JPS61161432A - Crystal type gas pressure gauge - Google Patents
Crystal type gas pressure gaugeInfo
- Publication number
- JPS61161432A JPS61161432A JP243785A JP243785A JPS61161432A JP S61161432 A JPS61161432 A JP S61161432A JP 243785 A JP243785 A JP 243785A JP 243785 A JP243785 A JP 243785A JP S61161432 A JPS61161432 A JP S61161432A
- Authority
- JP
- Japan
- Prior art keywords
- oscillator
- voltage
- pressure
- crystal
- gas pressure
- 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.)
- Granted
Links
- 239000013078 crystal Substances 0.000 title claims abstract description 66
- 238000006243 chemical reaction Methods 0.000 claims abstract description 9
- 230000005284 excitation Effects 0.000 abstract 2
- 230000002093 peripheral effect Effects 0.000 abstract 2
- 238000010586 diagram Methods 0.000 description 9
- 238000005259 measurement Methods 0.000 description 8
- 230000007423 decrease Effects 0.000 description 6
- 239000010453 quartz Substances 0.000 description 4
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 4
- 230000010355 oscillation Effects 0.000 description 3
- 210000000481 breast Anatomy 0.000 description 1
- 239000003990 capacitor Substances 0.000 description 1
- 238000004040 coloring Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
- 239000010931 gold Substances 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 238000003384 imaging method Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L9/00—Measuring steady of quasi-steady pressure of fluid or fluent solid material by electric or magnetic pressure-sensitive elements; Transmitting or indicating the displacement of mechanical pressure-sensitive elements, used to measure the steady or quasi-steady pressure of a fluid or fluent solid material, by electric or magnetic means
- G01L9/0001—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means
- G01L9/0008—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations
- G01L9/0022—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations of a piezoelectric element
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Fluid Pressure (AREA)
Abstract
Description
【発明の詳細な説明】
〔工業上の利用分野〕
本発明は水晶振−子を利用して、、その周囲の気体圧力
を測る気体圧力測定装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a gas pressure measuring device that uses a crystal pendulum to measure the gas pressure around the crystal pendulum.
本発明は水晶振動子を利用して、・その周囲の気
゛体圧力を測、る気体圧力測定@犬において、前記
水晶振動子5t−駆動する電圧を、周囲気体の圧力に応
じて自動釣に低減することによって、前述の従−来技術
の欠点を解決する手段全提供するものである。The present invention utilizes a crystal oscillator to
In the gas pressure measurement @ dog that measures body pressure, the above-mentioned drawbacks of the conventional technology are solved by automatically reducing the voltage driving the crystal oscillator 5t according to the pressure of the surrounding gas. It provides all the means to do so.
大気圧から10 )−ル(Torr)迄の気体圧やを
、1つのセンサで連続的に測り几いという工業的要求に
は根強いものがある。There is a deep-rooted industrial demand for continuous and precise measurement of gas pressure from atmospheric pressure to 10 Torr with a single sensor.
水晶振動子の共振周波数が、その周囲−気体の圧力が低
くなるにつれ増加するという現象、金利用し友水晶式気
体圧゛力計は、ある程度前記の工業的襖求に答えやもの
であるが、測定下限が10ト一ル程度であるという大き
な欠点を;汀している。父、熱伝−型真空計9例えばビ
ラニ真空計では測定下限が10〜10 トールであるが
、測定上限が10ト一ル程度であり、これも前記水晶式
気体圧力計と同様の欠点を有している。The phenomenon in which the resonant frequency of a quartz crystal oscillator increases as the pressure of the surrounding gas decreases, and the gold-based quartz crystal gas pressure dynamometer is, to some extent, an answer to the above-mentioned industrial need. However, it suffers from the major drawback that the lower limit of measurement is about 10 torr. For example, the Virani vacuum gauge has a lower measurement limit of 10 to 10 Torr, but an upper measurement limit of about 10 Torr, and this also has the same drawbacks as the crystal gas pressure gauge. are doing.
