JPH10160620A - Flow measurement device and flow distribution measurement device using the same - Google Patents
Flow measurement device and flow distribution measurement device using the sameInfo
- Publication number
- JPH10160620A JPH10160620A JP31902096A JP31902096A JPH10160620A JP H10160620 A JPH10160620 A JP H10160620A JP 31902096 A JP31902096 A JP 31902096A JP 31902096 A JP31902096 A JP 31902096A JP H10160620 A JPH10160620 A JP H10160620A
- Authority
- JP
- Japan
- Prior art keywords
- flow
- round bar
- sensor head
- metal films
- current
- 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.)
- Pending
Links
- 238000005259 measurement Methods 0.000 title claims abstract description 13
- 229910052751 metal Inorganic materials 0.000 claims abstract description 45
- 239000002184 metal Substances 0.000 claims abstract description 45
- 238000010438 heat treatment Methods 0.000 claims description 2
- 238000010586 diagram Methods 0.000 description 6
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 229910052720 vanadium Inorganic materials 0.000 description 2
- 239000000919 ceramic Substances 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 230000020169 heat generation Effects 0.000 description 1
- 229910052759 nickel Inorganic materials 0.000 description 1
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Aerodynamic Tests, Hydrodynamic Tests, Wind Tunnels, And Water Tanks (AREA)
Abstract
(57)【要約】
【課題】 狭いスペースの気体の流れ分布を計測する流
れ計測装置と流れ分布計測装置を提供する。
【解決手段】 間隔を隔てて配置され流れにほぼ直交す
る方向に軸方向を有する丸棒状の複数のセンサヘッド1
と、この各センサヘッド1に通電して加熱しこの発熱量
とセンサヘッド1周囲を流れる気体により奪われる熱量
とが平衡したときの電流値を用いて各センサヘッド1周
囲を流れる気体の流速と流れ角を演算する計測演算装置
3と、を備え、センサヘッド1は、絶縁性の丸棒4と、
この丸棒表面に付着した2枚の金属膜5a,5bとから
なり、この2枚の金属膜5a,5bは同一面積を有し丸
棒4の所定方向の直径に対して周方向に間隔を隔てて線
対称に配置され、前記所定方向は各丸棒とも同一方向で
あり、計測演算装置3は各金属膜5a,5bに電流を流
す。
(57) [Problem] To provide a flow measuring device and a flow distribution measuring device for measuring a flow distribution of a gas in a narrow space. SOLUTION: A plurality of round bar-shaped sensor heads 1 arranged at intervals and having an axial direction in a direction substantially orthogonal to the flow.
The current flowing through each sensor head 1 and the flow rate of the gas flowing around each sensor head 1 are calculated using the current value when the amount of heat generated and the amount of heat generated by the gas flowing around the sensor head 1 are balanced. A measurement calculation device 3 for calculating a flow angle, wherein the sensor head 1 includes an insulating round bar 4,
It consists of two metal films 5a and 5b attached to the surface of the round bar. The two metal films 5a and 5b have the same area and are spaced apart from each other in the circumferential direction with respect to the diameter of the round bar 4 in a predetermined direction. The predetermined direction is the same direction as each of the round bars, and the measurement and calculation device 3 causes a current to flow through each of the metal films 5a and 5b.
Description
【0001】[0001]
【発明の属する技術分野】本発明は、翼等の後方の流れ
とその分布を計測する計測装置に係わり、特に狭隘なス
ペースにおける流れおよびその分布を計測する装置に関
する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a measuring device for measuring a flow behind a wing or the like and its distribution, and more particularly to a device for measuring a flow and a distribution in a narrow space.
【0002】[0002]
【従来の技術】ファン圧縮機等の性能を把握するために
は、静翼のウェーク分布、つまり静翼後方の流れ分布を
計測する必要がある。従来は図5に示すように熊手2
(rake)型の支持具の先にセンサヘッド1を設け、
このセンサヘッド1にピトー管を設け流速分布を計測し
ていた。しかしピトー管では流れ角が計測できない。こ
のため図6に示すようにピトー管に代えてホットワイヤ
を交差したX型ホットワイヤを用いて流れ角を計測する
ことも行われている。このホットワイヤとは熱線風速計
に用いる白金線やタングステン線のことで、これに電流
を流して加熱し流体によって奪われる熱量と加熱による
熱量が平衡したときの電流から流体の流速が計測され
る。このホットワイヤを交差し両ホットワイヤの熱量の
比と両ホットワイヤに流入する流体の流れ角との関係を
表す実験データより流れ角を算出することができる。2. Description of the Related Art In order to grasp the performance of a fan compressor or the like, it is necessary to measure a wake distribution of a stationary blade, that is, a flow distribution behind a stationary blade. Conventionally, as shown in FIG.
