program stdalone;
type
mat96 = array [ 1 .. 32 , 1 .. 3 ] of real ;
vecb32 = array [ 1 .. 32 ] of boolean ;
vec32 = array [ 1 .. 32 ] of real ;
vec16 = array [ 1 .. 16 ] of real ;
vec8 = array [ 1 .. 8 ] of real ;
vec3 = array [ 1 .. 3 ] of real ;
mat16 = array [ 1 .. 4 , 1 .. 4 ] of real ;
const
We = 7. 292115E- 5; {WGS-84 earth rotation rate}
c = 299792458.0 ; {WGS-84 speed of light}
pi = 3.1415926535898 {WGS 84 value of pi} ;
Wedot = 7. 2921151467E- 5; {WGS 84 value of earth's rotation rate}
mu = 3. 986005E+ 14; {WGS 84 value of earth's univ. grav. par.}
F = - 4. 442807633E- 10; {relativistic correction term constant}
a = 6378137.0 ; {WGS-84 earth's semi major axis}
b = 6356752.31 ; {WGS-84 earth's semi minor axis}
e1sqr = ( a* a - b* b) / ( a* a) ; {first numerical eccentricity}
e2sqr = ( a* a - b* b) / ( b* b) ; {second numerical eccentricity}
var
inp, out: text;
Ttr, tau, Trc, T, Trel: real ;
Az, El, Cr, alpha, dTclck, dTiono, dRtrop, Lat, Lon: real ;
prn, i: integer ;
eph: array [ 1 .. 32 , 1 .. 16 ] of real ;
clk: array [ 1 .. 32 , 1 .. 5 ] of real ;
ion: vec8;
Praw, Pcor: vec32;
Xs: mat96;
SV: vecb32;
P: vec32;
Xr, Xlla, tmp3: vec3;
status: boolean ;
tmp16: vec16;
tmp5: array [ 1 .. 5 ] of real ;
{***************************************************************************}
procedure LLA2XYZ( Xi : vec3; {lat [rad], lon [rad] alt [m]}
var Xo : vec3) ; {ECEF X [m], Y [m] , Z[m]}
{this procedure converts WGS-84 Lat, Lon and Alt [above ellipsoid]
to ECEF XYZ}
var
N: real ;
begin
N : = a / sqrt ( 1.0 - e1sqr * sin ( Xi[ 1 ] ) * sin ( Xi[ 1 ] ) ) ;
Xo[ 1 ] : = ( N + Xi[ 3 ] ) * cos ( Xi[ 1 ] ) * cos ( Xi[ 2 ] ) ;
Xo[ 2 ] : = ( N + Xi[ 3 ] ) * cos ( Xi[ 1 ] ) * sin ( Xi[ 2 ] ) ;
Xo[ 3 ] : = ( N * ( 1.0 - e1sqr) + Xi[ 3 ] ) * sin ( Xi[ 1 ] ) ;
end ; {procedure LLA2XYZ}
{***************************************************************************}
procedure XYZ2LLA( Xi : vec3; {ECEF X [m], Y [m] , Z[m]}
var Xo : vec3) ; {lat [rad], lon [rad] alt [m]}
{this procedure converts WGS-84 ECEF XYZ to Lat, Lon, Alt [above ellipsoid]}
var
p, T, sT, cT, N, sig: real ;
begin
p : = sqrt ( Xi[ 1 ] * Xi[ 1 ] + Xi[ 2 ] * Xi[ 2 ] ) ;
T : = arctan ( ( Xi[ 3 ] * a) / ( p * b) ) ;
sT : = sin ( T) ; cT : = cos ( T) ;
Xo[ 1 ] : = arctan ( ( Xi[ 3 ] + e2sqr * b * sT * sT * sT)
/ ( p - e1sqr * a * cT * cT * cT) ) ;
if Xi[ 2 ] <> 0.0 then sig : = Xi[ 2 ] / abs ( Xi[ 2 ] ) else sig : = 1.0 ;
if Xi[ 1 ] = 0.0 then Xo[ 2 ] : = sig * pi / 2.0 else
begin
Xo[ 2 ] : = arctan ( Xi[ 2 ] / Xi[ 1 ] ) ;
if ( Xi[ 1 ] < 0.0 ) and ( Xi[ 2 ] >= 0.0 ) then Xo[ 2 ] : = Xo[ 2 ] + pi;
if ( Xi[ 1 ] < 0.0 ) and ( Xi[ 2 ] < 0.0 ) then Xo[ 2 ] : = Xo[ 2 ] - pi
end ;
N : = a / sqrt ( 1.0 - e1sqr * sin ( Xo[ 1 ] ) * sin ( Xo[ 1 ] ) ) ;
Xo[ 3 ] : = p / cos ( Xo[ 1 ] ) - N;
end ; {procedure XYZ2LLA}
{***************************************************************************}
procedure satpos( eph : vec16; {ephemeris}
Ttr : real ; {satellite GPS time}
var Trel: real ; {relativistic correction term}
var X : vec3) ; {satellite position}
var
M0, dn, ec, A, W0, i0, w, Wdot, Cuc, Cus, Crc, Crs, Cic, Cis, Toe, Idot: real ;
T, n0, n, M, E, Eold, snu, cnu, nu, phi, du, dr, di, u, r, i, Xdash, Ydash, Wc: real ;
k: integer ;
begin
{for clarity of code, copy the ephemeris parameters and convert to radians}
Crs : = eph[ 1 ] ;
dn : = eph[ 2 ] * pi;
M0 : = eph[ 3 ] * pi;
Cuc : = eph[ 4 ] ;
ec : = eph[ 5 ] ;
Cus : = eph[ 6 ] ;
A : = eph[ 7 ] * eph[ 7 ] ;
Toe : = eph[ 8 ] ;
Cic : = eph[ 9 ] ;
W0 : = eph[ 10 ] * pi;
Cis : = eph[ 11 ] ;
i0 : = eph[ 12 ] * pi;
Crc : = eph[ 13 ] ;
w : = eph[ 14 ] * pi;
Wdot: = eph[ 15 ] * pi;
idot: = eph[ 16 ] * pi;
T: = Ttr - Toe;
if T > 302400 then T : = T - 604800 ;
if T < - 302400 then T : = T + 604800 ;
n0 : = sqrt ( mu / ( A* A* A) ) ;
n : = n0 + dn;
M : = M0 + n* T;
E : = M; {start value for E}
repeat
Eold : = E;
E : = M + ec * sin ( E) ;
until abs ( E - Eold) < 1. 0e- 8;
snu : = sqrt ( 1 - ec* ec) * sin ( E) / ( 1 - ec* cos ( E) ) ;
cnu : = ( cos ( E) - ec) / ( 1 - ec* cos ( E) ) ;
if cnu = 0 then nu : = pi/ 2 * snu / abs ( snu)
else if ( snu = 0 ) and ( cnu > 0 ) then nu : = 0
else if ( snu = 0 ) and ( cnu < 0 ) then nu : = pi
else nu : = arctan ( snu/ cnu)
+ ord ( cnu<0 ) * pi * snu / abs ( snu) ;
phi : = nu + w;
du : = Cuc* cos ( 2 * phi) + Cus* sin ( 2 * phi) ;
dr : = Crc* cos ( 2 * phi) + Crs* sin ( 2 * phi) ;
di : = Cic* cos ( 2 * phi) + Cis* sin ( 2 * phi) ;
u : = phi + du;
r : = A* ( 1 - ec* cos ( E) ) + dr;
i : = i0 + idot* T + di;
Xdash : = r* cos ( u) ;
Ydash : = r* sin ( u) ;
Wc: = W0 + ( Wdot - Wedot) * T - Wedot* Toe;
X[ 1 ] : = Xdash* cos ( Wc) - Ydash* cos ( i) * sin ( Wc) ;
X[ 2 ] : = Xdash* sin ( Wc) + Ydash* cos ( i) * cos ( Wc) ;
X[ 3 ] : = Ydash* sin ( i) ;
Trel : = F * ec * eph[ 7 ] * sin ( E) {relativistic correction term}
end ; {procedure satpos}
{***************************************************************************}
procedure calcAzEl( Xs, {satellite ECEF XYZ}
Xu : vec3; {user ECEF XYZ}
var Az, {azimuth [rad]}
El : real ; {elevation [rad]}
var stat: boolean ) ; {calculation succeeded: stat = true}
var
R, p, x, y, z, s: real ;
e: array [ 1 .. 3 , 1 .. 3 ] of real ;
i, k: integer ;
d: vec3;
begin
x : = Xu[ 1 ] ;
y : = Xu[ 2 ] ;
z : = Xu[ 3 ] ;
p : = sqrt ( x* x + y* y) ;
if p = 0.0 then stat : = false else stat : = true ;
if stat then
begin
R : = sqrt ( x* x + y* y + z* z) ;
e[ 1 , 1 ] : = - y / p;
e[ 1 , 2 ] : = + x / p;
e[ 1 , 3 ] : = 0.0 ;
e[ 2 , 1 ] : = - x* z / ( p* R) ;
e[ 2 , 2 ] : = - y* z / ( p* R) ;
e[ 2 , 3 ] : = p / R;
e[ 3 , 1 ] : = x / R;
e[ 3 , 2 ] : = y / R;
e[ 3 , 3 ] : = z / R;
for k : = 1 to 3 do
begin
d[ k] : = 0.0 ;
for i : = 1 to 3 do d[ k] : = d[ k] + ( Xs[ i] - Xu[ i] ) * e[ k, i]
end ;
s : = d[ 3 ] / sqrt ( d[ 1 ] * d[ 1 ] + d[ 2 ] * d[ 2 ] + d[ 3 ] * d[ 3 ] ) ;
