JPH068498Y2 - Ceramic electromagnetic flowmeter - Google Patents
Ceramic electromagnetic flowmeterInfo
- Publication number
- JPH068498Y2 JPH068498Y2 JP3750688U JP3750688U JPH068498Y2 JP H068498 Y2 JPH068498 Y2 JP H068498Y2 JP 3750688 U JP3750688 U JP 3750688U JP 3750688 U JP3750688 U JP 3750688U JP H068498 Y2 JPH068498 Y2 JP H068498Y2
- Authority
- JP
- Japan
- Prior art keywords
- thermal conductivity
- temperature
- electromagnetic flowmeter
- measuring tube
- measuring
- 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
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- Measuring Volume Flow (AREA)
Description
【考案の詳細な説明】 〈産業上の利用分野〉 本考案はセラミックス製の測定管を有し、高温流体の流
速を測定するセラミックス電磁流量計において、測定管
外表面に接する電装部品を高温から保護するセラミック
ス電磁流量計に関するものである。[Detailed Description of the Invention] <Industrial field of application> The present invention has a ceramic measuring tube, and in a ceramic electromagnetic flowmeter for measuring the flow velocity of a high-temperature fluid, the electrical components in contact with the outer surface of the measuring tube should be protected from high temperature The present invention relates to a ceramic electromagnetic flowmeter to be protected.
〈従来の技術〉 第3図は従来より一般に使用されている従来例の構成説
明図である。<Prior Art> FIG. 3 is an explanatory view of a configuration of a conventional example which is generally used in the past.
図において、1はセラミックス製の円筒状の測定管であ
る。測定管1は、この場合は、アルミナ(Al2O3)が用
いられている。21,22は測定管1に対向して配置さ
れ導電性粉末を混合して測定管1と一体に焼成して形成
された柱状のサーメットの電極部である。In the figure, 1 is a cylindrical measuring tube made of ceramics. In this case, the measuring tube 1 is made of alumina (Al 2 O 3 ). Reference numerals 21 and 22 denote columnar cermet electrode portions which are arranged so as to face the measurement tube 1 and which are formed by mixing conductive powder and firing the mixture together with the measurement tube 1.
〈考案が解決しようとする課題〉 このようなセラミックス電磁流量計においては、測定管
1に磁気回路等の電気部品が外周側から取付けられてい
る為、電機部品の寿命等から、測定流体温度を、余り高
くすることが出来ない。<Problems to be Solved by the Invention> In such a ceramics electromagnetic flowmeter, since the electric parts such as the magnetic circuit are attached to the measuring tube 1 from the outer peripheral side, the measured fluid temperature is changed from the service life of the electric parts. , I can't make it too high.
例えば、内径r124mm、外径r240mmのアルミナの円
筒管(λ=18Kcal/m2hr℃)の内部に90℃の
温水を通し(α1=4000Kcal/m2hr℃=1m
/secの流速)、外面は大気に接するものとする(α
2=7.5Kcal/m2hr℃)とする。For example, hot water at 90 ° C. is passed through an alumina cylindrical tube (λ = 18 Kcal / m 2 hr ° C.) having an inner diameter r 1 24 mm and an outer diameter r 2 40 mm (α 1 = 4000 Kcal / m 2 hr ° C. = 1 m).
/ Velocity), the outer surface is in contact with the atmosphere (α
2 = 7.5 Kcal / m 2 hr ° C.).
α1,α2:熱伝達係数 測定管1の表面温度をtとすると、 熱流速ql={2π(90−t)}/[{1/(400
0×0.012)}+(1/18)1n(0.020/
0.012)]={2π(t−20)}/{1/(7.
5×0.02)} (2π/0.049)(90−t)=(2π/6.6
7)(t−20) 0.049t−0.049×20=6.67×90−
6.67t 6.719t=601.28 t=89.5℃ で定常状態における外面の温度は流体温度とさほど変ら
なくなる。α 1 , α 2 : Heat transfer coefficient If the surface temperature of the measuring tube 1 is t, heat flow rate ql = {2π (90−t)} / [{1 / (400
0 × 0.012)} + (1/18) 1n (0.020 /
0.012)] = {2π (t-20)} / {1 / (7.
