JPH0666828A - Vibration type acceleration meter - Google Patents
Vibration type acceleration meterInfo
- Publication number
- JPH0666828A JPH0666828A JP4216832A JP21683292A JPH0666828A JP H0666828 A JPH0666828 A JP H0666828A JP 4216832 A JP4216832 A JP 4216832A JP 21683292 A JP21683292 A JP 21683292A JP H0666828 A JPH0666828 A JP H0666828A
- Authority
- JP
- Japan
- Prior art keywords
- vibrator
- pendulum
- support
- frame
- fixed
- 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.)
- Withdrawn
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01P—MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
- G01P15/00—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration
- G01P15/02—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses
- G01P15/08—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values
- G01P2015/0805—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration
- G01P2015/0822—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration for defining out-of-plane movement of the mass
- G01P2015/0825—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration for defining out-of-plane movement of the mass for one single degree of freedom of movement of the mass
- G01P2015/0828—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration for defining out-of-plane movement of the mass for one single degree of freedom of movement of the mass the mass being of the paddle type being suspended at one of its longitudinal ends
Landscapes
- Gyroscopes (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】この発明は振動子を検出手段とし
て用いる振動式加速度計に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a vibration type accelerometer using a vibrator as a detecting means.
【0002】[0002]
【従来の技術】従来のこの種の振動式加速度計10の構
成を図3に示す。板状の振子11の板面方向の外周に枠
体12が配され、振子11の一端がヒンジ13を介して
枠体12に連結される。これら振子11、枠体12及び
ヒンジ13は例えば板状体から一体に形成され、ヒンジ
13はその厚さが薄くされて弾性変形可能とされる。ヒ
ンジ13がその枠体12との連結面を固定端としてたわ
むことにより、その固定端の幅方向と平行なヒンジ13
の軸心を回動軸14として、振子11はヒンジ13の回
りに回動可能とされている。2. Description of the Related Art The structure of a conventional vibration type accelerometer 10 of this type is shown in FIG. A frame body 12 is arranged on the outer periphery of the plate-like pendulum 11 in the plate surface direction, and one end of the pendulum 11 is connected to the frame body 12 via a hinge 13. The pendulum 11, the frame 12 and the hinge 13 are integrally formed of, for example, a plate-like body, and the hinge 13 has a reduced thickness and is elastically deformable. The hinge 13 bends with its connecting surface with the frame 12 as a fixed end, so that the hinge 13 parallel to the width direction of the fixed end.
The pendulum 11 is rotatable around the hinge 13 with the axis center of the as the rotation axis 14.
【0003】長手方向の両端がそれぞれやや幅広とされ
た略短冊状の振動子15の長手方向の一端15aが振子
11の板面11aのほぼ中央部にスペーサ16を介して
固定され、他端15bが、振子11が連結された側の枠
体12に同様にスペーサ17を介して固定される。振動
子15はこれらスペーサ16,17により振子11の板
面11aと所定量離間され、その板面11aとほぼ平行
に配設される。なお、振動子15は例えば水晶振動子が
用いられ、加速度検出時には励振手段(図示せず)によ
り固有振動数で励振される。One end 15a in the longitudinal direction of a substantially strip-shaped vibrator 15 whose both ends in the longitudinal direction are made slightly wider is fixed to approximately the center of the plate surface 11a of the pendulum 11 via a spacer 16 and the other end 15b. Is similarly fixed to the frame body 12 on the side to which the pendulum 11 is connected via a spacer 17. The vibrator 15 is separated from the plate surface 11a of the pendulum 11 by a predetermined amount by the spacers 16 and 17, and is arranged substantially parallel to the plate surface 11a. A crystal oscillator, for example, is used as the oscillator 15, and is excited at a natural frequency by an excitation unit (not shown) when acceleration is detected.
