The computation of the atmospheric trajectory, ground track and extrapolated ground level point of a fireball from eyewitness accounts |
1. Introduction
Three methods of computing the atmospheric trajectory of a fireball from eyewitness accounts are described, including the advantages and limitations of each. The three methods will be referred to as Azimuths First, Plane and Ground, and Intersecting Planes. It will be concluded that the last of these is far superior to the other two. Initially it is assumed that there are only two witnesses, which is the minimum number necessary to obtain a trigonometric solution. Following that will be a section on how to treat the observations from many more than two witnesses.It is assumed that all of the following conditions are fulfilled:
Each witness is interviewed | 1. In situ |
2. By a trained interviewer | |
3. Within a week of an event | |
The interviewer | 4. Measures the angles indicated by a witness |
5. With instruments | |
Witnesses are distributed | 6. On both sides of the fireball, so that some witnesses see the fireball move from left to right, and others see it move from right to left. |
If all of these conditions are not satisfied, a trigonometric solution should not be attempted. Any results arising from a calculation in which all of these conditions are not satisfied will be pure fiction and the computed atmospheric track and impact point will be grossly in error. It should also be noted that witness reports (other than purely descriptive reports) from witnesses in moving vehicles should not be used in quantitative calculations. In order of increasing unreliability of angular reports from moving vehicles are those from cars, boats and aircraft.
In the calculations described below, a Flat Earth is assumed. While each method can be modified to include the curvature of Earth, or the height of a witness above sea level, this is not at all justified - and it would be downright unscientific to include such minutiae - for eyewitness accounts, which typically have errors of several degrees or even tens of degrees. A Flat Earth model assumes that the height of the fireball (typically tens of km) is negligible compared with the radius of Earth (6371 km), and that the height of a witness above sea-level (at most in Canada, in the unlikely event that a witness was at the summit of Mount Logan and was also interviewed there, 5.95 km) is negligible compared with the typical fireball height of tens of km. It is doubtful whether a departure from a Flat Earth model is justifiable even from a wide-field photograph, although this will depend on the quality and what landmarks or skymarks are identifiable on the photograph.
I therefore propose that the following terms be standardized.
Witness A indicates the two points on the sky track, which correspond to two points on the atmospheric trajectory which I call K and L. Witness B indicates two points on the sky track, which correspond to two points (not necessarily the same two points that were indicated by witness A) on the atmospheric trajectory which I call M and N.
The position of an altazimuth point on the celestial sphere centred at a witness is to be denoted by the usual spherical coordinates (q , f). Here q is the zenith distance, or the complement of the altitude. The azimuth f is measured from the east point of the horizon counterclockwise (northward). (In the original report from an interviewer, azimuth will probably be given as measured from the north point of the horizon clockwise (eastward); it will be necessary to change this for conformity with the usual mathematical convention for spherical coordinates.) It is assumed that azimuth is given relative to true geographic coordinates and that any corrections for magnetic declination have been properly made.
(For the benefit of astronomers it might be mentioned here that in geophysics the term "magnetic declination" is used to describe the difference between true and magnetic north; this clearly is quite unrelated to the word "declination" as used in spherical astronomy.)
The directions to the four points indicated by the two witnesses are then given, in obvious notation, by
In this method, witness A indicates the directions to two points
K and L in the usual manner, and witness B indicates the directions
to the same two points K and L. Let K' and L' be the points
at ground level vertically below K and L, which are on the atmospheric
trajectory. That is to say, K' and L' are on the ground track.
The distances of K' and L' from the two witnesses are then easily found
simply by making a scale drawing as illustrated in figure 1, in which the
full lines represent the azimuths of K' and L' relative to A and B, and
the dashed line is the ground track.
This graphical method of locating K' and L' is so simple that many may
not wish to do it by trigonometrical calculation. However,
others will wish to programme the calculation for automatic computation,
and I therefore give here the coordinates of K' and L' in terms of the
measured data.:
(1)
(2)
and for L', merely substitute L and L' for K and K' in these equations.
