Position, Navigation, and Timing Technologies in the 21st Century

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Covers the latest developments in PNT technologies, including integrated satellite navigation, sensor systems, and civil applications Featuring sixty-four chapters that are divided into six parts, this two-volume work provides comprehensive coverage of the state-of-the-art in satellite-based position, navigation, and timing (PNT) technologies and civilian applications. It also examines alternative navigation technologies based on other signals-of-opportunity and sensors and offers a comprehensive treatment on integrated PNT systems for consumer and commercial applications.
Volume 1 of
contains three parts and focuses on the satellite navigation systems, technologies, and engineering and scientific applications. It starts with a historical perspective of GPS development and other related PNT development. Current global and regional navigation satellite systems (GNSS and RNSS), their inter-operability, signal quality monitoring, satellite orbit and time synchronization, and ground- and satellite-based augmentation systems are examined. Recent progresses in satellite navigation receiver technologies and challenges for operations in multipath-rich urban environment, in handling spoofing and interference, and in ensuring PNT integrity are addressed. A section on satellite navigation for engineering and scientific applications finishes off the volume.
Volume 2 of
consists of three parts and addresses PNT using alternative signals and sensors and integrated PNT technologies for consumer and commercial applications. It looks at PNT using various radio signals-of-opportunity, atomic clock, optical, laser, magnetic field, celestial, MEMS and inertial sensors, as well as the concept of navigation from Low-Earth Orbiting (LEO) satellites. GNSS-INS integration, neuroscience of navigation, and animal navigation are also covered. The volume finishes off with a collection of work on contemporary PNT applications such as survey and mobile mapping, precision agriculture, wearable systems, automated driving, train control, commercial unmanned aircraft systems, aviation, and navigation in the unique Arctic environment.
In addition, this text:
Serves as a complete reference and handbook for professionals and students interested in the broad range of PNT subjects Includes chapters that focus on the latest developments in GNSS and other navigation sensors, techniques, and applications Illustrates interconnecting relationships between various types of technologies in order to assure more protected, tough, and accurate PNT
will appeal to all industry professionals, researchers, and academics involved with the science, engineering, and applications of position, navigation, and timing technologies.pnt21book.com

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It is worth noting that the cdma2000 standard requires the BTS’s clock to be synchronized with GPS to within 10 μs, which translates to a range of approximately 3 km (the average cell size) [51]. Note that a PN offset of 1 (i.e. 64 chips) is enough to prevent significant interference from different BTSs. This translates to more than 15 km between BTSs. Subtracting 6 km from this value due to worst‐case synchronization with GPS (i.e. 3 km for each BTS), BTSs at 9 km or more from the serving BTS could cause interference (assuming all BTSs suffer from the worst‐case synchronizations). But 9 km is larger than the maximum distance for receiving cellular CDMA signals for ground receivers. Therefore, this synchronization requirement is enough to prevent severe interference between the short codes transmitted from different BTSs and maintains the CDMA system’s capability to perform soft hand‐offs [47]. The clock bias of the BTS can therefore be neglected for communication purposes. However, ignoring δt sin navigation applications can be disastrous, and it is therefore crucial for the receiver to know the BTS’s clock bias. The estimation of δt scan be accomplished via the frameworks discussed in Section 38.4.

38.5.1.6 Received Signal Model

Assuming the transmitted signal to have propagated through an additive white Gaussian noise channel with a power spectral density of картинка 254, a model of the received discrete‐time signal r [ m ] after radio frequency (RF) front‐end processing: down‐mixing, a quadrature approach to bandpass sampling [52], and quantization can be expressed as

(38.5) where t s t m δt TOF Δ t k δt TOF is the PN code phase of the BTS t m - фото 255

where t s( t m) ≜ δt TOF+ Δ( t k− δt TOF) is the PN code phase of the BTS, t m= mT sis the sample time expressed in receiver time, T sis the sampling period, δt TOFis the time of flight (TOF) from the BTS to the receiver, θ is the beat carrier phase of the received signal, and n [ m ] = n I[ m ] + jn Q[ m ] with n Iand n Qbeing independent and identically distributed Gaussian random sequences with zero mean and variance картинка 256. The receiver presented in Section 38.5.2will operate on the samples of r [ m ] in Eq. (38.5).