【0004】次に、加速度の検出方法を説明する。今、
例えば振子11を支持している枠体12に、振子11の
板面11aと垂直な方向に図3(B)に矢印で示したよ
うに加速度αが加わると、振子11は加速度αと逆方向
に加速度αに比例する大きさの慣性力を受け、回動軸1
4を中心として図中時計方向に回動する。この振子11
の回動により、振子11に一端15aが固定されている
振動子15は引張力を受け、振動子15の固有振動数が
上昇する。従って、固有振動数の変化の大きさ及び方向
を振動数検出手段(図示せず)で検出することにより、
入力加速度αの大きさ及び方向が検知される。Next, a method of detecting acceleration will be described. now,
For example, when acceleration α is applied to the frame body 12 supporting the pendulum 11 in a direction perpendicular to the plate surface 11a of the pendulum 11 as indicated by an arrow in FIG. 3B, the pendulum 11 moves in the direction opposite to the acceleration α. Receives an inertial force of a magnitude proportional to the acceleration α,
It rotates in the clockwise direction in FIG. This pendulum 11
Due to the rotation, the vibrator 15 whose one end 15a is fixed to the pendulum 11 receives a tensile force, and the natural frequency of the vibrator 15 increases. Therefore, by detecting the magnitude and direction of the change in the natural frequency by the frequency detection means (not shown),
The magnitude and direction of the input acceleration α is detected.
【0005】[0005]
【発明が解決しようとする課題】ところで、振子11、
枠体12及びヒンジ13の組立体を小型かつ簡易に形成
し、さらにそれらの良好な連結状態を得るためには、前
述したようにそれらを同一材で一体形成するのが好まし
く、その材料としてヒンジ13の良好なバネ特性及び機
械的強度さらに優れた加工精度が得られる点から石英板
が使用される。By the way, the pendulum 11,
In order to form the assembly of the frame 12 and the hinge 13 in a small size and easily, and to obtain a good connection state between them, it is preferable to integrally form them with the same material as described above. A quartz plate is used because it has good spring characteristics and mechanical strength of No. 13, and excellent processing accuracy.
【0006】しかしながら、石英の熱膨張係数は0.5
ppm/℃で、振動子15に使用される水晶の熱膨張係
数13.7ppm/℃と比較してかなり小さいため、環
境温度が変化すると、これら熱膨張係数の差により振動
子15と振子11及び枠体12との間において熱応力が
発生し、それによって振動子15が破断したり、あるい
は振動子15と振子11及び枠体12との各固定部にお
いてはがれが発生したりして加速度計が壊れるという問
題が生じていた。However, the coefficient of thermal expansion of quartz is 0.5.
Since ppm / ° C is considerably smaller than the thermal expansion coefficient of 13.7 ppm / ° C of the crystal used for the vibrator 15, when the environmental temperature changes, the difference between the thermal expansion coefficients causes the vibrator 15 and the pendulum 11 and Thermal stress is generated between the accelerometer and the frame body 12, which causes the vibrator 15 to break or peel off at the fixing portions of the vibrator 15 and the pendulum 11 and the frame body 12. There was a problem of breaking.
【0007】この発明の目的は上述した問題を解決し、
環境温度が変化しても振動子の長手方向に熱応力がほと
んど発生せず、従って環境温度の変化によって壊れるこ
とのない振動式加速度計を提供することにある。The object of the present invention is to solve the above mentioned problems,
It is an object of the present invention to provide a vibrating accelerometer in which thermal stress is hardly generated in the longitudinal direction of the vibrator even if the environmental temperature changes, and therefore the vibrator does not break due to the environmental temperature change.
【0008】[0008]
【課題を解決するための手段】この発明は振子と、その
振子の外周に配され、振子の一端とヒンジ結合され、か
つ振子と同一材で一体に形成された枠体と、振子に一端
が固定され、他端が枠体の振子が連結された側に延長さ
れた振動子と、その振動子と熱膨張係数がほぼ等しい材
料からなり、上記振動子の他端が一端に固定され、他端
が振動子の上記一端と対応した位置で枠体の両側に固定
された支持体とを具備するものである。According to the present invention, there is provided a pendulum, a frame body arranged on the outer periphery of the pendulum, hinged to one end of the pendulum, and integrally formed with the same material as the pendulum, and one end of the pendulum. The vibrator is fixed and has the other end extended to the side of the frame to which the pendulum is connected, and a vibrator made of a material having a thermal expansion coefficient substantially equal to that of the vibrator. The support is fixed to both sides of the frame at positions corresponding to the ends of the vibrator.
【0009】さらに、上記振動子を枠体と支持体との間
に位置させるものである。Further, the vibrator is located between the frame and the support.
