Time & Timers, and GPS Introduction

Total Page:16

File Type:pdf, Size:1020Kb

Time & Timers, and GPS Introduction FYS3240 PC-based instrumentation and microcontrollers Time & timers, and GPS introduction Spring 2014 – Lecture #11 Bekkeng, 20.12.2013 TAI and UTC time • International Atomic Time (TAI) as a time scale is a weighted average of the time kept by over 300 atomic clocks in over 60 national laboratories worldwide. • Coordinated Universal Time (UTC) is the primary time standard by which the world regulates clocks and time, and is based on TAI but with leap seconds added at irregular intervals to compensate for the slowing of the Earth's rotation. • Since 30 June 2012 when the last leap second was added TAI has been exactly 35 seconds ahead of UTC. The 35 seconds results from the initial difference of 10 seconds at the start of 1972, plus 25 leap seconds in UTC since 1972. • UTC is the time standard used for many internet and World Wide Web standards. The Network Time Protocol (NTP), designed to synchronize the clocks of computers over the Internet, encodes times using the UTC system. Synchronize PC clock to NTP server in Windows Note: this Internet time settings is not available when the computer is part of a domain (such as the domain UIO.no) Windows Time service Leap seconds • Time is now measured using stable atomic clocks • A leap second is a one-second adjustment that is occasionally applied to UTC time in order to keep its time of day close to the mean solar time. o Solar time is a reckoning of the passage of time based on the Sun's position in the sky. • Leap seconds are necessary partly because the length of the mean solar day is very slowly increasing, and partly because the atomic, fixed-length SI second, when adopted, was already a little shorter than the current value of the second of mean solar time. Since. 1967, the second has been defined to be the duration of 9,192,631,770 periods of the radiation corresponding to the transition between the two hyperfine levels of the ground state of the cesium 133 atom GPS time • GPS time is the atomic time scale implemented by the atomic clocks in the GPS ground control stations and the GPS satellites themselves. • Periodic corrections are performed to the on-board satellite clocks to keep them synchronized with ground station clocks. • GPS time is NOT corrected for leap seconds. • GPS time is NOT equal to UTC or TAI time. – GPS time remains at a constant offset of 19 seconds with TAI. – As of July 2012, GPS time is 16 seconds ahead of UTC because of the leap seconds added to UTC. – A new leap second correction will be added to UTC in 2016 – GPS time was set to match UTC in 1980 • However, the time offset from UTC is contained in the GPS broadcast message and is usually applied automatically by GPS receivers. From: http://leapsecond.com/java/gpsclock.htm A GPS satellite clock run faster (about 38 μs a day) due to velocity and gravity effects (follows the Relativity theory) Time dilation Computer clocks • Hardware clocks – Real Time Clock (RTC) is an integrated circuit on the motherboard. – The RTC has a battery backup power so that it tracks the time even while the computer is turned off. – Based on a 32.768 kHz quartz crystal oscillator. – Maximum resolution of 1 millisecond (1 kHz). • Software clocks – Maintained by the operating system, based on the RTC interrupts. – When the system starts it sets the system time to a value based on the real-time clock of the computer and then regularly updates the time based on interrupts from the RTC. • Timers/Counters – 8253/8254 PIT (Programmable Interval Timer) – APIC (Advanced Programmable Interrupt Controller) – ACPI (Advanced Configuration Programmable Interrupt) High-Resolution Timers/Counters • High Precision Event Timer (HPET) is a 64-bit up-counter with a frequency higher than 10 MHz. • Time Stamp Counter (TSC) is a 64-bit register in the CPU (cores) that increment each processor clock cycle. However, can be unreliable on a modern multicore computer due to: – multicore computers can have different values in their time-keeping registers. – variability of the CPU frequency due to power management technologies or performance technologies such as Intel Turbo Boost Technology. • A comparator can be used to generate an interrupt. Access the TSC (or HPET) timer using the Windows API functions QueryPerformanceCounter (μs resolution) and QueryPerformanceFrequency QueryPerformanceCounter(n) − QueryPerformanceCounter(n − 1) ∆푇 = QueryPerformanceFrequency QueryPerformance from LabVIEW TSC example Computer clock drift • A quartz clock typically drift more than 1 second in six days. • The software clock is a bad timekeeper! • The computer clock drifts away from