if s = 1.0 then El : = 0.5 * pi else El : = arctan ( s / sqrt ( 1.0 - s* s) ) ;
if ( d[ 2 ] = 0.0 ) and ( d[ 1 ] > 0.0 ) then Az : = 0.5 * pi else
if ( d[ 2 ] = 0.0 ) and ( d[ 1 ] < 0.0 ) then Az : = 1.5 * pi else
begin
Az : = arctan ( d[ 1 ] / d[ 2 ] ) ;
if d[ 2 ] < 0.0 then Az : = Az + pi else
if ( d[ 2 ] > 0.0 ) and ( d[ 1 ] < 0.0 ) then Az : = Az + 2.0 * pi
end ;
end ;
end ; {procedure calcAzEl}
{***************************************************************************}
procedure ionocorr ( ion : vec8; {iono correction coefficients from
nav message}
Latu, {user's latitude [rad]}
Lonu, {user's longitude [rad]}
Az, {SV azimuth [rad]}
El, {SV elevation [rad]}
Ttr : real ; {SV signal transmission time [sec]}
var dTiono: real ) ; {Ionospheric delay [sec]}
var
phi, Lati, Loni, Latm, T, F, x, per, amp: real ;
a0, a1, a2, a3, b0, b1, b2, b3: real ;
begin
{for clarity copy array}
a0 : = ion[ 1 ] ;
a1 : = ion[ 2 ] ;
a2 : = ion[ 3 ] ;
a3 : = ion[ 4 ] ;
b0 : = ion[ 5 ] ;
b1 : = ion[ 6 ] ;
b2 : = ion[ 7 ] ;
b3 : = ion[ 8 ] ;
{convert from radians to semicircles}
Latu : = Latu / pi; Lonu : = Lonu / pi; Az : = Az / pi; El : = El / pi;
{calculation}
phi : = 0.0137 / ( El + 0.11 ) - 0.022 ;
Lati : = Latu + phi * cos ( Az * pi) ;
if Lati > + 0.416 then Lati : = + 0.416 else if Lati < - 0.416 then Lati : = - 0.416 ;
Loni : = Lonu + phi * sin ( Az * pi) / cos ( Lati * pi) ;
Latm : = Lati + 0.064 * cos ( ( Loni - 1.617 ) * pi) ;
T : = 4. 32E+ 4 * Loni + Ttr;
while T >= 86400 do T : = T - 86400 else while T < 0 do T : = T + 86400 ;
F : = 1.0 + 16.0 * ( 0.53 - El) * ( 0.53 - El) * ( 0.53 - El) ;
per : = b0 + b1 * Latm + B2 * Latm * Latm + b3 * Latm * Latm * Latm;
if per < 72000.0 then per : = 72000.0 ;
x : = 2 * pi * ( T - 50400.0 ) / per;
amp : = a0 + a1 * Latm + A2 * Latm * Latm + a3 * Latm * Latm * Latm;
if amp < 0.0 then amp : = 0.0 ;
if abs ( x) >= 1.57 then dTiono : = F * 5. 0E- 9 else
dTiono : = F * ( 5. 0E- 9 + amp * ( 1.0 - x * x / 2.0 + x * x * x * x / 24.0 ) )
end ; {procedure ionocorr}
{***************************************************************************}
{At many places in the following procedure solve the subdeterminant value of a
4 x 4 array is required. For convenience the function sub is defined below}
function sub ( A : mat16; {input 4 x 4 array}
r, {row number to be deleted}
c : integer {column number to be deleted}
) : double; {value of 3 x 3 subdeterminant}
var
B: array [ 1 .. 3 , 1 .. 3 ] of double;
i, i1, j, j1: integer ;
begin
i1 : = 0 ;
for i : = 1 to 4 do if i <> r then
begin
i1 : = i1 + 1 ;
j1 : = 0 ;
for j : = 1 to 4 do if j <> c then
begin
j1 : = j1 + 1 ;
B[ i1, j1] : = A[ i, j]
end
end ;
sub : = + B[ 1 , 1 ] * ( B[ 2 , 2 ] * B[ 3 , 3 ] - B[ 2 , 3 ] * B[ 3 , 2 ] )
- B[ 2 , 1 ] * ( B[ 1 , 2 ] * B[ 3 , 3 ] - B[ 3 , 2 ] * B[ 1 , 3 ] )
+ B[ 3 , 1 ] * ( B[ 1 , 2 ] * B[ 2 , 3 ] - B[ 1 , 3 ] * B[ 2 , 2 ] ) ;
end ; {function sub}
{***************************************************************************}
procedure solve( Xs : mat96; {array with 3 columns and 32 rows
for the coordinates of the sat's}
SV : vecb32; {valid prn's}
P : vec32; {pseudoranges}
var Xr : vec3; {input of initial guess, output of
final position}
var Cr : real ; {receiver clock error}
var status: boolean ) ; {true: calculation OK, false: no solution}
{procedure solve requires the following types to be declared in the
main body of the program:
type
mat96 = array[1..32,1..3] of real;
vecb32 = array[1..32] of boolean;
vec32 = array[1..32] of real;
vec3 = array[1..3] of real;
mat16 = array[1..4,1..4] of real;}
var
prn, it, i, j, k: integer ;
R, L: array [ 1 .. 32 ] of real ;
A: array [ 1 .. 32 , 1 .. 4 ] of real ;
AL: array [ 1 .. 4 ] of real ;
AA, AAi: mat16;
n: longint ;
det: real ;
D: array [ 1 .. 4 ] of real ;
begin {procedure solve}
it : = 0 ; {iteration counter}
repeat {iterations}
it : = it + 1 ; {increase iteration counter}
for prn : = 1 to 32 do if SV[ prn] then
begin
R[ prn] : = {range from receiver to satellite}
sqrt ( ( Xr[ 1 ] - Xs[ prn, 1 ] ) * ( Xr[ 1 ] - Xs[ prn, 1 ] )
+ ( Xr[ 2 ] - Xs[ prn, 2 ] ) * ( Xr[ 2 ] - Xs[ prn, 2 ] )
+ ( Xr[ 3 ] - Xs[ prn, 3 ] ) * ( Xr[ 3 ] - Xs[ prn, 3 ] ) ) ;
L[ prn] : = P[ prn] - R[ prn] ; {range residual value}
for k : = 1 to 3 do A[ prn, k] : = ( Xr[ k] - Xs[ prn, k] ) / R[ prn] ;
A[ prn, 4 ] : = - 1.0 {A is the geometry matrix or model matrix}
end ;
For k : = 1 to 4 do {calculate A.L}
begin
AL[ k] : = 0.0 ;
for prn : = 1 to 32 do if SV[ prn] then
AL[ k] : = AL[ k] + A[ prn, k] * L[ prn]
end ;
for k : = 1 to 4 do for i : = 1 to 4 do {calculate A.A}
begin
AA[ k, i] : = 0.0 ;
for prn : = 1 to 32 do if SV[ prn] then
AA[ k, i] : = AA[ k, i] + A[ prn, k] * A[ prn, i]
end ;
{invert A.A}
det : = + AA[ 1 , 1 ] * sub( AA, 1 , 1 ) - AA[ 2 , 1 ] * sub( AA, 2 , 1 )
+ AA[ 3 , 1 ] * sub( AA, 3 , 1 ) - AA[ 4 , 1 ] * sub( AA, 4 , 1 ) ;
if det = 0.0 then status : = false else
begin
status : = true ;
for k : = 1 to 4 do for i : = 1 to 4 do
begin
n: = k + i; if odd ( n) then j : = - 1 else j : = 1 ;
AAi[ k, i] : = j * sub( AA, i, k) / det
end ;
{calculate (invA.A).(A.L)}
for k : = 1 to 4 do
begin
D[ k] : = 0.0 ;
for i : = 1 to 4 do D[ k] : = D[ k] + AAi[ k, i] * AL[ i]
end ;
{update position}
for k : = 1 to 3 do Xr[ k] : = Xr[ k] + D[ k] ;
end ;
until ( it = 6 ) {there is something wrong if more than 6 iterations are required}
or ( ( abs ( D[ 1 ] ) + abs ( D[ 2 ] ) + abs ( D[ 3 ] ) ) < 1. 0E- 2) {iteration criterion}
or ( not ( status) ) ; {calculation not succeeded}
Cr : = D[ 4 ] ; {receiver clock error}
if it = 6 then begin writeln ( 'solve it : ' , it) ; status : = false end ; {iteration not succeeded}
end ; {procedure solve}
{***************************************************************************}
begin {main}
{the following data should be available:
1. Pseudorange with receiver time of reception for each SV
2. Ephemeris and almanac for each SV
3. Iono coefficients}
{open input datafile}
assign( inp, 'inp.txt' ) ; reset( inp) ;
{read GPS time of reception}
readln ( inp) ; {skip comment line}
readln ( inp, Trc) ;
{read iono coefficients}
readln ( inp) ; {skip comment line}
for i : = 1 to 8 do readln ( inp, ion[ i] ) ;
readln ( inp) ; {skip comment line}
{read pseudoranges}
for prn : = 1 to 32 do SV[ prn] : = false ;
repeat
read ( inp, prn) ;
if prn <> 0 then
begin
readln ( inp, Praw[ prn] ) ;
SV[ prn] : = true
end
else readln ( inp) ;
until prn = 0 ;
readln ( inp) ; {skip comment line}
{read ephemeris- and clock data}
repeat
readln ( inp, prn) ;
for i : = 1 to 16 do readln ( inp, eph[ prn, i] ) ;
for i : = 1 to 5 do readln ( inp, clk[ prn, i] ) ;
until eof ( inp) ;
close( inp) ;
{user input of start position}
write ( 'Start position Lat [deg.dec], Lon [deg.dec], Alt [m] : ' ) ;
readln ( Xlla[ 1 ] , Xlla[ 2 ] , Xlla[ 3 ] ) ;
Xlla[ 1 ] : = Xlla[ 1 ] * pi / 180.0 ; Xlla[ 2 ] : = Xlla[ 2 ] * pi / 180.0 ;
{convert lat, ln, alt to ECEF X, Y, Z}
LLA2XYZ( Xlla, Xr) ;
{open output data file}
assign( out, 'output.txt' ) ; rewrite( out) ;
{assuming the receiver clock error and initial position not sufficiently
good known, I make two passes through the processing steps}
{PASS 1}
writeln ( out, 'PASS 1' ) ;
for prn : = 1 to 32 do if SV[ prn] then begin {do for each SV}
{set all transit times to nominal value and calculate time of transmission}
tau : = 0.075 ;
Ttr : = Trc - tau;
{calculate SV position and correct for earth rotation}
for i : = 1 to 16 do tmp16[ i] : = eph[ prn, i] ;
satpos( tmp16, Ttr, Trel, tmp3) ;
alpha : = tau * We;
Xs[ prn, 1 ] : = + tmp3[ 1 ] * cos ( alpha) + tmp3[ 2 ] * sin ( alpha) ;
Xs[ prn, 2 ] : = - tmp3[ 1 ] * sin ( alpha) + tmp3[ 2 ] * cos ( alpha) ;
Xs[ prn, 3 ] : = + tmp3[ 3 ] ;
writeln ( out, 'SV : ' , prn: 2 , Xs[ prn, 1 ] : 15 : 3 , Xs[ prn, 2 ] : 15 : 3 , Xs[ prn, 3 ] : 15 : 3 ) ;
{calculate azimuth and elevation}
for i : = 1 to 3 do tmp3[ i] : = Xs[ prn, i] ;
calcAzEl( tmp3, Xr, Az, El, status) ;
if not status then
begin writeln ( 'Error in calcAzEl - check input data' ) ; exit end ;
writeln ( out, 'Az, El : ' , prn: 2 , Az* 180.0 / pi: 11 : 3 , El* 180.0 / pi: 10 : 3 ) ;
{calculate pseudorange corrections and apply to pseudoranges}
{clock correction}
T : = Ttr - clk[ prn, 2 ] ;
{correct for week crossover}
if T > 302400 then T : = T - 604800 ;
if T < - 302400 then T : = T + 604800 ;
dTclck : = + clk[ prn, 5 ] + clk[ prn, 4 ] * T + clk[ prn, 3 ] * T * T
+ Trel - clk[ prn, 1 ] ;
{iono correction}
Lat : = Xlla[ 1 ] ; Lon : = Xlla[ 2 ] ;
ionocorr( ion, Lat, Lon, Az, El, Ttr, dTiono) ;
{tropo correction using standard atmosphere values}
dRtrop : = + 2.312 / sin ( sqrt ( El * El + 1. 904E- 3) )
+ 0.084 / sin ( sqrt ( El * El + 0. 6854E- 3) ) ;
writeln ( out, 'Corr : ' , prn: 2 , dTclck* c: 11 : 3 , dTiono* c: 10 : 3 , dRtrop: 10 : 3 ) ;
{correct pseudorange}
Pcor[ prn] : = Praw[ prn] + dTclck * c - dTiono * c - dRtrop
end ; {do for each SV}
{calculate receiver position}
solve( Xs, SV, Pcor, Xr, Cr, status) ;
if not status then
begin writeln ( 'Error in solve - check input data' ) ; exit end ;
writeln ( out, 'Pos XYZ: ' , Xr[ 1 ] : 12 : 3 , Xr[ 2 ] : 12 : 3 , Xr[ 3 ] : 12 : 3 , Cr: 12 : 3 ) ;
{convert back to Lat, Lon, Alt}
XYZ2LLA( Xr, Xlla) ;
{PASS 2 - The receiver position and -clock error is now well enough known
to calculate the final pseudorange corrections}
writeln ( out) ; writeln ( out, 'PASS 2' ) ;
{correct receiver clock}
Trc : = Trc + Cr / c;
for prn : = 1 to 32 do if SV[ prn] then begin {do for each SV}
{recalculate transit time and time of transmission}
tau : = ( Pcor[ prn] + Cr) / c;
Ttr : = Trc - tau;
{recalculate SV position and correct for earth rotation}
for i : = 1 to 16 do tmp16[ i] : = eph[ prn, i] ;
satpos( tmp16, Ttr, Trel, tmp3) ;
alpha : = tau * We;
Xs[ prn, 1 ] : = + tmp3[ 1 ] * cos ( alpha) + tmp3[ 2 ] * sin ( alpha) ;
Xs[ prn, 2 ] : = - tmp3[ 1 ] * sin ( alpha) + tmp3[ 2 ] * cos ( alpha) ;
Xs[ prn, 3 ] : = + tmp3[ 3 ] ;
writeln ( out, 'SV : ' , prn: 2 , Xs[ prn, 1 ] : 15 : 3 , Xs[ prn, 2 ] : 15 : 3 , Xs[ prn, 3 ] : 15 : 3 ) ;
{recalculate azimuth and elevation}
for i : = 1 to 3 do tmp3[ i] : = Xs[ prn, i] ;
calcAzEl( tmp3, Xr, Az, El, status) ;
if not status then
begin writeln ( 'Error in calcAzEl - check input data' ) ; exit end ;
writeln ( out, 'Az, El : ' , prn: 2 , Az* 180.0 / pi: 11 : 3 , El* 180.0 / pi: 10 : 3 ) ;
{recalculate pseudorange corrections and apply to pseudoranges}
{clock correction}
T : = Ttr - clk[ prn, 2 ] ;
{correct for week crossover}
if T > 302400 then T : = T - 604800 ;
if T < - 302400 then T : = T + 604800 ;
dTclck : = + clk[ prn, 5 ] + clk[ prn, 4 ] * T + clk[ prn, 3 ] * T * T
+ Trel - clk[ prn, 1 ] ;
{iono correction}
Lat : = Xlla[ 1 ] ; Lon : = Xlla[ 2 ] ;
ionocorr( ion, Lat, Lon, Az, El, Ttr, dTiono) ;
{tropo correction using standard atmosphere values}
dRtrop : = + 2.312 / sin ( sqrt ( El * El + 1. 904E- 3) )
+ 0.084 / sin ( sqrt ( El * El + 0. 6854E- 3) ) ;
writeln ( out, 'Corr : ' , prn: 2 , dTclck* c: 11 : 3 , dTiono* c: 10 : 3 , dRtrop: 10 : 3 ) ;
{correct pseudorange}
Pcor[ prn] : = Praw[ prn] + dTclck * c - dTiono * c - dRtrop + Cr
end ; {do for each SV}
{calculate receiver position}
solve( Xs, SV, Pcor, Xr, Cr, status) ;
if not status then
begin writeln ( 'Error in solve - check input data' ) ; exit end ;
writeln ( out, 'Pos XYZ: ' , Xr[ 1 ] : 12 : 3 , Xr[ 2 ] : 12 : 3 , Xr[ 3 ] : 12 : 3 , Cr: 12 : 3 ) ;
{convert back to Lat, Lon, Alt}
XYZ2LLA( Xr, Xlla) ;
writeln ( out, 'Pos LLA: ' , Xlla[ 1 ] * 180.0 / pi: 15 : 8 , Xlla[ 2 ] * 180.0 / pi: 15 : 8 , Xlla[ 3 ] : 12 : 3 ) ;
close( out)
end . {main}
program stdalone;