The sensor head 1 is provided at the tip of the (rake) type support,
The sensor head 1 was provided with a pitot tube to measure the flow velocity distribution. However, the pitot tube cannot measure the flow angle. Therefore, as shown in FIG. 6, an X-type hot wire crossing a hot wire is used instead of the pitot tube to measure the flow angle. The hot wire is a platinum wire or a tungsten wire used for a hot wire anemometer. The current is applied to the wire and heated. . The flow angle can be calculated from experimental data representing the relationship between the ratio of the calorific value of the two hot wires and the flow angle of the fluid flowing into the two hot wires.
【0003】[0003]
【発明が解決しようとする課題】このようなX型ホット
ワイヤで流れ角を計測する場合、Xの幅は5mm程度必
要であり、図5に示す熊手2に取り付けた場合、熊手2
の幅は25mm程度の幅となる。一方、小型の圧縮機の
静翼のウェーキ分布を計測するには、熊手2の幅は大き
くても5mm以内、つまり1mmピッチ程度で流速と流
れ角の分布を計測することが望ましい。When measuring the flow angle with such an X-type hot wire, the width of X needs to be about 5 mm, and when it is attached to the rake 2 shown in FIG.
Has a width of about 25 mm. On the other hand, in order to measure the wake distribution of the stator vanes of a small compressor, it is desirable to measure the distribution of the flow velocity and the flow angle at a pitch of at most 5 mm, that is, about 1 mm pitch, when the rake 2 is wide.
【0004】本発明は、上述の問題点に鑑みてなされた
もので、狭いスペースの気体の流れおよびこの分布を計
測する流れとその分布計測装置を提供することを目的と
する。The present invention has been made in view of the above problems, and has as its object to provide a gas flow in a narrow space, a flow for measuring the distribution of the gas, and a distribution measuring device therefor.
【0005】[0005]
【課題を解決するための手段】上記目的を達成するた
め、請求項1の発明では、丸棒状のセンサヘッドと、こ
のセンサヘッドに通電して加熱しこの発熱量とセンサヘ
ッド周囲を流れる気体により奪われる熱量とが平衡した
ときの電流値を用いてセンサヘッド周囲を流れる気体の
流速と流れ角を演算する計測演算装置と、を備え、前記
センサヘッドは、絶縁性の丸棒と、この丸棒表面に付着
した2枚の金属膜とからなり、この2枚の金属膜は同一
面積を有し丸棒の所定方向の直径に対して周方向に間隔
を隔てて線対称に配置され、前記計測演算装置は各金属
膜に電流を流す。In order to achieve the above object, according to the first aspect of the present invention, a round-bar-shaped sensor head, and an electric power supplied to the sensor head for heating, the amount of generated heat and a gas flowing around the sensor head. A measuring and calculating device for calculating the flow velocity and the flow angle of the gas flowing around the sensor head using the current value when the amount of heat deprived is equilibrated, wherein the sensor head has an insulating round bar, The two metal films have the same area and are arranged symmetrically at a circumferential distance with respect to the diameter of the round bar in a predetermined direction; The measurement operation device applies a current to each metal film.
【0006】丸棒には2枚の同一面積を有する金属膜が
間隙を有することにより互いに絶縁されて1つの直径に
対し線対称に付着している。各金属膜は通電される。丸
棒の2枚の金属膜の発熱量と周囲を流れる気体によって
奪われる熱量が平衡したときの電流値に基づく発熱量と
気体の流速との関係を予め実験的に求めておくことによ
り気体の流速を得ることができる。また平衡したときの
それぞれの金属膜の発熱量と気体の流れ角との関係を予
め実験的に求めておき、通電した電流から各金属膜の発
熱量を求め気体の流れ角を得ることができる。[0006] Two metal films having the same area are insulated from each other by a gap and are attached line-symmetrically to one diameter on the round bar. Each metal film is energized. The relationship between the calorific value based on the current value and the gas flow rate based on the current value when the calorific value of the two metal films of the round bar and the calorie removed by the gas flowing around are equilibrium is obtained experimentally in advance. A flow rate can be obtained. In addition, the relationship between the calorific value of each metal film and the gas flow angle when equilibrated is experimentally obtained in advance, and the calorific value of each metal film can be obtained from the supplied current to obtain the gas flow angle. .
