed between the portion supported by the main body of the displacement conversion mechanism and the pressure receiving element can be matched. .
以下、本発明の一実施例を第1図ないし第3図
を参照して説明する。 Hereinafter, one embodiment of the present invention will be described with reference to FIGS. 1 to 3.
第2図は、本発明を第1図に示す圧力伝送器に
適用した場合の連結軸18の構成を示す断面図で
ある。この図に示す連結軸18は、円柱状の第1
の軸部材19と、円筒状の第2の軸部材20とを
異なつて材料により形成し、これら2個の軸部材
19,20を同軸的に嵌合し、その端面で溶接、
結合してなるものである。 FIG. 2 is a sectional view showing the configuration of the connecting shaft 18 when the present invention is applied to the pressure transmitter shown in FIG. 1. The connecting shaft 18 shown in this figure is a cylindrical first
The shaft member 19 and the cylindrical second shaft member 20 are made of different materials, these two shaft members 19 and 20 are coaxially fitted, and their end faces are welded.
It is made by combining.
この場合、第1の軸部材19は、SuS316;熱
膨張率16×10-6/℃(以下、材料Aと称す)を用
いて形成され、一方、第2の軸部材20は、Ni
−SPAN C;熱膨張率8×10-6/℃(以下、材
料Bと称す)を用いて形成されている。また、本
体1はSuS316(熱膨張率;16×10-6/℃)固定電
極部分4a,4bはセラミツク(8×10-6/℃)、
支持リング5a,5b、移動電極10a,10b
は、Ni−SPAN C(8×10-6/℃)により形成
されている。 In this case, the first shaft member 19 is made of SuS316 with a coefficient of thermal expansion of 16×10 -6 /°C (hereinafter referred to as material A), while the second shaft member 20 is made of Ni
-SPAN C: Formed using a thermal expansion coefficient of 8×10 −6 /° C. (hereinafter referred to as material B). In addition, the main body 1 is made of SuS316 (thermal expansion coefficient: 16×10 -6 /℃), and the fixed electrode parts 4a and 4b are made of ceramic (8×10 -6 /℃),
Support rings 5a, 5b, moving electrodes 10a, 10b
is formed of Ni-SPAN C (8×10 −6 /° C.).
上記のように2種以上の異なつた材料からなる
軸部材19,20を結合して構成された連結軸1
8は、その熱膨張特性が各軸部材19,20の線
膨張率と、弾性定数と、結合に際してその初期残
留応力の与え方とによつて決まる。上記弾性定数
は、各軸部材19,20の材料及び寸法を考慮し
て設定することができ、また初期残留応力は2個
の軸部材19,20を結合(溶接等による)する
際に任意に与えることができる。 A connecting shaft 1 constructed by joining shaft members 19 and 20 made of two or more different materials as described above.
8, its thermal expansion characteristics are determined by the coefficient of linear expansion and elastic constant of each shaft member 19, 20, and how initial residual stress is applied upon connection. The above elastic constant can be set in consideration of the material and dimensions of each shaft member 19, 20, and the initial residual stress can be set arbitrarily when joining the two shaft members 19, 20 (by welding, etc.). can give.
今、基準温度における連結軸8の長さをlとす
る(したがつて基準温度ではベローズ先端部7a
と移動電極10a間の距離もlとなる。)。温度が
Δtだけ上昇すると、本体1、ベローズ部7,7
aと固定電極4b、支持リング5b、移動電極1
0aの熱膨張によつて、ベローズ先端部7aと移
動電極10a間の距離はl′となる。一方連結軸8
は、その熱膨張率をαとすると、
(1+αΔt)lの長さになる。 Now, assume that the length of the connecting shaft 8 at the reference temperature is l (therefore, at the reference temperature, the bellows tip 7a
The distance between the moving electrode 10a and the moving electrode 10a is also l. ). When the temperature increases by Δt, the main body 1 and the bellows parts 7, 7
a, fixed electrode 4b, support ring 5b, and moving electrode 1
Due to the thermal expansion of 0a, the distance between the bellows tip 7a and the moving electrode 10a becomes l'. One connection shaft 8
has a length of (1+αΔt)l, where α is the coefficient of thermal expansion.