type
   mat96 = array[1..32,1..3] of real;
   vecb32 = array[1..32] of boolean;
   vec32 = array[1..32] of real;
   vec16 = array[1..16] of real;
   vec8 = array[1..8] of real;
   vec3 = array[1..3] of real;
   mat16 = array[1..4,1..4] of real;

const
   We = 7.292115E-5;            {WGS-84 earth rotation rate}
   c = 299792458.0;             {WGS-84 speed of light}
   pi = 3.1415926535898         {WGS 84 value of pi};
   Wedot = 7.2921151467E-5;     {WGS 84 value of earth's rotation rate}
   mu = 3.986005E+14;           {WGS 84 value of earth's univ. grav. par.}
   F = -4.442807633E-10;        {relativistic correction term constant}
   a = 6378137.0;               {WGS-84 earth's semi major axis}
   b = 6356752.31;              {WGS-84 earth's semi minor axis}
   e1sqr = (a*a - b*b) / (a*a); {first  numerical eccentricity}
   e2sqr = (a*a - b*b) / (b*b); {second numerical eccentricity}

var
   inp, out: text;
   Ttr, tau, Trc, T, Trel: real;
   Az, El, Cr, alpha, dTclck, dTiono, dRtrop, Lat, Lon: real;
   prn, i: integer;
   eph: array[1..32,1..16] of real;
   clk: array[1..32,1..5] of real;
   ion: vec8;
   Praw, Pcor: vec32;
   Xs: mat96;
   SV: vecb32;
   P: vec32;
   Xr, Xlla, tmp3: vec3;
   status: boolean;
   tmp16: vec16;
   tmp5: array[1..5] of real;

