[go: up one dir, main page]

CN110470859B - A method for measuring the velocity of airflow direction in an air system - Google Patents

A method for measuring the velocity of airflow direction in an air system Download PDF

Info

Publication number
CN110470859B
CN110470859B CN201910904246.4A CN201910904246A CN110470859B CN 110470859 B CN110470859 B CN 110470859B CN 201910904246 A CN201910904246 A CN 201910904246A CN 110470859 B CN110470859 B CN 110470859B
Authority
CN
China
Prior art keywords
velocity
airflow
speed
pitot 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 - Fee Related
Application number
CN201910904246.4A
Other languages
Chinese (zh)
Other versions
CN110470859A (en
Inventor
刘高文
张苗
冯青
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Northwestern Polytechnical University
Original Assignee
Northwestern Polytechnical University
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Northwestern Polytechnical University filed Critical Northwestern Polytechnical University
Priority to CN201910904246.4A priority Critical patent/CN110470859B/en
Publication of CN110470859A publication Critical patent/CN110470859A/en
Application granted granted Critical
Publication of CN110470859B publication Critical patent/CN110470859B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P5/00Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft
    • G01P5/14Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft by measuring differences of pressure in the fluid
    • G01P5/16Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft by measuring differences of pressure in the fluid using Pitot tubes, e.g. Machmeter

Landscapes

  • Engineering & Computer Science (AREA)
  • Aviation & Aerospace Engineering (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Volume Flow (AREA)
  • Indicating Or Recording The Presence, Absence, Or Direction Of Movement (AREA)

Abstract

本发明涉及一种用于空气系统内气流方向速度测量的方法,仅需测量两个压力即一组差压便可直接得到方向速度。测量简便且大大降低了测量成本。通过对比发现本发明所提出的方向速度测量方法测量值与传统五孔针分析得到的同方向速度最大绝对偏差为4.72m/s,最大相对偏差为5.96%,准确度很高,可以准确的得到气流的方向速度。解决了传统气流方向速度大小测量方法缺失,测速时需要使用三维流速测量仪器,再根据三维流速结果确定各方向速度。存在使用成本高、使用条件严格、操作复杂等问题。

Figure 201910904246

The invention relates to a method for measuring the directional velocity of airflow in an air system. The directional velocity can be directly obtained only by measuring two pressures, that is, a set of differential pressures. The measurement is simple and the measurement cost is greatly reduced. Through comparison, it is found that the maximum absolute deviation of the measured value of the directional velocity measurement method proposed by the present invention and the velocity in the same direction obtained by the traditional five-hole needle analysis is 4.72m/s, and the maximum relative deviation is 5.96%. The accuracy is very high and can be accurately obtained. Directional velocity of the airflow. It solves the lack of the traditional method of measuring the velocity in the direction of airflow. When measuring the velocity, it is necessary to use a three-dimensional flow velocity measuring instrument, and then determine the velocity in each direction according to the three-dimensional flow velocity results. There are problems such as high use cost, strict use conditions, and complicated operation.

