gr-air-modes/python/mlat.py

197 lines
11 KiB
Python
Executable File

#!/usr/bin/python
import math
import numpy
from scipy.ndimage import map_coordinates
#functions for multilateration.
#this library is more or less based around the so-called "GPS equation", the canonical
#iterative method for getting position from GPS satellite time difference of arrival data.
#here, instead of multiple orbiting satellites with known time reference and position,
#we have multiple fixed stations with known time references (GPSDO, hopefully) and known
#locations (again, GPSDO).
#NB: because of the way this solver works, at least 3 stations and timestamps
#are required. this function will not return hyperbolae for underconstrained systems.
#TODO: get HDOP out of this so we can draw circles of likely position and indicate constraint
########################END NOTES#######################################
#this is a 10x10-degree WGS84 geoid datum, in meters relative to the WGS84 reference ellipsoid. given the maximum slope, you should probably interpolate.
#NIMA suggests a 2x2 interpolation using four neighbors. we'll go cubic spline JUST BECAUSE WE CAN
wgs84_geoid = numpy.array([[13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13,13], #90N
[3,1,-2,-3,-3,-3,-1,3,1,5,9,11,19,27,31,34,33,34,33,34,28,23,17,13,9,4,4,1,-2,-2,0,2,3,2,1,1], #80N
[2,2,1,-1,-3,-7,-14,-24,-27,-25,-19,3,24,37,47,60,61,58,51,43,29,20,12,5,-2,-10,-14,-12,-10,-14,-12,-6,-2,3,6,4], #70N
[2,9,17,10,13,1,-14,-30,-39,-46,-42,-21,6,29,49,65,60,57,47,41,21,18,14,7,-3,-22,-29,-32,-32,-26,-15,-2,13,17,19,6], #60N
[-8,8,8,1,-11,-19,-16,-18,-22,-35,-40,-26,-12,24,45,63,62,59,47,48,42,28,12,-10,-19,-33,-43,-42,-43,-29,-2,17,23,22,6,2], #50N
[-12,-10,-13,-20,-31,-34,-21,-16,-26,-34,-33,-35,-26,2,33,59,52,51,52,48,35,40,33,-9,-28,-39,-48,-59,-50,-28,3,23,37,18,-1,-11], #40N
[-7,-5,-8,-15,-28,-40,-42,-29,-22,-26,-32,-51,-40,-17,17,31,34,44,36,28,29,17,12,-20,-15,-40,-33,-34,-34,-28,7,29,43,20,4,-6], #30N
[5,10,7,-7,-23,-39,-47,-34,-9,-10,-20,-45,-48,-32,-9,17,25,31,31,26,15,6,1,-29,-44,-61,-67,-59,-36,-11,21,39,49,39,22,10], #20N
[13,12,11,2,-11,-28,-38,-29,-10,3,1,-11,-41,-42,-16,3,17,33,22,23,2,-3,-7,-36,-59,-90,-95,-63,-24,12,53,60,58,46,36,26], #10N
[22,16,17,13,1,-12,-23,-20,-14,-3,14,10,-15,-27,-18,3,12,20,18,12,-13,-9,-28,-49,-62,-89,-102,-63,-9,33,58,73,74,63,50,32], #0
[36,22,11,6,-1,-8,-10,-8,-11,-9,1,32,4,-18,-13,-9,4,14,12,13,-2,-14,-25,-32,-38,-60,-75,-63,-26,0,35,52,68,76,64,52], #10S
[51,27,10,0,-9,-11,-5,-2,-3,-1,9,35,20,-5,-6,-5,0,13,17,23,21,8,-9,-10,-11,-20,-40,-47,-45,-25,5,23,45,58,57,63], #20S
[46,22,5,-2,-8,-13,-10,-7,-4,1,9,32,16,4,-8,4,12,15,22,27,34,29,14,15,15,7,-9,-25,-37,-39,-23,-14,15,33,34,45], #30S
[21,6,1,-7,-12,-12,-12,-10,-7,-1,8,23,15,-2,-6,6,21,24,18,26,31,33,39,41,30,24,13,-2,-20,-32,-33,-27,-14,-2,5,20], #40S
[-15,-18,-18,-16,-17,-15,-10,-10,-8,-2,6,14,13,3,3,10,20,27,25,26,34,39,45,45,38,39,28,13,-1,-15,-22,-22,-18,-15,-14,-10], #50S
[-45,-43,-37,-32,-30,-26,-23,-22,-16,-10,-2,10,20,20,21,24,22,17,16,19,25,30,35,35,33,30,27,10,-2,-14,-23,-30,-33,-29,-35,-43], #60S
[-61,-60,-61,-55,-49,-44,-38,-31,-25,-16,-6,1,4,5,4,2,6,12,16,16,17,21,20,26,26,22,16,10,-1,-16,-29,-36,-46,-55,-54,-59], #70S
