CN113155468A - Streamline method aviation engine thrust correction method based on field test - Google Patents

Streamline method aviation engine thrust correction method based on field test Download PDF

Info

Publication number
CN113155468A
CN113155468A CN202110459087.9A CN202110459087A CN113155468A CN 113155468 A CN113155468 A CN 113155468A CN 202110459087 A CN202110459087 A CN 202110459087A CN 113155468 A CN113155468 A CN 113155468A
Authority
CN
China
Prior art keywords
section
static pressure
cross
measuring points
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.)
Granted
Application number
CN202110459087.9A
Other languages
Chinese (zh)
Other versions
CN113155468B (en
Inventor
王毅
任怡雪
房健
张淑婷
孔祥雪
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.)
Beijing Changcheng Institute of Metrology and Measurement AVIC
Original Assignee
Beijing Changcheng Institute of Metrology and Measurement AVIC
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 Beijing Changcheng Institute of Metrology and Measurement AVIC filed Critical Beijing Changcheng Institute of Metrology and Measurement AVIC
Priority to CN202110459087.9A priority Critical patent/CN113155468B/en
Publication of CN113155468A publication Critical patent/CN113155468A/en
Application granted granted Critical
Publication of CN113155468B publication Critical patent/CN113155468B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M15/00Testing of engines

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Volume Flow (AREA)

Abstract

The invention relates to the technical field of aero-engines. And designing a set of test method applied to the field test according to the pneumatic parameters required by the streamline thrust correction method in the calculation of the correction term. Parameters such as speed, static pressure difference and the like can be obtained through site distribution testing of a far front section 0, a far front section 0-f and a far front section 9, and air inlet impulse resistance, the sum of the pre-air inlet flow pipe and lip curling resistance, support resistance and bottom resistance can be obtained through correction term calculation. The method mainly solves the problem of measuring the curling resistance of the pre-inlet gas flow pipe and the lip, and the resistance value can be obtained by optimizing a streamline model by measuring the speed and static pressure information of any three positions in the section of 0-f.