一方、水晶振動子の共振抵抗が、その周囲気体の圧力に
広い範囲で依存性を有することが、最近明らかと、なり
、それを利2用すれば大気圧から10トールまで1つの
センサで連続的に測定町熊な気体圧力計が実現できるこ
とが明らかとなった。On the other hand, it has recently become clear that the resonant resistance of a crystal resonator is dependent on the pressure of the surrounding gas over a wide range, and if this fact is utilized, one sensor can continuously It has become clear that it is possible to realize a gas pressure gauge that is easy to measure.
これは、例えば月刊誌「計装J 、1984年。For example, the monthly magazine "Keiso J", 1984.
Vol、 27 /に7 r水晶振動子を使つ几超小
型真空センナの開発」の項に開示されている。Vol. 27/2007, 7. Development of an ultra-compact vacuum sensor using a crystal oscillator.
次に、水晶」辰動子の共振抵゛抗の圧力依存性を利用し
之気体圧力計の動作原理を図面によって説明する。Next, the principle of operation of a gas pressure gauge that utilizes the pressure dependence of the resonance resistance of a quartz crystal cylinder will be explained with reference to the drawings.
第11閾は気体上刃と水晶撮動子の特性値(共振抵抗値
と共嘔電流、共振周波数)の関係を示す図である。共振
同波数は気体の圧力が10トールを越えると変jヒし始
めるが、気体の圧力が10トール未満では気体圧力に対
する感度はほとんど零である。一方、水晶振動子の共振
抵抗は大気圧から10 トールまで、気体圧力に対して
感度を有している。この水晶振動を定′1圧駆動すれば
、同図において1・)で示すような共振電流−気体圧力
自壊が見られる。それは、前記共振抵抗値と同様に大気
圧から10 トールまで気体圧力に対する感+3
度tiする。従って、測定の容易さの点から、共振抵抗
値を測るよりは共振′(流(又は共振電圧)t−#する
方が良い。The eleventh threshold is a diagram showing the relationship between the characteristic values (resonance resistance value, resonance current, and resonance frequency) of the gas upper blade and the crystal camera element. The resonance frequency begins to change when the gas pressure exceeds 10 Torr, but when the gas pressure is less than 10 Torr, the sensitivity to gas pressure is almost zero. On the other hand, the resonant resistance of a crystal resonator is sensitive to gas pressure from atmospheric pressure to 10 Torr. If this crystal vibration is driven at a constant pressure of 1, a resonant current-gas pressure self-destruction as shown by 1.) in the same figure will be observed. It is sensitive to gas pressure from atmospheric pressure to 10 Torr +3 degrees ti, similar to the resonant resistance value. Therefore, from the viewpoint of ease of measurement, it is better to measure the resonance '(current (or resonance voltage) t-#) than to measure the resonance resistance value.
第2図社、本発明の対象である水晶式気体圧力計の゛「
匡子回路ブロック図である。大きくはPLL回路部と、
表示変換回路部と、表示部とから1成される。前記FL
U、回路部は、4圧又は電流に、Cりて制御される周波
数可変発振器1、水晶撮動子5の共振電流を電圧として
増幅する増幅器2、′前記増幅器2の出力信号と前記周
波数可変発振器1の出力信号との位相を比較し、その位
相差に比例濾波器4とから成る。前記低域4波゛器4“
の出力′;圧は前記周波数可変発振器1の発振周波数を
制御する。圧力センサである前記水晶振動子5は、前記
周波数可変発振器1の出力端子と前記増幅器20入力端
子に接続される。Fig. 2 Co., Ltd., of the crystal gas pressure gauge which is the object of the present invention.
