CN114330035A - High-speed aircraft aerodynamic performance evaluation method - Google Patents

High-speed aircraft aerodynamic performance evaluation method Download PDF

Info

Publication number
CN114330035A
CN114330035A CN202210224593.4A CN202210224593A CN114330035A CN 114330035 A CN114330035 A CN 114330035A CN 202210224593 A CN202210224593 A CN 202210224593A CN 114330035 A CN114330035 A CN 114330035A
Authority
CN
China
Prior art keywords
pulsation
aircraft
signal
wall
friction
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
CN202210224593.4A
Other languages
Chinese (zh)
Other versions
CN114330035B (en
Inventor
余明
傅亚陆
刘朋欣
袁先旭
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.)
Computational Aerodynamics Institute of China Aerodynamics Research and Development Center
Original Assignee
Computational Aerodynamics Institute of China Aerodynamics Research and Development Center
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 Computational Aerodynamics Institute of China Aerodynamics Research and Development Center filed Critical Computational Aerodynamics Institute of China Aerodynamics Research and Development Center
Priority to CN202210224593.4A priority Critical patent/CN114330035B/en
Publication of CN114330035A publication Critical patent/CN114330035A/en
Application granted granted Critical
Publication of CN114330035B publication Critical patent/CN114330035B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Aerodynamic Tests, Hydrodynamic Tests, Wind Tunnels, And Water Tanks (AREA)

Abstract

The invention discloses a method for evaluating aerodynamic performance of a high-speed aircraft, which relates to the field of aircraft research, and is based on the superposition effect and modulation effect of an outer-region large-scale turbulence structure on near-wall turbulence pulsation, and according to the generalized Reynolds ratio of speed-temperature pulsation, a model for predicting friction resistance and heat flow pulsation of a high-Reynolds-number wall turbulence is established, so that accurate prediction of the friction resistance and the heat flow pulsation of a compressible high-Reynolds-number turbulence wall based on flow field measurable signals is realized, and accurate evaluation of the aerodynamic performance of the high-speed aircraft is further realized.

