JPH0145853B2 - - Google Patents
Info
- Publication number
- JPH0145853B2 JPH0145853B2 JP57121273A JP12127382A JPH0145853B2 JP H0145853 B2 JPH0145853 B2 JP H0145853B2 JP 57121273 A JP57121273 A JP 57121273A JP 12127382 A JP12127382 A JP 12127382A JP H0145853 B2 JPH0145853 B2 JP H0145853B2
- Authority
- JP
- Japan
- Prior art keywords
- hot wire
- wire
- electric circuit
- lead
- retaining ring
- 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
- 239000000463 material Substances 0.000 claims description 19
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 claims description 18
- 239000012530 fluid Substances 0.000 claims 1
- 230000000149 penetrating effect Effects 0.000 claims 1
- 239000011521 glass Substances 0.000 description 5
- 229910000990 Ni alloy Inorganic materials 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 229910001030 Iron–nickel alloy Inorganic materials 0.000 description 1
- 238000002485 combustion reaction Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 238000007665 sagging Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/68—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using thermal effects
Landscapes
- Physics & Mathematics (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Volume Flow (AREA)
Description
【発明の詳細な説明】
本発明は熱線流量計に関し、特に熱線と電気回
路とを接続するリード線の構成に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a hot wire flowmeter, and particularly to the structure of a lead wire that connects a hot wire and an electric circuit.
従来の熱線流量計としては、例えば第1図〜第
4図に示すようなものがある。 Examples of conventional hot wire flowmeters include those shown in FIGS. 1 to 4.
これについて説明すると、例えば内燃機関の吸
入空気の通路1中に配設される保持リング2には
その壁部に4つの孔が形成されており、そのうち
2つの孔には電気回路と接続されるリード線3の
先端部付近をガラス4により封着(ガラスの粉を
入れて焼付)した小リング5を嵌合固着(ハンダ
付)し、これらリード線3の先端部を保持リング
2内に位置させてある。また、他の2つの孔には
リード線3の代わりにフツク6をガラス4により
封着した小リング5を嵌合固着し、これらフツク
6も保持リング2内に位置させてある。保持リン
グ2内には一対のリード線3の先端部間に途中で
2つのフツク6に係止させることによりコ字状に
して熱線(一般に白金線)7を張設してある。 To explain this, for example, a retaining ring 2 disposed in an intake air passage 1 of an internal combustion engine has four holes formed in its wall, two of which are connected to an electric circuit. A small ring 5 sealed (filled with glass powder and baked) with glass 4 near the tips of the lead wires 3 is fitted and fixed (soldered), and the tips of these lead wires 3 are positioned inside the retaining ring 2. I've let it happen. Furthermore, in place of the lead wires 3, small rings 5 having hooks 6 sealed with glass 4 are fitted and fixed in the other two holes, and these hooks 6 are also located within the retaining ring 2. Inside the retaining ring 2, a hot wire (generally a platinum wire) 7 is stretched in a U-shape by being engaged with two hooks 6 midway between the tips of a pair of lead wires 3.
そして、リード線3と電気回路との接続によ
り、回路的には第4図に示すように、熱線7
(Rh)と抵抗R1〜R3(R1は温度補償抵抗、R2は流
量調整抵抗、R3は基準抵抗)とによりブリツジ
回路が構成される。尚、図中R11及びR12はリ
ード線3の抵抗を示している。また、このブリツ
ジ回路への供給電流は、抵抗R2の端子電圧と抵
抗R3の端子電圧とに基づき差動増幅器8及びト
ランジスタ9,10を介して制御されるようにな
つている。例えば、流速が増大すると、熱線Rh
がより冷却されることによりその抵抗値が減少す
るが、このとき抵抗R3の端子電圧が増大して、
差動増幅器8の出力が低下し、これによりトラン
ジスタ9,10を介してブリツジ回路への供給電
流が増大するつまり、流速の変化に対し熱線Rh
の抵抗値を一定{Rh=R1・R3/R2−(R11+R
12)}に保つように供給電流を変化させ、抵抗
R3の端子電圧Umから流速を読取るのである。 By connecting the lead wire 3 and the electric circuit, the hot wire 7 is connected to the electric circuit as shown in FIG.
(Rh) and resistors R 1 to R 3 (R 1 is a temperature compensation resistor, R 2 is a flow rate adjustment resistor, and R 3 is a reference resistor) constitute a bridge circuit. Note that R1 1 and R1 2 in the figure indicate the resistance of the lead wire 3. Further, the current supplied to this bridge circuit is controlled via the differential amplifier 8 and transistors 9 and 10 based on the terminal voltage of the resistor R 2 and the terminal voltage of the resistor R 3 . For example, as the flow rate increases, the hot wire Rh
As it cools further, its resistance value decreases, but at this time the terminal voltage of resistor R3 increases,
The output of the differential amplifier 8 decreases, and the current supplied to the bridge circuit via the transistors 9 and 10 increases.