したがつてその差はΔl=l′−(1+αΔt)lとな
り
δ=K1/K1+K2Δl ………(1)
の長さだけ移動電極が移動し、出力誤差となつて
表われる。ここで、K1:ベローズ7のバネ定数、
K2:レンジスプリングのバネ定数である。 Therefore, the difference is Δl=l'-(1+αΔt)l, and the movable electrode moves by a length of δ=K 1 /K 1 +K 2 Δl (1), which appears as an output error. Here, K 1 : Spring constant of bellows 7,
K 2 : Spring constant of range spring.
δ=0として出力誤差を0とするにはΔl=0
すなわち、
α=l′−l/lΔt ………(2)
なる熱膨張率をもつ連結軸材質を選ぶ必要があ
る。 To set the output error to 0 with δ=0, Δl=0
In other words, it is necessary to select a material for the connecting shaft that has a coefficient of thermal expansion of α=l'-l/lΔt (2).
次に具体例を述べる。温度変化後のベローズ先
端部7a、移動電極10aの間の距離l′は、本体
および各部品の寸法と熱膨張率によつてきまる
が、今仮にl=20mm、l′=20.013mmであつたとす
ると、この状態で出力の温度変動を0にするため
には(2)式より、
α=l′−l/lΔt=20.013−20/20×50=13×10-6m
m/mm℃
(ただし温度変化Δt=50℃の場合)
したがつて、lが設計上変更できないとすると
この例では13×10-6mm/mm℃の熱膨張率をもつ材
料の選択が必要となる。 Next, a specific example will be described. The distance l' between the bellows tip 7a and the moving electrode 10a after the temperature change depends on the dimensions and coefficient of thermal expansion of the main body and each component, but if l = 20 mm and l' = 20.013 mm. Assuming that, in order to make the output temperature fluctuation zero in this state, from equation (2), α=l'-l/lΔt=20.013-20/20×50=13×10 -6 m
m/mm℃ (However, when temperature change Δt=50℃) Therefore, if l cannot be changed due to design, in this example it is necessary to select a material with a coefficient of thermal expansion of 13×10 -6 mm/mm℃. becomes.
しかし、加工性、強度、腐食性を考慮すると、
上記熱膨張率をもつ材料の選択ができない場合以
下の様にして、本発明を利用することができる。 However, considering workability, strength, and corrosivity,
If it is not possible to select a material having the above coefficient of thermal expansion, the present invention can be utilized in the following manner.
本発明による連結軸18の第1の軸部材19と
してSuS316(熱膨張率16×10-6mm/mm℃)第2の
軸部材20として、Ni−SPAN C(熱膨張率8
×10-6mm/mm℃)を選んだとする。各軸部材1
9,20の基準温度での長さを共に20mmとする
と、温度Δt=50℃の変化があつたときの第1の
軸部材19の長さl1、第2の軸部材20の長さl2
はそれぞれ、
l1=20×(1+16×10-6×50)=20.016
l2=20×(1+6×10-6×50)=20.006
の様になるはずであるが、今は両者は溶接等によ
り結合されているから、軸部材19としての、温
度変化(50℃)後の長さl′は
l′=l2+K20/K19+K20(l1−l2)
となる。ここで、K19:第1の部材のバネ定数、
K20:第2の部材のバネ定数である。 The first shaft member 19 of the connecting shaft 18 according to the present invention is SuS316 (coefficient of thermal expansion 16×10 -6 mm/mm°C), and the second shaft member 20 is Ni-SPAN C (coefficient of thermal expansion 8
×10 -6 mm/mm℃). Each shaft member 1
If the lengths of 9 and 20 at the reference temperature are both 20 mm, then the length l 1 of the first shaft member 19 and the length l of the second shaft member 20 when the temperature changes by Δt=50°C. 2
should be as follows: l 1 = 20 × (1 + 16 × 10 -6 × 50) = 20.016 l 2 = 20 × (1 + 6 × 10 -6 × 50) = 20.006, but currently both are welded etc. Therefore, the length l' of the shaft member 19 after the temperature change (50° C.) is l'=l 2 +K 20 /K 19 +K 20 (l 1 −l 2 ). Here, K 19 : Spring constant of the first member,
K 20 : Spring constant of the second member.