Description

Streamline method aviation engine thrust correction method based on field test
Technical Field
The invention relates to a flow line method aero-engine thrust correction method based on a field test, and belongs to the field of aero-engine measurement and calibration.
Background
When the aero-engine is tested on an indoor test bed, airflow can generate resistance on the engine and an engine moving frame due to injection, so that the engine thrust obtained through measurement is inaccurate, and therefore the measured thrust needs to be corrected on the indoor test bed to obtain the real thrust when the engine runs.
At present, the thrust correction of the domestic indoor test bed is a field test based on the theory of a section method, and the main problems are that a control body on the test is large in division area, the test is not accurate enough, the fluctuation on the measurement of differential pressure is large, and manual operation is large during point selection, so that the error of calculating a correction term is large. And the influence caused by differential pressure fluctuation in the flow line method is small, and error points can be eliminated according to the static pressure model, so that the possibility of manual operation is reduced.
However, the streamline correction term cannot be applied to a field test due to the existence of the integral term, so the invention provides the streamline aeronautical engine thrust correction method based on the field test, and the problem can be solved.
Disclosure of Invention
The invention aims to solve the problems that the existing testing method is inaccurate, the fluctuation is large in the measurement of differential pressure, and manual operation is large in point selection, so that the error of a calculated correction term is large, and provides a streamline normal aviation engine thrust correction method based on a field test. The method comprises the steps of obtaining pneumatic parameter values required by calculation of correction terms in thrust correction through a field test, then extracting and calculating a streamline profile characteristic curve and a static pressure distribution curve of a pre-inlet flow pipe required by the calculation according to the field test of an engine test bed, and finally carrying out thrust correction according to each correction term.
The purpose of the invention is realized by the following technical scheme.
The streamline method aviation engine thrust correction method based on the field test comprises the following steps:
step one, obtaining various correction values of thrust correction through field test
1. Determining the position of the measurement cross section:
a. and determining the position of a section 0, wherein the section 0 is generally placed at a position 5-7 d away from the lip of the engine, and d is the diameter of the air inlet of the engine. The air flow in the cross section is relatively uniform at this location.
b. And determining the position of the 9 section, wherein the 9 section has different positions for different types of engines, the 9 section is positioned at the tail nozzle or the inner culvert outlet section when the turbojet turbofan engine with the small bypass ratio is tested on site, and the 9 section is positioned at the outer culvert outlet section when the turbofan engine with the large bypass ratio is tested on site, as shown in figure 1.
c.0-f area measuring points need to be arranged at the position where the secondary flow is stable, the measuring points are generally placed at the position within 3m from the wall surface of a test room, and the f section of the lip and the f position 1m on the front side of the lip are generally taken as the sectionspCross-section as shown in figure 2.
2. Determining measurement parameters required in the correction term calculation, said parameters including:
a. resistance w of air-intake impulse0·v0
Wherein the average velocity v of the cross section is 00Intake air flow rate w0
b. Resistance of the stent
Figure BDA0003041706110000021
Wherein ρ is the airflow density; cd [ Cd ]iThe drag coefficient of the individual components was 2.05; a. theiIs the area of the blockage of a single component, in m2;ViIs the velocity of the gas flow over the area of the obstruction.
c. Sum of resistance F of pre-air inlet flow pipe and lip curlingpre-entry+Fbell═ 2 pi Δ p (x) y' (x) dx, with the axis of the engine as the x-axis, the direction pointing from the 0 cross-section to the 9 cross-section, the perpendicular direction to the test-shop floor as the y-axis, the direction is vertically upward, and the center of the far-ahead 0 cross-section is the origin of coordinates.
Where y (x) is a position coordinate that varies with x; p (x) is the static pressure value as x varies, and y' (x) is the derivative of y (x) with respect to x.
