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Mathematical Problems in Engineering
Volume 2010 (2010), Article ID 924275, 17 pages
http://dx.doi.org/10.1155/2010/924275
Research Article

Nonlinear and Dynamic Aerodynamic Models for Commercial Transport Aircraft with Adverse Weather Effects

1Department of Aviation Mechanical Engineering, China University of Science and Technology, Hen-Shan (312), Taiwan
2Department of Aeronautics and Astronautics, National Cheng Kung University, Taiwan
3Accident Investigation Division, Aviation Safety Council, Taiwan

Received 27 August 2009; Accepted 25 November 2009

Academic Editor: José Balthazar

Copyright © 2010 Ray C. Chang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

The flight dynamic equations in mathematics for aircraft response to the adverse weathers, such as wind shear, atmospheric turbulence, and in-flight icing, are nonlinear and unsteady. To effectively analyze the performance degradation and variations in stability of commercial aircraft that encountered these weather hazards, the nonlinear and dynamic (i.e., time dependent) aerodynamic models based on flight data would be needed. In the present paper, a numerical modeling method based on a fuzzy-logic algorithm will be presented to estimate the aerodynamic models for a twin-jet transport by using the flight data from the flight data recorder (FDR). The aerodynamic models having the capability to generate continuous stability derivatives, especially for sensitivity study of unknown factors in adverse weather conditions, will be demonstrated in this paper.

1. Introduction

Aircrafts in flight are frequently subject to atmospheric disturbances. The hazards due to these disturbances may be in the form of wind shear, turbulence (both clear-air and convective), thunderstorms, in-flight icing, and so forth. The severity of aircraft response to the disturbance is related to the dynamic aerodynamics that results from the instantaneous changes of aircraft flight attitudes. To provide the mitigation concepts and promote the understanding of aerodynamic responses of the commercial transport aircraft in adverse weather conditions, the nonlinear and dynamic (i.e., time-dependent) aerodynamic models based on flight data would be needed.

Regarding the flight data of commercial transport aircraft, the flight data recorder (FDR) is ICAO-regulated devices. The FDR, popularly referred to as a “black box”, is a mandatory device used to record specific aircraft parameters for event investigations. Although the data resolution and accuracy in the FDR are not as well defined as those in flight test, the predicted aerodynamic derivatives correlated well with the nominal values of transport aircraft in normal flight [1]. Therefore, the FDR data will be used in the present analysis.

In setting up the aerodynamic models to predict the required derivatives in aerodynamics, the traditional method of using the tabulated data derived from such methods as the maximum likelihood method (MMLE) [2], the least-square or the stepwise regression method [3], is very difficult to correlate complex functional relations among numerous parameters. In earlier development of the fuzzy-logic algorithm, Zadeh [4] used the fuzzy sets to simulate physical parameters with membership functions. The disadvantage in this approach is that the predicted curves in the functional approximation tend to be piecewise continuous. Therefore, it is not suitable when derivatives of the function are needed. In 1985, Takagi and Sugeno [5] used the internal functions, instead of the fuzzy sets, in developing the fuzzy-logic algorithm. In this approach, the main features are the internal functions, membership functions, and the output cells. The output curves in the prediction are smooth. The present development will be based on this second approach. This second approach, to be called the Fuzzy-Logic Modeling (FLM) technique [6, 7], is capable of correlating multiple parameters without assuming explicit functional relations.

Among the different adverse weathers, clear-air turbulence is all the more important in flight safety since it is hard to detect and predict. Clear-air turbulence is the leading cause of serious personal injuries in nonfatal accidents of commercial aircraft. One main type of motion that causes flight injuries in clear-air turbulence is the sudden plunging motion with the abrupt change in altitude. This paper presents FLM technique to establish unsteady aerodynamic models with six aerodynamic coefficients based on the datasets from the flight data recorder (FDR) of a twin-jet transport. The aerodynamic derivatives extracted from these aerodynamic models are then used to evaluate the variations in stability. The sensitivity study of unknown factors during the sudden plunging motion in severe clear-air turbulence will be demonstrated in this paper.

2. Theoretical Development

The general idea of the FLM technique is to set up the relations between its input and output variables of the whole system. The internal functions, membership functions, and outputs are three basic elements for the FLM approach. Two main tasks are involved in the FLM process. One is the identification of the coefficients of the internal functions, which is called parameter identification. The other one is structure identification to identify the optimal structure of fuzzy cells of the model. Details of the FLM technique are described in the followings [68].

2.1. Internal Functions

The fuzzy-logic model uses many internal functions to cover the defined ranges of the influencing parameters. Although the form of internal functions is very simple, it can represent a highly nonlinear relationship between the input and output for the whole system. These internal functions are assumed to be linear functions of input variables [8] as follows: 𝑃𝑖=𝑦𝑖𝑥1,𝑥2,,𝑥𝑟,,𝑥𝑘=𝑝𝑖0+𝑝𝑖1𝑥1++𝑝𝑖𝑟𝑥𝑟+𝑝𝑖𝑘𝑥𝑘,(2.1) where 𝑝𝑖𝑟, 𝑟=0,1,2,,𝑘, are the coefficients of internal functions 𝑦𝑖, and k is number of input variables; 𝑖=1,2,,𝑛, and n is the total number of fuzzy cells.