このときの連結軸18としての熱膨張率α18は、
α18=l′−l/lΔt
と表わせ、α18=13×16-6mm/mm℃を得るために
は、
13×10-6=l′−20/20×50より
l′=l20+K20/K19+K20(l1−l2)=20.013
を満たす様なK19、K20を決め必要がある。 At this time, the coefficient of thermal expansion α 18 for the connecting shaft 18 is expressed as α 18 = l′−l/lΔt, and in order to obtain α 18 = 13×16 −6 mm/mm°C, it is 13×10 −6 From =l'-20/20x50, it is necessary to determine K19 and K20 that satisfy l'= l20 + K20 / K19 + K20 ( l1 - l2 )=20.013.
すなわち、
K20/K19+K20=0.7 ………(3)
ここで、第1、第2の軸部材19,20のヤン
グ率が等しいものとするとK19、K20はそれぞれ
K19=A19/lE、K20=A20/lE ………(4)
(ここでA19、A20はそれぞれ第1、第2の軸部
材断面積である。)
(4)を(3)に代入すると、
A20/A19+A20=0.7 ………(5)
ここで設計上A19+A20=100mm2に限定されてい
ると、
A20=70mm2
A19=30mm2
となる。すなわち以上の様な条件(基準温度での
長さl=20mm、ヤング率は等しい、第1軸部材は
SuS316、第2軸部材はNi−SPAN C)において
熱膨張率13×10-6mm/mm℃の軸部材18を作るた
めには、第1の軸部材19の断面積と第2の軸部
材20の断面積との比は3:7にすればよい。 That is, K 20 /K 19 +K 20 = 0.7 (3) Here, assuming that the Young's moduli of the first and second shaft members 19 and 20 are equal, K 19 and K 20 are respectively K 19 = A 19 /lE, K 20 = A 20 /lE ......(4) (Here, A 19 and A 20 are the cross-sectional areas of the first and second shaft members, respectively.) Substitute (4) into (3) Then, A 20 /A 19 +A 20 = 0.7 (5) If A 19 + A 20 = 100 mm 2 due to design, A 20 = 70 mm 2 A 19 = 30 mm 2 . In other words, under the above conditions (length l = 20 mm at reference temperature, Young's modulus is equal, first shaft member is
SuS316, the second shaft member is Ni-SPAN C) In order to make the shaft member 18 with a thermal expansion coefficient of 13 × 10 -6 mm/mm°C, the cross-sectional area of the first shaft member 19 and the second shaft member The ratio to the cross-sectional area of 20 may be 3:7.
第3図は、上記の連結軸18と材料A及び材料
Bとの熱膨張特性を測定した結果を示すグラフ
で、横軸に温度変化を、また縦軸に膨張量をとつ
てある。この図には、連結軸18の熱膨張特性を
実線で材料Aの熱膨張特性を一点鎖線で、また材
料Bの熱膨張特性を破線で示した。なお、図示し
ないが、固定電極11aを支持する絶縁部材4a
−本体1−ベローズ7からなる系についての熱膨
張特性を測定した結果、上記連結軸18の特性と
近似的に等しい特性を得た。この図から分かるよ
うに、連結軸18は、材料Aと材料Bとの中間的
な熱膨張率を有し、更に温度変化量が大きい場合
に非線形的な熱膨張特性を示す。前述したよう
に、この熱膨張特性は、材料の選択、寸法の設
定、初期残留応力の与え方により任意に設定でき
るため、伝送器の本体1や絶縁部材4a,4b等
の複数の部材からなる部分の熱膨張特性に一致さ
せることが可能である。 FIG. 3 is a graph showing the results of measuring the thermal expansion characteristics of the connecting shaft 18 and materials A and B, in which the horizontal axis represents the temperature change and the vertical axis represents the amount of expansion. In this figure, the thermal expansion characteristics of the connecting shaft 18 are shown by a solid line, the thermal expansion characteristics of material A are shown by a dashed line, and the thermal expansion characteristics of material B are shown by a broken line. Although not shown, an insulating member 4a that supports the fixed electrode 11a
- As a result of measuring the thermal expansion characteristics of the system consisting of the main body 1 and the bellows 7, characteristics approximately equal to those of the connecting shaft 18 were obtained. As can be seen from this figure, the connecting shaft 18 has a coefficient of thermal expansion intermediate between that of material A and material B, and exhibits nonlinear thermal expansion characteristics when the amount of temperature change is large. As mentioned above, this thermal expansion characteristic can be set arbitrarily by selecting materials, setting dimensions, and applying initial residual stress. It is possible to match the thermal expansion properties of the part.