Figure 201910904246

Description

Method for measuring direction and speed of airflow in air system
Technical Field
The invention belongs to the field of air systems of aero-engines, and relates to a method for measuring the direction and the speed of air flow in an air system.
Background
The thrust-weight ratio of the aero-engine can be correspondingly improved by increasing the gas temperature before the turbine inlet of the aero-engine, and the engine thrust corresponding to the increase of the gas temperature before the turbine inlet of the aero-engine by 55 ℃ can be increased by about 10%. At present, the temperature of the front edge of a turbine of a modern aeroengine reaches up to 2000K, which far exceeds the upper temperature resistance limit of a metal material selected by the engine, the performance of the engine is more and more difficult to be improved by improving the temperature resistance of the material, and more low-temperature air needs to be extracted from an air compressor and effectively cooled for high-temperature parts of the turbine through an air flowing system in the engine.
The gas flow in an internal flow air system in a modern aeroengine accounts for about 20-30% of the total air inlet flow of the engine, and the gas mainly has the functions of cooling and sealing high-temperature parts of the engine, preventing gas from invading, controlling axial load of a bearing and the like, and directly influences the working reliability and the service life of the engine. The flow path structure of the air system is complicated, and therefore the flow of the cooling air is also complicated. The direction and the size of the airflow speed of the airflow passing through various throttling elements such as holes, nozzles or a rotating and static disc cavity are changed, and the accurate measurement of the speed of the airflow in a certain direction in the air system is of great significance to the design of the air system, for example, the circumferential speed is important to obtain the flow field characteristics.
The existing flow velocity measurement method mainly comprises a five-hole probe, a three-dimensional hot-wire anemometer, a laser Doppler current meter and an ion image velocimeter, the measurement values of the current flow velocity measurement method are three-dimensional flow velocities, the five-hole probe needs to measure pressure in five directions to further obtain the three-dimensional flow velocity, and the measurement is complex; the laser Doppler current meter and the ion image velocimeter are non-contact measuring instruments, and have high measuring cost and complex operation. When it is only necessary to obtain a certain directional velocity of the air flow in the air system, the use of these instruments is not entirely necessary and a more convenient and readily available method is needed.
Disclosure of Invention
Technical problem to be solved
In order to avoid the defects of the prior art, the invention provides a method for measuring the direction and the speed of air flow in an air system, and solves the problems of complex measurement, high measurement cost and complex operation of the conventional flow speed measurement method.
Technical scheme
A method for measuring the direction and speed of an air flow in an air system, characterized by the steps of:
step 1: estimating the speed and direction of the fluid to be measured by CFD numerical calculation software to obtain the total speed of the air flow at the measuring point to be measured and the speed in each direction;
step 2: under the condition that a pitot tube total pressure measuring point, namely an L-shaped short end of the pitot tube is aligned to a speed direction needing to be measured, selecting a static pressure measuring point direction with lower speed on the pitot tube as a static pressure measuring point according to a CFD (computational fluid dynamics) calculation result;
and step 3: reserving the total pressure measuring points on the pitot tube and the static pressure measuring points obtained in the step 2, and sealing the rest static pressure measuring points on the pitot tube;
and 4, step 4: fixing a pitot tube at a measuring point position to be measured, aligning a total pressure measuring point of the pitot tube to a speed direction to be measured, and respectively connecting a total pressure leading pipe and a static pressure leading pipe to a pressure gauge;
and 5: during the experiment, the total pressure and the static pressure of the pitot tube are measured, and the airflow direction speed is calculated according to the measured differential pressure and the Bernoulli equation:
Figure BDA0002212791250000021
in the formula, V is the speed of the airflow direction, m/s; pt-total pressure in the direction of the gas flow, Pa; p0-static airflow pressure, Pa; rho-gas flow density, kg/m3
Advantageous effects
The method for measuring the direction and the speed of the airflow in the air system can directly obtain the direction and the speed by only measuring two pressures, namely a group of differential pressures. The measurement is simple and convenient, and the measurement cost is greatly reduced. Through comparison, the maximum absolute deviation of the measured value of the direction speed measuring method provided by the invention and the same-direction speed obtained by the analysis of the traditional five-hole needle is 4.72m/s, the maximum relative deviation is 5.96 percent, the accuracy is very high, and the direction speed of the airflow can be accurately obtained. The method solves the problem that the traditional method for measuring the speed in the airflow direction is lacked, a three-dimensional flow velocity measuring instrument is required to be used when measuring the speed, and the speed in each direction is determined according to the three-dimensional flow velocity result. Has the problems of high use cost, strict use conditions, complex operation and the like.
Drawings
FIG. 1 rotating hole velocity vector diagram
FIG. 2 arrangement of the measuring device
FIG. 3 arrangement of the measuring device
FIG. 4 schematic view of a swirl orifice plate