the correct time. At the time of synchronization with a time server the clock is reset to the “correct time” (but with a small offset). • Could update the computer clock often, but a much better solution is to read UTC time directly from a timing card (such as NI PXI-6683) connected to GPS, IRIG-B or IEEE1588. Software / Operating System (OS) limits timing resolution and accuracy! The performance is system (hardware, OS) dependent. Satellite navigation • A satellite navigation system with global coverage is called a global navigation satellite system, or GNSS. – GPS (USA) – GLONASS (Russia) – GALILEO (EU): In-Orbit Validation • 30 satellites in 2019 – Compass (China): Chine + Asia-Pacific • 35 satellites in 2020 • A satellite navigation systems can give very accurate – Position – Velocity (doppler) – Time The Global positioning System (GPS) • Space segment – 24 (28/31) satellites orbiting the Earth at an altitude of approximately 20,200 km. The orbital period is about 12 hours – Six orbital planes with four satellites in each. – At least four satellites are visible from any point on the ground at any time • Control segment – Tracking stations around the world monitor and measure orbit and satellite clock correction parameters. These corrections are transmitted up to the satellites and broadcasted to the user segment. • User segment – GPS receivers, giving the user information about the receiver position, velocity and time Two satellites Triangulation in 3D One satellite Three satellites Satellite navigation Multipath • The GPS receiver compare the time of transmission of the coded signal from the satellite with the time of arrival at the receiver s = v * Δt • The velocity v is the velocity of electromagnetic waves in vacuum, including a model of the average delay in the troposphere and ionosphere • Variations in neutral density, temperature and humidity in the atmosphere, and electron density in the ionosphere, affects the velocity of electromagnetic waves, and therefore gives an error in the measured distance s • Orbit errors and multipath (due to reflections) also contribute to the total error in the measured distance to a satellite Index of refraction (n): n(λ) , c = f * λ TEC MAP TEC = Total Electron Content Satellite navigation in 3D • The distance to at least four satellites must be known! • Three satellites need for three distance measurements – Measure “signal time of flight” : s = v * t • The fourth satellites is needed in order to remove clock errors in the receiver unit – GPS satellites have calibrated atomic clocks, but a GPS receiver has only a standard quartz crystal oscillator – An error of 1 ms in the receiver clock gives a position error of 3*108 m/s * 1 ms = 300 km • Navigation data message from each satellite: – Satellite time (when the message was transmitted) + correction – Satellite position (when the message was transmitted), using ephemeris (orbit data) – Almanac data (orbit data etc. for ALL satellites) • More satellites gives better accuracy! Pseudorange The measured pseudorange 푃 푘 from a satellite k can be expressed as (since we can assume no clock error in the satellite): 푃 푘 = (푋푘 − 푥)2+ (푌푘 − 푦)2+ (푍푘 − 푧)2+ 푑 + 푣 = 휌푘 + 푑 + 푣 Where d is the position error due to receiver clock error, (Xk,Yk,Zk) is the known position of satellite k, (x,y,c) is the true receiver position, and 푣 is zero mean Gaussian white noise with variance σ2 GPS signals • Frequencies used in the GPS system: – L1: 1575.42 MHz –C/A code and P(Y) code – L2: 1227.60 MHz –P(Y) code – New civilian signals in the future • L2C, L5, and L1C • Every satellites transmit a unique PRN (pseudorandom noise) code (C/A code) • A doppler shift is introduces (on L1 and L2) due to relative motion between the satellite and the receiver • The receiver must perform a correlation (search in received data) in order to detect the PRN code from a satellite – local PRN codes are correlated with the navigation message New GPS signal L2C Differential GPS (DGPS) • Used to increase the GPS position accuracy (different types of DGPS) • Reference stations on known locations on the Earth can calculate the position based on the C/A coded signals, an compare with the known location of the station. This gives the position error from the GPS system, and this error can be broadcasted to all receivers • The accuracy depends on the distance from the reference station(s) GPS accuracy • GPS (C/A code) : 10 – 30 meters (only L1 used) • GPS (P(Y)-code) : 1 – 3 meters (military receivers, L1 and L2 used) – P(Y) is an encrypted code! • DGPS : 1 – 5 meters • CPDGPS : < 1 cm (static), < 5 cm (kinematic) • EGNOS : 1 – 5 meter (EGNOS is EU’s DGPS) CP = carrier phase Note: SA-code turned off in May 2000 ! .