上記のような連結軸18の熱膨張特性を適宜設
定した圧力伝送器によれば、受圧要素としてのベ
ローズ7と変位変換機構12の移動電極10a,
10bの中央部との間を連結する連結軸18の熱
膨張特性と、ベローズ7及びこのベローズ7と固
定電極11a,11bとの間に介在する部材(本
体1、絶縁部材4a等)の実効的な熱膨張特性と
を一致させることができるため、温度変動が生じ
た場合にも、レンジスプリング6が無用な変位を
起こさず、従つてゼロ点変動を生じることがな
い。 According to the pressure transmitter in which the thermal expansion characteristics of the connecting shaft 18 are appropriately set as described above, the bellows 7 as a pressure receiving element, the movable electrode 10a of the displacement conversion mechanism 12,
Thermal expansion characteristics of the connecting shaft 18 that connects the center part of the bellows 7 and the fixed electrodes 11a, 11b (main body 1, insulating member 4a, etc.) Since the range spring 6 can be made to match the thermal expansion characteristics, even if temperature fluctuation occurs, the range spring 6 will not undergo unnecessary displacement, and therefore zero point fluctuation will not occur.
なお、本発明は、上記実施例に示した連結軸の
構成に限定されるものではなく、第4図に示すよ
うに複数の軸部材22,23,24を軸線方向に
並列的及び直列的に適宜結合して連結軸25を構
成してもよく、各軸部材の材料、寸法等は、目的
に応じて適宜選択することができる。また、レン
ジスプリングの変位量を出力信号に変換する機構
は、上記静電容量式に限らず、可変インダクタン
ス式や歪ゲージ式等のものを適用することもでき
る。 Note that the present invention is not limited to the configuration of the connecting shaft shown in the above embodiment, and as shown in FIG. The connecting shaft 25 may be constructed by combining them as appropriate, and the material, dimensions, etc. of each shaft member can be appropriately selected depending on the purpose. Further, the mechanism for converting the displacement amount of the range spring into an output signal is not limited to the above-mentioned capacitance type, but a variable inductance type, a strain gauge type, etc. can also be applied.
以上の説明から明らかなように、本発明は、圧
力伝送器の受圧要素とレンジスプリングとを連結
する連結軸を2種以上の材料を結合して構成し、
この連結軸の熱膨張特性を適切に設定することに
より圧力伝送器の温度変動に伴うゼロ点変動を解
消したものであるから、従来のような高価な電気
的温度補償手段を必要としないため、温度特性の
優れた圧力伝送器を低価格で提供できるという効
果を有する。 As is clear from the above description, the present invention has a connecting shaft that connects a pressure receiving element of a pressure transmitter and a range spring by combining two or more types of materials,
By appropriately setting the thermal expansion characteristics of this connecting shaft, zero point fluctuations caused by temperature fluctuations in the pressure transmitter are eliminated, so there is no need for expensive electrical temperature compensation means as in the past. This has the effect of providing a pressure transmitter with excellent temperature characteristics at a low price.