The recorded data in FDR, such as flight altitude (), calibrated airspeed (CAS), angle of attack (𝛼), accelerometer readings (𝑎𝑥, 𝑎𝑦, and 𝑎𝑧), Euler angles (𝜃, 𝜙, and 𝜓), and so forth, is chosen as the input variables for a specific fuzzy model. In the present paper, 𝑦𝑖 is denoted as an estimated aerodynamic coefficient of force or moment, and 𝑥𝑟 are the variables of the input data. The numbers of the internal functions (i.e., cell’s numbers) are quantified by the membership functions.

2.2. Membership Functions

The values of each fuzzy variable, such as the angle of attack, are divided into several ranges; each of which represents a membership function with 𝐴(𝑥𝑟) as its membership grade. One membership function from each variable constitutes a fuzzy cell. For the 𝑖th cell, the corresponding membership grades are represented by 𝐴𝑖𝑟(𝑥𝑟), 𝑟=1,2,,𝑘. In other words, the membership functions allow the membership grades of the internal functions for a given set of input variables to be calculated. For a given system with input variables 𝑥1,𝑥2,,𝑥𝑟,𝑥𝑘, the recorded values of each input variables are normalized by using (𝑥𝑟𝑥𝑟,min)/(𝑥𝑟,max𝑥𝑟,min) to transform them into the ranges of [0,1]. The membership grading also ranges from 0 to 1, with “0” meaning no effect from the corresponding internal function and “1” meaning a full effect. Generally, overlapped straight lines, triangles, or trapezoids are frequently the shapes used to represent the grades. In this paper, the overlapped triangular membership function is used to represent the grades of internal functions.

The membership functions partition the input space into many fuzzy subspaces, which are called the fuzzy cells. The total number of fuzzy cells is𝑛=𝑁1×𝑁2××𝑁𝑟××𝑁𝑘. For a variable 𝑥𝑟, the number of membership function is 𝑁𝑟. Each fuzzy cell is in a different combination from others formed by taking one membership function from each input variable.

In the present application, triangular membership functions are used throughout. Let 𝑁 be the number of membership functions and let 𝑗 be the index for the 𝑗th membership functions. Then the membership grades can be described as follows [9]:

(1)𝑁=2, 𝐴(𝑥𝑟)=𝑥𝑟, 𝑗=1, 𝐴𝑥𝑟=1𝑥𝑟,𝑗=2,(2.2)(2)𝑗=3 to 𝑚, where 𝑚=max(0,(𝑁2)/2): 𝐴𝑥𝑟=𝑥𝑟𝑑𝑢,0𝑥𝑟𝑑𝑢,𝐴𝑥𝑟=1𝑥𝑟1𝑑𝑢,𝑑𝑢𝑥𝑟1,(2.3) where 𝑑𝑢=Δ𝑥1(𝑗2), and Δ𝑥1=1.0/(𝑁𝑚1),(3)𝑗𝑁𝑚,𝐴𝑥𝑟=𝑑𝑑𝑥𝑟𝑑𝑑,0𝑥𝑟𝑑𝑑,𝐴𝑥𝑟=𝑑𝑑𝑥𝑟𝑑𝑑1,𝑑𝑑𝑥𝑟1,(2.4) where 𝑑𝑑 = Δ𝑥2(𝑗𝑁+𝑚), and Δ𝑥2=1.0/(𝑚+1).
2.3. Fuzzy Rule and Output

A fuzzy cell is formed by taking one membership function from each variable. The total number of cells is the number of possible combinations by taking one membership function from each input variable. For every cell, it has a fuzzy rule to guide the input and output relations. The rule of the 𝑖th cell is stated [8] as follows: if 𝑥1 is 𝐴𝑖1(𝑥1), if  𝑥2  is 𝐴𝑖2(𝑥2), , and if 𝑥𝑘  is 𝐴𝑖𝑘(𝑥𝑘), then the cell output is

𝑃𝑖𝑥1,𝑥2,,𝑥𝑟,𝑥𝑘=𝑝𝑖0+𝑝𝑖1𝑥1++𝑝𝑖𝑟𝑥𝑟+𝑝𝑖𝑘𝑥𝑘,(2.5) where 𝑖=1,2,,𝑛 is the index of the cells, n is the total number of cells of the model; 𝑃𝑖(𝑥1,𝑥2,,𝑥𝑟,𝑥𝑘) is the internal function with parameters 𝑝𝑖0,𝑝𝑖1,,𝑝𝑖𝑟,𝑝𝑖𝑘 to be determined, and 𝐴𝑖𝑘(𝑥𝑘) denotes the membership grade for 𝑥𝑘. Each function covers a certain range of input variables.

In each fuzzy cell, the contribution to the outcome (i.e., the cell output) is based on the internal function (2.5). The final prediction of the outcome is the weighted average of all cell outputs after the process of reasoning algorithm. Because of this weighting among many factors over large ranges of possibilities, the word “fuzzy” is derived to describe the method. However, its prediction is never “fuzzy”. The output estimated by the fuzzy-logic algorithm corresponding to the jth input (𝑥1,𝑗,𝑥2,𝑗,,𝑥𝑟,𝑗,,𝑥𝑘,𝑗) is as follows:

̂𝑦𝑗=𝑛𝑖=1𝐴product𝑖𝑥1,𝑗,,𝐴𝑖𝑥𝑟,𝑗,,𝐴𝑖𝑥𝑘,𝑗𝑝𝑖𝑛𝑖=1𝐴product𝑖𝑥1,𝑗,,𝐴𝑖𝑥𝑟,𝑗,,𝐴𝑖𝑥𝑘,𝑗.(2.6) In (2.6) product[𝐴𝑖(𝑥1,𝑗),,𝐴𝑖(𝑥𝑟,𝑗),,𝐴𝑖(𝑥𝑘,𝑗)] is the weighted value of the 𝑖th cell, and the index j of the data set, where 𝑗=1,2,,𝑚, 𝑚 is the total number of the data record, and the “product” stands for product operator of its elements in this paper.