Description

High-speed aircraft aerodynamic performance evaluation method
Technical Field
The invention relates to the field of aircraft research, in particular to a method for evaluating aerodynamic performance of a high-speed aircraft.
Background
The aerodynamic design and evaluation of the aircraft are important links in the aircraft development process. The aerodynamic design of the aircraft is a process of optimally selecting the layout form and geometric parameters of the aircraft to improve the aerodynamic performance and the flight performance. The aircraft performance evaluation refers to the process of evaluating the performances of the aircraft such as pneumatics, flight control, stealth, structural strength, power and the like through wind tunnel tests, numerical calculation, flight simulation, flight tests and other means in the design and use processes of the aircraft. The two are organic whole, the quality of the aerodynamic design of the aircraft needs to be judged through evaluation, and the innovation of the aerodynamic design can continuously push the development of the evaluation method and means.
High Reynolds number wall turbulence is an important flow problem in the field of aerospace and has a high scientific/engineering value. Outer region with increasing Reynolds number: (
Figure 100002_DEST_PATH_IMAGE001
Figure 278866DEST_PATH_IMAGE002
At an outer scale, i.e.
Figure 100002_DEST_PATH_IMAGE003
) The large-scale motion is enhanced, and large-scale structures (the length is more than 2 times of the thickness of a boundary layer) above a logarithmic region have important influence on wall resistance, heat flow and near-wall turbulence pulsation. The influence rule of the outer region large-scale structure on the near-wall region small-scale (the length is less than 2 times of the boundary layer thickness) turbulence pulsation is deeply known, and the near-wall turbulence pulsation is accurately predicted, so that the method has important significance on the evaluation, optimization and development of the aerodynamic performance of the high-speed aircraft. A great deal of research has been carried out in recent years to reveal the contribution of turbulent pulsations to the mean resistance of the walls and to the mean heat flow. However, accurate prediction of average resistance and heat flow is not sufficientTo completely predict the aerodynamic performance of the aircraft. Researches show that strong shearing events caused by turbulence pulsation on the wall surface can cause local wall surface shearing stress and heat flow pulsation to exceed 3-5 times of the average value, and the structural strength insufficiency and the thermal protection failure of the high-speed aircraft are easily caused. Therefore, the method has important engineering application value for accurately predicting the wall resistance and the heat flow pulsation.
The outer region large scale structure can be aligned with the inner region
Figure 727165DEST_PATH_IMAGE004
Figure 100002_DEST_PATH_IMAGE005
Dimensionless for the inner scale, i.e. using the viscosity scale) turbulence effects, leaving "footprints" in the near-wall region, a phenomenon known as "stacking effects"; the strength of the small-scale turbulence pulsation of the near-wall area is enhanced in the large-scale high-speed area and weakened in the large-scale low-speed area, the small-scale pulsation of the inner area has strong correlation with the large-scale turbulence pulsation of the outer area, and the nonlinear interaction is called as amplitude modulation effect. Based on the superposition and modulation effects, Marusic et al of the university of Melben proposes a prediction model of the flow direction velocity pulsation in the near-wall region, and proposes a prediction method of the variation trend of the intensity of the wall friction resistance pulsation along with the Reynolds number based on the prediction model, but the model only aims at the incompressible wall turbulence and only qualitatively describes the wall friction resistance pulsation. While for compressible wall turbulence, the near wall predictive model is very limited to study. In compressible turbulence, the density-weighted velocity pulsation intensity is generally considered consistent with the incompressible turbulence results at the same reynolds number, and thus the variation in average density needs to be considered in the predictive model. Helm et al proposed a prediction model of near-wall velocity and temperature pulsation in 2014, which can give better velocity and temperature pulsation strength, wherein the prediction model of near-wall region temperature pulsation is similar to the model of velocity pulsation, however, there is no obvious correlation between the prediction formula and the strong Reynolds ratio, which results in unclear physical meaning of the prediction method and large error.
At present, a prediction method for friction resistance and heat flow pulsation of a compressible wall turbulent flow wall surface, which is accurate in prediction, good in universality and clear in physical significance, is not available, and therefore the aerodynamic performance evaluation result of the existing aircraft based on the friction resistance pulsation and the heat flow pulsation of the wall surface is not accurate.
Disclosure of Invention
The invention aims to improve the accuracy of aerodynamic performance evaluation of a high-speed aircraft.
In order to achieve the above object, the present invention provides a method for evaluating aerodynamic performance of a high-speed aircraft, the method comprising:
constructing an aircraft wall friction resistance pulsation prediction model and an aircraft wall heat flow pulsation prediction model;
obtaining first intermediate quantity data and second intermediate quantity data through numerical simulation or experimental calibration, wherein the first intermediate quantity data comprises: the method comprises the following steps of predicting a relevant modulation coefficient of the friction drag pulsation of the wall surface of the aircraft, predicting a relevant universal signal of the friction drag pulsation of the wall surface of the aircraft, predicting a relevant phase difference of the friction drag pulsation of the wall surface of the aircraft and predicting a relevant linear random estimation kernel function of the friction drag pulsation of the wall surface of the aircraft; the second intermediate quantity data comprises: the method comprises the following steps that a relevant modulation coefficient of prediction of the wall surface heat flow pulsation of the aircraft, a relevant general signal of prediction of the wall surface heat flow pulsation of the aircraft, a relevant phase difference of prediction of the wall surface heat flow pulsation of the aircraft and a linear random prediction kernel function of prediction of the wall surface heat flow pulsation of the aircraft are obtained;
