JPS6126913Y2 - - Google Patents
Info
- Publication number
- JPS6126913Y2 JPS6126913Y2 JP889381U JP889381U JPS6126913Y2 JP S6126913 Y2 JPS6126913 Y2 JP S6126913Y2 JP 889381 U JP889381 U JP 889381U JP 889381 U JP889381 U JP 889381U JP S6126913 Y2 JPS6126913 Y2 JP S6126913Y2
- Authority
- JP
- Japan
- Prior art keywords
- cylindrical resonator
- resonator
- fluid
- density
- cover
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 238000001514 detection method Methods 0.000 claims description 15
- 239000012530 fluid Substances 0.000 claims description 13
- 230000005284 excitation Effects 0.000 claims description 6
- 238000000034 method Methods 0.000 description 2
- 238000005070 sampling Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 1
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000003960 organic solvent Substances 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
Landscapes
- Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
Description
【考案の詳細な説明】
本考案は、実験室や研究室の卓上において使用
可能な卓上用密度計に関するものである。[Detailed Description of the Invention] The present invention relates to a tabletop density meter that can be used on a tabletop in a laboratory or laboratory.
従来公知の密度計として、例えば特公昭43−
26012号公報に示されているように、音又型に形
成したパイプ振動子に、被測定流体を導入し、こ
の振動子に生ずる横方向自由振動数から密度を知
るようにしたもの、あるいは、特公昭51−16794
号公報に示されているように円筒共振子の内側お
よび外側に被測定流体を流し、円筒共振子の円環
振動数から密度を知るようにしたもの等がある。 As a conventionally known density meter, for example, the
As shown in Publication No. 26012, a fluid to be measured is introduced into a pipe vibrator formed in the shape of an acoustic pipe, and the density is determined from the transverse free frequency generated in this vibrator, or Tokuko Showa 51-16794
As shown in the above publication, there is a method in which a fluid to be measured is caused to flow inside and outside a cylindrical resonator, and the density is determined from the annular frequency of the cylindrical resonator.
前者は被測定流体をパイプ振動子に導入させる
ためにサンプリングポンプ等が必要であり、ま
た、後者は円筒共振子を被測定流体が流れている
管路内に取付けなければならない等、いずれも装
置の設置や操作が煩しい欠点がある。また、いず
れも例えば試験管内に採取されたサンプルのよう
な微量の流体の密度測定はできない。 The former requires a sampling pump, etc. to introduce the fluid to be measured into the pipe resonator, and the latter requires a cylindrical resonator to be installed in the pipe through which the fluid to be measured flows. The disadvantage is that it is difficult to install and operate. Furthermore, neither method is capable of measuring the density of a minute amount of fluid, such as a sample collected in a test tube.
ここにおいて、本考案は、取扱いが容易で、微
量の流体の密度測定が可能な卓上用密度計を実現
しようとするものである。 Here, the present invention aims to realize a desk-top density meter that is easy to handle and capable of measuring the density of a minute amount of fluid.
第1図は本考案に係る密度計の一例を示す構成
断面図、第2図は一部を断面で示す構成斜視図で
ある。これらの図において、1は円筒共振子で、
一端側はフランジ11が、他端側はフランジ12
および他端側を閉じる底部13が設けられてい
る。他端側のフランジ12には、一端側の開口部
から入つた被測定流体が流出する貫通孔14が形
成してある。2は一方のフランジ12の段部に取
付けた円筒共振子1の励振手段、3は同じくフラ
ンジ12の段部に取付けた円筒共振子1の振動検
出手段で、ここではいずれもPZTを用いた場合を
例示してある。41,42はいずれも同一径のカ
バーであつて、カバー41は両端のフランジ1
1,12に結合して円筒共振子1の外側を覆い、
また、カバー42は一端がフランジ12に結合し
ていて細長い柄を構成するとともに、励振手段2
および振動検出手段3に接続されるリード線2
1,31を覆つている。5は円筒共振子1の底部
13に取付けた温度検出手段で、例えばサーミス
〓〓〓〓
タ、トランジスタが用いられており、円筒共振子
1内に流入した被測定流体の温度を検出する。こ
の温度検出手段は、温度補正用として利用される
ものであつて、必ずしも必要としない。カバー4
1と円筒共振子1との間に形成される部屋15内
は、大気圧あるいは一定圧力(真空も含む)の気
体が封入されている。 FIG. 1 is a sectional view showing an example of a density meter according to the present invention, and FIG. 2 is a perspective view showing a partially sectional view. In these figures, 1 is a cylindrical resonator,
One end has a flange 11, and the other end has a flange 12.
and a bottom portion 13 that closes the other end. A through hole 14 is formed in the flange 12 on the other end side, through which the fluid to be measured that has entered through the opening on the one end side flows out. 2 is an excitation means for the cylindrical resonator 1 attached to the stepped portion of one flange 12, and 3 is a vibration detection means for the cylindrical resonator 1 also attached to the stepped portion of the flange 12. In this example, PZT is used in both cases. is shown as an example. 41 and 42 are covers with the same diameter, and the cover 41 has the flanges 1 at both ends.