【0010】[0010]
【作用】上記のように構成されたこの発明では、環境温
度の変化による振動子の長手方向の伸縮量とその方向に
おける支持体の伸縮量とはほぼ等しいため、振動子の長
手方向において熱応力はほとんど発生しない。In the present invention configured as described above, since the amount of expansion and contraction of the vibrator in the longitudinal direction due to the change in environmental temperature and the amount of expansion and contraction of the support in that direction are substantially equal, thermal stress is generated in the longitudinal direction of the vibrator. Rarely occurs.
【0011】[0011]
【実施例】この発明の一実施例を図1に示す。矩形板状
の振子21の板面方向の外周に矩形状の枠体22が配さ
れ、振子21の一端が弾性変形可能とされたヒンジ23
を介して枠体22に連結される。これら振子21、枠体
22及びヒンジ23は同一材で一体に形成され、この例
においては材料として石英が使用される。即ち、石英製
の薄板に例えばレーザカットによりコ字状の穴24をあ
けて枠体22と、枠体22にそのコ字の開口部で支持さ
れる切片25とを形成し、化学エッチングによりその切
片25の支持端近傍の厚さを支持端に平行に薄くするこ
とによって、弾性変形するヒンジ23を形成する。ヒン
ジ23で分割された切片25の遊端側(支持端と反対
側)の部分が振子21となり、他方支持端側の部分は枠
体22の延長部となる。FIG. 1 shows an embodiment of the present invention. A hinge 23 in which a rectangular frame body 22 is arranged on the outer periphery in the plate surface direction of a rectangular plate-like pendulum 21 and one end of the pendulum 21 is elastically deformable.
It is connected to the frame body 22 via. The pendulum 21, the frame body 22, and the hinge 23 are integrally formed of the same material, and in this example, quartz is used as the material. That is, for example, a U-shaped hole 24 is formed in a thin quartz plate by laser cutting to form a frame body 22 and a section 25 supported by the U-shaped opening portion in the frame body 22 and chemically etched to form the section 25. By thinning the thickness of the section 25 near the support end in parallel with the support end, the hinge 23 that elastically deforms is formed. The free end side (opposite side to the support end) of the segment 25 divided by the hinge 23 serves as the pendulum 21, and the other support end side portion serves as an extension of the frame 22.
【0012】振子21の板面21aのほぼ中央部に略短
冊状の振動子15の長手方向の一端15aが直方体状の
スペーサ26を介して接着により固定される。振動子1
5には水晶振動子が使用される。振動子15の他端15
bは枠体22の振子21が連結された側に位置され、振
動子15と枠体22との間に配設される支持体27に接
着により固定される。One end 15a of the substantially rectangular vibrator 15 in the longitudinal direction is fixed by adhesion through a spacer 26 in the shape of a rectangular parallelepiped to approximately the center of the plate surface 21a of the pendulum 21. Oscillator 1
A crystal oscillator is used for 5. The other end 15 of the oscillator 15
b is located on the side of the frame body 22 to which the pendulum 21 is connected, and is fixed to the support body 27 arranged between the vibrator 15 and the frame body 22 by adhesion.
【0013】支持体27はT字の垂直部が幅広とされて
その垂直部にT字の水平部から凹溝が形成された形状の
板面27aを有し、その板面27aと垂直方向の寸法、
つまり支持体27の厚さは、T字の水平部の両端におい
て、振子21の板面21aと振動子15の一端15aと
の間隔、即ちスペーサ26の厚さとそれぞれ等しくさ
れ、他の部分はスペーサ26の厚さより小とされる。The support 27 has a plate surface 27a having a shape in which a vertical portion of the T-shape is widened and a groove is formed in the vertical portion from the horizontal portion of the T-shape. Size,
That is, the thickness of the support body 27 is equal to the distance between the plate surface 21a of the pendulum 21 and the one end 15a of the vibrator 15, that is, the thickness of the spacer 26 at both ends of the T-shaped horizontal portion, and the other portions are spacers. It is smaller than the thickness of 26.