obtaining a flow direction velocity signal and a span direction velocity signal of a first preset size structure in a first area, transforming the flow direction velocity signal and the span direction velocity signal into a spectrum space to obtain a first signal and a second signal,
obtaining a first superposition result of the flow direction speed signal in a second area and a second superposition result of the spread direction speed signal in the second area based on the first signal, the second signal and a linear random prediction kernel function related to aircraft wall friction resistance pulsation prediction;
calculating to obtain the friction pulsation of the wall surface of the aircraft by utilizing the friction pulsation prediction model of the wall surface of the aircraft based on the first superposition result, the second superposition result and the first intermediate quantity data;
calculating and obtaining the wall heat flow pulsation of the aircraft by using the wall heat flow pulsation prediction model of the aircraft based on the first superposition result and the second intermediate quantity data;
and evaluating the aerodynamic performance of the aircraft based on the aircraft wall friction resistance pulsation and the aircraft wall heat flow pulsation.
For convenience in description, the first area is briefly described as an outer area, the first preset size is briefly described as a large size, the second area is briefly described as an inner area, and the first preset size is briefly described as a small size in the description of the invention.
Preferably, the aircraft wall surface friction pulsation prediction model includes:
Figure 897115DEST_PATH_IMAGE006
Figure 100002_DEST_PATH_IMAGE007
wherein,
Figure 495587DEST_PATH_IMAGE008
as a variable of the spatial coordinates,
Figure 100002_DEST_PATH_IMAGE009
to predict the flow-to-wall shear stress ripple,
Figure 575538DEST_PATH_IMAGE010
to predict the development of wall shear stress pulsations,
Figure 100002_DEST_PATH_IMAGE011
for the generic signal of the de-superposition effect,
Figure 53793DEST_PATH_IMAGE012
in order to de-modulate the pervasive signal of the effect,
Figure 100002_DEST_PATH_IMAGE013
the modulation coefficients of the flow direction friction pulsation of the second preset-size structure on the wall surface of the aircraft are obtained for the flow direction speed signal and the spreading direction speed signal,
Figure 524088DEST_PATH_IMAGE014
the modulation coefficients of the flow direction speed signal and the spanwise speed signal to the spanwise friction drag pulsation of a second preset size structure on the wall surface of the aircraft,
Figure 100002_DEST_PATH_IMAGE015
in order to compensate the phase difference of the flow direction friction pulsation superposition effect to the modulation effect,
Figure 254147DEST_PATH_IMAGE016
for the phase difference of the spanwise superposition effect to the modulation effect,
Figure 100002_DEST_PATH_IMAGE017
for the superposition of the streaming velocity signal at the second region,
Figure 319098DEST_PATH_IMAGE018
is a superposition of the spanwise velocity signal at a second region.
The aircraft wall friction pulsation can be accurately predicted and obtained through the aircraft wall friction pulsation prediction model.
Preferably, the aircraft wall heat flow pulsation prediction model is as follows:
Figure 100002_DEST_PATH_IMAGE019
wherein,
Figure 515724DEST_PATH_IMAGE020
the prediction result of the heat flow pulsation of the wall surface of the aircraft,
Figure 4474DEST_PATH_IMAGE008
as a variable of the spatial coordinates,
Figure 100002_DEST_PATH_IMAGE021
is a universal signal of the pulsation of the heat flow,
Figure 272645DEST_PATH_IMAGE022
the modulation coefficients of the flow direction friction pulsation of the second preset-size structure on the wall surface of the aircraft are obtained for the flow direction speed signal and the spreading direction speed signal,
Figure 100002_DEST_PATH_IMAGE023
the modulation coefficients of the flow direction speed signal and the spread direction speed signal to the heat flow pulsation of the structure with the second preset size on the wall surface of the aircraft,
Figure 248560DEST_PATH_IMAGE024
for superposition at a second region of the streaming velocity signal,
Figure 100002_DEST_PATH_IMAGE025
in order to compensate the phase difference of the flow direction friction pulsation superposition effect to the modulation effect,
Figure 84929DEST_PATH_IMAGE026
the modulation phase difference is modulated for the heat flow superposition,
Figure 100002_DEST_PATH_IMAGE027
the heat flow for the first pre-sized structure is pulsed.
The aircraft wall heat flow pulsation can be accurately predicted and obtained through the aircraft wall heat flow pulsation prediction model.
Preferably, in the method
Figure 592134DEST_PATH_IMAGE028
And
Figure 100002_DEST_PATH_IMAGE029
the calculation method is as follows:
Figure 523049DEST_PATH_IMAGE030
Figure 100002_DEST_PATH_IMAGE031
wherein,
Figure 697679DEST_PATH_IMAGE032
in order to perform the inverse fourier transform,
Figure 100002_DEST_PATH_IMAGE033
in order to flow to the linear random pre-estimated kernel function,
Figure 236107DEST_PATH_IMAGE034
for the span-wise linear random prediction kernel function,
Figure 100002_DEST_PATH_IMAGE035
in order to flow to the wavelength(s),
Figure 620821DEST_PATH_IMAGE036
in order to be a fourier transform,
Figure 100002_DEST_PATH_IMAGE037
in order to flow to the speed signal,
Figure 230794DEST_PATH_IMAGE038
in order to develop the speed signal in the direction of the speed,
Figure 100002_DEST_PATH_IMAGE039
the center position of the first preset size structure of the outer area.
Preferably, in the method, the center of the first region with the first preset size structure is positionedDevice for placing
Figure 869717DEST_PATH_IMAGE039
The calculation method is as follows:
Figure 438102DEST_PATH_IMAGE040
Figure 100002_DEST_PATH_IMAGE041
Figure 44532DEST_PATH_IMAGE042
Figure 100002_DEST_PATH_IMAGE043
wherein,
Figure 192617DEST_PATH_IMAGE044
in order to obtain the friction reynolds number,
Figure 100002_DEST_PATH_IMAGE045
in order to obtain a kinematic viscosity of the composition,
Figure 951626DEST_PATH_IMAGE046
as a result of the total shear stress of the wall,
Figure 100002_DEST_PATH_IMAGE047
the density of the wall surface is shown as,
Figure 346704DEST_PATH_IMAGE048
in order to be the viscosity coefficient,
Figure 100002_DEST_PATH_IMAGE049
in order to determine the speed of the friction,
Figure 315797DEST_PATH_IMAGE050
in order to be a measure of the viscosity,
Figure 100002_DEST_PATH_IMAGE051
is the boundary layer thickness.