FIG. 2 is a block diagram of a box circuit. The main part is the PLL circuit section,
It is composed of a display conversion circuit section and a display section. Said FL
U, the circuit section includes a variable frequency oscillator 1 controlled by voltage or current, an amplifier 2 that amplifies the resonant current of the crystal sensor 5 as a voltage, and an output signal of the amplifier 2 and the frequency variable oscillator 1; The phase is compared with the output signal of the oscillator 1, and a proportional filter 4 is applied to detect the phase difference. The low frequency 4 wave generator 4"
The output '; pressure controls the oscillation frequency of the variable frequency oscillator 1. The crystal oscillator 5, which is a pressure sensor, is connected to the output terminal of the variable frequency oscillator 1 and the input terminal of the amplifier 20.
PLL回路の動作原理は既に広く知られているので、こ
こでは省略するが、前記周波数可変発振器1の発振周波
数は、前記周波数可変発振器1の出力信号即ち前記水晶
振動子5の駆動電圧と、前記増#A1善2の出力信号即
ち前記水晶振動子5を流れる′1流との位相差が零にな
るように常に制御されている。即ち、前記水晶撮動子5
は常に、それ自身の共振同波数にて駆動されていること
であり、水晶式気体圧力計を実用化する上で遁要な意味
をもつ。というのは、第1図に示す工う(ζ、水晶撮動
子の共振)!d波数は気体圧力によって変化するからで
ある。次に表示変換回路部は、前記増幅器2の信播を更
に増幅する主増幅器6、@記主増装置出力電圧の極性を
反転するインバータ8、及び前記インバータ8の出力電
圧にバイアスをかける几めのバッファ9とから成る。前
記バイアス量は可変抵抗器9aKよって任意に変えるこ
とができる表示部は、気体圧力をデジタル的に、又は、
アナログ的に表示する部分で、本例ではメータ10によ
り構成されていて、前記メータ10の振れ角から気体電
力を読み取るものである。Since the operating principle of the PLL circuit is already widely known, it is omitted here, but the oscillation frequency of the variable frequency oscillator 1 is determined by the output signal of the variable frequency oscillator 1, that is, the drive voltage of the crystal resonator 5, and the Control is always performed so that the phase difference between the output signal of the amplifier #A1 and the current '1 flowing through the crystal oscillator 5 becomes zero. That is, the crystal camera element 5
is always driven at the same wave number as its own resonance, which is extremely important for the practical use of crystal gas pressure gauges. This is due to the process shown in Figure 1 (ζ, resonance of the crystal camera)! This is because the d wave number changes depending on the gas pressure. Next, the display conversion circuit unit includes a main amplifier 6 that further amplifies the signal transmitted from the amplifier 2, an inverter 8 that inverts the polarity of the output voltage of the main extension device, and a device that biases the output voltage of the inverter 8. It consists of a buffer 9. The bias amount can be changed arbitrarily using the variable resistor 9aK.The display unit can display the gas pressure digitally or
This part is displayed in an analog manner, and in this example is constituted by a meter 10, and the gas power is read from the deflection angle of the meter 10.
前記水晶振動子の共振電流の圧力特性は第1図に示すよ
うに、周囲気体の圧力が低下するに従って共振電流−が
増加するので、電圧として増幅し、直流になおし、その
ままメータを尾切すると圧力が低下するに従いメータの
振れ角が増加し、常識に反する表示になる。そこで、前
記インパーク8によって、前記直流電圧の極性を反転し
、更に前記バッファ9によってバイアス電圧を加えるこ
とにより、第3図に示すようなメータ駆動′シ圧を得る
ことができる。ggs図の例では、大気圧Qζおいてメ
ータ駆動電圧が10VKなるように前記ノぐイアス・肴
が調整されている−このようにして、大気圧においてメ
ータの針が完全に振れ、低圧になるに従ってメータの橿
れ角が減少する通常の圧力表示t−帰ることができる。As shown in Figure 1, the pressure characteristics of the resonant current of the crystal resonator are as follows: As the pressure of the surrounding gas decreases, the resonant current increases, so if it is amplified as a voltage, converted to direct current, and the meter is turned off as it is, As the pressure decreases, the deflection angle of the meter increases, resulting in an unconventional reading. Therefore, by inverting the polarity of the DC voltage using the impark 8 and applying a bias voltage using the buffer 9, a meter driving pressure as shown in FIG. 3 can be obtained. In the example of the ggs diagram, the meter needle is adjusted so that the meter drive voltage is 10 VK at atmospheric pressure Qζ - in this way, the meter needle swings completely at atmospheric pressure, resulting in a low pressure. Accordingly, the torsion angle of the meter decreases and the normal pressure display can be returned to t.
