08.06.2013 Views

Bernese GPS Software Version 5.0 - Bernese GNSS Software

Bernese GPS Software Version 5.0 - Bernese GNSS Software

Bernese GPS Software Version 5.0 - Bernese GNSS Software

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

12. Ionosphere Modeling and Estimation<br />

f1,f2 are the frequencies associated with the carriers L1 and L2,<br />

FI(z) is the mapping function evaluated at the zenith distance z ′ ,<br />

E(β,s) is the vertical TEC (in TECU) as a function of geographic or geomagnetic latitude<br />

β and sun-fixed longitude s, and<br />

B4 = λ1 B1 − λ2 B2 is a constant bias (in meters) due to the initial phase ambiguities B1<br />

and B2 with their corresponding wavelengths λ1 and λ2.<br />

For each receiver, and satellite pass, at least one parameter B4 has to be solved for.<br />

12.3.1.1 Ionosphere Mapping on Zero- and Double-Difference Level<br />

Eqns. (12.10) are valid for zero-difference observations. In the double-difference case, the<br />

“ionospheric” observation equations look similar, with the exception that B4, the phase bias<br />

term, equals now λ1 N1 −λ2 N2 and that b4, the code bias term, vanishes. In the “ambiguityfixed”<br />

case, where the integers N1 and N2 are known, it is obviously no longer necessary to<br />

solve for B4.<br />

Ionosphere mapping on both zero- and double-difference level may be performed using the<br />

program <strong>GPS</strong>EST, considering <strong>GPS</strong>, GLONASS, or <strong>GPS</strong>/GLONASS-combined observations.<br />

There is a second program for ionosphere mapping, IONEST. This program, however,<br />

works only on the basis of <strong>GPS</strong> zero-difference observations and moreover does not take<br />

into account DCBs.<br />

The <strong>Bernese</strong> <strong>GPS</strong> <strong>Software</strong> supports three types of ionosphere models to represent the<br />

deterministic component of the ionosphere:<br />

(1) local models based on two-dimensional Taylor series expansions,<br />

(2) global (or regional) models based on spherical harmonic expansions, and<br />

(3) station-specific models, represented like (2).<br />

Note that the numbers enclosed in brackets correspond to the model type numbers internally<br />

used (see Figures 12.7 and 12.17).<br />

12.3.1.2 Local TEC Model<br />

The local TEC model – applicable in the vicinity of one or more dual-frequency station(s)<br />

– is represented by<br />

where<br />

E(β,s) =<br />

nmax <br />

n=0<br />

mmax <br />

m=0<br />

Enm (β − β0) n (s − s0) m , (12.11)<br />

nmax,mmax are the maximum degrees of the two-dimensional Taylor series expansion in<br />

latitude β and in longitude s,<br />

Enm are the (unknown) TEC coefficients of the Taylor series, i.e., the local ionosphere<br />

model parameters to be estimated, and<br />

β0,s0 are the coordinates of the origin of the development.<br />

Page 260 AIUB

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!