【0007】請求項2の発明では、間隔を隔てて配置さ
れ流れにほぼ直交する方向に軸方向を有する丸棒状の複
数のセンサヘッドと、この各センサヘッドに通電して加
熱しこの発熱量とセンサヘッド周囲を流れる気体により
奪われる熱量とが平衡したときの電流値を用いて各セン
サヘッド周囲を流れる気体の流速と流れ角を演算する計
測演算装置と、を備え、前記センサヘッドは、絶縁性の
丸棒と、この丸棒表面に付着した2枚の金属膜とからな
り、この2枚の金属膜は同一面積を有し丸棒の所定方向
の直径に対して周方向に間隔を隔てて線対称に配置さ
れ、前記所定方向は各丸棒とも同一方向であり、前記計
測演算装置は各金属膜に電流を流す。According to the second aspect of the present invention, a plurality of round bar-shaped sensor heads which are arranged at intervals and have an axial direction substantially perpendicular to the flow, and each of the sensor heads is energized and heated to generate heat. A measurement calculation device that calculates the flow velocity and flow angle of the gas flowing around each sensor head using the current value when the amount of heat taken by the gas flowing around the sensor head is balanced, and wherein the sensor head is insulated. Of a round bar and two metal films attached to the surface of the round bar. The two metal films have the same area and are spaced apart from each other in the circumferential direction with respect to the diameter of the round bar in a predetermined direction. And the predetermined direction is the same direction as each of the round bars, and the measurement and calculation device causes a current to flow through each metal film.
【0008】各丸棒には同一面積を有する2枚の金属膜
が間隙を有することにより互いに絶縁されて1つの直径
に対して線対称に付着されており、この金属膜は通電さ
れる。各丸棒の2枚の金属膜の発熱量と周囲を流れる気
体によって奪われる熱量が平衡したときの電流値と気体
の流速との関係を予め実験的に求めておくことにより気
体の流速を得ることができる。また平衡したときの両金
属膜の発熱量と気体の流れ角との関係を予め実験的に求
めておき、通電した電流から各金属膜の発熱量を求め気
体の流れ角を得ることができる。このような金属膜の付
着した丸棒を複数間隔を隔てて配置することにより、流
れの速度および流れ角の分布を得ることができる。な
お、丸棒の直径はX型ホットワイヤよりもかなり小さく
ても流速と流れ角の測定が可能であり、5本の手を有す
る熊手に取りつけた場合熊手の幅も小さくできるので、
狭隘なスペースの流れの分布を計測することができる。Each round bar is provided with two metal films having the same area, which are insulated from each other by having a gap and are attached in line symmetry with respect to one diameter, and the metal films are energized. The flow rate of the gas is obtained by experimentally obtaining in advance the relationship between the current value and the flow rate of the gas when the calorific value of the two metal films of each round bar and the heat quantity taken away by the gas flowing around are balanced. be able to. In addition, the relationship between the calorific value of both metal films and the gas flow angle when equilibrated is experimentally obtained in advance, and the calorific value of each metal film can be obtained from the supplied current to obtain the gas flow angle. By arranging such round bars with the metal film at a plurality of intervals, a distribution of flow velocity and flow angle can be obtained. In addition, even if the diameter of the round bar is considerably smaller than the X-type hot wire, the flow velocity and the flow angle can be measured, and the width of the rake can be reduced when it is attached to a rake having five hands.
The distribution of flow in a narrow space can be measured.