2.4. Parameter Identification

Given a set of membership functions for each input variable, the unknown coefficients of the internal functions are adjusted by using the Newton gradient-descent method. The accuracy of the established aerodynamic model through the fuzzy-logic algorithm is estimated by the sum of squared errors (SSEs) and the multiple correlation coefficients (𝑅2):

SSE=𝑚𝑗=1̂𝑦𝑗𝑦𝑗2𝑅,(2.7)2=1𝑚𝑗=1̂𝑦𝑗𝑦𝑗2𝑚𝑗=1𝑦𝑦𝑗2.(2.8)

In (2.7) and (2.8), where ̂𝑦𝑗, the output of the fuzzy-logic model at point 𝑗, is estimated by (2.6), 𝑦𝑗 is the data point used for the model training at point 𝑗, 𝑦 is the mean of the sample data, and 𝑚 is the total number of data points. The model training is to determine the unknown coefficients of the internal functions, 𝑝𝑖𝑟, by maximizing the value of 𝑅2. These coefficients are determined by the following iterative formula to minimize the sum of squared error (2.7): 𝑝𝑖𝑟,𝑡+1=𝑝𝑖𝑟,𝑡𝛼𝑟𝜕(SSE)𝜕𝑝𝑖𝑟,(2.9) where 𝛼𝑟 is the convergence factor or the step size in the gradient method; subscript index 𝑡 denotes the iteration sequence.

In usual, a large value of 𝛼𝑟 is chosen, such as 10, at the beginning to accelerate the process of convergence; the small value of less then 1 is taken to obtain more precise unknown coefficients of the internal functions, 𝑝𝑖𝑟, in model training process. After simplification, (2.9) becomes as follows.

For 𝑟=0,

𝑝𝑖0,𝑡+1=𝑝𝑖0,𝑡2𝛼0̂𝑦𝑗𝑦𝑗×𝐴product𝑖1𝑥1,,𝐴𝑖𝑟𝑥𝑟,𝑗,,𝐴𝑖𝑘𝑥𝑘,𝑗𝑛𝑠=1𝐴product𝑠1𝑥1,𝑗,,𝐴𝑠𝑟𝑥𝑟,𝑗,,𝐴𝑠𝑘𝑥𝑘,𝑗,(2.10a) and for 𝑟=1,2,,𝑘,

𝑝𝑖𝑟,𝑡+1=𝑝𝑖𝑟,𝑡2𝛼𝑟̂𝑦𝑗𝑦𝑗×𝐴product𝑖1𝑥1,,𝐴𝑖𝑟𝑥𝑟,𝑗,,𝐴𝑖𝑘𝑥𝑘,𝑗𝑥𝑟,𝑗𝑛𝑠=1𝐴product𝑠1𝑥1,𝑗,,𝐴𝑠𝑟𝑥𝑟,𝑗,,𝐴𝑠𝑘𝑥𝑘,𝑗.(2.10b)

The iteration during the search sequence stops when one of the following three criteria [6, 9] is satisfied:

(1)Cost=SSE𝑡<𝜀1,(2)RER=(SSE𝑡SSE𝑡1)/SSE𝑡<𝜀2,(3)𝑡=𝑡max.

In the above criteria, Cost=SSE𝑡 is the sum of squared errors (SSEs) in current iteration to be denoted by “Cost” and RER = (cost_current cost_previous)/cost_current to be denoted by “RER” (i.e., the relative error) for simplicity in descriptions; 𝜀1 and 𝜀2 are the required precision criteria, and 𝑡max is a specified maximum iteration number.

Given membership functions and the training data, this parameter identification procedure can be applied to establish a fuzzy-logic model. Although the procedure is well understood, to obtain a good model with the appropriate membership functions that are quite challenging, it requires numerical experimentation.

2.5. Model Structure Identification

In the fuzzy-logic model, the model structure is indicated by the number of membership functions. For a fuzzy-logic model with multiple variables, the structure is the combination of the numbers and forms of the membership functions assigned to all input variables. Since the sequence defines the one-to-one relationship between the numbers and the forms for each variable, the structure can be uniquely described by the numbers.

The model structure is optimized by maximizing (2.8). A search forward algorithm has been employed for the identification. At each search stage, there may be many fuzzy-logic models with different structure combinations. The search stage numbers are denoted by 𝑁𝑠. Out of all the possible intermediate fuzzy-logic models at each search stage, for an efficient search, only some structures are developed and evaluated. Two selection criteria, to be given below, are used to choose these structures. With the incremental sequence and the selection criteria, the search forward algorithm can be shown graphically in Figure 1.

924275.fig.001
Figure 1: Best model structure searching flow.

The step-by-step searching flow is summarized as follows [6].