Preferably, in the method
Figure 142938DEST_PATH_IMAGE027
The calculation method is as follows:
Figure 146666DEST_PATH_IMAGE052
wherein,
Figure 994537DEST_PATH_IMAGE032
in order to perform the inverse fourier transform,
Figure DEST_PATH_IMAGE053
for the linear random prediction kernel function associated with the heat flow,
Figure 575560DEST_PATH_IMAGE054
in order to flow to the wavelength(s),
Figure DEST_PATH_IMAGE055
in order to be a fourier transform,
Figure 3130DEST_PATH_IMAGE039
the center position of the first preset size structure of the first area,
Figure 799048DEST_PATH_IMAGE056
the temperature pulsation signal is a temperature pulsation signal of a first predetermined size structure at the center of the first area.
Preferably, in the method, the size of the first predetermined dimension is greater than 2 times the thickness of the boundary layer.
Preferably, in the method, the first region is a region with an outer dimension larger than 0.1, and the second region is a region with an inner dimension smaller than 50.
Preferably, the size of the second predetermined dimension in the method is less than or equal to 2 times the thickness of the boundary layer.
One or more technical schemes provided by the invention at least have the following technical effects or advantages:
the traditional prediction model only aims at the velocity pulsation, and only carries out qualitative estimation on the prediction of the wall friction pulsation, the prediction method makes up for the blank, realizes accurate prediction of the wall friction pulsation, can be conveniently popularized to other Mach number flows, and further realizes accurate evaluation of aerodynamic performance of the high-speed aircraft.
The traditional temperature pulsation prediction model and the strong Reynolds ratio are lack of obvious correlation, so that the error of the prediction model is large, the prediction method is based on the generalized Reynolds ratio derivation, the physical significance is clear, and the prediction error is remarkably reduced.
Drawings
The accompanying drawings, which are included to provide a further understanding of the embodiments of the invention and are incorporated in and constitute a part of this specification, illustrate embodiments of the invention and together with the description serve to explain the principles of the invention;
FIG. 1 is a schematic flow diagram of a method for evaluating aerodynamic performance of a high-speed aircraft;
FIG. 2 is a schematic diagram of joint probability density distribution of large-scale high-speed region condition statistics, in FIG. 2, the solid line is a DNS calculation result, and the dotted line is a prediction result;
FIG. 3 is a schematic diagram of joint probability density distribution of large-scale low-speed region condition statistics, in FIG. 3, the solid line is a DNS calculation result, and the dotted line is a prediction result;
FIG. 4 is a joint probability density distribution of large-scale high-speed region condition statistics, where a solid line in FIG. 4 is a DNS calculation result and a dotted line is a prediction result;
fig. 5 is a joint probability density distribution of the condition statistics of the large-scale low-speed region, in fig. 5, a solid line is a DNS calculation result, and a dotted line is a prediction result.
Detailed Description
In order that the above objects, features and advantages of the present invention can be more clearly understood, a more particular description of the invention will be rendered by reference to the appended drawings. It should be noted that the embodiments of the present invention and features of the embodiments may be combined with each other without conflicting with each other.
In the following description, numerous specific details are set forth in order to provide a thorough understanding of the present invention, however, the present invention may be practiced in other ways than those specifically described and thus the scope of the present invention is not limited by the specific embodiments disclosed below.
Example one
Referring to fig. 1, fig. 1 is a schematic flow chart of a method for evaluating aerodynamic performance of a high-speed aircraft, according to an embodiment of the present invention, the method includes:
constructing an aircraft wall friction resistance pulsation prediction model and an aircraft wall heat flow pulsation prediction model;
obtaining first intermediate quantity data and second intermediate quantity data through numerical simulation or experimental calibration, wherein the first intermediate quantity data comprises: the method comprises the following steps of predicting a relevant modulation coefficient of the friction drag pulsation of the wall surface of the aircraft, predicting a relevant universal signal of the friction drag pulsation of the wall surface of the aircraft, predicting a relevant phase difference of the friction drag pulsation of the wall surface of the aircraft and predicting a relevant linear random estimation kernel function of the friction drag pulsation of the wall surface of the aircraft; the second intermediate quantity data comprises: the method comprises the following steps that a relevant modulation coefficient of prediction of the wall surface heat flow pulsation of the aircraft, a relevant general signal of prediction of the wall surface heat flow pulsation of the aircraft, a relevant phase difference of prediction of the wall surface heat flow pulsation of the aircraft and a linear random prediction kernel function of prediction of the wall surface heat flow pulsation of the aircraft are obtained;
obtaining a flow direction velocity signal and a span direction velocity signal of a first preset size structure in a first area, transforming the flow direction velocity signal and the span direction velocity signal into a spectrum space to obtain a first signal and a second signal,
obtaining a first superposition result of the flow direction speed signal in a second area and a second superposition result of the spread direction speed signal in the second area based on the first signal, the second signal and a linear random prediction kernel function related to aircraft wall friction resistance pulsation prediction;
calculating to obtain the friction pulsation of the wall surface of the aircraft by utilizing the friction pulsation prediction model of the wall surface of the aircraft based on the first superposition result, the second superposition result and the first intermediate quantity data;
calculating and obtaining the wall heat flow pulsation of the aircraft by using the wall heat flow pulsation prediction model of the aircraft based on the first superposition result and the second intermediate quantity data;
