This invention was made, in part, by one or more employees of the U.S. government. The U.S. government has the right to make, use and/or sell the invention described herein without payment of compensation therefor, including but not limited to payment of royalties.
This invention relates to monitoring, analysis and graphic illustration of historical energy, location and orientation parameters for an aircraft in various phases of a flight.
An aircraft that is ascending following takeoff or descending on approach will have measurable kinetic energy and potential energy components, and these components will change with time in measurable, if not predictable, manners. Desirable energy states for both takeoff and landing can be determined from aircraft manufacturer guidance for these phases of flight. For example, where the approach occurs at an airport with an operable and reliable instrument landing system (ILS), the ILS system may provide data recorded on the aircraft to serve as a standard for comparing observed kinetic and potential energy components for an aircraft near the ground, below 2500 feet altitude and for an assumed straight path to a touchdown site. If the airport has no operable and reliable ILS, or if the aircraft is not near the ground, another mechanism for providing a standard for measurements or estimates is needed. On takeoff, where no electronic guidance comparable to the glideslope is available, the aircraft climb profile can be compared to manufacturer guidance or to observed performance for recorded aircraft departures from the particular airport.
The airline industry has become concerned with the problem of unstable aircraft approaches, because approach and landing accidents often begin as unstable approaches. An “unstable approach” is often defined as an approach where below a threshold altitude (1000 feet for IFR and 500 feet for VFR), the aircraft is not established on a proper glide path and with a proper air speed, with a stable descent rate and engine power setting, and with a proper landing configuration (landing gear and flaps extended). Airlines have developed approach procedures that call for abandonment of an approach that is determined to be unstable.
Development and testing of methods for detecting atypical flights by N.A.S.A. has revealed that high energy during an arrival phase (below 10,000 feet but before beginning an approach) is the most common reason for a flight to be identified as atypical or out of a statistically normal range. An atypical high energy arrival phase often corresponds to aircraft kinetic energy and/or potential energy that requires dissipation of 10–30 percent more energy than is required for a reference arrival phase. A reference arrival phase may correspond to about a 3 miles per 1000 feet elevation change (“3-to-1”) glide path slope and decelerating to an airspeed of about 250 knots during descent through 10,000 feet altitude to a standard reference speed around 2,500 feet altitude, when beginning an approach.
More than half of the high energy arrivals identified by atypicality analysis were brought under control within stabilized approach criteria; some of the remainder of the high energy arrivals were abandoned. In contrast, where these findings were used to define and search for a high-energy arrival exceedance, about three times as many excedances were detected; and the resulting unstable approaches were found to occur more frequently than the recoveries.
It may be possible to identify, by historical analysis, a first class of high energy arrivals where recovery and subsequent stabilization is possible and relatively easy, and a second class of high energy arrivals in which recovery and subsequent stabilization is likely to be difficult or impossible. However, the present procedures for determining presence of a reference (acceptable) approach include an electronic glide slope that extends linearly from the end of a target runway to the aircraft, whereas a reference aircraft approach path is curved and follows the electronic glide slope only from about 1,800 feet above the field to the end of the runway.
A 3-to-1 glide path slope, corresponding to decrease of 1,000 feet in altitude for every 3 nautical miles horizontal travel, is often desirable during an arrival phase. Air speed is 250 knots or less by regulation below 10,000 feet, and the aircraft decelerates to a lower reference speed before joining the approach path. These parameters are directly available but are unlikely to prove to be the only relevant parameters in determining whether a flight arrival phase is normal or other than normal.
When an energy component value or orientation component value for a completed flight of interest (referred to herein as a “target flight”) has been measured or observed and compared with a corresponding value for a reference flight, this information should be displayed for possible remedial action on a subsequent flight. A flight operator may also benefit from a display of one or more predictions, based upon the observed or measured target FP values, of the behavior of this FP value over a short time interval extending into the future.
What is needed is a system for displaying energy and other flight parameters associated with one or more phases of target flight, which permits historical analysis and visual and/or alphanumeric comparison of the target FP values with corresponding reference FP values for other flights. Preferably, the system should provide corresponding variables for a reference flight, for comparison with the target flight, and should provide a band surrounding of reference FP values that indicates values of that FP that are acceptable in executing a particular maneuver and ranges of values of that FP from which recovery to a reference flight configuration is unlikely or substantially impossible. Preferably, a difference between the target FP value and the reference FP value, and one or more time derivatives of this difference should be displayed and are used to predict values of this difference over a short time interval in the future.
