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Bernese GPS Software Version 5.0 - Bernese GNSS Software

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2. Fundamentals<br />

δi error of satellite clock at signal emission time t − τ<br />

rk(t) position of receiver k at signal reception time t,<br />

ri (t − τ) position of satellite i at signal emission time t − τ,<br />

˙r i (t) velocity of satellite at signal reception time,<br />

̺i k geometric distance between satellite i (at signal emission time t −τ) and receiver<br />

k (at signal reception time t).<br />

The geometric distance ̺ i k<br />

may be written as<br />

(c is the velocity of light) and at the same time as<br />

Using the approximation<br />

̺ i k<br />

= c τ (2.24)<br />

̺ i k = |rk(t) − r i (t − τ)| . (2.25)<br />

r i (t − τ) = r i (t) − ˙r i (t) τ (2.26)<br />

we obtain the following equation which may be solved for τ:<br />

<br />

c 2 − ˙r i (t) · ˙r i <br />

(t) τ 2 − 2 ˙r i <br />

(t) rk(t) − r i <br />

(t) τ−<br />

<br />

− rk(t) · rk(t) − 2 rk(t) · r i (t) + r i (t) · r i <br />

(t) = 0 . (2.27)<br />

2.3.1 Code Pseudoranges<br />

Using the known codes modulated onto the <strong>GPS</strong> carriers, receivers are able to measure the<br />

quantity<br />

P i k = c ((t + δk) − (t − τ + δ i )) , (2.28)<br />

which is called pseudorange (because it is biased by satellite and receiver clock errors).<br />

Introducing the geometric distance ̺i k the code pseudorange for frequency F may also be<br />

written as<br />

2.3.2 Phase Pseudoranges<br />

P i Fk = ̺i k + c δk − c δ i . (2.29)<br />

The <strong>GPS</strong> receiver measures the difference between two phases. The basic form of the observation<br />

equation is (see Eqn. (2.4))<br />

where<br />

ψ i Fk (t) = φFk(t) − φ i F (t − τ) + ni Fk<br />

, (2.30)<br />

ψi Fk (t) is the phase measurement (in cycles) at epoch t and frequency F,<br />

φFk(t) is the phase generated by the receiver oscillator at signal reception time t,<br />

φi F (t − τ) is the phase of the carrier at emission time t − τ, and<br />

is an unknown integer number of cycles (the so-called initial phase ambiguity).<br />

n i Fk<br />

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