第4図は、前記水晶撮動子5の駆動電圧対共振抵抗値の
特性(Fa囲気体圧力はlX10 トール以下)を示
す図である。前記水晶振動子5を、@動する・1圧がC
L5ボルト(実効値)ft越えると、前・記水晶撮勤子
は過励振状態になる。FIG. 4 is a diagram showing the characteristics of the drive voltage versus resonance resistance value of the crystal sensor 5 (Fa surrounding gas pressure is 1×10 Torr or less). The crystal oscillator 5 is moved @1 pressure is C
When L5 volts (effective value) ft is exceeded, the crystal sensor becomes over-excited.
しかしながら、水晶振動子の共振抵抗の圧力依存性を利
用する前述の従来構成による水晶式気体圧力計において
は、前記水晶振動子5を駆動する電圧が一定でちり、前
記水晶撮動子5が大気圧又はそれ以上の圧力下にある時
でも前記PLL1g回路部が正常に動作する工うに前記
水晶振動子5t−駆動する(圧の値t−固定すると、前
記水晶振動子5が非常に低い圧力下にある時、前記水晶
撮動子5の共振抵抗が小さくなるので、前記水晶振動子
5を・@効するべ圧が相対的に強大になり、過励撮状態
になる欠点が6つ九〇即ち、前記イく晶振動子5が過励
振状!法になると、前記水晶S@子5の振動洩れが大き
くなり共振電流の値が不安定になり測定精度を低下させ
る。又、当然、前記水晶−振動子5が遇励振状態にちれ
ば、その信頼性は低下し、はなはだしい場合は破損する
場合もあシ、実用上、看過しえない間@t−発生する。However, in the above-mentioned conventional crystal gas pressure gauge that utilizes the pressure dependence of the resonant resistance of the crystal resonator, the voltage for driving the crystal resonator 5 is constant and the crystal sensor 5 is large. The crystal oscillator 5t is driven so that the PLL 1g circuit operates normally even when the pressure is at atmospheric pressure or higher (if the pressure value t is fixed, the crystal oscillator 5 is driven under a very low pressure). , the resonant resistance of the crystal oscillator 5 becomes small, so the flat pressure acting on the quartz oscillator 5 becomes relatively strong, resulting in an overexcited imaging state. That is, when the crystal oscillator 5 becomes over-excited, the vibration leakage of the crystal oscillator 5 increases, the value of the resonant current becomes unstable, and the measurement accuracy decreases. If the crystal oscillator 5 falls into an unexcited state, its reliability will decrease, and in extreme cases it may even be damaged, which can occur for a period of time that cannot be overlooked in practice.
本発明は上記の事情に鑑み為され念もので、前記水晶振
動子5を駆動する電圧を、周囲気体の圧力に応じて自動
的に低減することによって、前述の従来技術の欠点を解
決する手段を提供するものである。The present invention was conceived in view of the above circumstances, and is a means of solving the drawbacks of the prior art described above by automatically reducing the voltage for driving the crystal oscillator 5 in accordance with the pressure of the surrounding gas. It provides:
以下、本発明を図によって説明する。@5図は本発明の
実施例を示す図である。前記周波数可変発振61の出力
電圧は、コンデンサj1aと抵抗11bKよって直流分
が取シ除かれ次後、正相増幅器11に印加される。前記
正相1vII’:’oT器11の利得は、スイッチ14
&が開状態の時は1、前記スイッチ14aが閉状態の時
は、抵抗11cの抵抗値’krt 、抵抗11dの抵抗
値をr2とすると、1+rl/rz となる。即ち、気
体圧力センナである水晶振動子5を駆動する電圧は前記
スイッチ14&を開閉することによって変え得る。次に
、前記水晶振動子5′t−流れる電流は抵抗2aKよっ
て電圧に変えられ、正相増幅器2で増幅される。Hereinafter, the present invention will be explained with reference to the drawings. @Figure 5 is a diagram showing an embodiment of the present invention. The output voltage of the variable frequency oscillation 61 is applied to the positive phase amplifier 11 after the DC component is removed by the capacitor j1a and the resistor 11bK. The positive phase 1vII':'The gain of the oT device 11 is determined by the switch 14
When & is in the open state, it is 1, and when the switch 14a is in the closed state, the resistance value 'krt of the resistor 11c and the resistance value of the resistor 11d are r2, then 1+rl/rz. That is, the voltage for driving the crystal oscillator 5, which is a gas pressure sensor, can be changed by opening and closing the switch 14&. Next, the current flowing through the crystal oscillator 5't is converted into voltage by the resistor 2aK and amplified by the positive phase amplifier 2.