FIG. 5 Pitot tube schematic
In the figure: 1 prewhirl disc, 2 prewhirl holes, 3 casings, 4 positions of pitot tubes, 5 total pressure measuring points of pitot tubes, 6-1 static pressure measuring points, 6-2 static pressure measuring points of pitot tubes, 7 total pressure channels and 8 static pressure channels
Detailed Description
The invention will now be further described with reference to the following examples and drawings:
the invention adopts the basic idea of measuring the total pressure and the static pressure of the airflow in a certain direction in order to solve the problem of measuring the speed of the airflow in the air system, and then determines the speed of the airflow by using the Bernoulli equation.
Step 1: and (3) estimating the speed and the direction of the fluid to be measured by adopting CFD numerical calculation software to obtain the total speed and the speed in each direction of the airflow at the required measuring point.
Step 2: and (3) pressure measurement of a total pressure measurement point of the pitot tube is controlled, namely the L-shaped short end of the pitot tube needs to be aligned to the direction of a speed incoming flow to be measured, the directions of all static pressure measurement points of the pitot tube are fixed when the direction of the total pressure measurement point is fixed, and the direction of the static pressure measurement point with a lower speed is selected as the static pressure measurement point according to the CFD calculation result. When the speed of the total pressure measuring point is ten times higher than that of the static pressure measuring point, the relative error brought by the method is only 0.5 percent.
And step 3: and (4) reserving the total pressure measuring points on the pitot tube and the static pressure measuring points obtained in the step two, and sealing the rest static pressure measuring points on the pitot tube.
And 4, step 4: and fixing the pitot tube at a measuring point position to be measured, aligning a total pressure measuring point of the pitot tube to the incoming flow direction of the speed to be measured, and respectively connecting the total pressure leading tube and the static pressure leading tube into a pressure gauge.
And 5: and (3) carrying out an experiment, reading the total pressure and the static pressure measured by the pitot tube, and calculating according to the measured differential pressure and a formula 1, namely a Bernoulli equation to obtain the speed of the airflow in the direction.
Figure BDA0002212791250000041
In the formula, V is the speed of the airflow direction, m/s; pt-total pressure in the direction of the gas flow, Pa; p0-static airflow pressure, Pa; rho-gas flow density, kg/m3
In an air system, when the airflow direction to be measured is the circumferential airflow speed, the selection of the static pressure measuring point can be based on the following principle: when the airflow is axially pre-rotated, the airflow has higher circumferential speed and axial speed, and the radial speed is lower, and pressure measuring holes arranged in the radial direction can be selected to replace static pressure; when the air flow is radially pre-rotated to be fed, the air flow has larger circumferential speed and radial speed, and the axial speed is smaller, so that the static pressure can be replaced by arranging pressure measuring holes in the axial direction.
In a word, the method for measuring the speed in the airflow direction is to measure the total pressure in the direction of the airflow required to be measured, select and reasonably arrange static pressure holes according to the speed distribution condition to approximately replace the static pressure of the airflow, and further obtain the speed in the airflow direction according to the Bernoulli equation.
To control the error of this directional velocity measurement method, the applicable conditions of this method need to be given. When only the error caused by the static pressure measurement point replacement is considered without considering the systematic error, the following error analysis can be performed:
suppose that the true static pressure at the measurement point is P0And the total pressure in the direction measured at the total pressure measuring point is as follows:
Figure BDA0002212791250000042
in the formula, Pt-the measured total directional pressure, Pa; p0The true static pressure at the measurement point, Pa. Vt-real direction velocity of air flow at the direction total pressure point, m/s.
And the approximate static pressure measured at the static pressure measurement points is:
Figure BDA0002212791250000051
in the formula, P(0)Measuring the static pressure, Pa, V at the measuring pointS-static pressure measurement point air flow velocity, m/s; .
The measured airflow direction velocities are known as:
Figure BDA0002212791250000052
in the formula V(t)-the velocity of the air flow direction measured at the measuring point, m/s.
From equation (5) it can be inferred that:
when in use
Figure BDA0002212791250000053
Then, 0.995V was foundt≤V(t)≤Vt (6)
Therefore, when the measuring point speed size is satisfied:
Figure BDA0002212791250000054
in the method, the relative deviation between the airflow direction speed calculated by the method and the real airflow direction speed is not more than 0.5%.
The relative error under different conditions can be listed according to equation (5), table 1:
airflow direction velocity/static pressure point velocity (V)t/VS) Relative error
10 0.5%
5 1.2%
3 6%
Example 1:
with reference to FIG. 1, the air flow is axially fedAfter reaching the static rotational flow disk 1 shown in the figure, the direction of the airflow is changed through the inclined hole 2, and the airflow has circumferential speed
Figure BDA0002212791250000055
Total velocity VoutAnd the included angle between the axial direction and the axial direction is theta. The size of the airflow deflection angle theta is related to the size and direction of the incoming flow speed, the deflection angle of the pre-rotation hole and the length-diameter ratio of the pre-rotation hole, and when the size and direction of the incoming flow speed are determined and the length-diameter ratio of the pre-rotation hole reaches a certain value, the airflow deflection angle theta is equal to the deflection angle of the pre-rotation hole.