Recommended publications
  • C:\Data\My Files\WP\PTTI\Proceedings TOC For
    34th Annual Precise Time and Time Interval (PTTI) Meeting TIMEKEEPING AND TIME DISSEMINATION IN A DISTRIBUTED SPACE-BASED CLOCK ENSEMBLE S. Francis Zeta Associates Incorporated B. Ramsey and S. Stein Timing Solutions Corporation J. Leitner, M. Moreau, and R. Burns NASA Goddard Space Flight Center R. A. Nelson Satellite Engineering Research Corporation T. R. Bartholomew Northrop Grumman TASC A. Gifford National Institute of Standards and Technology Abstract This paper examines the timekeeping environments of several orbital and aircraft flight scenarios for application to the next generation architecture of positioning, navigation, timing, and communications. The model for timekeeping and time dissemination is illustrated by clocks onboard the International Space Station, a Molniya satellite, and a geostationary satellite. A mathematical simulator has been formulated to model aircraft flight test and satellite scenarios. In addition, a time transfer simulator integrated into the Formation Flying Testbed at the NASA Goddard Space Flight Center is being developed. Real-time hardware performance parameters, environmental factors, orbital perturbations, and the effects of special and general relativity are modeled in this simulator for the testing and evaluation of timekeeping and time dissemination algorithms. 1. INTRODUCTION Timekeeping and time dissemination among laboratories is routinely achieved at a level of a few nanoseconds at the present time and may be achievable with a precision of a few picoseconds within the next decade. The techniques for the comparison of clocks in laboratory environments have been well established. However, the extension of these techniques to mobile platforms and clocks in space will require more complex considerations. A central theme of this paper – and one that we think should receive the attention of the PTTI community – is the fact that normal, everyday platform dynamics can have a measurable effect on clocks that fly or ride on those platforms.
    [Show full text]
  • Chapter 7. Relativistic Effects
    Chapter 7. Relativistic Effects 7.1 Introduction This chapter details an investigation into relativistic effects that could cause clock errors and therefore position errors in clock coasting mode. The chapter begins with a description of relativistic corrections that are already taken into account for the GPS satellites. Though these corrections are known and implemented [ICD-GPS-200, 1991], no similar corrections are made for GPS receivers that are in motion. Deines derived a set of missing relativity terms for GPS receivers [Deines, 1992], and these are considered in great detail here. A MATLAB simulation was used to predict the relativity effects based on the derivation of Deines, and flight data were used to determine if these effects were present. 7.2 Relativistic Corrections for the GPS Satellite The first effect considered stems from a Lorentz transformation for inertial reference frames. This effect from special relativity is derived from the postulate that the speed of light is constant in all inertial reference frames [Lorentz et. al., 1923]. The correction accounts for time dilation, i.e. moving clocks beat slower than clocks at rest. A standard example is as follows [Ashby and Spilker, 1996]. Consider a train moving at velocity v along the x axis. A light pulse is emitted from one side of the train and reflects against a mirror hung on the opposite wall. The light pulse is then received and the round trip time recorded. If the train car has width w (see Fig. 7.1), then the round trip time according to an observer on the train is: 110 Mirror w Light Pulse Emit/Receive Light Pulse Experiment as Observed on Board the Train Mirror (at time of reflection) v w Emit Pulse Receive Pulse Light Pulse Experiment as Viewed by a Stationary Observer Figure 7.1 Illustration of Time Dilation Using Light Pulses 111 2w t ' (7.1) train c where c is the speed of light.