(1) Specify the input variables 𝑥𝑟, 𝑟=1,2,,𝑘 and the output variable 𝑦.(2) Assume an initial structure, also called parent structure, as (𝑁10,𝑁20,,𝑁𝑟0,,𝑁𝑘0).(3) Begin at the search stage number 𝑁𝑠=𝑙 form all possible structures starting from the parent structure by adding one more membership function a time only to one input variable. Those all possible structures are called child structures as (𝑁10+1,𝑁20,,𝑁𝑟0,,𝑁𝑘0), (𝑁10,𝑁20+1,,𝑁𝑟0,,𝑁𝑘0),, and (𝑁10,𝑁20,,𝑁𝑟0,,𝑁𝑘0+1). Do the identification of internal coefficients in (2.1) for each child structure and then calculate its 𝑅2 by using (2.8).(4) Select the top 5 child structures among all calculated values of 𝑅2 as new parent structures for next search step 𝑁𝑠=𝑁𝑠+𝑙.(5) Go back to step (2) starting from the new parent structures and repeat the same procedures in steps (2) and (3) until the best structure is identified;(6) Pick out the maximum value of 𝑅2 among the child structures in each searching stage as 𝑅2max. The structure of the largest 𝑅2max corresponding to the all picking values is the optimal structure within a sensible 𝑁𝑠.

In the structure identification, parameter identification to determine the p-parameters according to (2.9) is also needed. But the number of iteration to determine the p-parameters is limited to 2000, so that the best structure is decided on a relative basis. After this last step, (2.9) is applied iteratively until both values of 𝑅2 and RER reach the requirements in the final parameter identification

3. Application to Aerodynamic Modeling

3.1. Flight Data

The twin-jet transport of the present study encountered clear-air turbulence in cruise flight at the altitude around 10,050 m. As a result, several passengers and cabin crews sustained injuries, because of which this event was classified as an accident. The present study was initiated to examine possible concepts of accident prevention in the future. The datasets used for the modeling are extracted from the FDR during turbulence encounter lasting for 92 seconds.

The main aircraft geometric and inertial characteristics are taken to be

𝑊 (take-off) = 1,431,800 N (321900 lb),𝑆= 260 m2  (2798.7 ft2), 𝑐= 6.608 m (21.68 ft), and 𝑏= 44.827 m (147.08 ft),𝐼𝑥𝑥= 10,710,000 kg-m2 (7,899,900 slugs-ft2), and 𝐼𝑦𝑦= 14,883,800 kg-m2 (10,978,000 slugs-ft2),𝐼𝑧𝑧= 25,283,271 kg-m2 (18,648,470 slugs-ft2) and 𝐼𝑥𝑧= 0.0 kg-m2.

The required operational parameters in FDR dataset for generating aerodynamic data files are time (𝑡), CAS, pressure altitude (), roll attitude (𝜙), pitch attitude (𝜃), magnetic heading (𝜓), longitudinal acceleration (𝑎𝑥), lateral acceleration (𝑎𝑦), vertical acceleration (𝑎𝑧), angle of attack (𝛼), aileron deflection (𝛿𝑎), elevator (𝛿𝑒), rudder (𝛿𝑟), stabilizer (𝛿𝑠), engine EPR, outside air temperature, wind speed, wind direction, and fuel flow rate. Since only the normal acceleration is recorded in 8 Hz resolution (i.e., 8 points per second), all other parameters are interpolated with a monotone cubic spline to the same sampling rate.

3.2. Compatibility Analysis

Typically, the longitudinal, lateral, and vertical accelerations (𝑎𝑥, 𝑎𝑦, 𝑎𝑧) along the (𝑥, 𝑦, 𝑧)-body axes of aircraft, angle of attack 𝛼, and the Euler angles (𝜙, 𝜃, and 𝜓) as well as all control deflections are available and recorded in the FDR of all transport aircraft. Since the recorded flight data may contain errors (or called biases), compatibility analysis is performed to remove them by satisfying the following kinematic equations:

̇̇̇𝑎𝜙=𝑝+𝑞sin𝜙tan𝜃+𝑟cos𝜙tan𝜃,(3.1)𝜃=𝑞cos𝜙𝑟sin𝜙,(3.2)̇𝜓=(𝑞sin𝜙+𝑟cos𝜙)sec𝜃,(3.3)𝑉=𝑥𝑎𝑔sin𝜃cos𝛼cos𝛽+𝑦+𝑎+𝑔sin𝜙cos𝜃sin𝛽𝑧𝑎+𝑔cos𝜙cos𝜃sin𝛼cos𝛽,(3.4)̇𝛼=𝑧𝑎+𝑔cos𝜃cos𝜙cos𝛼𝑥𝑔sin𝜃sin𝛼̇𝑎(𝑉cos𝛽)+𝑞tan𝛽(𝑝cos𝛼+𝑟sin𝛼),(3.5)𝛽=cos𝛽𝑦+𝑔cos𝜃sin𝜙𝑉𝑎+𝑝sin𝛼𝑟cos𝛼sin𝛽𝑧𝑎+𝑔cos𝜃cos𝜙sin𝛼𝑥𝑔sin𝜃cos𝛼𝑉,(3.6) where 𝑔 is acceleration due to gravity, 𝑉 is flight speed, 𝛽 is sideslip angle, 𝑝 is roll rate, 𝑞 is pitch rate, and 𝑟 is yaw rate in (3.1)–(3.6). Let the biases be denoted by 𝑏𝑎𝑥,𝑏𝑎𝑦,𝑏𝑎𝑧,𝑏𝑝,𝑏𝑞,𝑏𝑟,𝑏𝑉,𝑏𝛼,𝑏𝛽,𝑏𝜃,𝑏𝜙,and𝑏𝜓, respectively, for 𝑎𝑥, 𝑎𝑦, 𝑎𝑧, and so forth. These biases are estimated by minimizing the squared sum of the differences between the two sides of the above equations. These equations in vector form can be written as