As can also be seen from FIG. 1, the velocity of the air flow direction, e.g. the circumferential velocity, is obtained
Figure BDA0002212791250000056
The size of the flow coefficient is important for obtaining the air flow circulation characteristics, and the air flow rotation ratio, the air flow and axis angle and the like can be calculated, so that the size of the flow coefficient can be predicted.
Rotation ratio calculation formula:
Figure BDA0002212791250000057
wherein, the beta-rotation ratio;
Figure BDA0002212791250000058
-gas flow circumferential velocity, m/s; w-rotor angular velocity, rad/s; r-local rotor radius, m.
The air flow angle is shown in fig. 1, and the calculation formula is as follows:
Figure BDA0002212791250000061
in the formula, the angle between theta-airflow and an axis is included; vX-gas flow axial velocity, m/s.
Referring to fig. 2 and 3, the layout of a typical swirl generator and a measuring device in an air system is shown, wherein 1 is a swirl disk, 2 is a swirl inclined hole, 3 is an outer casing, and 4 indicates the position of a pitot tube. The airflow generates rotational flow after passing through the rotational flow disk, the direction is changed, and the pitot tube is arranged on one side of the airflow outflow rotational flow hole and can be used for measuring the circumferential speed of the airflow outflow rotational flow hole.
And the attached figure 4 is a schematic diagram of a pitot tube structure, wherein 5 is a total pressure measuring point, the direction is aligned with the circumferential speed of the airflow to be measured, 6-1 and 6-2 are static pressure measuring points, 6-1 is a radial position static pressure measuring point, and 6-2 is an axial position static pressure measuring point. 7 leading out a total pressure pipe connected with a total pressure channel of the differential pressure type scanning valve for measuring pressure, and 8 leading out a static pressure pipe connected with a static pressure channel of the differential pressure type scanning valve for measuring pressure. The static pressure measuring points are arranged in four directions, proper static pressure measuring points are selected according to actual conditions, the rest measuring points are sealed, when the relative error is controlled within 0.5%, and the speed in the total pressure direction needs to be more than ten times of the speed in the static pressure direction. After the differential pressure scanning valve measures the differential pressure, the circumferential speed of the air flow can be calculated according to the formula (1).
Example 2:
as shown in the figure, the airflow axially enters, the airflow direction changes after passing through the rotational flow pore plate shown in the figure 2, the circumferential speed with a certain size is obtained, and the circumferential speed of the airflow is obtained when the requirement is met
Figure BDA0002212791250000062
When the direction speed measuring method is used, the circumferential speed can be obtained
Figure BDA0002212791250000063
The size of (2). The specific parameters of the swirl orifice plate are shown in Table 2:
table 2: specific parameters of swirl orifice plate
Diameter of swirl orifice plate 304mm
Swirl orifice radial position 115mm
Diameter of swirl hole 7mm
Axial included angle of swirl hole 45°
Step 1: an appropriate static pressure measuring point needs to be selected on the pitot tube. As the rotational flow pore plate is axially pre-rotated to intake air, the numerical values of the axial speed and the circumferential speed of the airflow are larger, the numerical calculation results of a plurality of working conditions show that the radial speed of the rotational flow pore plate is smaller than 1m/s, the circumferential speeds of the measuring points under different working conditions are larger than 10m/s, and the application condition that the relative error is 0.5% is met, so the rest static pressure measuring points are sealed, and the measuring result of the pressure measuring point 6-1 at the radial position of the pitot tube is selected as the static pressure value.
Step 2: the measuring device pitot tube is arranged. The pitot tube is 10mm away from the axial position of the swirl orifice plate, and the radial position is the center of the swirl orifice. In conjunction with fig. 1 and 2, a pitot tube measurement position is shown at 4. And respectively connecting the total pressure leading pipe and the static pressure leading pipe into a differential pressure type scanning valve.
And step 3: the differential pressure is read, and the airflow circumferential velocity is obtained according to the equation (1).
To verify the correctness of the measurement method proposed by this patent, five holes are utilized herein to measure the circumferential velocity of the air flow at the same location.
The five-hole needle and the pitot tube are arranged at the same radial position and the same axial position behind the rotational flow orifice plate, and the circumferential angle is 180 degrees. And then processing the speed and direction measured by the five-hole needle to obtain the circumferential speed, comparing the circumferential speed with the measured data of the pitot tube, and verifying the correctness of the direction and the speed measured by the pitot tube.
The experimental condition of the measurement is given in table 3, the circumferential speed measured by the five-hole needle is compared with the pitot tube, and the maximum absolute deviation between the circumferential speed measured by the pitot tube and the circumferential speed measured by the five-hole needle is 4.72m/s, the maximum relative deviation is 5.96%, so that the high accuracy of the pitot tube on the measurement of the directional speed is realized, and the pitot tube has engineering application value.
Table 3: comparison of measurement conditions
Figure BDA0002212791250000071
Figure BDA0002212791250000081