1 and 12 to cover the outside of the cylindrical resonator 1,
Further, the cover 42 has one end connected to the flange 12 to form an elongated handle, and the excitation means 2
and a lead wire 2 connected to the vibration detection means 3
It covers 1,31. 5 is a temperature detection means attached to the bottom 13 of the cylindrical resonator 1, such as a thermistor.
A transistor is used to detect the temperature of the fluid to be measured that has flowed into the cylindrical resonator 1. This temperature detection means is used for temperature correction and is not necessarily required. cover 4
The chamber 15 formed between the resonator 1 and the cylindrical resonator 1 is filled with gas at atmospheric pressure or a constant pressure (including vacuum).
このように構成した装置は、全体が細長い棒状
で構成されるものであつて、この装置は第3図に
示すように例えば試験管内に採取された試料中に
挿入され、密度測定が行える。なお、採取された
試料が吸湿性であつたり、気化しやすい場合は、
柄の部分と試験管との間に図示するように栓6を
用いる。すなわち、棒状の先端部分は、円筒共振
子1があつて、これを被測定試料(流体)中に挿
入すると、試料は先端開口部から矢印aに示すよ
うに、円筒共振子1の内側に流入し、貫通孔14
から流出するようにして、円筒共振子1の内側に
満たされる。この状態で、励振手段2、振動検出
手段3を含んで形成される自励発振ループ(図示
せず)によつて円筒共振子1を円環振動させる。
ここで、円筒共振子1の共振周波数は、円筒共振
子1の内側に満たされた被測定試料の主として密
度Dに関連して変化する。なお、円筒共振子1の
内側と外側の圧力差による影響は、被測定試料の
圧力を例えば大気圧に等しくするとか、一定圧力
に維持することによりなくすることができ、温度
による影響は、円筒共振子1の材料を小さな温度
弾性係数をもつものとするか、あるいは温度検出
手段5からの信号を利用して補正する等して、無
視できる。 The device constructed in this way has an elongated rod shape as a whole, and as shown in FIG. 3, this device can be inserted into a sample taken in a test tube, for example, to measure the density. In addition, if the collected sample is hygroscopic or easily vaporized,
A stopper 6 is used between the handle and the test tube as shown. That is, the rod-shaped tip has the cylindrical resonator 1 attached thereto, and when this is inserted into the sample to be measured (fluid), the sample flows into the cylindrical resonator 1 from the tip opening as shown by arrow a. and through hole 14
The inside of the cylindrical resonator 1 is filled in such a way that it flows out from the cylindrical resonator 1. In this state, a self-excited oscillation loop (not shown) formed including the excitation means 2 and the vibration detection means 3 causes the cylindrical resonator 1 to vibrate in an annular manner.
Here, the resonant frequency of the cylindrical resonator 1 changes mainly in relation to the density D of the sample to be measured filled inside the cylindrical resonator 1. Note that the influence of the pressure difference between the inside and outside of the cylindrical resonator 1 can be eliminated by making the pressure of the sample to be measured equal to atmospheric pressure or maintaining it at a constant pressure. This can be ignored by making the material of the resonator 1 have a small coefficient of temperature elasticity, or by correcting it using the signal from the temperature detection means 5.
円筒共振子1の内側に被測定試料を満たした状
態で、円環振動をさせると、その共振周波数d
と被測定試料の密度Dとは、次式のような関係が
ある。 When the inside of the cylindrical resonator 1 is filled with a sample to be measured and subjected to circular vibration, its resonant frequency d
and the density D of the sample to be measured have a relationship as shown in the following equation.
ただし、o:密度0(真空中)における共振
周波数
K:円筒共振子1の直径、厚さ等に
よつて定まる定数
このように構成した装置によれば、密度検出部
を棒状の先端であつて、細長い構造とすることが
できるので、取扱いが容易で、微量の試料中にも
挿入できるうえに、サンプリングポンプ等の設置
は不要である。また、密度検出部の洗浄も、柄の
部分を手で支持し、先端部分を例えば有機溶剤中
に浸漬することによつて容易に行うことができ
る。 However, o: resonance frequency at density 0 (in vacuum) K: constant determined by the diameter, thickness, etc. of the cylindrical resonator 1 According to the device configured in this way, the density detection section is a rod-shaped tip. Since it can be made into an elongated structure, it is easy to handle and can be inserted into even a minute amount of sample, and there is no need to install a sampling pump or the like. Further, the density detection section can be easily cleaned by supporting the handle part by hand and immersing the tip part in an organic solvent, for example.
第4図〜第6図は本考案に係る密度計の他の例
を示す構成斜視図である。 4 to 6 are perspective views showing other examples of the density meter according to the present invention.