̇𝑧=𝑓(𝑥)=𝑓𝑥𝑚Δ𝑥,(3.7) where

𝑧=(𝑉,𝛼,𝛽,𝜃,𝜙,𝜓)𝑇,(3.8)𝑥𝑚=𝑎𝑥,𝑎𝑦,𝑎𝑧,𝑝,𝑞,𝑟,𝑉,𝛼,𝛽,𝜃,𝜙,𝜓𝑇Δ,(3.9)𝑥=𝑏𝑎𝑥,𝑏𝑎𝑦,𝑏𝑎𝑧,𝑏𝑝,𝑏𝑞,𝑏𝑟,𝑏𝑉,𝑏𝛼,𝑏𝛽,𝑏𝜃,𝑏𝜙,𝑏𝜑𝑇,(3.10) where the subscript “𝑚” indicates the measured or recorded values. The cost function is defined as

1𝐽=2̇𝑧𝑓𝑇𝑄̇z𝑓,(3.11) where 𝑄 is a weighting diagonal matrix with elements being 1.0 except the one for the slowly varying flight speed being 10.0 and ̇𝑧 is calculated with a central difference scheme with 𝑧𝑚, which is the measured value of 𝑧. The steepest descent optimization method is adopted to minimize the cost function. As a result of the analysis, variables not present in the FDR, such as 𝛽, 𝑝, 𝑞, and 𝑟, are also estimated.

The force and moment coefficients are obtained from the following flight dynamic equations [7, 10] about the airplane body axes:

𝑚𝑎𝑥=𝐶𝑥𝑞𝑆+𝑇𝑥,(3.12)𝑚𝑎𝑦=𝐶𝑦𝑞𝑆+𝑇𝑦,(3.13)𝑚𝑎𝑧=𝐶𝑧𝑞𝑆+𝑇𝑧𝐶,(3.14)𝑙𝑞𝑆𝑏=𝐼𝑥𝑥̇𝑝𝐼𝑥𝑧𝐼(̇𝑟+𝑝𝑞)𝑦𝑦𝐼𝑧𝑧𝐶𝑞𝑟,(3.15)𝑚𝑞𝑆𝑐=𝐼𝑦𝑦̇𝑞𝐼𝑥𝑧𝑟2𝑝2𝐼𝑧𝑧𝐼𝑥𝑥𝑟𝑝𝑇𝑚𝐶,(3.16)𝑛𝑞𝑆𝑏=𝐼𝑧𝑧̇𝑟𝐼𝑥𝑧𝐼(̇𝑝𝑞𝑟)𝑥𝑥𝐼𝑦𝑦𝑝𝑞,(3.17) where m is denoted as aircraft mass; 𝑞 is denoted as dynamic pressure; 𝑆 is denoted as wing reference area; 𝐶𝑥, 𝐶𝑧, and 𝐶𝑚 are denoted as longitudinal aerodynamic force and moment coefficients; 𝐶𝑦, 𝐶𝑙, and 𝐶𝑛 are denoted as lateral-directional aerodynamic force and moment coefficients; 𝐼𝑥𝑥, 𝐼𝑦𝑦, and 𝐼𝑧𝑧 are denoted as moments of inertia about 𝑥-, 𝑦-, and 𝑧-axes, respectively; 𝐼𝑥𝑦, 𝐼𝑥𝑧, and 𝐼𝑦𝑧 are denoted as products of inertia; 𝑇𝑥, 𝑇𝑦, 𝑇𝑧, and 𝑇𝑚 are denoted as thrust terms about 𝑥-, 𝑦-, 𝑧-axes, and in equation of pitching moment, respectively, in (3.7)–(3.12).

The above equations are used to determine all aerodynamic coefficients based on accelerometer readings (𝑎𝑥, 𝑎𝑦, and 𝑎𝑧), Euler angles (𝜙, 𝜃, and 𝜓), angular rates (𝑝, 𝑞, and 𝑟), and thrusts (𝑇𝑥, 𝑇𝑦, 𝑇𝑧, and 𝑇𝑚). The angular rates are estimated through compatibility analysis. Since thrusts were not measured during flight for most flight vehicles, those values and the effects on the forces and pitching moments in equations of (3.7), (3.8), (3.9), and (3.11) should be predicted by a thrust model.

3.3. Equivalent Harmonic Motion

The reduced frequency is a parameter to indicate the degree of unsteadiness in unsteady aerodynamics and is estimated in this paper by fitting the local trajectory with a harmonic motion. In the static case, the reduced frequency is 0. Large values of the reduced frequency imply the importance of unsteady aerodynamic effect. For longitudinal aerodynamics, the equivalent harmonic motion is the one based on the angle-of-attack variation following the classical unsteady aerodynamic theory of Theodorsen [11]. For lateral-directional aerodynamics, it is based on the time variation of roll angle [8].

