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Pseudo-Noise (PN) Ranging Systems - CCSDS

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<strong>CCSDS</strong> INFORMATIONAL REPORT CONCERNING PSEUDO-NOISE RANGING SYSTEMS<br />

Table 2-7: Normalized Acquisition Time (τacq-tot ) and Acquisition Time (Tacq) in<br />

Chips and Seconds Assuming fRC=1 MHz and for the Error Probability<br />

Pe2 = 5×10 -5 and a Chip Signal-to-<strong>Noise</strong> Ratio 2EC /N0 of -33 dB<br />

Sequence<br />

T2B 23 × 30.71 =<br />

706.3<br />

T4B 23 × 509.0 =<br />

11,707<br />

τacq-tot = τacq-23 =<br />

23 × τcor Tacq (in chips) Tacq (s)<br />

30,000 × 706.3 =<br />

21,189,900<br />

30,000 × 11,707 =<br />

351,210,000<br />

10.59<br />

175.6<br />

It is interesting to observe that for the on-board acquistion time (TACQ_S/C = TACQ Spacecraft)<br />

the following general expression applies:<br />

=<br />

T<br />

ACQ _ S / C<br />

= K<br />

a<br />

1<br />

· τ acq_<br />

tot ·<br />

F<br />

C<br />

<strong>CCSDS</strong> 414.0-G-1 Page 2-20 March 2010<br />

=<br />

−1<br />

2 [ Q ( Pe<br />

2 ) ]<br />

2E<br />

− 1 2<br />

−1<br />

[ Q ( P ) ] 1 [ Q ( Pe<br />

2)<br />

]<br />

Pr<br />

2<br />

N<br />

0<br />

e2<br />

1<br />

F<br />

C<br />

23 · τ<br />

=<br />

corr<br />

F<br />

C<br />

−1<br />

[ Q ( P ) ]<br />

e2<br />

Pr<br />

2<br />

N<br />

where τcorr , λ and ξ are related to C6 (L6 = 23).<br />

It can be seen that:<br />

0<br />

2<br />

=<br />

23·<br />

ξ<br />

c<br />

N<br />

0<br />

Pr<br />

2<br />

N<br />

0<br />

1<br />

ξ − ψ<br />

2<br />

τ<br />

acq_<br />

23<br />

2<br />

1<br />

F<br />

C<br />

1<br />

23 ·<br />

λξ<br />

– If the acquisition time is given as a function of the <strong>Ranging</strong> Signal Power over <strong>Noise</strong><br />

Spectral Density (PR/N0 in dBHz), then the dependence on the chip rate disappears.<br />

– If PR/N0 is reduced by 3 dB (i.e., from 27 to 24 dBHz), the acquisition time increases<br />

by a factor of 2, if PR/N0 is increased by 10 dB (i.e., from 27 to 37 dBHz), the<br />

acquisition is 10 times smaller. So the values in table 2-7 (evaluated for 27 dBHz)<br />

become respectively 5.29 s (for T2B) and 87.8 s (for T4B) for PR/N0 = 30 dBHz. Also<br />

the variation of the acqusition time based on the exponential law 10 (Pr/No-30)/10 is<br />

demonstrated.<br />

2<br />

=<br />

=

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