    [Show full text]
  • Lecture 12: March 18 12.1 Overview 12.2 Clock Synchronization
    CMPSCI 677 Operating Systems Spring 2019 Lecture 12: March 18 Lecturer: Prashant Shenoy Scribe: Jaskaran Singh, Abhiram Eswaran(2018) Announcements: Midterm Exam on Friday Mar 22, Lab 2 will be released today, it is due after the exam. 12.1 Overview The topic of the lecture is \Time ordering and clock synchronization". This lecture covered the following topics. Clock Synchronization : Motivation, Cristians algorithm, Berkeley algorithm, NTP, GPS Logical Clocks : Event Ordering 12.2 Clock Synchronization 12.2.1 The motivation of clock synchronization In centralized systems and applications, it is not necessary to synchronize clocks since all entities use the system clock of one machine for time-keeping and one can determine the order of events take place according to their local timestamps. However, in a distributed system, lack of clock synchronization may cause issues. It is because each machine has its own system clock, and one clock may run faster than the other. Thus, one cannot determine whether event A in one machine occurs before event B in another machine only according to their local timestamps. For example, you modify files and save them on machine A, and use another machine B to compile the files modified. If one wishes to compile files in order and B has a faster clock than A, you may not correctly compile the files because the time of compiling files on B may be later than the time of editing files on A and we have nothing but local timestamps on different machines to go by, thus leading to errors. 12.2.2 How physical clocks and time work 1) Use astronomical metrics (solar day) to tell time: Solar noon is the time that sun is directly overhead.
    [Show full text]
  • Clock Synchronization Clock Synchronization Part 2, Chapter 5
    Clock Synchronization Clock Synchronization Part 2, Chapter 5 Roger Wattenhofer ETH Zurich – Distributed Computing – www.disco.ethz.ch 5/1 5/2 Overview TexPoint fonts used in EMF. Motivation Read the TexPoint manual before you delete this box.: AAAA A • Logical Time (“happened-before”) • Motivation • Determine the order of events in a distributed system • Real World Clock Sources, Hardware and Applications • Synchronize resources • Clock Synchronization in Distributed Systems • Theory of Clock Synchronization • Physical Time • Protocol: PulseSync • Timestamp events (email, sensor data, file access times etc.) • Synchronize audio and video streams • Measure signal propagation delays (Localization) • Wireless (TDMA, duty cycling) • Digital control systems (ESP, airplane autopilot etc.) 5/3 5/4 Properties of Clock Synchronization Algorithms World Time (UTC) • External vs. internal synchronization • Atomic Clock – External sync: Nodes synchronize with an external clock source (UTC) – UTC: Coordinated Universal Time – Internal sync: Nodes synchronize to a common time – SI definition 1s := 9192631770 oscillation cycles of the caesium-133 atom – to a leader, to an averaged time, ... – Clocks excite these atoms to oscillate and count the cycles – Almost no drift (about 1s in 10 Million years) • One-shot vs. continuous synchronization – Getting smaller and more energy efficient! – Periodic synchronization required to compensate clock drift • Online vs. offline time information – Offline: Can reconstruct time of an event when needed • Global vs.