【0009】[0009]
【発明の実施の形態】以下、本発明の実施の形態につい
て図面を参照して説明する。図1は本発明の実施形態を
示す斜視図である。円筒状のセンサヘッド1は所定の間
隔で垂直に配置され、熊手2によって流れを乱さないよ
うに支持されている。計測演算装置3は各センサヘッド
1に電流を供給するとともにその電流値とセンサヘッド
1の抵抗値等から流れ速度、流れ角等を演算する。セン
サヘッド1は絶縁性の丸棒4、例えばセラミックスに金
属膜5を蒸着したもので、金属としてはニッケル等が用
いられる。金属膜5は1つの直径を線対称として配置さ
れた2つの金属膜5a,5bからなる。この金属膜5
a,5bは同一の面積を有し、1つの直径の方向は全て
のセンサヘッド1で同一であり、熊手2の前後方向とな
っている。熊手2は静翼6の後流に設定される。Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is a perspective view showing an embodiment of the present invention. The cylindrical sensor heads 1 are vertically arranged at predetermined intervals and supported by a rake 2 so as not to disturb the flow. The measurement calculation device 3 supplies a current to each sensor head 1 and calculates a flow velocity, a flow angle, and the like from the current value and the resistance value of the sensor head 1. The sensor head 1 is formed by depositing a metal film 5 on an insulating round bar 4, for example, ceramics, and uses nickel or the like as a metal. The metal film 5 is composed of two metal films 5a and 5b arranged so that one diameter is line-symmetric. This metal film 5
a and 5b have the same area, and the direction of one diameter is the same in all the sensor heads 1 and is the front-back direction of the rake 2. The rake 2 is set downstream of the stationary blade 6.
【0010】図2はセンサヘッド1と静翼6の断面図で
ある。各センサヘッド1は同一の直径方向を中心に対称
に金属膜5a,5bが蒸着され、両金属膜5a,5bは
間隙7により隔てられている。各金属膜5a,5bには
図示しない導線により電流が供給される。寸法の一例を
示すと、丸棒4の直径は0.2mm、金属膜5は1〜1
0μm程度であり、各センサヘッド1の中心間距離は
0.4〜0.6mm程度で、5本手の熊手2の場合全幅
3mm程度である。FIG. 2 is a sectional view of the sensor head 1 and the stationary blade 6. In each sensor head 1, metal films 5a and 5b are deposited symmetrically about the same diametric direction, and both metal films 5a and 5b are separated by a gap 7. A current is supplied to each of the metal films 5a and 5b by a conductor (not shown). As an example of the dimensions, the diameter of the round bar 4 is 0.2 mm, and the metal film 5 is 1-1.
The distance between the centers of the sensor heads 1 is about 0.4 to 0.6 mm, and the total width of the five rakes 2 is about 3 mm.
【0011】流速は熱線風速計と同様な方法により演算
される。金属膜5に電流を通して加熱し、気体の中に置
くと、丸棒4の軸方向金属膜5の単位長さ当たり失われ
る熱量Hと流速vの間には次式が成り立つ。 H=B√v+C …(1) ここでB,Cは装置定数である。金属膜5の電気抵抗を
R、電流をIとすれば、(1)式は次のようになる。 I2 R=B√v+C …(2)The flow velocity is calculated by a method similar to that of the hot wire anemometer. When the metal film 5 is heated by passing an electric current through the metal film 5 and placed in a gas, the following equation is established between the amount of heat H lost per unit length of the metal film 5 in the axial direction of the round bar 4 and the flow velocity v. H = B√v + C (1) where B and C are device constants. If the electric resistance of the metal film 5 is R and the current is I, the equation (1) is as follows. I 2 R = B√v + C (2)
【0012】供給する熱量と気体により失われる熱量が
平衡したとき、つまり通電する電流値が一定値に落ち着
いたときの電流値IS を(2)式に代入することにより
流速vを求めることができる。この場合の電流Iは金属
膜5a,5bを直列に接続したときの電流とするとよ
い。なお電圧をVとすればV=IRであるので、(2)
の左辺はIVで表すことができ、これにより抵抗Rの値
(これは温度により変化する)は必ずしも必要ではな
い。When the amount of heat to be supplied and the amount of heat lost by the gas are balanced, that is, the current value I S at the time when the value of the supplied current has settled to a constant value is substituted into the equation (2) to obtain the flow velocity v. it can. The current I in this case may be a current when the metal films 5a and 5b are connected in series. Note that if the voltage is V, V = IR, so (2)
Can be represented by IV, so that the value of the resistor R (which varies with temperature) is not necessary.
【0013】図3は測定した流速vの一例を示す図であ
る。横軸は時間を表し、縦軸は流速vを示す。流速vは
こきざみに変動しており、平均値をvm、変動幅をΔv
とすると、変動幅と平均値との比Δv/vm(乱れ度)
を得ることができる。FIG. 3 is a diagram showing an example of the measured flow velocity v. The horizontal axis represents time, and the vertical axis represents flow velocity v. The flow velocity v fluctuates in steps, the average value is vm, and the fluctuation width is Δv
Then, the ratio Δv / vm (fluctuation degree) between the fluctuation width and the average value
Can be obtained.
