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18-Geom-B2 Satellite Navigation · May 2016

Question 5 of 8: The Cycle Slip Phenomenon and Its Consequences

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format: National Exams, May 2016 — 3 hours, closed book (approved Casio/Sharp non-programmable calculators only). EIGHT questions: Q1–Q6 are mandatory (80 marks) and the candidate answers one of Q7/Q8 (20 marks) for a total of 100. This is a theory paper — answers are in essay form, with one short symbolic construction (Q6 double differencing) and one analytic development (Q2 DOP). All eight questions, including both Q7 and Q8, are solved below for completeness.

Reference texts: Hofmann-Wellenhof, Lichtenegger & Wasle, GNSS — Global Navigation Satellite Systems (Springer, 2008); Leick, Rapoport & Tatarnikov, GPS Satellite Surveying (4th ed., Wiley, 2015); Kaplan & Hegarty, Understanding GPS/GNSS: Principles and Applications (3rd ed., Artech House); Groves, Principles of GNSS, Inertial, and Multisensor Integrated Navigation Systems (2nd ed., Artech House, 2013) for Q8; Natural Resources Canada — Canadian Geodetic Survey (CSRS-PPP service, Canadian Active Control System). Canadian frame throughout (NAD83(CSRS), NRCan reference products).

Question 5: The Cycle Slip Phenomenon and Its Consequences (10 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

What a cycle slip is. A carrier-phase observation consists of two parts: a fractional phase that the receiver measures directly and continuously, and an integer number of whole cycles — the ambiguity \(N\) — that the receiver counts by keeping an unbroken lock on the signal since the start of tracking. A cycle slip is a sudden discontinuity in that integer count: the receiver momentarily loses phase lock and, when it resumes, the accumulated cycle count is off by an integer number of wavelengths, while the fractional phase remains correct. The observation therefore jumps by an integer number of cycles at the instant of the slip and stays biased by that same integer thereafter.

Carrier phase Φ (cycles)epoch tcycle slip (ΔN cycles)t = t₀
Cycle slip: the smoothly ramping carrier-phase time series jumps by an integer number of cycles ΔN at the instant of lock loss (t₀), then continues to ramp with the same slope but a constant integer offset.

Causes. Cycle slips arise whenever the tracking loop loses the signal, even briefly: obstruction of the line of sight (trees, buildings, bridges, the operator’s body), low signal-to-noise ratio at low elevation, strong ionospheric scintillation, severe multipath, high receiver dynamics, or receiver-firmware failures. They are common in kinematic work through obstructed environments and are the reason continuous tracking cannot always be assumed.

Consequences in data processing. Because the whole precision of carrier-phase positioning depends on the integer ambiguity being a single known constant, an undetected cycle slip is serious:

Detection and repair. Slips are detected by testing quantities that should vary smoothly: differences of the phase between epochs (and their higher-order differences), the phase-minus-code combination, the geometry-free (ionospheric) combination \(L_1-L_2\), the Melbourne–Wübbena wide-lane combination, or triple differences (which show a slip as a single outlier epoch). Once located, a slip is repaired by estimating the integer jump \(\Delta N\) and adding it back to all subsequent observations, restoring the single constant ambiguity; if it cannot be repaired reliably, a new ambiguity parameter is introduced from the slip epoch onward.