38.5.2 CDMA Receiver Architecture

This section details the architecture of a cellular CDMA navigation receiver, which consists of three main stages: signal acquisition, tracking, and message decoding [18]. The receiver utilizes the pilot signal to detect the presence of a CDMA signal and then tracks it. Section 38.5.2.1describes the correlation process in the receiver. Sections 38.5.2.2and 38.5.2.3discuss the acquisition and tracking stages, respectively. Section 38.5.2.4details decoding the sync and paging channel messages.

38.5.2.1 Correlation Function

Given samples of the baseband signal exiting the RF front‐end defined in Eq. (38.5), the cellular CDMA receiver first wipes off the residual carrier phase and match‐filters the resulting signal. The output of the matched filter can be expressed as

(38.6) where is the beat carrier phase estimate and h is a pulse shaping filter - фото 257

where картинка 258is the beat carrier phase estimate, and h is a pulse shaping filter, which is a discrete‐time version of the one used to shape the spectrum of the transmitted signal, with a finite‐impulse response (FIR) given in Table 38.3. The samples m ′ of the FIR in Table 38.3are spaced by картинка 259.

Table 38.3 FIR of the pulse shaping filter used in cdma2000 [50]

Source: 3GPP2, “Physical layer standard for cdma2000 spread spectrum systems (C.S0002‐E),” 3rd Generation Partnership Project 2 (3GPP2), TS C.S0002‐E, June 2011. Reproduced with permission of 3CPP2.

m h [ m ′] m h [ m ′] m h [ m ′]
0, 47 −0.02528832 8, 39 0.03707116 16, 31 −0.01283966
1, 46 −0.03416793 9, 38 −0.02199807 17, 30 −0.14347703
2, 45 −0.03575232 10, 37 −0.06071628 18, 29 −0.21182909
3, 44 −0.01673370 11, 36 −0.05117866 19, 28 −0.14051313
4, 43 0.02160251 12, 35 0.00787453 20, 27 0.09460192
5, 42 0.06493849 13, 34 0.08436873 21, 26 0.44138714
6, 41 0.09100214 14, 33 0.12686931 22, 25 0.78587564
7, 40 0.08189497 15, 32 0.09452834 23, 24 1.0

Next, x [ m ] is correlated with a local replica of the spreading PN sequence. In a digital receiver, the correlation operation is expressed as

(38.7) Position Navigation and Timing Technologies in the 21st Century - изображение 260

Position Navigation and Timing Technologies in the 21st Century - изображение 261

where Z kis the k ‐th subaccumulation, N sis the number of samples per subaccumulation, and картинка 262is the code start time estimate over the k ‐th subaccumulation. The code phase can be assumed to be approximately constant over a short subaccumulation interval T sub= N s T s; hence, картинка 263. It is worth mentioning that theoretically, T subcan be made arbitrarily large since no data is transmitted on the pilot channel. Practically, T subis mainly limited by the stability of the BTS and receiver oscillators. In the following, T subis set to one PN code period. The carrier phase estimate is modeled as where is the apparent Doppler frequency estimate over the i th - фото 264, where картинка 265is the apparent Doppler frequency estimate over the i ‐th subaccumulation, and θ 0is the initial beat carrier phase of the received signal. As in a GPS receiver, the value of θ 0is set to zero in the acquisition stage and is subsequently updated in the tracking stage. The apparent Doppler frequency is assumed to be constant over a short T sub. Substituting for r [ m ] and x [ m ], defined in Eqs. (38.5)– (38.6), into Eq. (38.7), it can be shown that

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