抵抗2b、抵抗2cは、前記正相増幅器2の利得を決定
する。前記正相増幅器2の出力の一部は、前記位相比較
器3に印加されPLL回路部を完成する。前記正相増幅
器2の出力の他の一部はフンデン?6’a K & ’
)直流分が除去され逆相増幅器6′に印加される。抵抗
6’bの値をr3、抵抗6’cの値t” r4 、抵抗
6’(lの値’jc r s とすると、前記逆相増幅
器6′の利得は、スイッチ14bが開状態の時は(r
4 + r s ) / r s となり、前記スイッ
チ14bが閉状態の時はr5/rl となる。即ち、
前記スイッチ14bが開閉によシ前記逆相増幅器乙の利
得を変え得る。ここで、前記スイッチ14aと前記スイ
ッチ14bとは、リレー14によって連動するもので、
前記スイッチ14aが1の時は前記スイッチ14bも開
、前記スイッチ14aが閉の時は前記スイッチ14bも
閉である。The resistor 2b and the resistor 2c determine the gain of the positive phase amplifier 2. A part of the output of the positive phase amplifier 2 is applied to the phase comparator 3 to complete the PLL circuit section. Is the other part of the output of the positive phase amplifier 2 normal? 6'a K&'
) The DC component is removed and applied to the anti-phase amplifier 6'. Assuming that the value of the resistor 6'b is r3, the value of the resistor 6'c is t''r4, and the value of the resistor 6'(l is 'jc r s), the gain of the anti-phase amplifier 6' is when the switch 14b is in the open state. is (r
4+rs)/rs, and when the switch 14b is closed, it becomes r5/rl. That is,
The switch 14b can change the gain of the negative phase amplifier B by opening and closing. Here, the switch 14a and the switch 14b are interlocked by a relay 14,
When the switch 14a is 1, the switch 14b is also open, and when the switch 14a is closed, the switch 14b is also closed.
具体的には、r I= r @ =r 3 =10キロ
オーム、r4 == r6 =100キロオームである
。前記スイッチ14.aと14t+が開状態の時、前記
正相増幅器の利得は1で、前記水晶振動子を駆動する電
圧は250 ミ9ボルトでちゃ、前記逆相増幅器6の利
得は20である。これは、前記水晶振動子5の周囲気体
の圧力が低い時に相当する。Specifically, r I = r @ = r 3 = 10 kilohms, r4 == r6 = 100 kilohms. Said switch 14. When a and 14t+ are open, the gain of the positive phase amplifier is 1, the voltage driving the crystal oscillator is 250 m9 volts, and the gain of the negative phase amplifier 6 is 20. This corresponds to when the pressure of the gas surrounding the crystal resonator 5 is low.
次に、前記スイッチ14a、14bが閉状態の時、前記
正相増幅器11の利得は2となシ、前記水晶振動子5t
−ffi動する電圧は50 Q ミ17ボルトとなシ、
前記逆相増幅器6′の利得は10となる。Next, when the switches 14a and 14b are closed, the gain of the positive phase amplifier 11 is 2, and the crystal oscillator 5t
-ffi operating voltage is 50 Q and 17 volts,
The gain of the anti-phase amplifier 6' is 10.