5 × 0.02)} (2π / 0.049) (90−t) = (2π / 6.6
7) (t-20) 0.049t-0.049x20 = 6.67x90-
At 6.67t 6.719t = 601.28t = 89.5 ° C., the temperature of the outer surface in the steady state does not change much from the fluid temperature.
このことから、測定管1に接する電装関係部品の寿命等
から、自ずと流体温度には、制限が生ずる。For this reason, the fluid temperature is naturally limited due to the life of the electrical components related to the measuring tube 1.
本考案は、この問題点を、解決するものである。The present invention solves this problem.
本考案の目的は高温側の測定可能範囲を広げ得る性能の
向上されたセラミックス電磁流量計を提供するにある。An object of the present invention is to provide a ceramics electromagnetic flowmeter with improved performance capable of expanding the measurable range on the high temperature side.
〈課題を解決するための手段〉 この目的を達成するために、本考案は、測定流体が流れ
るセラミックス製の測定管を具備するセラミックス電磁
流量計において、 前記測定管が内周から外周方向に熱伝導率が低くなるよ
うに低熱伝導性を有する絶縁性セラミックス粉末に高熱
伝導性を有する絶縁性セラミックス粉末を混合して形成
されたことを特徴とするセラミックス電磁流量計を構成
したものである。<Means for Solving the Problems> In order to achieve this object, the present invention provides a ceramics electromagnetic flowmeter equipped with a ceramics measuring tube through which a measuring fluid flows, wherein the measuring tube is heated from the inner circumference to the outer circumference. The ceramic electromagnetic flowmeter is characterized in that it is formed by mixing an insulating ceramic powder having a low thermal conductivity with an insulating ceramic powder having a high thermal conductivity so as to have a low conductivity.
〈作用〉 以上の構成において、測定管を内周から外周方向に向か
うにつれて熱伝導率を減少させるように構成したので、
測定管外周面の温度を測定流体温度より低くすることが
できる。<Operation> In the above configuration, since the measurement tube is configured to decrease the thermal conductivity from the inner circumference toward the outer circumference,
The temperature of the outer peripheral surface of the measuring pipe can be made lower than the temperature of the measuring fluid.
また、定常状態以外の非定常状態、例えば、熱衝撃的な
測定流体の急激な変化に対しても、有効な温度上昇緩和
が出来る。Further, it is possible to effectively mitigate the temperature rise even in an unsteady state other than the steady state, for example, a rapid change of the measurement fluid due to thermal shock.
以下、実施例に基づき詳細に説明する。Hereinafter, detailed description will be given based on examples.
〈実施例〉 第1図は本考案の一実施例の要部構成説明図で、であ
る。<Embodiment> FIG. 1 is an explanatory view of a main part configuration of an embodiment of the present invention.
図において、第3図と同一記号は同一機能を表わす。In the figure, the same symbols as in FIG. 3 represent the same functions.
3は内周から外周方向に熱伝導率が低くなるように低熱
伝導性を有する絶縁性セラミックス粉末に高熱伝導性を
有する絶縁性セラミックス粉末を混合して形成された測
定管である。Reference numeral 3 is a measuring tube formed by mixing an insulating ceramic powder having a low thermal conductivity with an insulating ceramic powder having a high thermal conductivity so that the thermal conductivity decreases from the inner circumference to the outer circumference.
31,32,33は外周方向に向かって、熱伝導率が低
くなるように熱伝導率を徐々に変化させた部分を示す。Reference numerals 31, 32, and 33 indicate portions in which the thermal conductivity is gradually changed so that the thermal conductivity decreases toward the outer peripheral direction.
この場合は、31部分は熱衝撃性の高い窒化珪素(Si3N
4)で出来ている。In this case, the 31st part is made of silicon nitride (Si 3 N
It is made of 4 ).
32,33部分では、より熱伝導率がかなり低いが、強
度的に勝れたジルコニア(ZrO2)の割合いを、例え
ば、50%,100%にする。The 32 and 33 parts have considerably lower thermal conductivity, but the ratio of zirconia (ZrO 2 ) which is superior in strength is set to, for example, 50% and 100%.