These needs are met by the invention, which provides a method and system for displaying time variation of one or more flight parameter values, including but not limited to total energy, kinetic energy, potential energy, applied power, vertical speed, height above ground, relevant drag indices and angle of attack for an aircraft in motion and for variation with time of any of these variables with one or more of approximately 20 primary parameters that arise in an energy configuration analysis of the aircraft. More particularly, the system can compare selected variables for the target flight with corresponding variables for a reference flight in a selected flight phase (e.g., approach to touchdown or takeoff). Optionally, the system displays target flight parameter values and indicates what actions might have been taken during the flight to bring the target flight parameter values within a percentage band of historical data for the flight parameter(s). A display of a flight parameter value may be graphical, alphanumeric, or a combination of graphical and alphanumeric.
The system displays a percentage band PB including a selected percentage value p, in a range such as 70%≦p≦95% of all historic data for a given flight parameter for a similar environment. The system also measures (or estimates) and displays a target FP value for a flight of interest under similar environmental conditions, for comparison. Optionally, when the target FP value lies outside the PB, the system performs a further analysis to identify what anomalies are sources of these conditions.
In one embodiment, the system measures and analyzes relevant parameter values for an ascending or descending aircraft to determine if an energy and/or orientation FP value of the target flight is within, or is outside of, a range for a normal flight. This invention can be used in post-flight review of flight data and/or as part of a flight operations quality assurance program to alert an analyst to presence of an anomalous or atypical energy state in historical data.
This measurement/estimation/analysis process may include the following:
(i) providing an estimate or measurement of a target flight parameter value FP(tn) (referred to as a “measured target FP value”) of an aircraft flight parameter during a selected phase (e.g., takeoff, ascent, descent or approach) of a flight, at each of a sequence of measurement (or estimation) times tn (n=1, . . . , N; N≧2);
(ii) providing and displaying a percentage band (“PB”) of historical data FP(tn;hist;m) (m=1, . . . , M; M≧2) for the flight parameter of interest, drawn from historical FP values for M flights under similar conditions;
(iii) determining if the target FP value for the measurement time tn lies within the PB;
(iv) when the target FP value does not lie within the PB, visually or aurally indicating this, and optionally recommending at least one action that may begin to bring subsequently received FP values for the target flight within the PB for future measurement times tn; and
(v) when the target FP value lies within the PB, optionally displaying this value and the band for the measurement time tn.
Flight parameters that can be monitored, analyzed and/or displayed using this approach include: kinetic energy KE(t)=m(t)·v(t)2/2+ω·I·ω/2; potential energy PE(t)=m(t)·g··h(t); energy component E(t)=d1·KE(t)+d2·PE(t), where (d1,d2) are selected non-negative real numbers; energy component time derivative (d/dt)E(t), thrust power, vertical speed, ground air speed, aircraft mass, height above ground, flap position, speed brake position, landing gear position, other drag indices, roll, pitch and/or yaw angles; and angle of attack.
KE(t)=m(t)·v(t)2/2+ω(τ)·I(t)·ω(t)/2, (1)
PE(t)=m(t)·g··h(t), (2)
where m(t) is the instantaneous aircraft mass (taking account of fuel consumption), I(t) is an instantaneous moment of inertia tensor for the aircraft, o(t) is an aircraft rotation vector, computed with reference to a center of gravity or other selected location determined with reference to the aircraft (optional), v(t)=dx/dt is the instantaneous aircraft velocity and h(t) is the instantaneous height of aircraft cg above local reference height, such as local ground height. The rotational component of kinetic energy may be negligible or may be ignored for other reasonsFor an approach to touchdown, the flight parameter of greatest concern is often kinetic energy KE(t).
E(tn)=d1·KE(tn)+d2·PE(tn) (3)
of an energy component of an aircraft during an ascent phase or descent phase of a target flight, at each of a first sequence of times (n=1, . . . , N1; N1≧2), where d1 and d2 are selected real values, not both 0. In step 22, the system provides or computes a reference value E(t′n;ref) of the energy component at a time, t=t′n, determined with reference to the time tn (n=1, . . . , N1). The time sequence {t′n} may substantially coincide with the sequence {tn}, or each time value t′n may be displaced by a calculable or measurable amount from the corresponding time value tn. In step 23, the system computes an index of comparison value C1{E(tn), E(t′n;ref)} of the measured and reference energy components for at least one time value pair (tn,t′n). When the comparison index value C1 lies outside a selected range for this index, the system interprets this condition as indicating that the measured energy component is anomalous or non-normal or may lead to an unstable aircraft maneuver, in step 24.