[-53,-54,-55,-52,-48,-42,-38,-38,-29,-26,-26,-24,-23,-21,-19,-16,-12,-8,-4,-1,1,4,4,6,5,4,2,-6,-15,-24,-33,-40,-48,-50,-53,-52], #80S
[-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30,-30]], #90S
dtype=numpy.float)
#ok this calculates the geoid offset from the reference ellipsoid
#combined with LLH->ECEF this gets you XYZ for a ground-referenced point
def wgs84_height(lat, lon):
yi = numpy.array([9-lat/10.0])
xi = numpy.array([18+lon/10.0])
return float(map_coordinates(wgs84_geoid, [yi, xi]))
#WGS84 reference ellipsoid constants
wgs84_a = 6378137.0
wgs84_b = 6356752.314245
wgs84_e2 = 0.0066943799901975848
wgs84_a2 = wgs84_a**2 #to speed things up a bit
wgs84_b2 = wgs84_b**2
#convert ECEF to lat/lon/alt without geoid correction
#returns alt in meters
def ecef2llh((x,y,z)):
ep = math.sqrt((wgs84_a2 - wgs84_b2) / wgs84_b2)
p = math.sqrt(x**2+y**2)
th = math.atan2(wgs84_a*z, wgs84_b*p)
lon = math.atan2(y, x)
lat = math.atan2(z+ep**2*wgs84_b*math.sin(th)**3, p-wgs84_e2*wgs84_a*math.cos(th)**3)
N = wgs84_a / math.sqrt(1-wgs84_e2*math.sin(lat)**2)
alt = p / math.cos(lat) - N
lon *= (180. / math.pi)
lat *= (180. / math.pi)
return [lat, lon, alt]
#convert lat/lon/alt coords to ECEF without geoid correction, WGS84 model
#remember that alt is in meters
def llh2ecef((lat, lon, alt)):
lat *= (math.pi / 180.0)
lon *= (math.pi / 180.0)
n = lambda x: wgs84_a / math.sqrt(1 - wgs84_e2*(math.sin(x)**2))
x = (n(lat) + alt)*math.cos(lat)*math.cos(lon)
y = (n(lat) + alt)*math.cos(lat)*math.sin(lon)
z = (n(lat)*(1-wgs84_e2)+alt)*math.sin(lat)
return [x,y,z]
#do both of the above to get a geoid-corrected x,y,z position
def llh2geoid((lat, lon, alt)):
(x,y,z) = llh2ecef((lat, lon, alt + wgs84_height(lat, lon)))
return [x,y,z]
c = 299792458 / 1.0003 #modified for refractive index of air, why not
#this function is the iterative solver core of the mlat function below
#we use limit as a goal to stop solving when we get "close enough" (error magnitude in meters for that iteration)
#basically 20 meters is way less than the anticipated error of the system so it doesn't make sense to continue
#it's possible this could fail in situations where the solution converges slowly
#THIS WORKS PLEASE DON'T MESS WITH IT
def mlat_iter(stations, prange_obs, guess = [0,0,0], limit = 20, maxrounds = 100):
xerr = [1e9, 1e9, 1e9, 1e9]
rounds = 0
while numpy.linalg.norm(xerr[:3]) > limit:
#get p_i, the estimated pseudoranges based on the latest position guess
prange_est = [[numpy.linalg.norm(station - guess)] for station in stations]
#get the difference d_p^ between the observed and calculated pseudoranges
dphat = prange_obs - prange_est
#create a matrix of partial differentials to find the slope of the error in X,Y,Z,t directions
H = numpy.array([(numpy.array(-stations[row,:])+guess) / prange_est[row] for row in range(len(stations))])
H = numpy.append(H, numpy.ones(len(prange_obs)).reshape(len(prange_obs),1)*c, axis=1)
#now we have H, the Jacobian, and can solve for residual error
solved = numpy.linalg.lstsq(H, dphat)
xerr = solved[0].flatten()
guess += xerr[:3] #we ignore the time error for xguess
rounds += 1
if rounds > maxrounds:
raise MlatNonConvergeError("Failed to converge!")
return (guess, xerr[3])
#func mlat:
#uses a modified GPS pseudorange solver to locate aircraft by multilateration.