これは、前記水晶撮動子5のr!4囲気体の圧力が高い
時に相当する。即ち、周囲気体圧力が低くなると圧力が
高い時に比べ、前記水晶振動子5を駆動する電圧は半分
になるが、一方、前記逆相増幅器6′の利得は2倍にな
るので、前記メータ10の指示値を何ら変えることなく
、前記水晶!M動子を過励振状態にすることを防ぐこと
ができる。尚、抵抗10aは前記メータ10に流れる電
流を制限している。This is the r! of the crystal camera 5. This corresponds to when the pressure of the surrounding gas is high. That is, when the ambient gas pressure is low, the voltage driving the crystal oscillator 5 is halved compared to when the pressure is high, but on the other hand, the gain of the anti-phase amplifier 6' is doubled, so that the meter 10 is The above crystal without changing the indicated value! It is possible to prevent the M oscillator from being overexcited. Note that the resistor 10a limits the current flowing to the meter 10.
前記表示変換回路部におけるバッファ9の出力電圧の一
部はコンパレータ12に印加される。前記コンパレータ
12の出力電圧は抵抗13aを介し、トランジスタ15
1に活性化し、前記リレー14Kt流を流し、前記スイ
ッチ14a、14bを閉状態にする、即ち、前記コンパ
レータ12によって、前記水晶振動子5を駆動する電圧
を変える。尚、ダイオード14cは前記リレー14の逆
起電圧を吸収し前記トランジスタ13を保護する。A part of the output voltage of the buffer 9 in the display conversion circuit section is applied to the comparator 12. The output voltage of the comparator 12 is applied to the transistor 15 via the resistor 13a.
1, the relay 14Kt flow is made to flow, and the switches 14a and 14b are closed, that is, the voltage for driving the crystal resonator 5 is changed by the comparator 12. Note that the diode 14c absorbs the back electromotive voltage of the relay 14 and protects the transistor 13.
又、抵抗15bは、前記リレー14に流れる電流を適正
な値にするものである。Further, the resistor 15b is used to adjust the current flowing through the relay 14 to an appropriate value.
前記コンパレータ12の基準電圧は、具体的には約55
ボルトに選ばれる。この時、前記水晶撮動子5の周囲気
体の圧力は1トールである。即ち、周囲気体の圧力が1
トールより・も高いと、前記コンパレータ12の出力′
電圧は「正」となり、前記スイッチ14a、14bは閉
状態となり、前記水晶振動子5は500 ミ17ボルト
で駆動される。次に周囲気体の圧力が1トールを下まわ
ると、前記コンパレータ12の出力電圧は「負」となり
、前記スイッチ14a、14bは開となり、前記水晶振
動子5は250 ミ17ボルトで駆動される。ここで、
前記逆相増幅器6′の利得は周囲気体圧力が1ト一ル以
上の場合に較べ2倍になるので、前記水晶振動子の駆動
電圧が半分になっても、前記メータ10の指示は、その
事によっては変化せず、測定に何ら支障をきtさない。Specifically, the reference voltage of the comparator 12 is about 55
Selected by Bolt. At this time, the pressure of the gas surrounding the crystal camera 5 is 1 Torr. That is, the pressure of the surrounding gas is 1
If the output of the comparator 12 is higher than
The voltage becomes "positive", the switches 14a and 14b are closed, and the crystal resonator 5 is driven at 500 mm and 17 volts. Then, when the pressure of the ambient gas falls below 1 Torr, the output voltage of the comparator 12 becomes "negative", the switches 14a, 14b are opened, and the crystal 5 is driven at 250 mm and 17 volts. here,
Since the gain of the anti-phase amplifier 6' is twice that when the ambient gas pressure is 1 Torr or more, even if the driving voltage of the crystal oscillator is halved, the reading on the meter 10 remains the same. In some cases, it does not change and does not interfere with measurement.