and evaluating the aerodynamic performance of the aircraft based on the aircraft wall friction resistance pulsation and the aircraft wall heat flow pulsation.
The method adopts the existing technical means to realize the evaluation of the aerodynamic performance of the aircraft based on the wall friction pulsation of the aircraft and the wall heat flow pulsation of the aircraft, for example, the aerodynamic performance of the aircraft can be evaluated by adopting the local distribution of the wall friction and the heat flow pulsation, the extremely high friction and the high heat flow events which are easy to cause structural damage and the failure of a heat protection device, and the like.
The method is described in detail below with reference to specific steps:
from the near-wall (i.e., inner zone) velocity pulsations, wall friction pulsations are predicted:
firstly, the total shear stress of the wall surface is determined
Figure 880136DEST_PATH_IMAGE046
Wall surface density
Figure 27084DEST_PATH_IMAGE047
And coefficient of viscosity
Figure 976454DEST_PATH_IMAGE048
The friction speed can be defined
Figure 689195DEST_PATH_IMAGE049
And a viscosity scale
Figure 550972DEST_PATH_IMAGE050
Figure DEST_PATH_IMAGE057
Figure 897465DEST_PATH_IMAGE043
(1)
Definition of Friction Reynolds number
Figure 197997DEST_PATH_IMAGE044
Figure 171769DEST_PATH_IMAGE045
Kinematic viscosity:
Figure 266764DEST_PATH_IMAGE041
(2)
superscript for variables dimensionless by viscosity scale "+"means.
The basic idea of the prediction model is to consider the superposition of a pervasive signal which is independent of the Reynolds number of an inner region in the near-wall turbulence pulsation and an outer region large-scale signal, wherein the outer region large-scale signal has an amplitude modulation effect on the near-wall small-scale pulsation. Thus, following the velocity ripple, the wall friction ripple prediction model can be written in the form (the following physical quantities are dimensionless by a viscosity scale defined by wall mean shear stress, viscosity coefficient and density):
Figure 450620DEST_PATH_IMAGE058
(3)
Figure DEST_PATH_IMAGE059
(4)
wherein the subscript (.) x And (·) z Respectively representing the flow direction and the spreading direction;
Figure 476214DEST_PATH_IMAGE008
for space coordinate variables, left side of equation
Figure 101231DEST_PATH_IMAGE009
Figure 429444DEST_PATH_IMAGE010
For wall shear stress pulsation in flow and spread directionThe predicted outcome of (a "wall" refers to a solid surface); the two terms on the right side of the equation represent the modulating effect and the superposition effect of the outer region large scale structure on the near wall small scale pulsation, respectively ("near wall" i.e., inner region turbulence). In the first item, the first item is,
Figure 710383DEST_PATH_IMAGE011
and
Figure 618297DEST_PATH_IMAGE012
for a generic signal that de-superimposes and modulates effects,
Figure 425716DEST_PATH_IMAGE017
and
Figure 49464DEST_PATH_IMAGE018
in addition to the superposition of the outer large-scale signal at the near wall,
Figure 880017DEST_PATH_IMAGE022
and
Figure 388358DEST_PATH_IMAGE060
the modulation coefficients corresponding to the flow direction and the span direction respectively,
Figure DEST_PATH_IMAGE061
and
Figure 660071DEST_PATH_IMAGE016
the phase difference of the modulation is the sum-pair of the flow direction and the spread direction, respectively.
The large-scale shear stress pulsation is determined by an outer region large-scale speed pulsation signal and is given by a spectrum space linear random estimation method:
Figure 533349DEST_PATH_IMAGE062
(5)
Figure DEST_PATH_IMAGE063
(6)
wherein,
Figure 303728DEST_PATH_IMAGE033
and
Figure 350181DEST_PATH_IMAGE034
respectively, the kernel functions of linear random estimation of flow direction and span direction, and the independent variable is the wavelength of flow direction
Figure 69875DEST_PATH_IMAGE064
The central position of the outer zone large-scale structure is taken as
Figure 51738DEST_PATH_IMAGE040
. The meaning expressed by the above formula is: utilizing Fourier transform (FFT) to flow the outer region to the velocity signal in large scale
Figure 856883DEST_PATH_IMAGE037
And spanwise velocity signal
Figure 441448DEST_PATH_IMAGE038
Transformation to spectral space
Figure DEST_PATH_IMAGE065
And
Figure 937020DEST_PATH_IMAGE066
multiplying by linear random prediction kernel function
Figure 214418DEST_PATH_IMAGE033
And
Figure 913384DEST_PATH_IMAGE034
then through inverse Fourier transform
Figure DEST_PATH_IMAGE067
Transformation to physical space.
In the prediction model, an outer region large-scale signal is an input signal; other parameters need to be calibrated by high-precision numerical simulation or experimental data.
Based on the generalized Reynolds ratio, the near-wall heat flow pulsation is obtained by prediction:
to better understand the pulsation of the physical quantity, the reynolds average and Favre average are first defined. A general physical quantity
Figure 301640DEST_PATH_IMAGE068
Reynolds average of
Figure DEST_PATH_IMAGE069
Corresponding turbulence pulsation is
Figure 651718DEST_PATH_IMAGE070
Namely:
Figure DEST_PATH_IMAGE071
(7)
having a Favre average of
Figure 834438DEST_PATH_IMAGE072
Corresponding turbulence pulsation is
Figure DEST_PATH_IMAGE073
Namely:
Figure 20700DEST_PATH_IMAGE074
(8)
defining root mean square
Figure DEST_PATH_IMAGE075
(or referred to as pulse intensity):
Figure 947067DEST_PATH_IMAGE076
(9)
the generalized Reynolds simulation indicates a strong correlation between velocity and temperature pulsation in a compressible wall turbulence, and it is easy to judge that there is also a strong correlation between wall friction and heat flow. Gaviglio-based proposed modificationAdvancing Reynolds analogous relation (GSRA), i.e. velocity and temperature pulsation intensity
Figure DEST_PATH_IMAGE077
And
Figure 948390DEST_PATH_IMAGE078
the relation between:
Figure DEST_PATH_IMAGE079
(10)
wherein
Figure 442957DEST_PATH_IMAGE080
And
Figure DEST_PATH_IMAGE081
to determine the reynolds average velocity and temperature profile,
Figure 975569DEST_PATH_IMAGE082
the ratio of specific heat is shown as the ratio,
Figure DEST_PATH_IMAGE083
the local reynolds number is the local reynolds number,
Figure 830262DEST_PATH_IMAGE084
is the average total temperature distribution. Further assume velocity pulsation
Figure DEST_PATH_IMAGE085
And temperature pulsation
Figure 764720DEST_PATH_IMAGE086
The correlation can be directly carried out by the above formula, which is derived as follows:
Figure DEST_PATH_IMAGE087
(11)
in the formula
Figure 226925DEST_PATH_IMAGE088
To be fixedSpecific heat under pressure. Equation (11) can also be written as:
Figure DEST_PATH_IMAGE089
(12)
equal simultaneous derivation of both sides to obtain wall friction pulsation