The streamline model of the control body is y (x) ═ aebx+c。
Wherein a, b and c are three coefficients, and the coefficients are calculated by measuring the x coordinate position and the section radius of any 3 points on the pre-air inlet flow pipe and a closed curve.
The radius of the section of the pre-air inlet flow pipe reaches the hair through measuring 0 sectionW 'is used as the secondary flow velocity of any three cross sections between engine lips (referred to as the 0-f region)'0=ρv′0-fA' calculates the area of the secondary flow of the cross section, passing through A0-fThe area of the pre-inlet airflow pipe of the section is obtained as A-A', and then the radius of the pre-inlet airflow pipe of the section is calculated.
Wherein, w'0Intake air flow rate, v ', of secondary flow'0-fFor measuring the mean value of the secondary flow velocity of the cross section, A' is the secondary flow cross section area of the cross section, A0-fThe sectional area of the pre-inlet airflow pipe is measured.
The static pressure difference of each point on the control flow line is related to the radius of the pre-air inlet flow pipe, and the model is delta P (x) menx+r。
Wherein m, n and r are three coefficients, and the static pressure difference value between any three section secondary flow parts between the section 0 and the lip of the engine (0-f area) and the section 0 is measured, and the x coordinate position of the section can be used for calculating a closed curve.
d. Bottom resistance Fbase=(P9-P0)(A8-A9)。
Wherein, P9-P0Is the static pressure difference between the 9 section and the 0 section, A8-A9Is the area of the tail nozzle.
3. Determining the measurement mode of each parameter:
the section a.0 is composed of 5 multiplied by 5 measuring points, and 25 wind speed measuring points and 25 total static pressure measuring points are arranged on the measuring bent to measure the wind speed and the total static pressure of the section 0. The 0 section measurement bent is shown in fig. 3.
b. The air flow speed on the bracket is provided with an anemometer on the windward side of the bracket.
c.f cross-section and f p3 wind speed measuring points and 3 total static pressure measuring points are respectively arranged at the secondary flow stabilization part of the section to measure wind speed and total static pressure values. The static pressure difference is the difference between the measuring point on the section and the static pressure corresponding to the section position of 0. f and fpAnd 6 static pressure measuring points for measuring the section and 6 static pressure measuring points at corresponding height positions on the section 0 are respectively connected into a differential pressure sensor to measure the static pressure difference.
d. The surface of the outer duct of the tail nozzle of the engine is provided with 4 static pressure sensors, and the measured surface static pressure value is shown in figure 1.
The overall station arrangement is shown in figure 2.
4. The measured data processing method comprises the following steps:
a.0 section average velocity v0Obtained by averaging 25 measured points, i.e.
Figure BDA0003041706110000031
b.f sectional static pressure difference Δ pf=pf-p0Wherein p isfIs the average value of three static pressure measuring points of the f section
Figure BDA0003041706110000032
p0Is the average value of 25 measuring points of 0 section
Figure BDA0003041706110000033
fpStatic pressure difference of cross section
Figure BDA0003041706110000034
Wherein
Figure BDA0003041706110000035
Is fpAverage value of three static pressure measuring points of cross section
Figure BDA0003041706110000036
Section f andpthe velocity of the secondary flow of the cross section is taken as the average value of three velocity measuring points
Figure BDA0003041706110000037
c.9 static cross-sectional pressure p9Taking the average value of 4 static pressure measuring points
Figure BDA0003041706110000038
Step two, F obtained by the step onepre-entry+FbellThe calculation result of the correction term is used for obtaining the corrected real thrust Fg
Fg=FM+w0·v0-Fpre-entry-Fbell+Fcradle+Fbase
Advantageous effects
The invention solves the following problems:
1. the method solves the problem that the streamline method cannot be applied to field test at present, and can actually measure the pneumatic parameter values required in calculation of the streamline method.
2. The method solves the problem that the cross section method is influenced by artificial point selection errors in use, and error points are removed through curve fitting.
3. The influence of the non-uniform airflow on the thrust correction is reduced.
Drawings
FIG. 19 is a schematic view of a cross-sectional position selection;
FIG. 2 is a diagram of the overall layout of the test room;
FIG. 30 is a schematic view of a cross-sectional measurement bent;