Claims (1)

1.一种用于空气系统内气流方向速度测量的方法,其特征在于步骤如下:1. a method for measuring the air flow direction velocity in the air system, is characterized in that the steps are as follows: 步骤1:采用CFD数值计算软件对需要测量的流体速度大小及方向进行预估,得到所需测量测点处气流的总速度以及各方向速度大小;Step 1: Use the CFD numerical calculation software to estimate the size and direction of the fluid velocity to be measured, and obtain the total velocity of the airflow at the required measurement point and the velocity in each direction; 步骤2:在皮托管总压测点即皮托管L形短端对准需要测量的速度方向的情况下,根据CFD计算结果,选取皮托管上速度小于总压测点速度十分之一的的静压测点方向作为静压测点;Step 2: Under the condition that the total pressure measuring point of the pitot tube, that is, the L-shaped short end of the pitot tube, is aligned with the speed direction to be measured, according to the CFD calculation result, select the one whose speed on the pitot tube is less than one-tenth of the speed of the total pressure measuring point. The direction of the static pressure measuring point is used as the static pressure measuring point; 步骤3:保留皮托管上的总压测点与步骤2中得到的静压测点,对皮托管上其余静压测点进行密封;Step 3: Keep the total pressure measurement points on the pitot tube and the static pressure measurement points obtained in step 2, and seal the rest of the static pressure measurement points on the pitot tube; 步骤4:将皮托管固定在所需测量的测点位置,皮托管总压测点对准需要测量的速度方向并分别将总压引压管与静压引压管接入压力表;Step 4: Fix the pitot tube at the position of the measuring point to be measured, align the total pressure measuring point of the pitot tube with the speed direction to be measured, and connect the total pressure impulse pipe and the static pressure impulse pipe to the pressure gauge respectively; 步骤5:实验时,测得皮托管的总压和静压,根据测得差压和伯努利方程计算得到气流方向速度大小:Step 5: During the experiment, measure the total pressure and static pressure of the pitot tube, and calculate the velocity in the airflow direction according to the measured differential pressure and Bernoulli equation:
Figure FDA0002927603820000011
Figure FDA0002927603820000011
式中,V-气流方向速度,m/s;Pt-气流方向总压,Pa;P0-气流静压,Pa;ρ-气流密度,kg/m3In the formula, V-airflow direction velocity, m/s; Pt -airflow direction total pressure, Pa ; P0-airflow static pressure, Pa; ρ-airflow density, kg/ m3 .
CN201910904246.4A 2019-09-24 2019-09-24 A method for measuring the velocity of airflow direction in an air system Expired - Fee Related CN110470859B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910904246.4A CN110470859B (en) 2019-09-24 2019-09-24 A method for measuring the velocity of airflow direction in an air system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910904246.4A CN110470859B (en) 2019-09-24 2019-09-24 A method for measuring the velocity of airflow direction in an air system