Figure 642906DEST_PATH_IMAGE090
And heat flow pulsation
Figure DEST_PATH_IMAGE091
The association of (1):
Figure 645497DEST_PATH_IMAGE092
(13)
suppose large-scale friction pulsation
Figure DEST_PATH_IMAGE093
And heat flow pulsation
Figure 575407DEST_PATH_IMAGE094
Satisfy strong reynolds analog relation GSRA:
Figure DEST_PATH_IMAGE095
(14)
from the quasi-stationary, constant, quasi-uniform assumption, the following small-scale pulsations are proposed (subscript:)
Figure 536410DEST_PATH_IMAGE096
) Correction of (2):
Figure DEST_PATH_IMAGE097
(15)
wherein,
Figure 964986DEST_PATH_IMAGE098
is a small-scale friction drag pulsation, and the friction drag pulsation is small,
Figure DEST_PATH_IMAGE099
is a large scale flow direction velocity pulsation. For a general physical quantity
Figure 912213DEST_PATH_IMAGE100
Figure DEST_PATH_IMAGE101
Given the strong dependence of large-scale velocity and temperature pulsations, the large-scale heat flow pulsations are expressed as:
Figure 821263DEST_PATH_IMAGE102
(16)
writing the small-scale heat flow pulsation as universal signal and modulation coefficient
Figure DEST_PATH_IMAGE103
In the form of:
Figure 812222DEST_PATH_IMAGE104
(17)
wherein the function
Figure DEST_PATH_IMAGE105
Is defined as:
Figure 72302DEST_PATH_IMAGE106
(18)
substituting equation (16) into equation (18), suppose
Figure DEST_PATH_IMAGE107
As a constant, we obtain:
Figure 557641DEST_PATH_IMAGE108
(19)
substituting (17) to obtain:
Figure DEST_PATH_IMAGE109
(20)
Figure 508149DEST_PATH_IMAGE110
(21)
further assume that the generic signal of heat flow pulsation can be written as:
Figure DEST_PATH_IMAGE111
(22)
the small scale heat flow pulsation can be written as:
Figure 545375DEST_PATH_IMAGE112
(23)
the large-scale speed in the above formula is replaced by the wall friction pulsation, and the wall average heat flow is used for non-dimensionalization, so that the prediction model of the wall heat flow pulsation is as follows:
Figure 496013DEST_PATH_IMAGE113
(24)
wherein the large-scale heat flow pulsation is obtained by a linear random estimation method of a spectrum space:
Figure 50622DEST_PATH_IMAGE114
(25)
modulation factor
Figure 137527DEST_PATH_IMAGE115
Universal signal
Figure 611234DEST_PATH_IMAGE116
Phase difference of superposition pair modulation
Figure 970540DEST_PATH_IMAGE117
And linear random pre-estimated kernel function
Figure 125578DEST_PATH_IMAGE118
Given by direct numerical simulation or experimental calibration.
The method is based on the superposition effect and modulation effect of the outer region large-scale turbulence structure on the near-wall turbulence pulsation and the generalized Reynolds ratio of speed-temperature pulsation, obtains a high Reynolds number wall turbulence wall friction resistance and heat flow pulsation prediction model, and realizes accurate evaluation of aerodynamic performance of the high-speed aircraft based on the 2 models.
The construction idea of the prediction model of the friction resistance and the heat flow pulsation of the middle and high Reynolds number wall turbulence wall surface which is invalid is as follows:
the wall friction resistance and the heat flow are considered to be composed of large-scale and small-scale signals; the large scale has a modulation effect on the small scale signal, and the small scale pervasive signal without the modulation effect has nothing to do with Reynolds number and Mach number. Therefore, the wall friction can be written as a superposition of the small-scale pulse of the large-scale modulation and the large-scale signal. Further, according to the strong correlation between the speed and the temperature pulsation, a prediction model of the wall surface heat flow pulsation is derived.
Example two
The second embodiment of the present invention will be described in detail with reference to specific examples:
in application, the modulation coefficient, the phase difference of modulation pair superposition, the linear correlation kernel function and the like in the model need to be directly numerically simulated and calibrated by the medium Reynolds number/the high Reynolds number, and the model can be suitable for other parameters after being calibrated.
When in use, the input signals are as follows: the outer zone large-scale velocity pulsation can be given by low-resolution numerical simulation or experimental measurement; outputting a signal: wall friction and heat flow pulsation signals.
The accuracy of the prediction result of the method is verified through joint Probability Density (PDF), and the parameters are calculated as follows: the incoming flow Mach number is 3.0, the total incoming flow temperature is 300K, the wall surface temperature is 420K, and the Reynolds number is 42000. As shown in fig. 2-5. The result in the graph shows that the statistical results of PDF (Portable document Format) and Direct Numerical Simulation (DNS) given by the prediction method are well matched, the prediction method can accurately reflect the superposition and modulation effects of the large-scale pulsation of the outer region on the near-wall turbulence, and the accuracy of the prediction method is proved.
FIG. 2 is a schematic diagram of joint probability density distribution of large-scale high-speed region condition statistics, in FIG. 2, the solid line is a DNS calculation result, and the dotted line is a prediction result; fig. 3 is a schematic diagram of joint probability density distribution of large-scale low-speed region condition statistics, in fig. 3, a solid line is a DNS calculation result, and a dotted line is a prediction result.
FIG. 4 is a joint probability density distribution of large-scale high-speed region condition statistics, where a solid line in FIG. 4 is a DNS calculation result and a dotted line is a prediction result; fig. 5 is a joint probability density distribution of the condition statistics of the large-scale low-speed region, in fig. 5, a solid line is a DNS calculation result, and a dotted line is a prediction result.
While preferred embodiments of the present invention have been described, additional variations and modifications in those embodiments may occur to those skilled in the art once they learn of the basic inventive concepts. Therefore, it is intended that the appended claims be interpreted as including preferred embodiments and all such alterations and modifications as fall within the scope of the invention.
It will be apparent to those skilled in the art that various changes and modifications may be made in the present invention without departing from the spirit and scope of the invention. Thus, if such modifications and variations of the present invention fall within the scope of the claims of the present invention and their equivalents, the present invention is also intended to include such modifications and variations.