以上述べてきたように、本発明によれば、気体圧力表示
値に変化を与えることなしに、気体圧力がある値以下に
なると自動的に気体圧力センナである水晶撮動子を駆動
する電圧を低減することができ、水晶振動子を使用する
上で最も避けなければならない過励振を防止し、気体圧
力の測定精度を向上し、且つ、水晶振動子の寿命を長く
することができる。又、本発明は、大気圧以上の圧力全
測定する時にも、水晶振動子の駆動電圧を自由に選べる
ので有用である。As described above, according to the present invention, when the gas pressure falls below a certain value, the voltage that drives the crystal sensor, which is the gas pressure sensor, is automatically adjusted without changing the gas pressure display value. It is possible to prevent overexcitation, which is the most important thing to avoid when using a crystal resonator, to improve the measurement accuracy of gas pressure, and to extend the life of the crystal resonator. Further, the present invention is useful because the drive voltage of the crystal resonator can be freely selected even when measuring all pressures higher than atmospheric pressure.
第1図は水晶振動子の特性値(共振抵抗、共振電流、共
振周波数)と周囲気体圧力との関係を示す図、第2図は
本発明の水晶式気体圧力計の電子回路ブロック図、第3
図はメータ駆動電圧と周囲気体圧力との関係を示す図、
第4図は前記水晶振動子を駆動する電圧とその共振抵抗
との関係を示す図、第5図は本発明の実施例を示す図で
ある。
1・・・周波数可変発振器 2・・・増幅器3・・・位
相比較器 4・・・低域濾波器5・・・水晶振動
子 6′・・・主増幅器7・・・整流器
8・・・インバータ9・・・バッファ 1G
・・・メータ11・・・正相増幅器 12・・・コ
ンパレータ13・・・トランジスタ 14・・・リレ
ー14a、14b・・・スイッチ
6′・・・逆相増幅器
第1図
乳体の圧力どkぬり
O101001000
M浪レベJしし(mVr腐つ
第4図Fig. 1 is a diagram showing the relationship between the characteristic values of the crystal resonator (resonant resistance, resonant current, resonant frequency) and the ambient gas pressure; Fig. 2 is a block diagram of the electronic circuit of the crystal gas pressure gauge of the present invention; 3
The figure shows the relationship between meter drive voltage and ambient gas pressure.
FIG. 4 is a diagram showing the relationship between the voltage for driving the crystal resonator and its resonance resistance, and FIG. 5 is a diagram showing an embodiment of the present invention. 1... Frequency variable oscillator 2... Amplifier 3... Phase comparator 4... Low pass filter 5... Crystal oscillator 6'... Main amplifier 7... Rectifier
8...Inverter 9...Buffer 1G
...Meter 11...Positive phase amplifier 12...Comparator 13...Transistor 14...Relay 14a, 14b...Switch 6'...Negative phase amplifier Fig. 1 Breast body pressure k Coloring O101001000 M Rage Level J Shishi (mVr rott figure 4
Claims (1)
濾波器、増幅器より成るフェーズ・ロックド・ループ回
路(PLL回路)部と、前記周波数可変発振器に接続さ
れた水晶振動子と、前記PLL回路部に接続された表示
変換回路部と、前記表示変換回路部に接続された表示部
とを有し、前記水晶振動子の共振抵抗値、又は共振電流
値、又は共振電圧値から、前記水晶振動子の周囲気体の
圧力を測定する水晶式気体圧力計において、前記表示部
に印加される電圧をある基準電圧と比較する比較器、前
記比較器の出力電圧によって駆動されるスイッチ、前記
スイッチによって利得が変化し、そのうちの1個は前記
水晶振動子を駆動し、他の1個は前記水晶振動子の共振
電流を増幅する2個の増幅器、とによって構成されるこ
とを特徴とする水晶式気体圧力計。At least a phase-locked loop circuit (PLL circuit) section consisting of a variable frequency oscillator, a phase comparator, a low-pass filter, and an amplifier, a crystal resonator connected to the variable frequency oscillator, and the PLL circuit section. It has a display conversion circuit unit connected to the display conversion circuit unit and a display unit connected to the display conversion circuit unit, and the display unit has a display unit connected to the display conversion circuit unit. A crystal gas pressure gauge that measures the pressure of surrounding gas includes a comparator that compares the voltage applied to the display with a certain reference voltage, a switch driven by the output voltage of the comparator, and a gain that changes with the switch. and two amplifiers, one of which drives the crystal oscillator and the other amplifies the resonant current of the crystal oscillator. .