FIG. 4 is a graph of a measured streamline parameter fit;
FIG. 5 is a graph of a parameter fit of measured static pressure distribution.
Detailed Description
The invention is further described with reference to the following figures and examples.
Example 1
The data processing and analysis process will be described by taking a 12m × 12m test bed and a test run condition with an injection ratio of 1.7 as an example.
The following table 1 is a parameter table obtained by actual measurement.
TABLE 1 pneumatic parameter table in actual measurement test workshop
Figure BDA0003041706110000041
Figure BDA0003041706110000051
Step one, obtaining various correction values of thrust correction through field test
1. Determining the position of the measurement cross section:
a. the position of the 0 section was determined, and the 0 section was placed 8.3m before the lip of the engine.
b. And (3) determining the position of the section 9, wherein when the turbofan engine with the large bypass ratio is tested on site, the section 9 is positioned at the bypass outlet section, as shown in the right diagram of fig. 1.
c.0-f area measuring points need to be arranged at the secondary flow stable position and are placed at the position 3m away from the wall surface of the test room, and the section f of the lip is taken and the f section is 1m away from the front side of the lippCross-section as shown in figure 2.
2. Determining measurement parameters required in the correction term calculation, said parameters including:
a. resistance w of air-intake impulse0·v0
Wherein the average velocity v of the cross section is 00Intake air flow rate w0
b. Resistance of the stent
Figure BDA0003041706110000052
Wherein ρ is the airflow density; cd [ Cd ]iThe drag coefficient of the individual components was 2.05; a. theciIs the area of the blockage of a single component, in m2;VciIs the velocity of the gas flow over the area of the obstruction.
c. Sum of resistance F of pre-air inlet flow pipe and lip curlingpre-entry+Fbell═ 2 pi Δ p (x) y' (x) dx, with the axis of the engine as the x-axis, the direction pointing from the 0 cross-section to the 9 cross-section, the perpendicular direction to the test-shop floor as the y-axis, the direction is vertically upward, and the center of the far-ahead 0 cross-section is the origin of coordinates.
Where y (x) is a position coordinate that varies with x; p (x) is the static pressure value as x varies, and y' (x) is the derivative of y (x) with respect to x.
The streamline model of the control body is y (x) ═ aebx+c。
Wherein a, b and c are three coefficients, and the coefficients are calculated by measuring the x coordinate position and the section radius of any 3 points on the pre-air inlet flow pipe and a closed curve.
The section radius of the pre-intake airflow pipe is measured by measuring the secondary flow velocity of any three sections from the 0 section to the engine lip (called a 0-f area), and adopting w'0=ρv′0-fA' calculates the area of the secondary flow of the cross section, passing through A0-fThe area of the pre-inlet airflow pipe of the section is obtained as A-A', and then the radius of the pre-inlet airflow pipe of the section is calculated.
Wherein, w'0Intake air flow rate, v ', of secondary flow'0-fFor measuring the mean value of the secondary flow velocity of the cross section, A' is the secondary flow cross section area of the cross section, A0-fThe sectional area of the pre-inlet airflow pipe is measured.
The static pressure difference of each point on the control flow line is related to the radius of the pre-air inlet flow pipe, and the model is delta P (x) menx+r。
Wherein m, n and r are three coefficients, and the static pressure difference value between any three section secondary flow parts between the section 0 and the lip of the engine (0-f area) and the section 0 is measured, and the x coordinate position of the section can be used for calculating a closed curve.
d. Bottom resistance Fbase=(P9-P0)(A8-A9)。
Wherein, P9-P0Is the static pressure difference between the 9 section and the 0 section, A8-A9Is the area of the tail nozzle.
3. Determining the measurement mode of each parameter:
the section a.0 is composed of 5 multiplied by 5 measuring points, and 25 wind speed measuring points and 25 total static pressure measuring points are arranged on the measuring bent to measure the wind speed and the total static pressure of the section 0. The 0 section measurement bent is shown in fig. 3.
b. The air flow speed on the bracket is provided with an anemometer on the windward side of the bracket.