第4図は、円筒共振子1の他方のフランジに結
合するカバー42をフレキシブルチユーブで構成
し、先端の密度検出部を湾曲した奥にある試料中
まで容易に到達できるようにしたものである。こ
の例は、例えば人間や動物の体内中の特定個所に
おける流体密度を検出するような場合に有効であ
る。 In FIG. 4, the cover 42 connected to the other flange of the cylindrical resonator 1 is constructed of a flexible tube, so that the density detection section at the tip can easily reach the inside of the curved sample. This example is effective, for example, when detecting fluid density at a specific location within the body of a human or animal.
第5図は、先端の密度検出部とここから延びる
柄の部分とを軸を異にして連結させたものであ
る。 In FIG. 5, the density detection section at the tip and the handle extending from this section are connected with different axes.
第6図は、先端の密度検出部と、柄の部分とを
T字形状となるように連結させたものである。 FIG. 6 shows a device in which the density detection section at the tip and the handle are connected to form a T-shape.
第5図、第6図の各実施例では、円筒共振子1
は両端開放の構造となつている。 In each of the embodiments shown in FIGS. 5 and 6, the cylindrical resonator 1
has a structure with both ends open.
なお、上記の各実施例において、円筒共振子1
を覆うカバー41と、リード線を覆うカバー42
とを同一径としたが異なる径としてもよく、カバ
ー42の一端側はフランジ部42以外に、カバー
41に結合するようにしてもよい。 In each of the above embodiments, the cylindrical resonator 1
and a cover 42 for covering the lead wires.
However, they may have different diameters, and one end of the cover 42 may be connected to the cover 41 in addition to the flange portion 42 .
以上説明したように、本考案によれば、取扱い
が容易で、微量の流体の密度測定が行なえる卓上
用密度計が実現できる。 As explained above, according to the present invention, it is possible to realize a desktop densitometer that is easy to handle and can measure the density of a minute amount of fluid.
第1図は本考案に係る密度計の一例を示す構成
断面図、第2図は一部を断面で示す構成図、第3
図は本考案に係る密度計の使用態様を示す説明
図、第4図〜第6図は本考案に係る密度計の他の
例を示す構成斜視図である。
1……円筒共振子、11,12……フランジ
部、2……励振手段、3……振動検出手段、4
1,42……カバー、5……温度検出手段。
〓〓〓〓
FIG. 1 is a cross-sectional view showing an example of the density meter according to the present invention, FIG. 2 is a partially cross-sectional view showing the structure, and FIG.
The figure is an explanatory diagram showing how the densitometer according to the present invention is used, and FIGS. 4 to 6 are perspective views showing other examples of the densitometer according to the present invention. DESCRIPTION OF SYMBOLS 1... Cylindrical resonator, 11, 12... Flange part, 2... Excitation means, 3... Vibration detection means, 4
1, 42...Cover, 5...Temperature detection means. 〓〓〓〓
Claims (1)
なくとも一端が開放しておりそこから被測定流体
が流入し内部に被測定流体が満たされるようにし
た構造の円筒共振子、前記各フランジ部に結合し
前記円筒共振子の外側を覆うカバー、前記円筒共
振子を励振する励振手段、前記円筒共振子の振動
を検出する検出手段、前記フランジ部のうちの少
なくとも一方又は前記カバーに一端が結合し前記
励振手段と振動検出手段に接続されるケーブルを
覆うようにした細長い柄を構成するケースを具備
し、前記円筒共振子とこの円筒共振子を覆うカバ
ーとの間に形成される部屋内に大気圧又は一定圧
力の気体を封入するようにした卓上用密度計。 A cylindrical resonator having a structure in which each end has a flange portion and at least one end is open so that a fluid to be measured flows in therefrom and the fluid to be measured is filled inside the resonator; a cover that covers the outside of the cylindrical resonator; an excitation means that excites the cylindrical resonator; a detection means that detects the vibration of the cylindrical resonator; one end of which is coupled to at least one of the flange portions or the cover and which vibrates with the excitation means. The case is equipped with a case having an elongated handle that covers a cable connected to the detection means, and the chamber formed between the cylindrical resonator and the cover covering the cylindrical resonator is kept at atmospheric pressure or a constant pressure. A desktop density meter that encloses gas.
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP889381U JPS6126913Y2 (en) | 1981-01-23 | 1981-01-23 | |
US06/330,175 US4429564A (en) | 1981-01-23 | 1981-12-14 | Vibration type density meter |
GB8201395A GB2093998B (en) | 1981-01-23 | 1982-01-19 | Vibration-type density meter |
CA000394732A CA1175544A (en) | 1981-01-23 | 1982-01-22 | Vibration-type density meter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP889381U JPS6126913Y2 (en) | 1981-01-23 | 1981-01-23 |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS57122552U JPS57122552U (en) | 1982-07-30 |
JPS6126913Y2 true JPS6126913Y2 (en) | 1986-08-12 |
Family
ID=29807035
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP889381U Expired JPS6126913Y2 (en) | 1981-01-23 | 1981-01-23 |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6126913Y2 (en) |
-
1981
- 1981-01-23 JP JP889381U patent/JPS6126913Y2/ja not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS57122552U (en) | 1982-07-30 |
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