| 3 |
|
{ |
| 4 |
|
Source distribution coordinates (degrees). |
| 5 |
|
|
| 6 |
< |
Theta is measured from the negative z-axis, |
| 7 |
< |
phi is measured from the positive x-axis |
| 8 |
< |
according to the right-hand rule. |
| 6 |
> |
Theta is measured from the negative z-axis. |
| 7 |
> |
Phi is measured from the positive x-axis (0 degrees) |
| 8 |
> |
towards the negative y-axis (90 degrees). |
| 9 |
|
|
| 10 |
|
srcB_vert and srcB_horiz are angles |
| 11 |
|
used in type B photometry. |
| 18 |
|
the x,y,z axes, are given in meters regardless of the |
| 19 |
|
units being used in the scene file. |
| 20 |
|
|
| 21 |
+ |
cylcorr function provides the same correction for a |
| 22 |
+ |
cylinder whose central axis is aligned with the Z-axis. |
| 23 |
+ |
|
| 24 |
|
A1 - optional multipier |
| 25 |
|
A2,A3,A4 - X,Y,Z dimensions of axis-aligned box (in meters!) |
| 26 |
+ |
or |
| 27 |
+ |
A2,A3 - diameter and height of Z-aligned cylinder (meters) |
| 28 |
|
} |
| 29 |
|
{ local definitions } |
| 30 |
|
boxprojection = abs(Dx)*A3*A4 + abs(Dy)*A2*A4 + abs(Dz)*A2*A3; |
| 31 |
|
lboxprojection = ( noneg(abs(Px-Dx*Ts)-A2/2)*A3*A4 + |
| 32 |
|
noneg(abs(Py-Dy*Ts)-A3/2)*A2*A4 + |
| 33 |
|
noneg(abs(Pz-Dz*Ts)-A4/2)*A2*A3 ) / Ts; |
| 34 |
+ |
cylprojection = A2*A3*sqrt(1-Dz*Dz) + PI/4*A2*A2*abs(Dz); |
| 35 |
|
|
| 36 |
|
flatcorr(v) = corr(v) / Rdot; { correction for flat sources } |
| 37 |
|
corr(v) = if(AC-.5, A1*v, v); { multiplier correction } |
| 38 |
|
boxcorr(v) = A1 * v / boxprojection; { correction for emitting box } |
| 39 |
|
lboxcorr(v) = A1 * v / lboxprojection; { local box correction } |
| 40 |
+ |
cylcorr(v) = A1 * v / cylprojection; { cylinder correction } |
| 41 |
|
|
| 42 |
|
src_theta = Acos(Dz) / DEGREE; { 0-180 } |
| 43 |
< |
src_phi = mod( atan2(Dy, Dx) / DEGREE, 360 ); { 0-360 } |
| 43 |
> |
src_phi = mod( Atan2(Dy, -Dx) / DEGREE, 360 ); { 0-360 } |
| 44 |
|
{ bilateral symmetry } |
| 45 |
|
src_phi2 = tri( src_phi, 180 ); { 0-180 } |
| 46 |
|
{ quadrilateral symmetry } |