このようにすれば、窒化珪素(Si3N4)の熱伝導率λ31
=0.02cal/cmsec℃=7.2Kcal/m2h
r℃およびジルコニア(ZrO2)の熱伝導率λ33=
0.006cal/cmsec℃=2.16Kcal/m2
hr℃、また、混合部分はリニア則が成立つとして、3
2部分(Si3N450%ZrO250%)の熱伝導率λ32=
4.7Kcal/m2hr℃、 測定管3において、測定流体が90℃のときの測定管3
の外周の温度を求めると、 測定管3、部分31,32,33の半径をr1=0.1
m,r31=0.012m,r32=0.013m,r33=
0.0135mとする。In this way, the thermal conductivity λ 31 of silicon nitride (Si 3 N 4 )
= 0.02 cal / cmsec ° C. = 7.2 Kcal / m 2 h
Thermal conductivity of r ° C. and zirconia (ZrO 2 ) λ 33 =
0.006cal / cmsec ° C = 2.16Kcal / m 2
hr ° C, and assuming that the linear rule holds for the mixed part, 3
Thermal conductivity of 2 parts (Si 3 N 4 50% ZrO 2 50%) λ 32 =
4.7 Kcal / m 2 hr ° C., in measuring tube 3, measuring tube 3 when the measuring fluid is 90 ° C.
When the temperature of the outer circumference of is measured, the radius of the measuring tube 3 and the portions 31, 32, 33 is r 1 = 0.1
m, r 31 = 0.012 m, r 32 = 0.013 m, r 33 =
It will be 0.0135 m.
測定管3の表面温度tとすると、 熱流速ql={2π(90−t)}/[{1/(400
0×0.012)}+(1/7.2)1n(0.013
/0.012)+(1/4.7)1n(0.0135/
0.013)+(1/2.16)1n(0.1/0.0
135)]={2π(t−20)}/{1/(7.5×
0.02)} (2π/0.967)(90−t)=(2π/6.6
7)(t−20) 0.967t−0.967×20=6.67×90−
6.67t 7.637t=619.64 t=81.1℃ で従来より10℃ぐらい低く表面温度を押えることが出
来る。Assuming that the surface temperature t of the measuring pipe 3 is heat flow rate ql = {2π (90−t)} / [{1 / (400
0 × 0.012)} + (1 / 7.2) 1n (0.013
/0.012) + (1 / 4.7) 1n (0.0135 /
0.013) + (1 / 2.16) 1n (0.1 / 0.0
135)] = {2π (t-20)} / {1 / (7.5 ×
0.02)} (2π / 0.967) (90−t) = (2π / 6.6
7) (t-20) 0.967t-0.967x20 = 6.67x90-
6.67t 7.637t = 619.64 t = 81.1 ° C, which is about 10 ° C lower than the conventional surface temperature.
以上の構成において、測定管を内周から外周方向に向か
うにつれて熱伝導率を減少させるように構成したので、
測定管外周面の温度を測定流体温度より低くすることが
できる。In the above configuration, since the measurement tube is configured to decrease the thermal conductivity from the inner circumference toward the outer circumference,
The temperature of the outer peripheral surface of the measuring pipe can be made lower than the temperature of the measuring fluid.
また、定常状態以外の非定常状態、例えば、熱衝撃的な
測定流体の急激な変化に対しても、有効な温度上昇緩和
が出来る。Further, it is possible to effectively mitigate the temperature rise even in an unsteady state other than the steady state, for example, a rapid change of the measurement fluid due to thermal shock.
この結果、測定管3の表面の温度を流体温度より低くす
ることができ、電装部品等の信頼性の改善を図る事がで
きる。As a result, the temperature of the surface of the measuring tube 3 can be made lower than the fluid temperature, and the reliability of electrical components and the like can be improved.
第2図は本考案の他の実施例の要部構成説明図である。FIG. 2 is an explanatory view of the essential structure of another embodiment of the present invention.
本実施例においては、測定管3の内周から外周方向の途
中に、熱伝導率の最も低い33部分を設けたものであ
る。In this embodiment, 33 parts having the lowest thermal conductivity are provided midway from the inner circumference to the outer circumference of the measuring tube 3.