【0014】図4は流れ角θの算出方法を説明する図で
ある。(A)は金属膜5a,5b、流れ角θの関係を示
す。(B)は金属膜5aで発生している熱量Ea、金属
膜5bで発生している熱量Ebと流れ角θとの関係を示
す図である。各熱量Ea,Ebは金属膜5a,5bに供
給される熱量とこの周囲を流れる気体によって奪われる
熱量が平衡したときの熱量である。平衡したか否かは供
給する電流が一定値に落ち着いたか否かで判定でき、こ
の一定値の電流より各熱量Ea,Ebを算出することが
できる。なおEaとEbから算出した流れ角θが相違す
るときは、平均の角度θmをとるようにするとよい。FIG. 4 is a diagram for explaining a method of calculating the flow angle θ. (A) shows the relationship between the metal films 5a and 5b and the flow angle θ. (B) is a diagram showing the relationship between the amount of heat Ea generated in the metal film 5a, the amount of heat Eb generated in the metal film 5b, and the flow angle θ. The amounts of heat Ea and Eb are the amounts of heat when the amount of heat supplied to the metal films 5a and 5b and the amount of heat taken by the gas flowing therearound are balanced. Whether or not equilibrium can be determined by whether or not the supplied current has settled to a constant value, and the heat amounts Ea and Eb can be calculated from the constant value current. When the flow angle θ calculated from Ea and Eb is different, it is preferable to take an average angle θm.
【0015】[0015]
【発明の効果】以上の説明より明らかなように、本発明
は、丸棒に2枚の金属膜を付着したセンサヘッドに通電
して発熱量を計測することにより、流速、流れ角、さら
に乱れ度を算出することができる。またこのセンサヘッ
ドを熊手の手にそれぞれ設けることにより極めてコンパ
クトな流れ分布計測装置を得ることができる。As is apparent from the above description, according to the present invention, the current flow rate, the flow angle, and the turbulence are further measured by applying a current to a sensor head in which two metal films are attached to a round bar and measuring the amount of heat generated. The degree can be calculated. Also, by providing the sensor heads on the hands of a rake, a very compact flow distribution measuring device can be obtained.
【図1】本発明の実施形態を示す斜視図である。FIG. 1 is a perspective view showing an embodiment of the present invention.
【図2】静翼とセンサヘッドの断面図である。FIG. 2 is a sectional view of a stationary blade and a sensor head.
【図3】流速、平均流速、乱れ度を示す図である。FIG. 3 is a diagram showing a flow velocity, an average flow velocity, and a turbulence degree.
【図4】流れ角とセンサヘッドの発熱量との関係を示す
図である。FIG. 4 is a diagram illustrating a relationship between a flow angle and a heat generation amount of a sensor head.
【図5】従来の流れ分布測定装置を示す図である。FIG. 5 is a diagram showing a conventional flow distribution measuring device.
【図6】X型ホットワイヤを示す図である。FIG. 6 is a view showing an X-type hot wire.
1 センサヘッド 2 熊手 3 計測演算装置 4 丸棒 5,5a,5b 金属膜 6 静翼 7 間隙 DESCRIPTION OF SYMBOLS 1 Sensor head 2 Rake 3 Measurement arithmetic unit 4 Round bar 5, 5a, 5b Metal film 6 Stator blade 7 Gap
Claims (2)
ッドに通電して加熱しこの発熱量とセンサヘッド周囲を
流れる気体により奪われる熱量とが平衡したときの電流
値を用いてセンサヘッド周囲を流れる気体の流速と流れ
角を演算する計測演算装置と、を備え、前記センサヘッ
ドは、絶縁性の丸棒と、この丸棒表面に付着した2枚の
金属膜とからなり、この2枚の金属膜は同一面積を有し
丸棒の所定方向の直径に対して周方向に間隔を隔てて線
対称に配置され、前記計測演算装置は各金属膜に電流を
流すことを特徴とする流れ計測装置。1. A sensor head having a round bar shape and a current value obtained when the amount of heat generated by energizing and heating the sensor head and the amount of heat deprived by gas flowing around the sensor head are equilibrated. A measuring and calculating device for calculating the flow velocity and the flow angle of the flowing gas, wherein the sensor head comprises an insulating round bar and two metal films adhered to the surface of the round bar. The flow measurement is characterized in that the metal films have the same area and are arranged line-symmetrically at intervals in the circumferential direction with respect to the diameter of the round bar in a predetermined direction, and the measurement operation device supplies a current to each metal film. apparatus.
