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Bernese GPS Software Version 5.0 - Bernese GNSS Software

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11. Troposphere Modeling and Estimation<br />

For local and small regional campaigns, relative troposphere errors are much more important<br />

and more difficult to model. To a first order, the station height bias due to a relative<br />

troposphere error may be computed as<br />

where<br />

∆h = ∆̺0 r<br />

cos zmax<br />

∆h is the induced station height bias,<br />

∆̺ 0 r is the relative tropospheric zenith delay error, and<br />

zmax is the maximum zenith angle of the observation scenario.<br />

(11.1)<br />

In this order of magnitude formula, it is assumed that the satellites are uniformly distributed<br />

over the sky above the observing sites. Due to the fact that <strong>GPS</strong> orbits all have inclinations<br />

of 55 o with respect to the Earth’s equator, this assumption is not true, actually. [Santerre,<br />

1991] studies the implications of a non-uniform satellite distribution.<br />

In any case, Eqn. (11.1) indicates that a relative troposphere bias of only 1 cm leads to an<br />

error of approximately 3 cm in the estimated relative station height for an elevation cutoff<br />

angle of 20 o . This error increases to 19 cm for an elevation cutoff angle of 3 o .<br />

According to [Beutler et al., 1988] the corresponding formula for the impact of an absolute<br />

troposphere error reads as<br />

∆ℓ<br />

ℓ =<br />

∆̺0 a<br />

(11.2)<br />

where<br />

Re cos zmax<br />

ℓ, ∆ℓ are the baseline length and the associated bias,<br />

∆̺0 a is the absolute troposphere bias in zenith direction (common to both endpoints of<br />

the baseline), and<br />

is the Earth’s radius.<br />

Re<br />

Eqn. (11.2) implies that an absolute troposphere bias of 10 cm induces a scale bias of<br />

0.05 ppm for an elevation cutoff angle of 20 o and of 0.3 ppm for a cutoff angle of 3 o , a<br />

relatively small effect compared to the height error caused by a relative troposphere bias.<br />

Nevertheless, this effect should be taken into account for baselines longer than about 20 km.<br />

Again, a uniform satellite distribution in a spherical shell centered above the stations down<br />

to a maximum zenith distance of zmax was assumed when deriving Formula (11.2).<br />

In a certain sense, an absolute troposphere error is very similar to an error caused by the<br />

ionosphere. The main difference between the two effects is due to the circumstance that<br />

tropospheric refraction is produced from the lowest levels of the atmosphere (99% below<br />

10 km) whereas the ionospheric shell height is about 400 km. As a consequence of this,<br />

tropospheric refraction tends to be much more site-specific than ionospheric refraction.<br />

Let us now focus on the correlation of the troposphere zenith delay parameters with the<br />

station height. If troposphere parameters are estimated together with station height and<br />

receiver clock parameters a large correlation between these three parameter types is found<br />

which depends on the elevation cutoff angle applied in the data analysis. Table 11.1 gives<br />

Page 240 AIUB

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