〈考案の効果〉 以上説明したように、本考案は、測定流体が流れるセラ
ミックス製の測定管を具備するセラミックス電磁流量計
において、 前記測定管が内周から外周方向に熱伝導率が低くなるよ
うに低熱伝導性を有する絶縁性セラミックス粉末に高熱
伝導性を有する絶縁性セラミックス粉末を混合して形成
されたことを特徴とするセラミックス電磁流量計を構成
した。<Effects of the Invention> As described above, the present invention provides a ceramics electromagnetic flowmeter having a ceramics measuring tube through which a measuring fluid flows, so that the measuring tube has a low thermal conductivity from the inner circumference to the outer circumference. A ceramic electromagnetic flowmeter was constructed by mixing an insulating ceramic powder having low thermal conductivity with an insulating ceramic powder having high thermal conductivity.
すなわち、測定管を内周から外周方向に向かうにつれて
熱伝導率を減少させるように構成したので、測定管外周
面の温度を測定流体温度より低くすることができる。That is, since the thermal conductivity of the measuring pipe is reduced from the inner circumference toward the outer circumference, the temperature of the outer circumferential surface of the measuring pipe can be lower than the temperature of the measuring fluid.
また、定常状態以外の非定常状態、例えば、熱衝撃的な
測定流体の急激な変化に対しても、有効な温度上昇緩和
が出来る。Further, it is possible to effectively mitigate the temperature rise even in an unsteady state other than the steady state, for example, a rapid change of the measurement fluid due to thermal shock.
この結果、測定管の表面の温度を流体温度より低くする
ことができ、電装部品等の信頼性の改善を図る事ができ
る。As a result, the temperature of the surface of the measuring tube can be made lower than the fluid temperature, and the reliability of electrical components and the like can be improved.
したがって、本考案によれば、高温側の測定可能範囲を
広げ得る性能の向上されたセラミックス電磁流量計を実
現することができる。Therefore, according to the present invention, it is possible to realize a ceramics electromagnetic flowmeter with improved performance capable of expanding the measurable range on the high temperature side.
第1図は本考案の一実施例の要部構成説明図、第2図は
本考案の他の実施例の要部構成説明図、第3図は従来よ
り一般に使用されている従来例の構成説明図である。 21,22……電極部、3……測定管、31,32,3
3……部分。FIG. 1 is an explanatory view of a main part configuration of an embodiment of the present invention, FIG. 2 is an explanatory view of a main part configuration of another embodiment of the present invention, and FIG. 3 is a structure of a conventional example which is generally used conventionally. FIG. 21, 22 ... Electrode part, 3 ... Measuring tube, 31, 32, 3
3 ... part.
Claims (1)
を具備するセラミックス電磁流量計において、 前記測定管が内周から外周方向に熱伝導率が低くなるよ
うに低熱伝導性を有する絶縁性セラミックス粉末に高熱
伝導性を有する絶縁性セラミックス粉末を混合して形成
されたことを特徴とするセラミックス電磁流量計。1. A ceramic electromagnetic flowmeter comprising a ceramic measuring tube through which a measuring fluid flows, the insulating ceramic powder having low thermal conductivity such that the measuring tube has a low thermal conductivity from the inner circumference to the outer circumference. A ceramics electromagnetic flowmeter, characterized by being formed by mixing an insulating ceramics powder having high thermal conductivity with.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3750688U JPH068498Y2 (en) | 1988-03-22 | 1988-03-22 | Ceramic electromagnetic flowmeter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3750688U JPH068498Y2 (en) | 1988-03-22 | 1988-03-22 | Ceramic electromagnetic flowmeter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01141412U JPH01141412U (en) | 1989-09-28 |
| JPH068498Y2 true JPH068498Y2 (en) | 1994-03-02 |
Family
ID=31264086
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3750688U Expired - Lifetime JPH068498Y2 (en) | 1988-03-22 | 1988-03-22 | Ceramic electromagnetic flowmeter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH068498Y2 (en) |
-
1988
- 1988-03-22 JP JP3750688U patent/JPH068498Y2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01141412U (en) | 1989-09-28 |
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