A variety of comparison indices C1 can be used here. Some examples are: (1) a first ratio E(tn)/E(t′n;ref); (2) a second ratio E(t′n;ref)/E(tn); (3) a difference E(tn)−E(t′n;ref)}; (4) an absolute difference |E(tn)−E(t′n;ref)|; (5) a normalized difference {E(tn)−E(t′n;ref)}/{a−E(tn)+(1−a)·E(t′n;ref)}, where a is a selected real value in a range 0≦a≦1; (6) a weighted average of the differences KE(tn)−KE(t′n;ref) and/or PE(tn)−PE(t′n;ref), such as
where p is a selected positive number (e.g., p=1 or 2 or 3.14) and {wn}n is a sequence of weight values (preferably, but not necessarily, non-negative); and (7) a monotonic function of one or more of the preceding combinations.
The comparison index C1 may use two or more point values, E(tn) and E(t′n;ref), or may use a weighted average of these values, such as the average
The analysis may be extended to consider time rates of change, (d/dt)KE(t) and/or (d/dt)PE(t), of the kinetic and/or potential energy components at a sequence of one or more times {tn}n (n=1, . . . , N2; N2≧1), plus corresponding reference time rates of change, (d/dt)E(t;ref), at a sequence of times {t′n}n determined with reference to the time sequence {tn}n. Another comparison index, C2{(d/dt)E(tn), (d/dt)E(t′n;ref)}, which may be the same or different from the comparison index C1, is computed and compared with a second selected range to determine if the aircraft flight is anomalous or non-normal or is within a normal range. Again, the comparison index C2 may use point values or a weighted average of the values (d/dt)E(t) and/or (d/dt)E(t;ref).
The analysis may be further extended to consider a third comparison index, C3{E(tn), E(t′n;ref), (d/dt)E(tn), (d/dt)E(t″n;ref)}, that depends upon some or all of the estimated values and time rates of change of the estimated values of the energy components. Again, the comparison index C3 may use point values or a weighted average of the values E(t) and/or E(t;ref) and/or (d/dt)E(t)/dt and/or (d/dt)E(t;ref).
A formulation of, and use of, the equations of motion of a target aircraft flight, including the effects of gravity, variable wind speeds, drag and lift forces on various control surfaces, variation of aircraft mass due to fuel consumption, and variable thrust, is set forth in an Appendix. A thrust vector is determined, as a function of the location coordinates, that will move the aircraft from an initial velocity vector v0(x0,y0,z0) to a desired final velocity vector vf(xf,yf,zf) as part of a takeoff phase or as part of an approach phase for a flight. The aircraft kinetic energy is a sum as in Eq. (1).
Each aircraft has an associated group of drag indices, one for each activatable drag appliance (landing gear, wing flap, spoiler/speed brake, etc.). Each drag index has a maximum value where the drag appliance is fully activated and has a spectrum of drag values extending from zero activation through partial activation to full activation of the appliance, as illustrated schematically in
Monitoring of thrust power developed by the engine(s) of the aircraft is straightforward and is an important control variable in change of the energy component E(t) defined in Eq. (3). Thrust developed can be estimated using measured fuel flow rate, temperature within the engine(s) and other relevant variables.
Aircraft angle of attack can be measured, made available and recorded on the aircraft.
The flight parameter value FP(tn) for the target flight is then compared with values FP(tn;hist;m) in the band PB, as illustrated in
Where the target FP value FP(tn) lies substantially outside the percentage band PB for that measurement time, the system optionally performs a further analysis to (i) indicate presence of an atypical or anomalous FP value; (ii) estimate a percentage band (e.g., highest or lowest 1.5 percent in the statistical polulation of values for that FP) in which the FP value falls; and/or (iii) identify one or more sources of the anomalous value.
For example, where the kinetic energy of the target aircraft on approach was too large relative to the FP values within the PB, indicating that the approach velocity was too large, the system may identify a kinetic energy value for a preceding waypoint or for a preceding altitude during descent that was much higher than an acceptable value. These recommendations are made for an already-completed flight but may be useful in comparing similarly atypical target flights that are completed.
This application is a Continuation In Part of U.S. Ser. No. 10/956,523, filed 22 Sep. 2004 now U.S. Pat. No. 7,075,457.
Number | Name | Date | Kind |
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5915273 | Germanetti | Jun 1999 | A |
6985091 | Price | Jan 2006 | B1 |
Number | Date | Country | |
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Parent | 10956523 | Sep 2004 | US |
Child | 11066650 | US |