{***************************************************************************}

procedure LLA2XYZ(Xi : vec3;      {lat [rad], lon [rad] alt [m]}
              var Xo : vec3);     {ECEF X [m], Y [m] , Z[m]}
{this procedure converts WGS-84 Lat, Lon and Alt [above ellipsoid]
 to ECEF XYZ}

var
   N: real;
begin
N := a / sqrt(1.0 - e1sqr * sin(Xi[1]) * sin(Xi[1]));
Xo[1] := (N                 + Xi[3]) * cos(Xi[1]) * cos(Xi[2]);
Xo[2] := (N                 + Xi[3]) * cos(Xi[1]) * sin(Xi[2]);
Xo[3] := (N * (1.0 - e1sqr) + Xi[3]) * sin(Xi[1]);
end; {procedure LLA2XYZ}

{***************************************************************************}

procedure XYZ2LLA(Xi : vec3;      {ECEF X [m], Y [m] , Z[m]}
              var Xo : vec3);     {lat [rad], lon [rad] alt [m]}
{this procedure converts WGS-84 ECEF XYZ to Lat, Lon, Alt [above ellipsoid]}

var
   p, T, sT, cT, N, sig: real;
begin
p := sqrt(Xi[1] * Xi[1] + Xi[2] * Xi[2]);
T := arctan((Xi[3] * a) / (p * b));
sT := sin(T); cT := cos(T);
Xo[1] := arctan((Xi[3] + e2sqr * b * sT * sT * sT)
         / (p - e1sqr * a * cT * cT * cT));
if Xi[2] <> 0.0 then sig := Xi[2] / abs(Xi[2]) else sig := 1.0;
if Xi[1] = 0.0 then Xo[2] := sig * pi / 2.0 else
   begin
   Xo[2] := arctan(Xi[2]/Xi[1]);
   if (Xi[1] < 0.0) and (Xi[2] >= 0.0) then Xo[2] := Xo[2] + pi;
   if (Xi[1] < 0.0) and (Xi[2] < 0.0) then Xo[2] := Xo[2] - pi
   end;
N := a / sqrt(1.0 - e1sqr * sin(Xo[1]) * sin(Xo[1]));
Xo[3] := p / cos(Xo[1]) - N;