【0014】支持体27はそのT字の垂直部の先端28
aが枠体22の振子21が連結された側に位置されて振
動子15の他端15bと接着固定され、他方厚さが大と
された両端部28b,28cが振動子15の一端15a
と対応した位置で、振子21の両側に位置する枠体22
にそれぞれ接着固定される。従って、支持体27はこれ
ら両端部28b,28c以外では、振子21及び枠体2
2と所定量離間されてほぼ平行対向した状態とされる。The support 27 has a tip 28 of the vertical portion of the T-shape.
a is located on the side of the frame 22 to which the pendulum 21 is connected and is fixedly adhered to the other end 15b of the vibrator 15, while the other end portions 28b and 28c having a large thickness have one end 15a of the vibrator 15.
The frame bodies 22 located on both sides of the pendulum 21 at positions corresponding to
Each is fixed by adhesion. Therefore, the support body 27 has the pendulum 21 and the frame body 2 except for the both end portions 28b and 28c.
2 is separated by a predetermined amount and is in a state of being substantially parallel and opposed.
【0015】なお、振動子15の一端15aが固定され
ているスペーサ26は支持体27のT字の垂直部に形成
されている凹溝29内に位置され、振動子15はその凹
溝29のほぼ中心上に位置される。上述したように、振
動子15と枠体22との間に配され、振動子15の他端
15bが一端に固定され、他端が振動子15の一端15
aと対応した位置で枠体22の両側に固定される支持体
27は、振動子15と熱膨張係数がほぼ等しい材料によ
り形成される。この例では振動子15に水晶振動子(熱
膨張係数=13.7ppm/℃)を用いているため、支
持体27には例えば熱膨張係数が13.7ppm/℃で
水晶と等しい値をもつモネル金属が使用される。The spacer 26, to which one end 15a of the vibrator 15 is fixed, is positioned in a groove 29 formed in the vertical portion of the T-shape of the support 27, and the vibrator 15 has a groove 29 of the groove 29. It is located almost on the center. As described above, it is arranged between the vibrator 15 and the frame body 22, the other end 15b of the vibrator 15 is fixed to one end, and the other end is the one end 15 of the vibrator 15.
The support bodies 27 fixed to both sides of the frame body 22 at positions corresponding to a are made of a material having a thermal expansion coefficient substantially equal to that of the vibrator 15. In this example, since a crystal oscillator (coefficient of thermal expansion = 13.7 ppm / ° C.) is used for the oscillator 15, the support 27 has, for example, a monel having a coefficient of thermal expansion of 13.7 ppm / ° C. and a value equal to that of crystal. Metal is used.
【0016】上記のように構成された振動式加速度計3
0における加速度の検出は、図3に示した従来の振動式
加速度計10と同様にして行われる。即ち、枠体22に
図1(B)に矢印で示す加速度αが加わると、振子21
は慣性力を受け、ヒンジ23がたわんで振子21はヒン
ジ23の回りに図中時計回り方向に回動する。励振手段
(図示せず)により励振されている振動子15は振子2
1により引張力を受け、振動子15の固有振動数が上昇
する。従って、固有振動数の変化の大きさ及び方向を振
動数検出手段(図示せず)で検出することにより、入力
加速度αの大きさ及び方向を検知することができる。The vibration type accelerometer 3 constructed as described above.
The detection of the acceleration at 0 is performed in the same manner as the conventional vibration type accelerometer 10 shown in FIG. That is, when the acceleration α indicated by the arrow in FIG.
Receives an inertial force, the hinge 23 bends, and the pendulum 21 rotates around the hinge 23 in the clockwise direction in the drawing. The vibrator 15 excited by the exciting means (not shown) is the pendulum 2.
1, the tensile force is received, and the natural frequency of the vibrator 15 increases. Therefore, the magnitude and direction of the input acceleration α can be detected by detecting the magnitude and direction of the change in natural frequency with the frequency detection means (not shown).
【0017】次に、この振動式加速度計30における環
境温度の変化の影響について説明する。前述したよう
に、熱膨張係数がほぼ等しい材料からなる振動子15と
支持体27とは、それぞれその端部15aと28b,2
8cとが同一材で一体形成されている振子21と枠体2
2とに振動子15の長手方向における同一位置で固定さ
れ、さらにそれぞれ同一方向に延長されて他方の端部1
5bと28aとが互いに固定されている。従って、環境
温度が変化してもそれら端部15a及び28b,28c
は常に振動子15の長手方向において同一位置に位置
し、かつ振動子15の長手方向の伸縮量とその方向にお
ける支持体27の伸縮量とはほぼ等しいため、振動子1
5の長手方向においてこれら振動子15と支持体27と
の間及びそれらと振子21あるいは枠体22との間には
熱応力はほとんど発生しない。Next, the influence of the change in environmental temperature on the vibration type accelerometer 30 will be described. As described above, the vibrator 15 and the support 27, which are made of materials having substantially the same coefficient of thermal expansion, have their ends 15a, 28b and 2 respectively.