The distances a, b, c, d indicated in figure 1 are:
(3)
and similarly in an obvious manner for the others.
The x- and y-coordinates of K and L on the atmospheric trajectory are,
of course, the same as those of K' and L', and their z-coordinates (heights)
are
(4)
and (5)
The two ways of calculating each of these serves as a check against arithmetic mistakes.
Assuming that K is higher than L (if it isn't the meteoroid is rising, not falling), the coordinates of the extrapolated ground level point O are
(6)
(7)
This point is, of course, on the ground track. The impact point, also on the ground track, will fall short of this point by an amount that cannot be determined from geometric considerations alone.
While this method is simple and straightforward it has one very severe limitation, which renders its use invalid except in most unlikely circumstances, namely, it is essential that the two witnesses indicate the same two points on the atmospheric trajectory. This might, on rare occasion, be possible, if there were two well-defined flares unambiguously marking two specific and unmistakable points on the atmospheric trajectory and the investigator is certain that each witness has indicated these same two points. In practice it is almost never the case that two witnesses indicate the same two points. The problem is infinitely compounded if there are many more than two witnesses. If the above analysis is carried out on the erroneous assumption that the two witnesses have indicated the same two points, the computed ground track will be totally erroneous and not even approximately correct.
The situation is illustrated in figure 2. The dashed line is the true ground track. K' and L' are the ground projections of the two points indicated by witness A, and M' and N' are the ground projections of the two points indicated by witness B. The dash-dotted line is the erroneous ground track. In the example (by no means an extreme one) of figure 2, the angle between the correct and erroneous ground tracks is 58 degrees. In figure 2 we indicate the points K" and L", which are the quite erroneously-deduced positions of K' and L'. We see further that the distances a, b, c, d, which should correctly be, respectively, AK', AL', BM', BN', will be erroneously taken to be AK", AL", BK", BL". The heights deduced from these erroneous values will be absurdly wrong and the deduced extrapolated ground level point is likely to be many hundreds or even more than a thousand kilometres from the correct point and nowhere near the correct ground track.
Figure 2
Witness A, situated at the point (x_{A} , y_{A}
), indicates the directions to two points, K and L, described by spherical
coordinates ( q_{AK} , f_{AK}
) , ( q_{AL} , f_{AL
}).
The atmospheric trajectory of the fireball must lie in the plane that includes
the witness and the vectors from the witness to K and L. The equation
to this plane is
(8)
This can be written in the form
P_{A}x + Q_{A}y + R_{A}z + 1 = 0 (9)
and it intersects the ground in the line (not the ground track!)
P_{A }x + Q_{A}y + 1 = 0. (10)
Similarly the plane defined by witness B intersects the ground in a line
P_{B}x + Q_{B}y + 1 = 0. (11)
The solution of equations (10) and (11) gives the coordinates of the extrapolated ground-level point.
It would be possible to write expressions for the coordinates of the ground-level point explicitly in terms of the original data, and the investigator might like to try to do this, though it is more likely that the entire procedure will be carried out numerically, step-by-step.
This method is simple and it has the great advantage over the Azimuths
First method that it does not require that the two witnesses indicate
the same two points. While it does quickly produce the extrapolated
ground-level point, it is to be remembered that the impact point falls
on the ground track short of the extrapolated ground-level point, and the
method has not determined the ground track, so that we do not know in what
direction to search starting from the extrapolated ground-level point.
As described in section 5, each witness and the directions to the indicated points describes a plane, the two planes being given by
P_{A}x + Q_{A}y + R_{A}z + 1 = 0 (12)
and P_{B}x + Q_{B }y + R_{B}z + 1 = 0. (13)
Equation (12) is just equation (9) repeated, and the method of setting it up is described in section 5. The atmospheric trajectory is in each of these planes; that is to say the atmospheric trajectory is the intersection of the two planes and indeed equations (12) and (13) are the equations to the atmospheric trajectory. (For those who may not be conversant with algebraic geometry in three dimensions, a line in three dimensional space is always represented by two equations.)