Claims (9)

1. A method for evaluating aerodynamic performance of a high-speed aircraft, the method comprising:
constructing an aircraft wall friction resistance pulsation prediction model and an aircraft wall heat flow pulsation prediction model;
obtaining first intermediate quantity data and second intermediate quantity data through numerical simulation or experimental calibration, wherein the first intermediate quantity data comprises: the method comprises the following steps of predicting a relevant modulation coefficient of the friction drag pulsation of the wall surface of the aircraft, predicting a relevant universal signal of the friction drag pulsation of the wall surface of the aircraft, predicting a relevant phase difference of the friction drag pulsation of the wall surface of the aircraft and predicting a relevant linear random estimation kernel function of the friction drag pulsation of the wall surface of the aircraft; the second intermediate quantity data comprises: the method comprises the following steps that a relevant modulation coefficient of prediction of the wall surface heat flow pulsation of the aircraft, a relevant general signal of prediction of the wall surface heat flow pulsation of the aircraft, a relevant phase difference of prediction of the wall surface heat flow pulsation of the aircraft and a linear random prediction kernel function of prediction of the wall surface heat flow pulsation of the aircraft are obtained;
obtaining a flow direction velocity signal and a span direction velocity signal of a first preset size structure in a first area, transforming the flow direction velocity signal and the span direction velocity signal into a spectrum space to obtain a first signal and a second signal,
obtaining a first superposition result of the flow direction speed signal in a second area and a second superposition result of the spread direction speed signal in the second area based on the first signal, the second signal and a linear random prediction kernel function related to aircraft wall friction resistance pulsation prediction;
calculating to obtain the friction pulsation of the wall surface of the aircraft by utilizing the friction pulsation prediction model of the wall surface of the aircraft based on the first superposition result, the second superposition result and the first intermediate quantity data;
calculating and obtaining the wall heat flow pulsation of the aircraft by using the wall heat flow pulsation prediction model of the aircraft based on the first superposition result and the second intermediate quantity data;
and evaluating the aerodynamic performance of the aircraft based on the aircraft wall friction resistance pulsation and the aircraft wall heat flow pulsation.
2. The high-speed aircraft aerodynamic performance evaluation method according to claim 1, wherein the aircraft wall friction pulsation prediction model comprises:
Figure DEST_PATH_IMAGE001
Figure 499107DEST_PATH_IMAGE002
wherein,
Figure DEST_PATH_IMAGE003
as a variable of the spatial coordinates,
Figure 524832DEST_PATH_IMAGE004
to predict the flow-to-wall shear stress ripple,
Figure DEST_PATH_IMAGE005
to predict the development of wall shear stress pulsations,
Figure 742930DEST_PATH_IMAGE006
for the generic signal of the de-superposition effect,
Figure DEST_PATH_IMAGE007
in order to de-modulate the pervasive signal of the effect,
Figure 145092DEST_PATH_IMAGE008
the modulation coefficients of the flow direction friction pulsation of the second preset-size structure on the wall surface of the aircraft are obtained for the flow direction speed signal and the spreading direction speed signal,
Figure DEST_PATH_IMAGE009
the modulation coefficients of the flow direction speed signal and the spanwise speed signal to the spanwise friction drag pulsation of a second preset size structure on the wall surface of the aircraft,
Figure 282813DEST_PATH_IMAGE010
in order to compensate the phase difference of the flow direction friction pulsation superposition effect to the modulation effect,
Figure DEST_PATH_IMAGE011
for the phase difference of the spanwise superposition effect to the modulation effect,
Figure 745018DEST_PATH_IMAGE012
for the superposition of the streaming velocity signal at the second region,
Figure DEST_PATH_IMAGE013
is a superposition of the spanwise velocity signal at a second region.
3. The high-speed aircraft aerodynamic performance evaluation method according to claim 1, wherein the aircraft wall heat flow pulsation prediction model is:
Figure 951877DEST_PATH_IMAGE014
wherein,
Figure DEST_PATH_IMAGE015
the prediction result of the heat flow pulsation of the wall surface of the aircraft,
Figure 157731DEST_PATH_IMAGE016
as a variable of the spatial coordinates,
Figure DEST_PATH_IMAGE017
is a universal signal of the pulsation of the heat flow,
Figure 884378DEST_PATH_IMAGE018
the modulation coefficients of the flow direction friction pulsation of the second preset-size structure on the wall surface of the aircraft are obtained for the flow direction speed signal and the spreading direction speed signal,
Figure DEST_PATH_IMAGE019
the modulation coefficients of the flow direction speed signal and the spread direction speed signal to the heat flow pulsation of the structure with the second preset size on the wall surface of the aircraft,
Figure 268217DEST_PATH_IMAGE020
for superposition at a second region of the streaming velocity signal,
Figure DEST_PATH_IMAGE021
in order to compensate the phase difference of the flow direction friction pulsation superposition effect to the modulation effect,
Figure 713105DEST_PATH_IMAGE022
the modulation phase difference is modulated for the heat flow superposition,
Figure DEST_PATH_IMAGE023
the heat flow for the first pre-sized structure is pulsed.
4. The high-speed aircraft aerodynamic performance evaluation method according to claim 2,
Figure 440759DEST_PATH_IMAGE024
and
Figure DEST_PATH_IMAGE025
the calculation method is as follows:
Figure 553071DEST_PATH_IMAGE026
Figure DEST_PATH_IMAGE027
wherein,
Figure 357079DEST_PATH_IMAGE028
in order to perform the inverse fourier transform,
Figure DEST_PATH_IMAGE029
in order to flow to the linear random pre-estimated kernel function,
Figure 289263DEST_PATH_IMAGE030
for the span-wise linear random prediction kernel function,
Figure DEST_PATH_IMAGE031
in order to flow to the wavelength(s),
Figure 319143DEST_PATH_IMAGE032
in order to be a fourier transform,
Figure DEST_PATH_IMAGE033
in order to flow to the speed signal,
Figure 20382DEST_PATH_IMAGE034
in order to develop the speed signal in the direction of the speed,
Figure DEST_PATH_IMAGE035
the center position of the first preset size structure of the first area is shown.
5. The method of claim 4, wherein the first region is centered on a first predetermined size structure
Figure 244559DEST_PATH_IMAGE035
The calculation method is as follows:
Figure 929618DEST_PATH_IMAGE036
Figure DEST_PATH_IMAGE037
Figure 15386DEST_PATH_IMAGE038
Figure DEST_PATH_IMAGE039
wherein,
Figure 571132DEST_PATH_IMAGE040
in order to obtain the friction reynolds number,
Figure DEST_PATH_IMAGE041
in order to obtain a kinematic viscosity of the composition,
Figure 467675DEST_PATH_IMAGE042
as a result of the total shear stress of the wall,
Figure DEST_PATH_IMAGE043
the density of the wall surface is shown as,
Figure 108872DEST_PATH_IMAGE044
in order to be the viscosity coefficient,
Figure DEST_PATH_IMAGE045
in order to determine the speed of the friction,
Figure 998331DEST_PATH_IMAGE046
in order to be a measure of the viscosity,
Figure DEST_PATH_IMAGE047
is the boundary layer thickness.
6. The high-speed aircraft aerodynamic performance evaluation method according to claim 3,
Figure 923430DEST_PATH_IMAGE048
the calculation method is as follows:
Figure DEST_PATH_IMAGE049
wherein,
Figure 505721DEST_PATH_IMAGE028
in order to perform the inverse fourier transform,
Figure 899794DEST_PATH_IMAGE050
for the linear random prediction kernel function associated with the heat flow,
Figure DEST_PATH_IMAGE051
in order to flow to the wavelength(s),
Figure 75167DEST_PATH_IMAGE032
in order to be a fourier transform,
Figure 871084DEST_PATH_IMAGE035
the center position of the first preset size structure of the first area,
Figure 889856DEST_PATH_IMAGE052
the temperature pulsation signal is a temperature pulsation signal of a first predetermined size structure at the center of the first area.
7. The high-speed aircraft aerodynamic performance evaluation method according to claim 1, wherein the first predetermined dimension is greater than 2 boundary layer thicknesses in size.
8. The high-speed aircraft aerodynamic performance evaluation method of claim 1, wherein the first region is a region having an outer dimension greater than 0.1 and the second region is a region having an inner dimension less than 50.
9. The high-speed aircraft aerodynamic performance evaluation method according to claim 2, characterized in that the second predetermined dimension is less than or equal to 2 boundary layer thicknesses in size.
CN202210224593.4A 2022-03-09 2022-03-09 High-speed aircraft aerodynamic performance evaluation method Active CN114330035B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202210224593.4A CN114330035B (en) 2022-03-09 2022-03-09 High-speed aircraft aerodynamic performance evaluation method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202210224593.4A CN114330035B (en) 2022-03-09 2022-03-09 High-speed aircraft aerodynamic performance evaluation method