Keep the resistance value constant {Rh=R 1・R 3 /R 2 −(R1 1 +R
1 2 )}, and the resistance
The flow velocity is read from the terminal voltage Um of R3 .
ところで、リード線3は、熱線7架設後に熱線
7にたるみが発生しない様な剛性を有すること、
及び、熱線7とほぼ同等の線膨張係数を有するこ
と、を条件として材質が選定される。 By the way, the lead wire 3 should have such rigidity that no slack will occur in the hot wire 7 after the hot wire 7 is installed.
The material is selected on the condition that it has a coefficient of linear expansion that is almost the same as that of the hot wire 7.
このため従来は、上記の条件を満たすものとし
て、Fe−Ni合金又はNi線を使用していた。 For this reason, conventionally, Fe--Ni alloy or Ni wire has been used as a material that satisfies the above conditions.
しかしながら、リード線3の材料としてこれら
のものを使用すると、Fe−Niでは抵抗値が2.99
mΩ/mm、抵抗温度係数が3577ppm/℃、Niで
は抵抗値が0.763mΩ/mm、抵抗温度係数が
4702ppm/℃と、抵抗値が大きいばかりか、抵抗
温度係数も大きいため、熱線7への通電開始直後
と通電開始数分後ではリード線3自体の電流によ
る発熱により、それらの抵抗値(R11,R12)
が大きく変化し、これに基づいて熱線7の抵抗値
(Rh)すなわち熱線7への供給電流が変化してし
まい、第5図に示す如く、通電開始直後には同一
流量でも流量計の出力値が変化し、安定状態とな
るまでに時間がかかるという問題点があつた。 However, when these materials are used for the lead wire 3, the resistance value of Fe-Ni is 2.99.
mΩ/mm, resistance temperature coefficient is 3577ppm/℃, resistance value is 0.763mΩ/mm, resistance temperature coefficient is 0.763mΩ/mm for Ni.
4702ppm/℃, which is not only a large resistance value, but also a large resistance temperature coefficient. , R1 2 )
changes greatly, and based on this, the resistance value (Rh) of the hot wire 7, that is, the current supplied to the hot wire 7 changes. The problem was that it took a long time to change and reach a stable state.
本発明はこのような従来の問題点に鑑みてなさ
れたもので、リード線の保持リングにより保持さ
れる部分から熱線の取付部側は従来と同じ材料と
するが、電気回路との接続部側を別材料すなわち
電流値の変化に対して抵抗値の変化の少ない材
料、言換えれば抵抗値若しくは抵抗温度係数の少
なくとも一方が小さい材料で形成し、各材料でそ
れぞれ形成されたものをつなぎ合わせて使用する
ことにより、熱線を確実に支持しながらも、通電
開始直後から安定した特性が得られるようにした
ものである。 The present invention was made in view of such conventional problems, and the part from the part held by the lead wire holding ring to the hot wire mounting part side is made of the same material as in the past, but the part connected to the electric circuit is made of the same material as in the past. are made of a different material, that is, a material whose resistance value changes little with changes in current value, in other words, a material with a small resistance value or a small resistance temperature coefficient, and the parts made of each material are connected together. By using it, stable characteristics can be obtained immediately after the start of energization while supporting the hot wire reliably.
以下、本発明を第6図に示す一実施例に基づい
て説明する。 The present invention will be explained below based on an embodiment shown in FIG.
熱線の取付部側のリード線11は従来と同じ材
料、すなわち、熱線を確実に支持し得るに十分な
剛性を有し、且つ熱線とほぼ同等の線膨張係数を
有する材料、具体的にはFe−Ni合金又はNi線に
より形成し、小リング5を貫通させてガラス4に
より封着する。そして、このリード線11に電気
回路との接続部側のリード線12を接続する。 The lead wire 11 on the side where the hot wire is attached is made of the same material as the conventional material, that is, a material that has sufficient rigidity to reliably support the hot wire and has a coefficient of linear expansion almost equal to that of the hot wire, specifically Fe. - It is made of Ni alloy or Ni wire, and is sealed with glass 4 through which the small ring 5 passes. Then, a lead wire 12 on the connection portion side with an electric circuit is connected to this lead wire 11.
電気回路との接続部側のリード線12は、抵抗
値及び抵抗温度係数の小さい材料、例えばCu線
(抵抗値0.068mΩ/mm、抵抗温度係数1040ppm/
℃)により形成する。 The lead wire 12 on the connection side with the electric circuit is made of a material with a low resistance value and temperature coefficient of resistance, such as Cu wire (resistance value 0.068 mΩ/mm, temperature coefficient of resistance 1040 ppm/
℃).