As in section 5, the extrapolated ground-level point can be found by
putting z = 0 in each of these two equations, to form equations (10) and
(11), and solving these equations for x and y. If instead of putting
z = 0 we eliminate z between equations (12) and (13), we shall obtain
a linear equation in x and y , and this equation is the equation to
the ground track, which will include both the extrapolated ground-level
point and the impact point. As pointed out earlier, geometric considerations
alone cannot determine the distance between these two points.
What is certain, at least, is that the impact point is between the extrapolated
ground-level point and the more forward of L' or N', which are the ground-level
points vertically below the second points for the two witnesses.
For any point (x , y) on the ground track, the corresponding height
z on the atmospheric trajectory can be found from either (or, preferably,
both, as an arithmetic check) of equations (12) or (13). If
Dx
, Dy , Dz are the
differences between the coordinates of any two points on the atmospheric
trajectory, the true angle of descent y below the horizontal is given by
The method of computing the pre-encounter orbit presuming that the position and velocity vectors before atmospheric entry are known, is outlined in a separate MIAC document by the author.
Typically the distribution of witnesses will be somewhat clumpy. There are likely to be several witnesses within two or three km of each other in each town or village visited by the investigators. (I have used the plural here - it order to obtain the necessary measurements from a wide area within a week, it is necessary to have a team of trained investigators.) In addition there will be a few isolated witnesses from rural areas. Each group of witnesses (whether of several people in a town, or a "group" of one individual in the countryside) must be counted as a single observation site and an average sky track for all the witnesses in that group must be determined. The differences in apparent sky tracks reported by individuals within a few km of each other are not trigonometrical differences and must not be treated as such., but differences in recollection.
The altitudes and azimuths of the first and last points for each witness within a group can be plotted on graph paper and joined to show the several indicated sky tracks. There will be appreciable variation among them, and, if one of more are obviously completely and unrealistically different from the general trend of the rest, they should probably at this stage be discarded.
The next stage is to draw a "least-squares sky track" through the remaining (undiscarded) first and second points for all the witnesses within the group. The least-squares calculation is best carried out by a mathematically and statistically trained investigator. Most "packaged" least-squares programs are, technically, least-squares "regressions of y upon x", and such a regression is entirely inappropriate here. It should be assumed that the random errors in altitude and in azimuth are equally likely, so what has to be minimized is the sum of the squares of the perpendicular (not vertical) distances of each point from the computed regression line, or, more correctly, since we are dealing with the celestial sphere, the sum of the squares of the great circle distances of each point from the computed regression line.
This least-squares sky track then forms the average sky track for all the members within that (closely-spaced) group. When combining this group with others, the group can be given a weight proportional to the square root of the number of witnesses in the group. (It is my practice - after having done numerous interviews - not to attempt to assign a weight to individual witnesses based on a "gut feeling" of how reliable a particular witness was. I give zero weight to any witness in a moving vehicle, whether car, boat or aircraft, and perhaps to any witness who had obviously not seen the same thing as everyone else; but I have found no rational way to quantify my "gut feeling" - probably quite unfairly wrong - about the reliability of individual witnesses.)
We then have to "pair" each group on one side of the trajectory with every group in turn on the other side. Groups on the same side of the trajectory must not be paired with each other. In the latter case the angles between the intersecting planes are small and the errors in determining the line of intersection are hopelessly large - an error of a degree in the angle of intersection being easily capable of shifting the ground track by thousands of kilometres or even placing the atmospheric trajectory beneath the ground.
If there are N_{1} groups on one side of the trajectory and
N_{2} on the other, the number of pairings will be N_{1}N_{2},
so you will calculate N_{1}N_{2 }extrapolated ground-level
points and N_{1}N_{2} ground tracks. A least-squares
ground track from all of these, and a "centre of gravity" extrapolated
ground-level point can then be calculated, giving a weight proportional
to the geometric mean of the weights you have given to each of the two
groups.
Having determined the "centre of gravity" extrapolated ground-level
point, you then go there to search not for meteorites but for additional
witnesses.
10 January 2002 -- Copyright J Tatum