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP243785A JPS61161432A (en) | 1985-01-10 | 1985-01-10 | Crystal type gas pressure gauge |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP243785A JPS61161432A (en) | 1985-01-10 | 1985-01-10 | Crystal type gas pressure gauge |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS61161432A true JPS61161432A (en) | 1986-07-22 |
JPH0380253B2 JPH0380253B2 (en) | 1991-12-24 |
Family
ID=11529243
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP243785A Granted JPS61161432A (en) | 1985-01-10 | 1985-01-10 | Crystal type gas pressure gauge |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61161432A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01148932A (en) * | 1987-12-04 | 1989-06-12 | Nagano Keiki Seisakusho:Kk | Gas pressure gauge |
JPH01291137A (en) * | 1988-05-17 | 1989-11-22 | Yokogawa Electric Corp | Vibration type transducer |
CN106123940A (en) * | 2015-05-05 | 2016-11-16 | 北京康智乐思网络科技有限公司 | A kind of data acquisition unit and acquisition method |
-
1985
- 1985-01-10 JP JP243785A patent/JPS61161432A/en active Granted
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01148932A (en) * | 1987-12-04 | 1989-06-12 | Nagano Keiki Seisakusho:Kk | Gas pressure gauge |
JPH01291137A (en) * | 1988-05-17 | 1989-11-22 | Yokogawa Electric Corp | Vibration type transducer |
CN106123940A (en) * | 2015-05-05 | 2016-11-16 | 北京康智乐思网络科技有限公司 | A kind of data acquisition unit and acquisition method |
Also Published As
Publication number | Publication date |
---|---|
JPH0380253B2 (en) | 1991-12-24 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US4741213A (en) | Quartz-type gas pressure gauge | |
US6510737B1 (en) | Inertial rate sensor and method with improved tuning fork drive | |
US20100206074A1 (en) | Oscillation drive device, physical quantity measurement device and electronic apparatus | |
JP3327912B2 (en) | Linear oscillator | |
US20090078045A1 (en) | Driver device, physical quantity measuring device, and electronic instrument | |
US7859351B2 (en) | Driver device, physical quantity measuring device, and electronic instrument | |
JPS6184535A (en) | Crystal type gas manometer | |
JPS61161432A (en) | Crystal type gas pressure gauge | |
JPH01313728A (en) | Crystal vacuum gauge | |
JPS62228126A (en) | Gas pressure gauge | |
JPS62190905A (en) | Surface acoustic wave device | |
JP3139656B2 (en) | Signal conversion circuit | |
JPH02503252A (en) | high voltage amplifier | |
JPH0374934B2 (en) | ||
JPH042894B2 (en) | ||
JPS60222734A (en) | Method and apparatus for detecting force | |
JPH049451B2 (en) | ||
US3991410A (en) | Analog storage circuit including a piezoelectric element | |
JPH0454800A (en) | Ultrasonic sensor | |
JPH01318424A (en) | Triangular wave generation circuit | |
JPS59141026A (en) | Vacuum gauge | |
JPS62130325A (en) | Crystal type gas manometer | |
SU476663A1 (en) | Measuring instrument of speed of the device for automatic adjustment of the signal generator level | |
JPH08247801A (en) | Transducer and gas mater using thereof | |
KR960013754B1 (en) | Integral Capacitor Measurement Circuit with Series Resistance Compensation |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
EXPY | Cancellation because of completion of term |