Publications (2)

Publication Number Publication Date
CN110470859A CN110470859A (en) 2019-11-19
CN110470859B true CN110470859B (en) 2021-04-20

Family

ID=68516555

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910904246.4A Expired - Fee Related CN110470859B (en) 2019-09-24 2019-09-24 A method for measuring the velocity of airflow direction in an air system

Country Status (1)

Country Link
CN (1) CN110470859B (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111856072B (en) * 2020-07-29 2021-10-15 中国汽车工程研究院股份有限公司 A kind of airflow velocity calculation method, system, equipment and a kind of storage medium

Citations (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58500217A (en) * 1981-02-23 1983-02-10 ロ−ズマウント インコ. Pressure sensors for measuring airspeed, altitude and angle of attack
CN2731454Y (en) * 2004-09-03 2005-10-05 江苏大学 Probe unit
CN102033137A (en) * 2009-10-06 2011-04-27 精工爱普生株式会社 Speed detector and swing tool having the same
GB2446827B (en) * 2007-02-23 2011-06-29 Associated Instr Repairs Ltd Pitot-static device
CN203443970U (en) * 2013-09-23 2014-02-19 国家电网公司 Direction controllable pitot tube
CN204832239U (en) * 2015-05-22 2015-12-02 中国神华能源股份有限公司 Portable gas velocity measuring device
CN105203796A (en) * 2015-10-10 2015-12-30 国网山东省电力公司电力科学研究院 Pitot tube measuring device used for primary air leveling and provided with ruler and method
JP2016014651A (en) * 2014-06-30 2016-01-28 ザ・ボーイング・カンパニーTheBoeing Company Mems-based conformal air speed sensor
CN106092538A (en) * 2016-06-17 2016-11-09 西北工业大学 A kind of for axial rotation hole discharge coefficient measure device and do not rotate method
US9568345B2 (en) * 2013-04-25 2017-02-14 Hon Hai Precision Industry Co., Ltd. Dust measurement system for filter
CN107228690A (en) * 2017-04-10 2017-10-03 中国计量科学研究院 It is a kind of not by non-measured direction flow rate effect Pitotmeter or flowmeter
CN107270982A (en) * 2016-02-27 2017-10-20 山东大学(威海) A kind of gas flow measurement experimental provision of measurement apparatus movement
CN109061219A (en) * 2018-07-18 2018-12-21 湖南大学 Actual measurement device and method with reference to static pressure, wind speed and direction is provided under typhoon environment

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
RU2157980C2 (en) * 1997-01-28 2000-10-20 Центральный аэродинамический институт им. проф. Н.Е. Жуковского Fuselage pitot-static tube with a strut
US8578790B2 (en) * 2010-08-11 2013-11-12 Russell P. Secor Apparatus for measurement of ducted air
CN102298071A (en) * 2011-05-20 2011-12-28 南京信息工程大学 Device and method for measuring wind speed and wind direction
CN103729505B (en) * 2013-12-23 2017-01-18 苏州纽威阀门股份有限公司 CFD (computational fluid dynamics) based method for computing equivalent length of valve
CN107270979B (en) * 2017-05-18 2019-10-18 东方电气集团东方汽轮机有限公司 A kind of aerodynamic testing air-flow measurement device