end; {procedure XYZ2LLA}

{***************************************************************************}

procedure satpos(eph : vec16;    {ephemeris}
                 Ttr : real;     {satellite GPS time}
             var Trel: real;     {relativistic correction term}
             var X   : vec3);    {satellite position}

var
  M0, dn, ec, A, W0, i0, w, Wdot, Cuc, Cus, Crc, Crs, Cic, Cis, Toe, Idot: real;
  T, n0, n, M, E, Eold, snu, cnu, nu, phi, du, dr, di, u, r, i, Xdash, Ydash, Wc: real;
  k: integer;

begin
{for clarity of code, copy the ephemeris parameters and convert to radians}
Crs := eph[1];
dn  := eph[2] * pi;
M0  := eph[3] * pi;
Cuc := eph[4];
ec  := eph[5];
Cus := eph[6];
A   := eph[7] * eph[7];
Toe := eph[8];
Cic := eph[9];
W0  := eph[10] * pi;
Cis := eph[11];
i0  := eph[12] * pi;
Crc := eph[13];
w   := eph[14] * pi;
Wdot:= eph[15] * pi;
idot:= eph[16] * pi;

T:= Ttr - Toe;
if T >  302400 then T := T - 604800;
if T < -302400 then T := T + 604800;

n0 := sqrt(mu / (A*A*A));
n := n0 + dn;

M := M0 + n*T;
E := M; {start value for E}
repeat
   Eold := E;
   E := M + ec * sin(E);
   until abs(E - Eold) < 1.0e-8;

snu := sqrt(1 - ec*ec) * sin(E) / (1 - ec*cos(E)); 
cnu := (cos(E) - ec) / (1 - ec*cos(E)); 
if cnu = 0 then nu := pi/2 * snu / abs(snu)
else if (snu = 0) and (cnu > 0) then nu := 0
else if (snu = 0) and (cnu < 0) then nu := pi
else nu := arctan(snu/cnu)
+ ord(cnu<0) * pi * snu / abs(snu);

phi := nu + w;

du := Cuc*cos(2*phi) + Cus*sin(2*phi);
dr := Crc*cos(2*phi) + Crs*sin(2*phi);
di := Cic*cos(2*phi) + Cis*sin(2*phi);

u := phi + du;
r := A*(1 - ec*cos(E)) + dr;
i := i0 + idot*T +di;

Xdash := r*cos(u);
Ydash := r*sin(u);

Wc:= W0 + (Wdot - Wedot)*T - Wedot*Toe;

X[1] := Xdash*cos(Wc) - Ydash*cos(i)*sin(Wc);
X[2] := Xdash*sin(Wc) + Ydash*cos(i)*cos(Wc);
X[3] := Ydash*sin(i);

Trel := F * ec * eph[7] * sin(E) {relativistic correction term}

end; {procedure satpos}

{***************************************************************************}

procedure calcAzEl(Xs,              {satellite ECEF XYZ}
                   Xu  :  vec3;     {user ECEF XYZ}
               var Az,              {azimuth [rad]}
                   El  : real;      {elevation [rad]}
               var stat: boolean);  {calculation succeeded: stat = true}

var
   R, p, x, y, z, s: real;
   e: array[1..3,1..3] of real;
   i, k: integer;
   d: vec3;

begin

x := Xu[1];
y := Xu[2];
z := Xu[3];
p := sqrt(x*x + y*y);
if p = 0.0 then stat := false else stat := true;

if stat then
   begin

   R := sqrt(x*x + y*y + z*z);
   e[1,1] := - y / p;
   e[1,2] := + x / p;
   e[1,3] := 0.0;
   e[2,1] := - x*z / (p*R);
   e[2,2] := - y*z / (p*R);
   e[2,3] := p / R;
   e[3,1] := x / R;
   e[3,2] := y / R;
   e[3,3] := z / R;

   for k := 1 to 3 do
      begin
      d[k] := 0.0;
      for i := 1 to 3 do d[k] := d[k] + (Xs[i] - Xu[i]) * e[k,i]
      end;

   s := d[3] / sqrt(d[1]*d[1] + d[2]*d[2] + d[3]*d[3]);
   if s = 1.0 then El := 0.5 * pi else El := arctan(s / sqrt(1.0 - s*s));

   if (d[2] = 0.0) and (d[1] > 0.0) then Az := 0.5 * pi else
      if (d[2] = 0.0) and (d[1] < 0.0) then Az := 1.5 * pi else
         begin
         Az := arctan(d[1] / d[2]);
         if d[2] < 0.0 then Az := Az + pi else
            if (d[2] > 0.0) and (d[1] < 0.0) then Az := Az + 2.0 * pi
         end;

   end;

end; {procedure calcAzEl}

{***************************************************************************}

procedure ionocorr (ion   :vec8;    {iono correction coefficients from
                                     nav message}
                    Latu,           {user's latitude [rad]}
                    Lonu,           {user's longitude [rad]}
                    Az,             {SV azimuth [rad]}
                    El,             {SV elevation [rad]}
                    Ttr   : real;   {SV signal transmission time [sec]}
                var dTiono: real);  {Ionospheric delay [sec]}

var
  phi, Lati, Loni, Latm, T, F, x, per, amp: real;
  a0, a1, a2, a3, b0, b1, b2, b3: real;

begin

{for clarity copy array}
a0 := ion[1];
a1 := ion[2];
a2 := ion[3];
a3 := ion[4];
b0 := ion[5];
b1 := ion[6];
b2 := ion[7];
b3 := ion[8];

{convert from radians to semicircles}
Latu := Latu / pi; Lonu := Lonu / pi; Az := Az / pi; El := El / pi;