For the longitudinal motion, the time history of the angle of attack (𝛼) and time rate of angle of attack (𝑑𝛼/𝑑𝑡, or ̇𝛼) are fitted with one of a harmonic motion at any instant [7, 12] as follows:

𝛼(𝑡)=𝛼+𝛼cos𝜔𝑡+𝜙,(3.18)̇𝛼(𝑡)=𝑎𝜔sin𝜔𝑡+𝜙,(3.19) where those terms on the left hand side of (3.13) and (3.14) are given and the unknowns are the local mean angle of attack (𝛼), the local amplitude of the harmonic motion (𝑎), the phase lag (𝜙), and the angular frequency (𝜔). These unknowns are calculated through an optimization method by minimizing the following cost function (least squares):

𝐽=𝑛𝑖=1𝛼𝑖𝛼+𝑎cos𝜔𝑡𝑖+𝜙2+̇𝛼𝑖𝛼+𝑎𝜔sin𝜔𝑡𝑖+𝜙2.(3.20)

In (3.15), 𝛼𝑖 is the measured value at point 𝑖 and 𝑛 is the number of the data points used in the optimization. For the case in the present study, 𝑛=20 is found to be the best value. The 20 points preceding and including the current time are employed in (3.15). The least-square method is found to converge well and gives reasonably accurate results. The lateral-directional equivalent reduced frequency is computed in the same manner.

The local equivalent reduced frequency in the longitudinal motion is defined as

𝑘1=𝜔𝑐𝑉,(3.21) where 𝑐 is the mean chord length of wing airfoil section.

The lateral-directional equivalent reduced frequency is defined as

𝑘2=𝜔𝑏𝑉,(3.22) where 𝑏 is the wing span.

3.4. Fuzzy-Logic Thrust Model

As shown before, the thrust terms appear in the force equations and the pitching moment equations (3.7)–(3.9) and (3.11). Since the values of thrust for aircraft in flight cannot be directly measured in the current state of the art, they are not recorded in the FDR. The manufacturers of airplanes and engines and safety agencies agreed that using such parameters as the Mach number, airspeed, flight altitude, temperature, the rpm of the pressure compressors, and engine pressure ratios is adequate to estimate the engine thrust. A realistic thrust model is quite complex and cannot be represented by any simple equation. Since such thrust model is not available for the present study, a realistic one tied to the recorded engine performance parameters will be developed with the fuzzy-logic algorithm.

For a commercial aircraft, most likely only the axial force and the pitching moment are affected by thrust. This assumption will be made in this paper. Theoretically, clear-air turbulence (i.e., random change in 𝑢, 𝑤 (or 𝛼), and 𝑣 (or 𝛽) affects the engine performance through its effects on static and dynamic distortions at the engine face. However, the effects of clear-air turbulence on the engine parameters and the thrust magnitude are not known and, therefore, are ignored.

For this purpose, data from the flight manual for the fuel flow rates (̇𝑚𝑓) at various altitudes (), weights (𝑊), Mach numbers (𝑀), calibrated airspeed (CAS), engine pressure ratios (EPRs) in cruise flight are utilized. Note that the drag polar for a given aircraft is generally not known to most researchers. To estimate it and, hence, the thrust magnitude in cruise, the assumption of a design lift-to-drag ratio (𝐿/𝐷) of 17.5 is made. This value of lift-to-drag in cruise is assumed based on the past design experience for twin-jet transports. In the flight manual, various weights, altitudes, Mach numbers, CAS, EPR, and fuel flow rates in cruise are tabulated. The lift coefficient can be calculated at each flight condition immediately. As a result, the drag coefficient can be estimated from the assumption of lift-to-drag ratio. Therefore, the design thrust in cruise at various Mach numbers can be estimated. For the Pratt & Whitney turbofan engines, thrust (𝑇) is defined by EPR, so that the thrust model is set up as

𝑇=𝑓,𝑊,𝑀,CAS,EPR,̇𝑚𝑓.(3.23)

For GE turbofan engines, the rpm of the low-pressure compressor (𝑁1) is used to set the level of thrust, so that the thrust model is set up as

𝑇=𝑓,𝑊,𝑀,CAS,𝑁1,̇𝑚𝑓.(3.24)

In the present study, the P & W turbofan engines powering one twin-jet transport will be illustrated. The actual thrust in operation is obtained by using the recorded variables in the FDR, in particular the fuel flow rates.

In the present study, the P & W engines powering the twin-jet commercial aircraft will be illustrated.

The following climb equation [13] is to be satisfied in the least-square sense over a 5-second internal:

𝑊𝑔𝑑𝑉𝐷𝑑𝑡=𝑇𝐷𝑊sin𝛾,(3.25)𝑊=𝐷𝐿cos𝛾.(3.26)

All these equations are still valid in descent with negative climb angles (𝛾). The above equations are further employed for parameter identification in the process of modeling.

Once the thrust model is generated as a function of h, W, M, CAS, EPR, and ̇𝑚𝑓 with the flight conditions of climbing, cruise, and descent, one can estimate the thrust magnitude by inserting these flight variables from the FDR into the model.

3.5. Fuzzy-Logic Unsteady Aerodynamic Models

Modeling means to establish the numerical relationship among certain variables of interest. In the fuzzy-logic model, more complete necessary influencing flight variables can be included to capture all possible effects on aircraft response to atmospheric disturbances. For longitudinal aerodynamics, the models are assumed to be of the form [6]

𝐶𝑥,𝐶𝑧,𝐶𝑚=𝑓𝛼,̇𝛼,𝑞,𝑘1,𝛽,𝛿𝑒,𝑀,𝑝,𝛿𝑠,𝑞,(3.27) where the left-hand side represents the coefficients of axial force (𝐶𝑥), normal force (𝐶𝑧), and pitching moment (𝐶𝑚), respectively. All variables on the right-hand side of (3.22) have been defined in the previous section. It should be noted that the stabilizer angle (𝛿𝑠) is included here, because it varies, though slowly, in flight to provide pitch trim (i.e., reducing the total static pitching moment to 0.0). The roll rate is included here because it is known that an aircraft under high aerodynamic loads at transonic speeds may have its longitudinal stability derivatives affected when additional disturbance due to roll rate is imposed.