8c and pendulum 21 and frame 2 integrally formed of the same material
2 and 2 are fixed at the same position in the longitudinal direction of the vibrator 15 and are further extended in the same direction to form the other end 1
5b and 28a are fixed to each other. Therefore, even if the environmental temperature changes, these end portions 15a and 28b, 28c
Is always located at the same position in the longitudinal direction of the vibrator 15, and the amount of expansion and contraction of the vibrator 15 in the longitudinal direction is substantially equal to the amount of expansion and contraction of the support 27 in that direction.
In the longitudinal direction of 5, the thermal stress hardly occurs between the vibrator 15 and the support 27 and between them and the pendulum 21 or the frame 22.
【0018】図2はこの発明の他の実施例を示したもの
であり、この例においては振動子15は枠体22と支持
体27との間に位置される。つまり、振動子15の一端
15aと振子21との間に配されるスペーサ26はその
厚さが薄くされ、図2(B)に示すように振動子15は
振子21及び枠体22に近接して平行対向される。振動
子15の他端15bは支持体27の枠体22と対向する
側の板面27bにおいて、そのT字の垂直部の先端に一
体に突出形成された取付部28dに固定される。FIG. 2 shows another embodiment of the present invention, in which the vibrator 15 is located between the frame 22 and the support 27. That is, the spacer 26 disposed between the one end 15a of the vibrator 15 and the pendulum 21 has a small thickness, and the vibrator 15 is close to the pendulum 21 and the frame body 22 as shown in FIG. Parallel to each other. The other end 15b of the vibrator 15 is fixed to a mounting portion 28d integrally formed on the tip of the vertical portion of the T-shape on the plate surface 27b of the support 27 facing the frame body 22.
【0019】支持体27の板面27bからの、T字の水
平部の両端部28b,28cの突出高さは、振子21の
板面21aに対する振動子15の上面15cの高さより
大とされて、振動子15と支持体27との互いに対向面
15cと27bとは所定量離間され、この離間量と等し
い高さで取付部28dは板面27bに対して突出形成さ
れている。なお、この実施例において支持体27の振動
子15の一端15aと対向する部分に形成されている凹
溝29は、振動子15に励振手段及び振動数検出手段か
らの配線を接続するための逃げである。The protruding heights of both end portions 28b and 28c of the T-shaped horizontal portion from the plate surface 27b of the support 27 are set to be larger than the height of the upper surface 15c of the vibrator 15 with respect to the plate surface 21a of the pendulum 21. The opposing surfaces 15c and 27b of the vibrator 15 and the support body 27 are spaced from each other by a predetermined amount, and the mounting portion 28d is formed so as to project from the plate surface 27b at a height equal to this spacing amount. In this embodiment, the concave groove 29 formed in the portion of the support 27 facing the one end 15a of the vibrator 15 is a clearance for connecting the vibrator 15 with wiring from the excitation means and the frequency detection means. Is.
【0020】図2に示した実施例では図1に示した実施
例と比較して振動子15をヒンジ23に近接した位置に
配設することができるため、入力加速度に対する良好な
検出感度を得ることができる。なお、これら図1及び図
2に示した実施例ではいずれも検出手段として1個の振
動子15を用いているが、振子21の他方の板面21b
側にも同様に、即ち振子21の板面21aに平行な中心
面に対して対称に振動子15、スペーサ26及び支持体
27を配設して振動子15を2個用い、それら2個の振
動子15の出力を差動出力として取出す構成としてもよ
い。この構成では検出感度を向上させることができ、か
つ例えば温度変化などによる振動子15の固有振動数の
ずれを打ち消し、そのずれの影響を受けないようにする
ことができる。In the embodiment shown in FIG. 2, the vibrator 15 can be arranged closer to the hinge 23 as compared with the embodiment shown in FIG. 1, so that good detection sensitivity for input acceleration can be obtained. be able to. In each of the embodiments shown in FIGS. 1 and 2, one vibrator 15 is used as the detecting means, but the other plate surface 21b of the pendulum 21 is used.