#replies is a list of reports, in ([lat, lon, alt], timestamp) format
#altitude is the barometric altitude of the aircraft as returned by the aircraft, if any
#returns the estimated position of the aircraft in (lat, lon, alt) geoid-corrected WGS84.
#let's make it take a list of tuples so we can sort by them
def mlat(replies, altitude):
sorted_replies = sorted(replies, key=lambda time: time[1])
stations = [sorted_reply[0] for sorted_reply in sorted_replies]
timestamps = [sorted_reply[1] for sorted_reply in sorted_replies]
nearest_llh = stations[0]
stations_xyz = numpy.array([llh2geoid(station) for station in stations])
#the absolute time shouldn't matter at all except perhaps in
#maintaining floating-point precision; in other words you can
#add a constant here and it should fall out in the solver as time error
prange_obs = [[c*stamp] for stamp in timestamps]
#if no alt, use a reasonably large number (in meters)
#since if all your stations lie in a plane (they basically will),
#there's a reasonable solution at negative altitude as well
if altitude is None:
altitude = 20000
firstguess = numpy.array(llh2ecef((nearest_llh[0], nearest_llh[1], altitude)))
prange_obs = numpy.array(prange_obs)
xyzpos, time_offset = mlat_iter(stations_xyz, prange_obs, firstguess, maxrounds=100)
llhpos = ecef2llh(xyzpos)
return (llhpos, time_offset)
#tests the mlat_iter algorithm using sample data from Farrell & Barth (p.147)
def farrell_barth_test():
pranges = numpy.array([[22228206.42],
[24096139.11],
[21729070.63],
[21259581.09]])
svpos = numpy.array([[7766188.44, -21960535.34, 12522838.56],
[-25922679.66, -6629461.28, 31864.37],
[-5743774.02, -25828319.92, 1692757.72],
[-2786005.69, -15900725.80, 21302003.49]])
#this is the "correct" resolved position, not the real receiver position
known_pos = numpy.array( [-2430745.0959362, -4702345.11359277, 3546568.70599656])
pos, time_offset = mlat_iter(svpos, pranges)
print "Position: ", pos
print "LLH: ", ecef2llh(pos)
error = numpy.linalg.norm(pos - known_pos)
print "Error: ", error
if error < 1e-3:
print "Farrell & Barth test OK"
else:
raise Exception("ERROR: Failed Farrell & Barth test")
if __name__ == '__main__':
#check to see that you haven't screwed up mlat_iter
farrell_barth_test()
#construct simulated returns from these stations
teststations = [[37.76225, -122.44254, 100], [37.680016,-121.772461, 100], [37.385844,-122.083082, 100], [37.701207,-122.309418, 100]]
testalt = 8000
testplane = numpy.array(llh2ecef([37.617175,-122.400843, testalt]))
tx_time = 10 #time offset to apply to timestamps
teststamps = [tx_time+numpy.linalg.norm(testplane-numpy.array(llh2geoid(station))) / c for station in teststations]
print "Actual pranges: ", sorted([numpy.linalg.norm(testplane - numpy.array(llh2geoid(station))) for station in teststations])
replies = [(station, stamp) for station,stamp in zip(teststations, teststamps)]
ans, offset = mlat(replies, testalt)
error = numpy.linalg.norm(numpy.array(llh2ecef(ans))-numpy.array(testplane))
rng = numpy.linalg.norm(llh2geoid(ans)-numpy.array(llh2geoid(teststations[0])))
print "Resolved lat/lon/alt: ", ans
print "Error: %.2fm" % (error)
print "Range: %.2fkm (from first station in list)" % (rng/1000)
print "Aircraft-local transmit time: %.8fs" % (offset)