c.f cross-section and f p3 wind speed measuring points and 3 total static pressure measuring points are respectively arranged at the secondary flow stabilization part of the section to measure wind speed and total static pressure values. The static pressure difference is the difference between the measuring point on the section and the static pressure corresponding to the section position of 0. f and f p6 static pressure measuring points for cross section measurement are respectively corresponding to 6 static pressure measuring points at corresponding height positions on the cross section of 0And (5) connecting a differential pressure sensor to measure the static pressure difference.
d. The surface of the outer duct of the tail nozzle of the engine is provided with 4 static pressure sensors, and the measured surface static pressure value is shown in figure 1.
The overall station arrangement is shown in figure 2.
4. The measured data processing method comprises the following steps:
a.0 section average velocity v0Obtained by averaging 25 measured points, i.e.
Figure BDA0003041706110000071
b.f sectional static pressure difference Δ pf=pf-p0Wherein p isfIs the average value of three static pressure measuring points of the f section
Figure BDA0003041706110000072
p0Is the average value of 25 measuring points of 0 section
Figure BDA0003041706110000073
fpStatic pressure difference of cross section
Figure BDA0003041706110000074
Wherein
Figure BDA0003041706110000075
Is fpAverage value of three static pressure measuring points of cross section
Figure BDA0003041706110000076
Section f andpthe velocity of the secondary flow of the cross section is taken as the average value of three velocity measuring points
Figure BDA0003041706110000077
c.9 static cross-sectional pressure p9Taking the average value of 4 static pressure measuring points
Figure BDA0003041706110000078
5. According to the above distribution and data processing method:
a. resistance w of air-intake impulse0·v0
Wherein v is0=9.77m/s;
b. Resistance of the stent
Figure BDA0003041706110000079
Wherein the content of the first and second substances,
ρ=1.09;
Cdithe drag coefficient of the individual components was 2.05;
Aciis the area of the blockage of a single component, in m2,Ac1=1.54m2,Ac2=1.66m2
VciIs the velocity of the air flowing over the obstruction area, Vc1=8.59m/s,Vc2=4.05m/s;
Calculating the resistance of the support
Figure BDA00030417061100000710
c. Sum of resistance F of pre-air inlet flow pipe and lip curlingpre-entry+Fbell═ 2 pi Δ p (x) y' (x) dx, with the axis of the engine as the x-axis, the direction pointing from the 0 cross-section to the 9 cross-section, the perpendicular direction to the test-shop floor as the y-axis, the direction is vertically upward, and the center of the far-ahead 0 cross-section is the origin of coordinates.
Where y (x) is a position coordinate that varies with x; p (x) is the static pressure value as x varies, and y' (x) is the derivative of y (x) with respect to x.
Area of 0 section pre-inlet airflow pipe 51.7m2,The radius of the pre-inlet airflow pipe is calculated to be 4.1m, the distance between the 0 section and the lip is 8.3m, the radius of the curled edge is 1.74m, the distance between the straight section of the air inlet and the lip is 9.2m, and the radius is 0.8 m. Therefore, the profile curve has three characteristic points of (0, 4.1), (8.3, 1.74) and (9.2 and 0.8), and the streamline model is y-0.09401 e after fitting calculation0.3872x+4.1. The fitted image is shown in fig. 4.
Based on measured 0 section static pressure p0=100410.26Pa,fpStatic pressure of cross section
Figure BDA0003041706110000081
Static pressure p of f cross sectionfObtaining three characteristic points of static pressure fitting, namely 100425.3Pa and measuring point positions, calculating differential pressure to obtain three characteristic points of (0, 0), (8.8, 4.74) and (9.1, 15.04), and calculating the static pressure difference distribution model to be delta P2.85 multiplied by 10 after fitting calculation- 8e2.193x+0.4818. The fitted image is shown in fig. 5.
The obtained streamline description and static pressure difference are distributively carried into Fpre-entry+FbellCalculating the sigma 2 pi delta pyy' to obtain the value F of the pre-air inlet pipe and the lip curling resistancepre-entry+Fbell=86N。
d. Bottom resistance Fbase=(P9-P0)(A8-A9)
Wherein the content of the first and second substances,
P9=100236.97Pa;
A8-A9=0.15m2
to determine the bottom resistance Fbase=(P9-P0)(A8-A9)=-173.29×0.15=26N。
Step two, F obtained by the step onepre-entry+FbellThe calculation result of the correction term is used for obtaining the corrected real thrust Fg
Fg=FM+w0·v0-Fpre-entry-Fbell+Fcradle+Fbase
The above detailed description is intended to illustrate the objects, aspects and advantages of the present invention, and it should be understood that the above detailed description is only exemplary of the present invention and is not intended to limit the scope of the present invention, and any modifications, equivalents, improvements and the like made within the spirit and principle of the present invention should be included in the scope of the present invention.