Similarly, on the side, that is, the vibrator 15, the spacer 26, and the support 27 are arranged symmetrically with respect to the center plane parallel to the plate surface 21a of the pendulum 21, and two vibrators 15 are used. The output of the vibrator 15 may be taken out as a differential output. With this configuration, it is possible to improve the detection sensitivity, and it is possible to cancel the deviation of the natural frequency of the vibrator 15 due to, for example, a temperature change, so that it is not affected by the deviation.
【0021】[0021]
【発明の効果】以上説明したように、この発明によれば
振子に長手方向の一端が固定された振動子の他端を振動
子と熱膨張係数がほぼ等しい材料からなる支持体の一端
に固定し、その支持体の他端を振動子の一端と対応した
位置で、振子の外周に振子と同一材で一体形成された枠
体の両側に固定することにより、環境温度が変化しても
振動子の長手方向において熱応力がほとんど発生せず、
従って環境温度の変化によって振動子が破断したり、あ
るいはその固定部においてはがれが発生したりすること
のない振動式加速度計を得ることができる。As described above, according to the present invention, the other end of the vibrator whose one end in the longitudinal direction is fixed to the pendulum is fixed to one end of the support made of a material having a thermal expansion coefficient substantially equal to that of the vibrator. Then, by fixing the other end of the support at a position corresponding to one end of the vibrator on both sides of a frame integrally formed on the outer periphery of the pendulum with the same material as the pendulum, vibrations will occur even if the environmental temperature changes. Almost no thermal stress is generated in the longitudinal direction of the child,
Therefore, it is possible to obtain a vibrating accelerometer in which the vibrator is not broken due to the change of the environmental temperature or the fixed portion thereof does not peel off.
【0022】なお、図3に示した従来の振動式加速度計
10において、例えば振子11、枠体12及びヒンジ1
3を振動子15と熱膨張係数がほぼ等しい材料により一
体形成できれば、環境温度が変化しても振動子15と振
子11及び枠体12との間に熱応力がほとんど発生しな
いようにすることができ、即ち上述したこの発明の効果
と同じ効果を得ることができる。水晶振動子と熱膨張係
数がほぼ等しい材料としては、例えばこの発明の実施例
で支持体の材料として例示したモネル金属やエルジロイ
があげられる。In the conventional vibration type accelerometer 10 shown in FIG. 3, for example, a pendulum 11, a frame 12 and a hinge 1 are used.
If 3 can be integrally formed with the vibrator 15 by a material having a substantially equal thermal expansion coefficient, it is possible to prevent thermal stress from being generated between the vibrator 15 and the pendulum 11 and the frame 12 even if the environmental temperature changes. That is, the same effect as the effect of the present invention described above can be obtained. Examples of the material having a thermal expansion coefficient substantially equal to that of the crystal unit include Monel metal and Elgiloy which are exemplified as the material of the support in the embodiment of the present invention.
【0023】しかしながら、モネル金属はバネ特性が悪
くて良好に弾性変形するヒンジを形成することができ
ず、またエルジロイはバネ特性は良好なものの、機械的
強度が不充分でヒンジが破断する恐れがあり、さらに薄
板化により反りが発生し、高精度の形状寸法を得ること
ができないという欠点があり、これら材料の使用は振動
式加速度計の性能及び信頼性を大幅に損なうものとな
る。However, Monel metal has a poor spring property and cannot form a hinge which is elastically deformed well. Elgiloy has a good spring property, but its mechanical strength is insufficient and the hinge may be broken. However, there is a drawback that a thin plate causes warpage and a highly accurate shape and dimension cannot be obtained. Use of these materials greatly impairs the performance and reliability of the vibration accelerometer.
【0024】これに対してこの発明では、支持体を設け
て熱応力の発生を解消するものであるため、振子、枠体
及びヒンジを構成する材料は熱膨張係数にとらわれるこ
となく、それらの形成に最適なものを使用することがで
き、つまり振動式加速度計の各部をそれぞれ最適な材料
で構成できるという効果がある。On the other hand, in the present invention, since the support is provided to eliminate the generation of thermal stress, the materials forming the pendulum, the frame and the hinge are formed without being restricted by the thermal expansion coefficient. It is possible to use the most suitable one, that is, there is an effect that each part of the vibration type accelerometer can be made of an optimum material.