る方向に軸方向を有する丸棒状の複数のセンサヘッド
と、この各センサヘッドに通電して加熱しこの発熱量と
センサヘッド周囲を流れる気体により奪われる熱量とが
平衡したときの電流値を用いて各センサヘッド周囲を流
れる気体の流速と流れ角を演算する計測演算装置と、を
備え、前記センサヘッドは、絶縁性の丸棒と、この丸棒
表面に付着した2枚の金属膜とからなり、この2枚の金
属膜は同一面積を有し丸棒の所定方向の直径に対して周
方向に間隔を隔てて線対称に配置され、前記所定方向は
各丸棒とも同一方向であり、前記計測演算装置は各金属
膜に電流を流すことを特徴とする流れ分布計測装置。2. A plurality of sensor heads in the form of a round bar which are arranged at intervals and have an axial direction substantially perpendicular to the flow, and each of the sensor heads is energized and heated to generate heat and flow around the sensor heads. A measurement calculation device that calculates the flow velocity and flow angle of the gas flowing around each sensor head using the current value when the amount of heat deprived by the gas is equilibrated, and the sensor head has an insulating round bar and And two metal films attached to the surface of the round bar. The two metal films have the same area and are arranged symmetrically at a circumferential distance from a diameter of the round bar in a predetermined direction. The predetermined direction is the same direction for each of the round bars, and the measurement and calculation device applies a current to each metal film.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31902096A JPH10160620A (en) | 1996-11-29 | 1996-11-29 | Flow measurement device and flow distribution measurement device using the same |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31902096A JPH10160620A (en) | 1996-11-29 | 1996-11-29 | Flow measurement device and flow distribution measurement device using the same |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH10160620A true JPH10160620A (en) | 1998-06-19 |
Family
ID=18105617
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP31902096A Pending JPH10160620A (en) | 1996-11-29 | 1996-11-29 | Flow measurement device and flow distribution measurement device using the same |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH10160620A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN113639953A (en) * | 2021-10-13 | 2021-11-12 | 中国空气动力研究与发展中心超高速空气动力研究所 | Point type heat flow sensor installation method for wind tunnel pneumatic heat test |
-
1996
- 1996-11-29 JP JP31902096A patent/JPH10160620A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN113639953A (en) * | 2021-10-13 | 2021-11-12 | 中国空气动力研究与发展中心超高速空气动力研究所 | Point type heat flow sensor installation method for wind tunnel pneumatic heat test |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| EP0242412B1 (en) | Method and apparatus for measuring fluid flow | |
| Jiang et al. | Theoretical and experimental studies of micromachined hot-wire anemometers | |
| US4787251A (en) | Directional low differential pressure transducer | |
| US4244217A (en) | Gas flow monitor | |
| EP0809090A1 (en) | Fluid thermal mass flow sensor | |
| US2870305A (en) | Constructions for anemometers of the hot wire type | |
| US7971478B2 (en) | Wind sensor | |
| JPH08201327A (en) | Thermal conductivity meter | |
| JPH045945B2 (en) | ||
| NL8302378A (en) | FLOW METER. | |
| GB2067293A (en) | Directional heat loss anemometer transducer | |
| CN101849174B (en) | fluid detector | |
| US20050044950A1 (en) | AC type flowmeter and method of mapping flow rate data for the same | |
| JPH08166268A (en) | Thermal flow meter | |
| JPH10148554A (en) | Flowmeter | |
| US5347876A (en) | Gas flowmeter using thermal time-of-flight principle | |
| JPS6231285B2 (en) | ||
| JPH10160620A (en) | Flow measurement device and flow distribution measurement device using the same | |
| US5582628A (en) | Unit and system for sensing fluid velocity | |
| JPH10160619A (en) | Three-dimensional flow measurement device and flow distribution measurement device using the same | |
| US6553828B1 (en) | Cooled dual element thermocouple computer and flow velocity measurement method | |
| JPH06230021A (en) | Thermosensitive anemometer and fluidic flowmeter using the same | |
| US2849880A (en) | Thermal anemometers | |
| JP3405862B2 (en) | Thermal flow sensor | |
| JPH027431B2 (en) |