このようにすれば、熱線と電気回路との間のほ
とんどの部分は抵抗値及び抵抗温度係数の小さい
リード線12により構成されるから、前記R11,
R12が小さいばかりか、それらの温度変化が少
なく、これにより前記Rhの値の変化も小さくな
り、通電開始後の出力変化が小さくなる。よつ
て、通電開始直後から安定した測定精度が得られ
る。 In this way, most of the portion between the hot wire and the electric circuit is constituted by the lead wire 12 having a small resistance value and resistance temperature coefficient, so that the R1 1 ,
Not only is R1 2 small, but the temperature change therein is also small, so the change in the value of Rh is also small, and the output change after the start of energization is small. Therefore, stable measurement accuracy can be obtained immediately after the start of energization.
また、熱線の取付部については十分な剛性を有
するリード線11により構成されるから、熱線の
たるみ等も防止できる。 Furthermore, since the hot wire attachment portion is constructed of the lead wire 11 having sufficient rigidity, it is possible to prevent the hot wire from sagging.
以上説明したように本発明によれば、熱線と電
気回路とをつなぐリード線のうち熱線の取付部側
を比較的剛性を有する材料で形成し、電気回路と
の接続部側を電気が流れることにより抵抗値の変
化が少ない材料で形成するようにしたため、リー
ド線の影響による通常開始直後の出力特性の変化
を抑制して安定した特性を得ることができる一
方、熱線を確実に支持できてたるみ等を防止でき
るという効果が得られる。 As explained above, according to the present invention, among the lead wires that connect the hot wire and the electric circuit, the side where the hot wire is attached is made of a relatively rigid material, and electricity flows through the side where the hot wire is connected to the electric circuit. Since it is made of a material that has a small change in resistance value, it is possible to suppress changes in the output characteristics immediately after the start due to the influence of the lead wires and obtain stable characteristics. This has the effect of preventing such problems.
第1図は従来例を示す熱線流量計の要部斜視
図、第2図は同上の断面図、第3図は第1図中の
リード線の斜視図、第4図は熱線流量計の回路
図、第5図は従来における通電開始後の出力特性
の変化の様子を示す線図、第6図は本発明の一実
施例を示すリード線の斜視図である。
1……吸入空気通路、2……保持リング、4…
…ガラス、5……小リング、6……フツク、7,
Rh……熱線、11……熱線の取付部側のリード
線、12……電気回路との接続部側のリード線。
Fig. 1 is a perspective view of the main parts of a conventional hot wire flowmeter, Fig. 2 is a sectional view of the same as above, Fig. 3 is a perspective view of the lead wire in Fig. 1, and Fig. 4 is a circuit of the hot wire flowmeter. 5 is a diagram showing how the output characteristics change after the start of energization in the conventional case, and FIG. 6 is a perspective view of a lead wire showing an embodiment of the present invention. 1...Intake air passage, 2...Retaining ring, 4...
...Glass, 5...Small ring, 6...Hook, 7,
Rh...Heat wire, 11...Lead wire on the side where the heat wire is attached, 12...Lead wire on the side where it connects to the electric circuit.
Claims (1)
の壁部を貫通させて電気回路とつながれた一対の
リード線を保持させ、保持リング内の一対のリー
ド線間に熱線を取付けてなる熱線流量計におい
て、前記リード線の保持リングにより保持される
部分から熱線の取付部側を比較的剛性を有する材
料で形成し、前記部分より電気回路との接続部側
を電流値の変化に対して抵抗値の変化の少ない材
料で形成したことを特徴とする熱線流量計。1 A hot wire made by holding a pair of lead wires connected to an electric circuit by penetrating the wall of a retaining ring disposed in a fluid passage, and attaching a hot wire between the pair of lead wires inside the retaining ring. In the flowmeter, the part of the lead wire held by the retaining ring to the hot wire attachment part is made of a relatively rigid material, and the part connected to the electric circuit is made of a relatively rigid material, and the part of the lead wire that is connected to the electric circuit is made of a material that is resistant to changes in current value. A hot wire flowmeter characterized by being made of a material with little change in resistance value.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57121273A JPS5912315A (en) | 1982-07-14 | 1982-07-14 | Hot wire flowmeter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57121273A JPS5912315A (en) | 1982-07-14 | 1982-07-14 | Hot wire flowmeter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5912315A JPS5912315A (en) | 1984-01-23 |
| JPH0145853B2 true JPH0145853B2 (en) | 1989-10-05 |
Family
ID=14807166
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57121273A Granted JPS5912315A (en) | 1982-07-14 | 1982-07-14 | Hot wire flowmeter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5912315A (en) |
-
1982
- 1982-07-14 JP JP57121273A patent/JPS5912315A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5912315A (en) | 1984-01-23 |
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