Claims (1)

1. The streamline method aviation engine thrust correction method based on the field test is characterized by comprising the following steps: the method comprises the following steps:
step one, obtaining various correction values of thrust correction through field test
1) Determining the position of the measurement cross section:
a. determining the position of a section 0, wherein the section 0 is placed at a position 5-7 d away from an engine lip, and d is the diameter of an engine inlet; the air flow of the section at the position is more uniform;
b. determining the position of the 9 section, wherein the 9 section has different positions for different types of engines, when the turbojet turbofan engine with small bypass ratio is tested on site, the 9 section is positioned at the tail nozzle or the inner bypass outlet section, and when the turbofan engine with large bypass ratio is tested on site, the 9 section is positioned at the outer bypass outlet section;
c.0-f area measuring points need to be arranged at the secondary flow stable position and are placed at the position within 3m from the wall surface of the test room, and the section f of the lip is taken as the section and the f at the position 1m on the front side of the lippA cross section;
2) determining measurement parameters required in the correction term calculation, said parameters including:
a. resistance w of air-intake impulse0·v0
Wherein the average velocity v of the cross section is 00Intake air flow rate w0
b. Resistance of the stent
Figure FDA0003041706100000011
Wherein ρ is the airflow density; cd [ Cd ]iThe drag coefficient of the individual components was 2.05; a. theciIs the area of the blockage of a single component, in m2;VciIs the velocity of the gas flowing over the obstruction area;
c. sum of resistance F of pre-air inlet flow pipe and lip curlingpre-entry+Fbell═ 2 pi Δ p (x) y' (x) dx, with the axis of the engine as the x-axis, the direction pointing from the 0 cross-section to the 9 cross-section, the perpendicular direction to the test room being the y-axis, the direction being vertically upward, the center of the cross-section far ahead 0 being the origin of coordinates;
where y (x) is a position coordinate that varies with x; p (x) is the static pressure value as a function of x, y' (x) is the derivative of y (x) with respect to x;
the streamline model of the control body is y (x) ═ aebx+c;
Wherein a, b and c are three coefficients, and the closed curve is calculated by measuring the x coordinate position and the section radius of any 3 points on the pre-air inlet flow pipe;
the section radius of the pre-air inlet flow pipe is measured between the section 0 and the lip of the engine, namely a 0-f area, and the secondary flow velocities of any three sections are adopted as w'0=ρv′0-fA' calculates the area of the secondary flow of the cross section, passing through A0-fObtaining the area of the pre-inlet airflow pipe of the section as A-A', and then calculating the radius of the pre-inlet airflow pipe of the section;
wherein, w'0Intake air flow rate, v ', of secondary flow'0-fFor measuring the mean value of the secondary flow velocity of the cross section, A' is the secondary flow cross section area of the cross section, A0-fThe sectional area of the pre-inlet gas flow pipe is a measured section;
the static pressure difference of each point on the control flow line is related to the radius of the pre-air inlet flow pipe, and the model is delta P (x) menx+r;
Wherein m, n and r are three coefficients, and a closed curve can be calculated by measuring static pressure difference values between a secondary flow part of any three sections and the section 0 and an x coordinate position of the section between the section 0 and the lip of the engine, namely a 0-f area;
d. bottom resistance Fbase=(P9-P0)(A8-A9);
Wherein, P9-P0Is the static pressure difference between the 9 section and the 0 section, A8-A9Is the area of the tail nozzle;
3) determining the measurement mode of each parameter:
a.0 section is composed of 5 multiplied by 5 measuring points, 25 wind speed measuring points and 25 total static pressure measuring points are arranged on a measuring bent frame to measure the wind speed and the total static pressure of the 0 section; the 0 section measuring bent is shown in figure 3;
b. an anemometer is arranged on the windward side of the bracket at the airflow speed on the bracket;
c.f cross-section and fp3 wind speed measuring points and 3 total static pressure measuring points are respectively arranged at the secondary flow stabilization part of the section to measure wind speed and total static pressure values; the static pressure difference is the difference between a measuring point on the section and the static pressure corresponding to the section position of 0; f and fpRespectively connecting 6 static pressure measuring points of the section measurement and 6 static pressure measuring points of corresponding height positions on the section 0 into a differential pressure sensor, and measuring static pressure difference;
d. the surface of the outer duct of the tail nozzle of the engine is provided with 4 static pressure sensors, and the measured surface static pressure value is shown in figure 1; the overall measuring point arrangement is shown in FIG. 2;
4) the measured data processing method comprises the following steps:
a.0 section average velocity v0Obtained by averaging 25 measured points, i.e.
Figure FDA0003041706100000021
b.f sectional static pressure difference Δ pf=pf-p0Wherein p isfIs the average value of three static pressure measuring points of the f section
Figure FDA0003041706100000022
p0Is the average value of 25 measuring points of 0 section
Figure FDA0003041706100000023
fpStatic pressure difference of cross section
Figure FDA0003041706100000024
Wherein
Figure FDA0003041706100000025
Is fpAverage value of three static pressure measuring points of cross section
Figure FDA0003041706100000026
Section f andpthe velocity of the secondary flow of the cross section is taken as the average value of three velocity measuring points
Figure FDA0003041706100000031
c.9 static cross-sectional pressure p9Taking the average value of 4 static pressure measuring points
Figure FDA0003041706100000032
Step two, F obtained by the step onepre-entry+FbellThe calculation result of the correction term is used for obtaining the corrected real thrust Fg
Fg=FM+w0·v0-Fpre-entry-Fbell+Fcradle+Fbase
CN202110459087.9A 2021-04-27 2021-04-27 Streamline method aviation engine thrust correction method based on field test Active CN113155468B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202110459087.9A CN113155468B (en) 2021-04-27 2021-04-27 Streamline method aviation engine thrust correction method based on field test