For the lateral-directional aerodynamics [8],

𝐶𝑦,𝐶𝑙,𝐶𝑛=𝑓𝛼,𝛽,𝜙,𝑝,𝑟,𝑘2,𝛿𝑎,𝛿𝑟̇𝛽,𝑀,̇𝛼,,(3.28) where the left-hand side represents the coefficients of side force (𝐶𝑦), rolling moment (𝐶𝑙), and yawing moment (𝐶𝑛), respectively.

4. Numerical Results and Discussions

In the present study, the accuracy of the established unsteady aerodynamic models with six aerodynamic coefficients by using FLM technique is estimated by the sum of squared errors (SSEs) and the square of multiple correlation coefficients (𝑅2). Figure 2 presents the aerodynamic coefficients of normal force 𝐶𝑧, pitching moment 𝐶𝑚, rolling moment 𝐶𝑙, and yawing moment 𝐶𝑛 predicted by the unsteady aerodynamic models. The predicted data by the final models have good agreement with the flight data. The Cm-data scattering is most likely caused by turbulence-induced buffeting on the structure, in particular on the horizontal tail. Once the aerodynamic models are set up, one can calculate all necessary derivatives to analyze the stability.

fig2
Figure 2: Predicted aerodynamic coefficients in normal force and moments for a twin-jet transport encountering severe clear-air turbulence at cruise altitudes around 10,050 m.

The fuzzy-logic aerodynamic models are capable of generating the continuous derivatives for the static and dynamic stability study of a twin-jet transport in turbulence response. Firstly, how the fuzzy-logic prediction is achieved will be illustrated with one numerical example in the 𝐶𝑧 calculation. At first, the range for each variable is defined to be larger than what actually occurred in the present set of 𝐶𝑧  data as follows: [𝛼]=[13,12], [̇𝛼]=[54,50], [𝑞]=[20,10], [𝑘1]=[0,0.6], [𝛽]=[7,3], [𝛿𝑒]=[10,6], [𝑀]=[0,1.6], [𝑝]=[24,38], [𝛿𝑠]=[3,3], and [𝑞]=[4.964,21.746].

For the first cell (1,1,1,1,1,1,1,1,1,1), the coefficients in (2.1) after model training are found to be 𝑝1𝑘= (2.61755, 1.26662, 1.42338, 2.07962, 0.44241, 2.78017, 1.78150, 1.30818, 1.82872, 1.67592, 1.13787).

Assume that in the following flight conditions 𝐶𝑧 is to be predicted: 𝛼=6.91015 deg.; ̇𝛼=2.95510 deg/sec; 𝑞=1.16609 deg/sec; 𝑘1=0.01965; 𝛽=1.55252; 𝛿𝑒=0.68120 deg; 𝑀=0.77279; 𝑝=2.62359 deg/sec; 𝛿𝑠=0.13930 deg; 𝑞=11.0545 kpa.

These values of variables are converted to [0,1]. For example, 𝑥𝛼=[6.91015(13)]/[12(13)]=0.79641.

Other variable values are converted in the same way. It follows that the cell internal function becomes 𝑃1=2.61755+(1.26662)(0.79641)+(1.42338)(0.54764)+(2.07962)(0.70554)(0.44241)(0.03275)+(2.78017)(0.54475)+(1.7815)(0.66758)+(1.30818)(0.48299)+(1.82872)(0.34478+(1.67592)(0.47678)+(1.13787)(0.3730)=11.04817.

The membership functions for the first cell are exactly equal to 𝑥𝑟, being 0.79641, 0.54764, and so forth. Their product can be calculated to be 1.08536𝐸 004. Therefore, the contribution of the first cell to the total output is 11.04817 * 1.08536𝐸004= 1.19912𝐸003.

The total output from all cells can be calculated to be 5.9962; while the denominator in (2.6) is calculated to be 7.46459. Therefore, the final prediction is 0.8033. Comparing with data of 0.81038, this prediction has an error of 0.88%.

To examine the stability characteristics, it is imperative to understand the flight environment in detail. The corresponding flight data are presented in Figure 3. In general, one uses 𝑎𝑛 instead of 𝑎𝑧 for turbulence intensity study. Note 𝑎𝑛 is the same as 𝑎𝑧 in this paper. The variation of normal acceleration is presented in Figure 3(a), showing the highest 𝑎𝑛 being 1.75 g around 𝑡=3930 seconds and the lowest being 0.02 g around 𝑡=3932 seconds. Figure 3(b) shows that 𝛼 is approximately in phase with 𝑎𝑛. When 𝑎𝑛 is the highest (around 𝑡=3930 seconds), the aircraft rapidly plunging downward with the altitude () reaching the lowest as shown in Figure 3(c); and 𝛼 is highest about 6.5 deg. in Figure 3(b). At the same time, M is around 0.77 in Figure 3(d). Since α reaches a value about 6.5 deg in transonic flight, compressibility effect is important. It should be noted that the turbulent vertical wind field was not measured or estimated in the FDR, but is included in the total 𝛼.

fig3
Figure 3: The time history of flight variables for a twin-jet transport in sever clear-air turbulence at the altitude around 10,050 m in transonic flight.