第1図は、本発明を適用する圧力伝送器の一例
を示す断面図、第2図は、本発明の一実施例とし
ての連結軸の断面図、第3図は第2図に示す連結
軸の熱膨張特性を説明するためのグラフ、第4図
は、本発明の変形例を示すための連結軸の断面図
である。
1……本体、6……レンジスプリング、7……
ベローズ(受圧要素)、12……変位変換機構、
18,25……連結軸、19……第1の軸部材、
20……第2の軸部材、22,23,24……軸
部材。
Fig. 1 is a sectional view showing an example of a pressure transmitter to which the present invention is applied, Fig. 2 is a sectional view of a connecting shaft as an embodiment of the present invention, and Fig. 3 is a sectional view of the connecting shaft shown in Fig. 2. FIG. 4 is a cross-sectional view of a connecting shaft showing a modification of the present invention. 1... Body, 6... Range spring, 7...
Bellows (pressure receiving element), 12...displacement conversion mechanism,
18, 25... Connection shaft, 19... First shaft member,
20... Second shaft member, 22, 23, 24... Shaft member.
Claims (1)
に、前記本体の内部に前記受圧要素の変位量を出
力信号に変換するための変位変換機構が設けら
れ、前記受圧要素と前記変位変換機構との間が連
結軸により連結されてなる圧力伝送器において、
前記連結軸が、異なる材料からなる少なくとも2
種類の軸部材を積層すると共に、これらの軸部材
の長さ方向の両端部を一体に連結して構成されて
いることを特徴とする圧力伝送器。1. A pressure receiving element is provided on one side of the transmitter main body, and a displacement conversion mechanism for converting the amount of displacement of the pressure receiving element into an output signal is provided inside the main body, and the pressure receiving element and the displacement conversion mechanism are In a pressure transmitter that is connected by a connecting shaft,
The connecting shaft is made of at least two different materials.
A pressure transmitter characterized in that it is constructed by laminating different types of shaft members and integrally connecting both longitudinal ends of these shaft members.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18236382A JPS5972034A (en) | 1982-10-18 | 1982-10-18 | Pressure transmitter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18236382A JPS5972034A (en) | 1982-10-18 | 1982-10-18 | Pressure transmitter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5972034A JPS5972034A (en) | 1984-04-23 |
| JPH029702B2 true JPH029702B2 (en) | 1990-03-05 |
Family
ID=16116998
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18236382A Granted JPS5972034A (en) | 1982-10-18 | 1982-10-18 | Pressure transmitter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5972034A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0528395U (en) * | 1991-09-26 | 1993-04-16 | 有限会社タスクフオ−ス | Doll running toy |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57151545U (en) * | 1981-03-19 | 1982-09-22 |
-
1982
- 1982-10-18 JP JP18236382A patent/JPS5972034A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5972034A (en) | 1984-04-23 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| FI72809C (en) | Capacitive pressure sensor with insulated sensory membrane. | |
| US6205861B1 (en) | Transducer having temperature compensation | |
| US4670733A (en) | Differential pressure transducer | |
| KR950013299B1 (en) | Pressure transducer | |
| US4878385A (en) | Differential pressure sensing apparatus | |
| JPH0230450B2 (en) | ||
| US3168718A (en) | Electric pressure transducer | |
| US3047022A (en) | Pressure responsive device | |
| US4306460A (en) | Differential pressure transducer | |
| US3290945A (en) | Differential pressure responsive device | |
| JPH029702B2 (en) | ||
| JPH0528770B2 (en) | ||
| US4680972A (en) | Pressure transducer | |
| US3271720A (en) | Corrector or pressure-sensitive diaphragm or capsule | |
| US4520675A (en) | Pressure or pressure difference measuring transducer | |
| EP0775303B1 (en) | Very high pressure gauge with plate shaped Bourdon element | |
| JP2546013B2 (en) | Capacitive differential pressure detector | |
| JPS601402Y2 (en) | Capacitive differential pressure transmitter | |
| JPS6261897B2 (en) | ||
| IE55965B1 (en) | Pressure transducer | |
| US3765256A (en) | Low range high overload differential pressure transducer | |
| JPS604118Y2 (en) | Pipe pressure sensor | |
| SU1068388A1 (en) | Pressure transducer | |
| JPS5850300Y2 (en) | pressure transmitter | |
| JPS6140054B2 (en) |