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202110459087.9A CN113155468B (en) 2021-04-27 2021-04-27 Streamline method aviation engine thrust correction method based on field test

Publications (2)

Publication Number Publication Date
CN113155468A true CN113155468A (en) 2021-07-23
CN113155468B CN113155468B (en) 2022-07-15

Family

ID=76871364

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202110459087.9A Active CN113155468B (en) 2021-04-27 2021-04-27 Streamline method aviation engine thrust correction method based on field test

Country Status (1)

Country Link
CN (1) CN113155468B (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114383850A (en) * 2021-12-10 2022-04-22 厦门大学 Open test bed thrust correction method under natural wind condition
CN117113887A (en) * 2023-10-24 2023-11-24 中国航空工业集团公司北京长城计量测试技术研究所 Method and device for correcting additional resistance of air inlet channel of indoor test bed of aero-engine

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20070276601A1 (en) * 2006-05-25 2007-11-29 Rolls-Royce Plc Thrust correction
CN102053017A (en) * 2009-11-09 2011-05-11 沈阳黎明航空发动机(集团)有限责任公司 Method and system for testing air flow field of indoor engine test-bed
CN102393305A (en) * 2011-10-28 2012-03-28 沈阳黎明航空发动机(集团)有限责任公司 Method for calibrating pushing force of trial run table inside engine room
CN104596769A (en) * 2014-12-14 2015-05-06 中国航空工业集团公司北京长城计量测试技术研究所 Real thrust measuring and calculating method for test run of aero-engine on indoor test bed

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20070276601A1 (en) * 2006-05-25 2007-11-29 Rolls-Royce Plc Thrust correction
CN102053017A (en) * 2009-11-09 2011-05-11 沈阳黎明航空发动机(集团)有限责任公司 Method and system for testing air flow field of indoor engine test-bed
CN102393305A (en) * 2011-10-28 2012-03-28 沈阳黎明航空发动机(集团)有限责任公司 Method for calibrating pushing force of trial run table inside engine room
CN104596769A (en) * 2014-12-14 2015-05-06 中国航空工业集团公司北京长城计量测试技术研究所 Real thrust measuring and calculating method for test run of aero-engine on indoor test bed

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
任怡雪 等: "航空发动机气动附加阻力修正测点布置与试验", 《计测技术》 *
王辰辰 等: "航空矢量发动机试车台推力校准技术综述", 《计测技术》 *
艾延廷 等: "基于流截法的航空发动机室内试车推力校准", 《沈阳航空航天大学学报》 *

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114383850A (en) * 2021-12-10 2022-04-22 厦门大学 Open test bed thrust correction method under natural wind condition
CN117113887A (en) * 2023-10-24 2023-11-24 中国航空工业集团公司北京长城计量测试技术研究所 Method and device for correcting additional resistance of air inlet channel of indoor test bed of aero-engine
CN117113887B (en) * 2023-10-24 2024-01-23 中国航空工业集团公司北京长城计量测试技术研究所 Method and device for correcting additional resistance of air inlet channel of indoor test bed of aero-engine

Also Published As

Publication number Publication date
CN113155468B (en) 2022-07-15

Similar Documents

Publication Publication Date Title
CN113155468B (en) Streamline method aviation engine thrust correction method based on field test
CN108225717B (en) Measuring method for internal flow resistance in wind tunnel test
Langston et al. Three-dimensional flow within a turbine cascade passage
Johnson et al. The development of wake flow in a centrifugal impeller
US20140208755A1 (en) Gas Turbine Air Mass Flow Measuring System and Methods for Measuring Air Mass Flow in a Gas Turbine Inlet Duct
CN111649948A (en) Air inlet system for annular blade cascade performance tester
JP2014145763A (en) Systems and methods for measuring flow profile in turbine engine flow path
KR101869648B1 (en) Flow rate calibration device for wind tunnel model and method thereof
CN113916486A (en) Low-speed wind tunnel rapid pressure measurement and control method based on multi-parameter pressure regression algorithm
CN114323540B (en) Half-mould blowing high-lift wind tunnel test method and device for conveyor
CN113188799B (en) Aero-engine thrust correction method based on speed difference extreme value method
JP5569383B2 (en) Pulsating flow measurement method and gas flow measurement device
CN208534819U (en) Device for the test of fan aeroperformance
JP2006162417A (en) Total pressure/static pressure measuring venturi system flow measuring device
CN114383850B (en) Open test bed thrust correction method under natural wind condition
JP7421769B2 (en) Duct pressure measurement structure and wind tunnel test equipment
CN111498141B (en) Method and device for realizing real-time monitoring of airflow angle based on micro probe
CN115575074B (en) High-speed wind tunnel ventilation model internal resistance measurement uncertainty analysis method
CN114528778B (en) Air flow measuring method based on bell mouth flow tube speed distribution model
CN211904600U (en) False tail branch for measuring internal resistance of ventilation model
CN115708089A (en) Flow tube calibration data processing method
CN114659793B (en) Wind speed and direction envelope determination method for open-air test run experiment of engine
CN115575080B (en) Method for accurately measuring internal resistance of high-speed wind tunnel ventilation model
CN117007274B (en) Subsonic wind tunnel loop mass flow measurement method
Zhang et al. Mach number and freestream turbulence effects on turbine vane aerodynamic losses

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