{calculation}
phi := 0.0137 / (El + 0.11) - 0.022;
Lati := Latu + phi * cos (Az * pi);
if Lati > +0.416 then Lati := +0.416 else if Lati < -0.416 then Lati := -0.416;
Loni := Lonu + phi * sin(Az * pi) / cos(Lati * pi);
Latm := Lati + 0.064 * cos((Loni - 1.617) * pi);
T := 4.32E+4 * Loni + Ttr;
while T >= 86400 do T := T - 86400 else while T < 0 do T := T + 86400;
F := 1.0 + 16.0 * (0.53 - El) * (0.53 - El) * (0.53 - El);
per := b0 + b1 * Latm + B2 * Latm * Latm + b3 * Latm * Latm * Latm;
if per < 72000.0 then per := 72000.0;
x := 2 * pi * (T - 50400.0) / per;
amp := a0 + a1 * Latm + A2 * Latm * Latm + a3 * Latm * Latm * Latm;
if amp < 0.0 then amp := 0.0;
if abs(x) >= 1.57 then dTiono := F * 5.0E-9 else
   dTiono := F * (5.0E-9 + amp * (1.0 - x * x / 2.0 + x * x * x * x /24.0))

end; {procedure ionocorr}

{***************************************************************************}

{At many places in the following procedure solve the subdeterminant value of a
 4 x 4 array is required. For convenience the function sub is defined below}

function sub (A : mat16;      {input 4 x 4 array}
              r,              {row number to be deleted}
              c : integer     {column number to be deleted}
              ) : double;     {value of 3 x 3 subdeterminant}

var
  B: array[1..3,1..3] of double;
  i, i1, j, j1: integer;

begin
i1 := 0;
for i := 1 to 4 do if i <> r then
   begin
   i1 := i1 + 1;
   j1 := 0;
   for j := 1 to 4 do if j <> c then
      begin
      j1 := j1 + 1;
      B[i1,j1] := A[i,j]
      end
   end;
sub := + B[1,1]*(B[2,2]*B[3,3] - B[2,3]*B[3,2])
       - B[2,1]*(B[1,2]*B[3,3] - B[3,2]*B[1,3])
       + B[3,1]*(B[1,2]*B[2,3] - B[1,3]*B[2,2]);
end; {function sub}

{***************************************************************************}

procedure solve(Xs    : mat96;    {array with 3 columns and 32 rows
                                   for the coordinates of the sat's}
                SV    : vecb32;   {valid prn's}
                P     : vec32;    {pseudoranges}
            var Xr    : vec3;     {input of initial guess, output of
                                   final position}
            var Cr    : real;     {receiver clock error}
            var status: boolean); {true: calculation OK, false: no solution}

{procedure solve requires the following types to be declared in the
 main body of the program:
 type
    mat96 = array[1..32,1..3] of real;
    vecb32 = array[1..32] of boolean;
    vec32 = array[1..32] of real;
    vec3 = array[1..3] of real;
    mat16 = array[1..4,1..4] of real;}

var
   prn, it, i, j, k: integer;
   R, L: array[1..32] of real;
   A: array[1..32,1..4] of real;
   AL: array[1..4] of real;
   AA, AAi: mat16;
   n: longint;
   det: real;
   D: array[1..4] of real;


begin {procedure solve}

it := 0; {iteration counter}

repeat {iterations}

   it :=it + 1; {increase iteration counter}

   for prn := 1 to 32 do if SV[prn] then
      begin
      R[prn] :=  {range from receiver to satellite}
         sqrt((Xr[1] - Xs[prn,1]) * (Xr[1] - Xs[prn,1])
            + (Xr[2] - Xs[prn,2]) * (Xr[2] - Xs[prn,2])
            + (Xr[3] - Xs[prn,3]) * (Xr[3] - Xs[prn,3]));
      L[prn] := P[prn] - R[prn]; {range residual value}
      for k := 1 to 3 do A[prn,k] := (Xr[k] - Xs[prn,k]) / R[prn];
      A[prn,4] := -1.0 {A is the geometry matrix or model matrix}
      end;

   For k :=1 to 4 do {calculate A.L}
      begin
      AL[k] := 0.0;
      for prn := 1 to 32 do if SV[prn] then
         AL[k] := AL[k] + A[prn,k] * L[prn]
      end;

   for k := 1 to 4 do for i := 1 to 4 do {calculate A.A}
      begin
      AA[k,i] :=0.0;
      for prn := 1 to 32 do if SV[prn] then
         AA[k,i] := AA[k,i] + A[prn,k] * A[prn,i]
      end;

   {invert A.A}
   det := + AA[1,1] * sub(AA,1,1) - AA[2,1] * sub(AA,2,1)
          + AA[3,1] * sub(AA,3,1) - AA[4,1] * sub(AA,4,1);
   if det = 0.0 then status := false else
      begin

      status := true;

      for k := 1 to 4 do for i := 1 to 4 do
         begin
         n:= k + i; if odd(n) then j := -1 else j :=1;
         AAi[k,i] := j * sub(AA,i,k) / det
         end;

      {calculate (invA.A).(A.L)}
      for k := 1 to 4 do
         begin
         D[k] := 0.0;
         for i := 1 to 4 do D[k] := D[k] + AAi[k,i] * AL[i]
         end;

      {update position}
      for k := 1 to 3 do Xr[k] := Xr[k] + D[k];

      end;

   until (it = 6){there is something wrong if more than 6 iterations are required}
      or ((abs(D[1]) + abs(D[2]) + abs(D[3])) < 1.0E-2) {iteration criterion}
         or (not(status)); {calculation not succeeded}

Cr := D[4]; {receiver clock error}

if it = 6 then begin writeln('solve it : ',it); status := false end; {iteration not succeeded}

end; {procedure solve}

{***************************************************************************}

begin {main}
{the following data should be available:
 1. Pseudorange with receiver time of reception for each SV
 2. Ephemeris and almanac for each SV
 3. Iono coefficients}

{open input datafile}
assign(inp,'inp.txt'); reset(inp);

{read GPS time of reception}
readln(inp); {skip comment line}
readln(inp,Trc);

{read iono coefficients}
readln(inp); {skip comment line}
for i := 1 to 8 do readln(inp,ion[i]);

readln(inp); {skip comment line}
{read pseudoranges}
for prn := 1 to 32 do SV[prn] := false;
repeat
   read(inp,prn);
   if prn <> 0 then
      begin
      readln(inp,Praw[prn]);
      SV[prn] := true
      end
   else readln(inp);
   until prn = 0;

readln(inp); {skip comment line}
{read ephemeris- and clock data}
repeat
   readln(inp,prn);
   for i := 1 to 16 do readln(inp,eph[prn,i]);
   for i := 1 to 5 do readln(inp,clk[prn,i]);
   until eof(inp);
close(inp);