Patent Citations (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58500217A (en) * 1981-02-23 1983-02-10 ロ−ズマウント インコ. Pressure sensors for measuring airspeed, altitude and angle of attack
CN2731454Y (en) * 2004-09-03 2005-10-05 江苏大学 Probe unit
GB2446827B (en) * 2007-02-23 2011-06-29 Associated Instr Repairs Ltd Pitot-static device
CN102033137A (en) * 2009-10-06 2011-04-27 精工爱普生株式会社 Speed detector and swing tool having the same
US9568345B2 (en) * 2013-04-25 2017-02-14 Hon Hai Precision Industry Co., Ltd. Dust measurement system for filter
CN203443970U (en) * 2013-09-23 2014-02-19 国家电网公司 Direction controllable pitot tube
JP2016014651A (en) * 2014-06-30 2016-01-28 ザ・ボーイング・カンパニーTheBoeing Company Mems-based conformal air speed sensor
CN204832239U (en) * 2015-05-22 2015-12-02 中国神华能源股份有限公司 Portable gas velocity measuring device
CN105203796A (en) * 2015-10-10 2015-12-30 国网山东省电力公司电力科学研究院 Pitot tube measuring device used for primary air leveling and provided with ruler and method
CN107270982A (en) * 2016-02-27 2017-10-20 山东大学(威海) A kind of gas flow measurement experimental provision of measurement apparatus movement
CN106092538A (en) * 2016-06-17 2016-11-09 西北工业大学 A kind of for axial rotation hole discharge coefficient measure device and do not rotate method
CN107228690A (en) * 2017-04-10 2017-10-03 中国计量科学研究院 It is a kind of not by non-measured direction flow rate effect Pitotmeter or flowmeter
CN109061219A (en) * 2018-07-18 2018-12-21 湖南大学 Actual measurement device and method with reference to static pressure, wind speed and direction is provided under typhoon environment

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
《Supersonic flow measurement and computation of a lobed-mixer for trapped vortex combustors》;A. Brankovic;《ICIASF 2001 Record, 19th International Congress on Instrumentation in Aerospace Simulation Facilities (Cat. No.01CH37215)》;20010830;全文 *
《探头偏转角对皮托管测速精度影响分析》;杨欢;《测控技术》;20121018;第31卷(第10期);第12页-第15页 *
《皮托管式静压探针气动性能的CFD 和试验对比研究》;刘绪鹏;《航空发动机》;20190415;第45卷(第2期);全文 *

Also Published As

Publication number Publication date
CN110470859A (en) 2019-11-19

Similar Documents

Publication Publication Date Title
Aschenbruck et al. Influence of a multi-hole pressure probe on the flow field in axial-turbines
CN111089702A (en) Probe for measuring full parameters of subsonic three-dimensional steady-state flow field
Klausmann et al. Transonic compressor Darmstadt—Open test case
CN120293445B (en) A grate leakage test device and method suitable for low Reynolds number flow
CN110470859B (en) A method for measuring the velocity of airflow direction in an air system
CN106092538A (en) A kind of for axial rotation hole discharge coefficient measure device and do not rotate method
Toni et al. Unsteady flow field measurements in an industrial centrifugal compressor
CN111677683B (en) Method and device for testing pneumatic performance of micro fan based on flow compensation method
CN113495001B (en) Device and method for measuring entrainment flow ratio of disk cavity of gas compressor
CN111498141B (en) A method and device for real-time monitoring of airflow angle based on micro-probe
Guidotti et al. Experimental and numerical analysis of the flow field in the impeller of a centrifugal compressor stage at design point
CN115950493B (en) A flow rate testing system and testing method suitable for subsonic flow channels
CN115525996B (en) Turbine working blade flow characteristic rotation correction method and system
Kluge et al. Sensitivity analysis, design, instrumentation, and experimental validation of a novel labyrinth seal rig
Benvenuti Aerodynamic Development of Stages for Industrial Centrifugal Compressors: Part 1—Testing Requirements and Equipment—Immediate Experimental Evidence
Jäger et al. The Fundamental Research And New Concepts Compressor-LTF’s new low-speed axial compressor test rig for atmospheric and sub-atmospheric operation
Tamaki Study on flow fields in high specific speed centrifugal compressor with unpinched vaneless diffuser
Xi et al. Experimental and numerical investigations on flow losses of a u-bend and return channel system for centrifugal compressor
CN211696880U (en) Probe for measuring full parameters of subsonic three-dimensional steady-state flow field
Jaffa Unsteady measurement techniques for turbomachinery flows
CN110608815A (en) A method for measuring the relative total temperature of the airflow in the rotating disc chamber
Methel An experimental comparison of diffuser designs in a centrifugal compressor
Eck et al. Rotor Clearance Flow Measurements Employing a Novel Miniature Sensor
Town et al. Total pressure correction of a sub-miniature five-hole probe in areas of pressure gradients
JP2018200215A (en) Fluid machinery monitoring system, fluid machinery monitoring device, and fluid machinery monitoring method

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20210420

Termination date: 20210924

CF01 Termination of patent right due to non-payment of annual fee