【図1】(A)はこの発明による振動式加速度計の一実
施例を示す斜視図、(B)は(A)のAA断面図。FIG. 1A is a perspective view showing an embodiment of a vibration type accelerometer according to the present invention, and FIG. 1B is a sectional view taken along line AA of FIG.
【図2】(A)はこの発明による振動式加速度計の他の
実施例を示す斜視図、(B)は(A)のAA断面図。2A is a perspective view showing another embodiment of the vibration type accelerometer according to the present invention, and FIG. 2B is a sectional view taken along line AA of FIG.
【図3】(A)は従来の振動式加速度計を示す斜視図。
(B)は(A)のAA断面図。FIG. 3A is a perspective view showing a conventional vibration type accelerometer.
(B) is AA sectional drawing of (A).
15 振動子 21 振子 22 枠体 23 ヒンジ 27 支持体 15 Transducer 21 Pendulum 22 Frame 23 Hinge 27 Support
Claims (2)
され、かつその振子と同一材で一体に形成された枠体
と、 上記振子に一端が固定され、他端が上記枠体の上記振子
が連結された側に延長された振動子と、 その振動子と熱膨張係数がほぼ等しい材料からなり、上
記振動子の他端が一端に固定され、他端が振動子の上記
一端と対応した位置で上記枠体の両側に固定された支持
体と、 を具備する振動式加速度計。1. A pendulum, a frame body arranged on the outer periphery of the pendulum, hinged to one end of the pendulum, and integrally formed of the same material as the pendulum, and one end fixed to the pendulum, and the like. An oscillator whose end is extended to the side of the frame to which the pendulum is connected and made of a material having a thermal expansion coefficient substantially equal to that of the oscillator, and the other end of the oscillator is fixed to one end and the other end is A vibrating accelerometer, comprising: a support fixed to both sides of the frame at a position corresponding to the one end of the vibrator.
間に位置していることを特徴とする請求項1記載の振動
式加速度計。2. The vibratory accelerometer according to claim 1, wherein the vibrator is located between the frame and the support.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4216832A JPH0666828A (en) | 1992-08-14 | 1992-08-14 | Vibration type acceleration meter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4216832A JPH0666828A (en) | 1992-08-14 | 1992-08-14 | Vibration type acceleration meter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0666828A true JPH0666828A (en) | 1994-03-11 |
Family
ID=16694598
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4216832A Withdrawn JPH0666828A (en) | 1992-08-14 | 1992-08-14 | Vibration type acceleration meter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0666828A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013096806A (en) * | 2011-10-31 | 2013-05-20 | Seiko Epson Corp | Physical quantity detection device, physical quantity detector and electronic apparatus |
JP2014021094A (en) * | 2012-07-24 | 2014-02-03 | Seiko Epson Corp | Manufacturing method for physical quantity detector, physical quantity detector, electronic apparatus and movable body |
KR20190114754A (en) | 2018-03-29 | 2019-10-10 | 다이키 인더스트리 코퍼레이션 리미티드 | Device for processing cross-section of pipe |
-
1992
- 1992-08-14 JP JP4216832A patent/JPH0666828A/en not_active Withdrawn
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013096806A (en) * | 2011-10-31 | 2013-05-20 | Seiko Epson Corp | Physical quantity detection device, physical quantity detector and electronic apparatus |
JP2014021094A (en) * | 2012-07-24 | 2014-02-03 | Seiko Epson Corp | Manufacturing method for physical quantity detector, physical quantity detector, electronic apparatus and movable body |
KR20190114754A (en) | 2018-03-29 | 2019-10-10 | 다이키 인더스트리 코퍼레이션 리미티드 | Device for processing cross-section of pipe |
US11052439B2 (en) | 2018-03-29 | 2021-07-06 | Daiki Industry Co., Ltd. | Device for processing cross section of pipe |
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Legal Events
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A300 | Withdrawal of application because of no request for examination |
Free format text: JAPANESE INTERMEDIATE CODE: A300 Effective date: 19991102 |