The aerodynamic derivatives extracted from the unsteady aerodynamic models can be calculated with two approaches, first one being the central difference method [7] and the other being the forced small-amplitude oscillation method [14]. The longitudinal stability derivative (𝐶𝑚𝛼) is extracted from the model of 𝐶𝑚. It is evaluated with the central difference approach as follows:

𝐶𝑚𝛼=𝐶𝑚(𝛼+Δ𝛼,)𝐶𝑚(𝛼Δ𝛼,)2Δ𝛼,(4.1) where Δ𝛼=0.5 degree represents that αis perturbed by 0.5 degree while keeping all other variables unchanged. The roll damping (𝐶𝑙𝑝) is extracted from the models of 𝐶𝑙 with the central difference approach as follows:

𝐶𝑙𝑝=𝐶𝑙(,𝑝+Δ𝑝,)𝐶𝑙(,𝑝Δ𝑝,)2Δ𝑝,(4.2) where Δ𝑝 deg/sec. Similarly, all other aerodynamic derivatives are calculated by using the same method.

The time period between 3927.5 seconds and 3932.5 seconds is emphasized in evaluating the stability characteristics, because of the plunging motion that affects the flight safety the most. In order to evaluate the variations in characteristics, the units of all aerodynamic derivatives are converted to rad-1. The main longitudinal and lateral-directional stability derivatives along the flight path are presented in Figure 4. It should be noted that these derivatives are evaluated at the instantaneous conditions, instead of about the trim conditions as have been traditionally done. From the point of view in static stability, initially, the configuration has longitudinal stability (𝐶𝑧𝛼<0 and 𝐶𝑚𝛼<0) as shown in Figure 4(a), stable longitudinal damping (𝐶𝑚𝑞<0) in Figure 4(b), lateral stability (𝐶𝑙𝛽<0) and directional stability (𝐶𝑛𝛽>0) in Figure 4(c), small roll damping (𝐶𝑙𝑝<0) and insufficient directional damping (𝐶𝑛𝑟 small or positive) in Figure 4(d). During the plunging motion, in the period between t = 3928.5 seconds. and t = 3930.5 seconds, 𝐶𝑚𝛼>0 and 𝐶𝑙𝛽>0, so that the static stability becomes unstable. The aerodynamic instability is most likely caused by the motion that produces a time-dependent pressure distribution on the aircraft surface involving compressibility effects.

fig4
Figure 4: The time history of main longitudinal and lateral-directional of the static stability derivatives along the flight path.

Figure 5 presents the time history of main longitudinal and lateral-directional oscillatory derivatives along the flight path to associate with ̇𝛼 and ̇𝛽-derivatives. Note that in Figure 5(a), the oscillatory derivatives are defined as

fig5
Figure 5: The time history of main longitudinal and lateral-directional oscillatory derivatives along the flight path.

𝐶𝑚𝑞osc=𝐶𝑚𝑞+𝐶𝑚̇𝛼𝐶,(4.3)𝑧𝑞osc=𝐶𝑧𝑞+𝐶𝑧̇𝛼(4.4)

In Figure 4(c), the oscillatory derivatives are defined as

𝐶𝑙𝑝osc=𝐶𝑙𝑝+𝐶𝑙̇𝛽𝐶sin𝛼,(4.5)𝑛𝑟osc=𝐶𝑛𝑟𝐶𝑛̇𝛽cos𝛼.(4.6)

During the plunging motion, the values have some differences between oscillatory and damping derivatives in Figures 5(a) and 5(c) due to the effects of the dynamic derivatives (i.e., ̇𝛼 and ̇𝛽-derivatives). The effects of ̇𝛼-derivative on (𝐶𝑧𝑞)osc, and ̇𝛽-derivative on (𝐶𝑙𝑝)osc are small. However, the effect of ̇𝛼-derivative on (𝐶𝑚𝑞)osc is to improve the stability in pitch after t = 3929.5 seconds; while the effects of ̇𝛽-derivative is to cause the directional stability more unstable (i.e., (𝐶𝑛𝑟)osc more positive). These results indicate that the turbulent crosswind has the effects on directional stability and damping. Although the dynamic derivatives tend to be small for the present configuration, these are much helpful to understand the unknown factors of instability characteristics. To be stable, (𝐶𝑧𝑞)osc<0, (𝐶𝑚𝑞)osc<0, (𝐶𝑙𝑝)osc<0, and (𝐶𝑛𝑟)osc<0. Physically, if it is unstable, the motion will be divergent in oscillatory motions.

5. Concluding Remarks

The main objective in this paper was to illustrate the nonlinear unsteady aerodynamic models based on the FLM technique having the capability to evaluate the variations in stability of commercial aircraft with adverse weather effects. It was shown that the FLM technique was capable of handling nonlinear and unsteady aerodynamic environment exhibited for a twin-jet transport in severe clear-air turbulence with sudden plunging motion in transonic flight. The predicted results showed that the models could produce relatively accurate aerodynamic coefficients and several derivatives for the assessment of stability characteristics, especially for the sensitive study of unknown factors in adverse weather conditions.

Acknowledgments

This research project is sponsored by a grant, NSC 98-2221-E-157-005, from National Science Council (NSC). The accomplishment in this project is part of the requirements set by the Aviation Safety Council (ASC), Taiwan.

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