{user input of start position}
write('Start position Lat [deg.dec], Lon [deg.dec], Alt [m] : ');
   readln(Xlla[1],Xlla[2],Xlla[3]);
Xlla[1] := Xlla[1] * pi / 180.0; Xlla[2] :=Xlla[2] * pi / 180.0;
{convert lat, ln, alt to ECEF X, Y, Z}
LLA2XYZ(Xlla,Xr);

{open output data file}
assign(out,'output.txt'); rewrite(out);

{assuming the receiver clock error and initial position not sufficiently
 good known, I make two passes through the processing steps}

{PASS 1}
writeln(out,'PASS 1');

for prn := 1 to 32 do if SV[prn] then begin {do for each SV}

   {set all transit times to nominal value and calculate time of transmission}
   tau := 0.075;
   Ttr := Trc - tau;

   {calculate SV position and correct for earth rotation}
   for i := 1 to 16 do tmp16[i] := eph[prn,i];
   satpos(tmp16,Ttr,Trel,tmp3);
   alpha := tau * We;
   Xs[prn,1] := + tmp3[1] * cos(alpha) + tmp3[2] * sin(alpha);
   Xs[prn,2] := - tmp3[1] * sin(alpha) + tmp3[2] * cos(alpha);
   Xs[prn,3] := + tmp3[3];
   writeln(out,'SV     : ',prn:2,Xs[prn,1]:15:3,Xs[prn,2]:15:3,Xs[prn,3]:15:3);

   {calculate azimuth and elevation}
   for i := 1 to 3 do tmp3[i] := Xs[prn,i];
   calcAzEl(tmp3,Xr,Az,El,status);
   if not status then
      begin writeln('Error in calcAzEl - check input data'); exit end;
   writeln(out,'Az, El : ',prn:2,Az*180.0/pi:11:3,El*180.0/pi:10:3);

   {calculate pseudorange corrections and apply to pseudoranges}

   {clock correction}
   T := Ttr - clk[prn,2];
   {correct for week crossover}
   if T >  302400 then T := T - 604800;
   if T < -302400 then T := T + 604800;

   dTclck := + clk[prn,5] + clk[prn,4] * T + clk[prn,3] * T * T
             + Trel - clk[prn,1];

   {iono correction}
   Lat := Xlla[1] ; Lon := Xlla[2];
   ionocorr(ion,Lat,Lon,Az,El,Ttr,dTiono);

   {tropo correction using standard atmosphere values}
   dRtrop := + 2.312 / sin(sqrt(El * El + 1.904E-3))
             + 0.084 / sin(sqrt(El * El + 0.6854E-3));

   writeln(out,'Corr   : ',prn:2,dTclck*c:11:3,dTiono*c:10:3,dRtrop:10:3);

   {correct pseudorange}
   Pcor[prn] := Praw[prn] + dTclck * c - dTiono * c - dRtrop

   end; {do for each SV}

{calculate receiver position}
solve(Xs,SV,Pcor,Xr,Cr,status);
if not status then
   begin writeln('Error in solve - check input data'); exit end;
writeln(out,'Pos XYZ: ',Xr[1]:12:3,Xr[2]:12:3,Xr[3]:12:3,Cr:12:3);
{convert back to Lat, Lon, Alt}
XYZ2LLA(Xr,Xlla);

{PASS 2 - The receiver position and -clock error is now well enough known
 to calculate the final pseudorange corrections}
writeln(out); writeln(out,'PASS 2');

{correct receiver clock}
Trc := Trc + Cr / c;

for prn := 1 to 32 do if SV[prn] then begin {do for each SV}

   {recalculate transit time and time of transmission}
   tau := (Pcor[prn] + Cr) / c;
   Ttr := Trc - tau;

   {recalculate SV position and correct for earth rotation}
   for i := 1 to 16 do tmp16[i] := eph[prn,i];
   satpos(tmp16,Ttr,Trel,tmp3);
   alpha := tau * We;
   Xs[prn,1] := + tmp3[1] * cos(alpha) + tmp3[2] * sin(alpha);
   Xs[prn,2] := - tmp3[1] * sin(alpha) + tmp3[2] * cos(alpha);
   Xs[prn,3] := + tmp3[3];
   writeln(out,'SV     : ',prn:2,Xs[prn,1]:15:3,Xs[prn,2]:15:3,Xs[prn,3]:15:3);

   {recalculate azimuth and elevation}
   for i := 1 to 3 do tmp3[i] := Xs[prn,i];
   calcAzEl(tmp3,Xr,Az,El,status);
   if not status then
      begin writeln('Error in calcAzEl - check input data'); exit end;
   writeln(out,'Az, El : ',prn:2,Az*180.0/pi:11:3,El*180.0/pi:10:3);

   {recalculate pseudorange corrections and apply to pseudoranges}

   {clock correction}
   T := Ttr - clk[prn,2];
   {correct for week crossover}
   if T >  302400 then T := T - 604800;
   if T < -302400 then T := T + 604800;
   dTclck := + clk[prn,5] + clk[prn,4] * T + clk[prn,3] * T * T
             + Trel - clk[prn,1];

   {iono correction}
   Lat := Xlla[1]; Lon := Xlla[2];
   ionocorr(ion,Lat,Lon,Az,El,Ttr,dTiono);

   {tropo correction using standard atmosphere values}
   dRtrop := + 2.312 / sin(sqrt(El * El + 1.904E-3))
             + 0.084 / sin(sqrt(El * El + 0.6854E-3));

   writeln(out,'Corr   : ',prn:2,dTclck*c:11:3,dTiono*c:10:3,dRtrop:10:3);

   {correct pseudorange}
   Pcor[prn] := Praw[prn] + dTclck * c - dTiono * c - dRtrop + Cr

   end; {do for each SV}

{calculate receiver position}
solve(Xs,SV,Pcor,Xr,Cr,status);
if not status then
   begin writeln('Error in solve - check input data'); exit end;
writeln(out,'Pos XYZ: ',Xr[1]:12:3,Xr[2]:12:3,Xr[3]:12:3,Cr:12:3);
{convert back to Lat, Lon, Alt}
XYZ2LLA(Xr,Xlla);
writeln(out,'Pos LLA: ',Xlla[1]*180.0/pi:15:8,Xlla[2]*180.0/pi:15:8,Xlla[3]:12:3);

close(out)
end. {main}