Publications (2)

Publication Number Publication Date
CN114330035A true CN114330035A (en) 2022-04-12
CN114330035B CN114330035B (en) 2022-05-24

Family

ID=81033525

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202210224593.4A Active CN114330035B (en) 2022-03-09 2022-03-09 High-speed aircraft aerodynamic performance evaluation method

Country Status (1)

Country Link
CN (1) CN114330035B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115600440A (en) * 2022-12-14 2023-01-13 中国空气动力研究与发展中心计算空气动力研究所(Cn) Aircraft surface aerodynamic force and aerodynamic heat prediction method, device, equipment and medium

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006122307A2 (en) * 2005-05-10 2006-11-16 Newport Corporation Apparatus and methods for estimation of initial phase of a brushless motor
CN109871602A (en) * 2019-01-30 2019-06-11 西安工程大学 A kind of critical heat flux density prediction technique returned based on Gaussian process
CN111339701A (en) * 2020-02-26 2020-06-26 河海大学 Pipeline leakage characteristic Godunov simulation method based on Brunone dynamic friction resistance
CN113158338A (en) * 2021-04-13 2021-07-23 中国空气动力研究与发展中心计算空气动力研究所 Rapid turbulence wall function aerodynamic force prediction method based on coarse grid
CN113505543A (en) * 2021-06-18 2021-10-15 中国空气动力研究与发展中心计算空气动力研究所 Aircraft wall surface heat flow analysis method
CN113536461A (en) * 2021-07-15 2021-10-22 北京航空航天大学 Turbulence model correction method for aerodynamic heat prediction of hypersonic velocity intense shock wave flow field
CN113656986A (en) * 2021-09-16 2021-11-16 深能科技(山东)有限公司 Method for rapidly calculating long-term operation heat exchange performance of intermediate-deep geothermal buried pipe
CN114154441A (en) * 2022-02-10 2022-03-08 中国空气动力研究与发展中心计算空气动力研究所 Method for generating and simulating and calculating environmental turbulence field of aircraft

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006122307A2 (en) * 2005-05-10 2006-11-16 Newport Corporation Apparatus and methods for estimation of initial phase of a brushless motor
CN109871602A (en) * 2019-01-30 2019-06-11 西安工程大学 A kind of critical heat flux density prediction technique returned based on Gaussian process
CN111339701A (en) * 2020-02-26 2020-06-26 河海大学 Pipeline leakage characteristic Godunov simulation method based on Brunone dynamic friction resistance
CN113158338A (en) * 2021-04-13 2021-07-23 中国空气动力研究与发展中心计算空气动力研究所 Rapid turbulence wall function aerodynamic force prediction method based on coarse grid
CN113505543A (en) * 2021-06-18 2021-10-15 中国空气动力研究与发展中心计算空气动力研究所 Aircraft wall surface heat flow analysis method
CN113536461A (en) * 2021-07-15 2021-10-22 北京航空航天大学 Turbulence model correction method for aerodynamic heat prediction of hypersonic velocity intense shock wave flow field
CN113656986A (en) * 2021-09-16 2021-11-16 深能科技(山东)有限公司 Method for rapidly calculating long-term operation heat exchange performance of intermediate-deep geothermal buried pipe
CN114154441A (en) * 2022-02-10 2022-03-08 中国空气动力研究与发展中心计算空气动力研究所 Method for generating and simulating and calculating environmental turbulence field of aircraft

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
张伟伟: ""基于CFD技术的高效气动弹性分析方法研究"", 《中国优秀博硕士学位论文全文数据库(博士) 工程科技Ⅱ辑》 *
沈鹏飞 等: ""马赫6柱-裙构型激波/湍流边界层干扰摩阻统计特性"", 《航空学报》 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115600440A (en) * 2022-12-14 2023-01-13 中国空气动力研究与发展中心计算空气动力研究所(Cn) Aircraft surface aerodynamic force and aerodynamic heat prediction method, device, equipment and medium

Also Published As

Publication number Publication date
CN114330035B (en) 2022-05-24

Similar Documents

Publication Publication Date Title
Law et al. Time-varying wind load identification from structural responses
Sun Simulation of pavement roughness and IRI based on power spectral density
CN107256204B (en) Experimental device and method for multipoint vibration response frequency domain prediction based on transfer function
US6704664B2 (en) Fatigue sensitivity determination procedure
Li et al. A novel long short-term memory neural-network-based self-excited force model of limit cycle oscillations of nonlinear flutter for various aerodynamic configurations
Errico et al. The modelling of the flow-induced vibrations of periodic flat and axial-symmetric structures with a wave-based method
Raveh CFD-based models of aerodynamic gust response
Van Binh et al. A peak factor for non-Gaussian response analysis of wind turbine tower
CN114330035B (en) High-speed aircraft aerodynamic performance evaluation method
CN114595647B (en) Magnetic levitation flight wind tunnel pneumatic structure coupling simulation evaluation method
CN105260568A (en) Super high-rise building wind load inverse analysis method based on discrete Kalman filtering
CN102521482B (en) Space-earth conversion method of aerodynamic force in viscid interference effect
Lo et al. Predictability of turbulent flow in street canyons
CN116663448A (en) SST turbulence model correction method for Mars atmosphere under high enthalpy flow condition
Xiaojian et al. A scaling procedure for panel vibro-acoustic response induced by turbulent boundary layer
CN113408218B (en) Flow noise simulation method based on disturbance equation
CN113051846B (en) Wall surface first layer grid thickness estimation method considering compressible and heat conduction effects
Sparrow et al. Heat transfer and skin friction for turbulent boundary-layer flow longitudinal to a circular cylinder
Zheng et al. Identify the spatially-correlated random fluctuating pressure on structure from strain data
CN103617338A (en) Method and device for rapidly calculating hypersonic viscosity force of aircraft
He et al. A multi-scale wavelet finite element model for damage detection of beams under a moving load
Jansen Large-eddy simulation using unstructured grids
Tamaki et al. Wall-Modeled Large-Eddy Simulation of Transonic Buffet over NASA-CRM Using FFVHC-ACE
Chen Determination of flutter derivatives via a neural network approach
da Silva Reis et al. Chaos analysis of a single-bay flutter panel

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