    [Show full text]
  • Relativity and the Universe Gravitational Potential
    Relativity and the Universe Gravitational Potential Arindam Sinha∗y February 5, 2014 Abstract This paper reconciles General Relativity (GR) and Mach's Principle into a consistent, simple and intuitive alternative theory of gravitation. The Universe's ubiquitous background gravi- tational potential plays an important role in relativity concepts. This gravitational potential (energy per unit mass) far from all massive bodies is c2, which determines unit rest mass/energy, and is the essence behind E = mc2. The Universal matter distribution creates a local inertial rest frame at every location, in which the Universe gravitational potential is a minimum. A velocity in this frame increases this gravitational potential through net blue shift of Universal gravity, causing velocity time dilation, which is a gravitational effect identical to gravitational time dilation. Velocity time dilation from this increase of gravitational potential is found to be same as computed from the low velocity approximation of Lorentz factor. The current Lorentz Factor is applicable only in situations where a local potential is dominant compared to the Universe potential. Time dilation increases with velocity, but does not become boundless for general rectilinear motion in the Universe. Speed of light is not the maximum possible speed in such situations, but only in circumstances where the Lorentz Factor is the appropriate metric. Gravitational time dilation is derived first, and velocity time dilation is derived from it. The mathematics becomes much simpler and more
    [Show full text]
  • A Nobel Prize Clock-Watching in Great Court Compromising With
    Issue 10 • Spring 2010 A Nobel Prize Clock-watching in Great Court Compromising with Apartheid Restoration in the Wren A Trinity Memoir New Fellows Ethics and the Genome French Cricket SPIDERS AND PIGEONS: THE PRESSURES ON THE GREAT COURT CLOCK By Hugh Hunt This is a double anniversary year for Smith’s mechanism to attain still the Great Court Clock. It was 400 greater accuracy. years ago in 1610 that the clock was At the heart of the monitoring first installed. Its dial was small and system is a tiny infrared beam that modest, but in 1726 our masterful is interrupted every 1½ seconds by master Bentley had it replaced by the swing of the pendulum—once something grander. The 1610 clock is per “tick”. The signal is recorded by still running in the tower of Orwell’s a PC which also records the one- village church. pulse-per-second output of a GPS As Graham Chinner reported in The receiver—accurate to 10 nanoseconds, Fountain of Autumn 2009, the Bentley so they say. A computer compares the clock mechanism was coincidentally ticks with the GPS to compute the replaced a century ago, in 1910, thanks drift of the clock and the amplitude to a bequest from Lord Grimthorpe. of the pendulum’s swing, producing a His “double three-legged gravity new data point every three seconds. escapement” was made famous in 1859 A weather station also records when installed in the Great Clock in temperature, barometric pressure is 104 milliseconds per day per gram. Westminster (“Big Ben”). In the 50 years and humidity.
    [Show full text]
  • Distributed Systems: Synchronization
    Chapter 3: Distributed Systems: Synchronization Fall 2013 Jussi Kangasharju Chapter Outline n Clocks and time n Global state n Mutual exclusion n Election algorithms Kangasharju: Distributed Systems 2 Time and Clocks What we need? How to solve? Real time Universal time (Network time) Interval length Computer clock Order of events Network time (Universal time) NOTE: Time is monotonous Kangasharju: Distributed Systems 3 Measuring Time n Traditionally time measured astronomically n Transit of the sun (highest point in the sky) n Solar day and solar second n Problem: Earth’s rotation is slowing down n Days get longer and longer n 300 million years ago there were 400 days in the year ;-) n Modern way to measure time is atomic clock n Based on transitions in Cesium-133 atom n Still need to correct for Earth’s rotation n Result: Universal Coordinated Time (UTC) n UTC available via radio signal, telephone line, satellite (GPS) Kangasharju: Distributed Systems 4 Hardware/Software Clocks n Physical clocks in computers are realized as crystal oscillation counters at the hardware level n Correspond to counter register H(t) n Used to generate interrupts n Usually scaled to approximate physical time t, yielding software clock C(t), C(t) = αH(t) + β n C(t) measures time relative to some reference event, e.g., 64 bit counter for # of nanoseconds since last boot n Simplification: C(t) carries an approximation of real time n Ideally, C(t) = t (never 100% achieved) n Note: Values given by two consecutive clock queries will differ only if clock resolution is sufficiently smaller than processor cycle time Kangasharju: Distributed Systems 5 Problems with Hardware/Software Clocks n Skew: Disagreement in the reading of two clocks n Drift: Difference in the rate at which two clocks count the time n Due to physical differences in crystals, plus heat, humidity, voltage, etc.
    [Show full text]
  • A Terahertz Molecular Clock on CMOS Using High-Harmonic-Order Interrogation of Rotational Transition for Medium-/Long-Term Stability Enhancement
    566 IEEE JOURNAL OF SOLID-STATE CIRCUITS, VOL. 56, NO. 2, FEBRUARY 2021 A Terahertz Molecular Clock on CMOS Using High-Harmonic-Order Interrogation of Rotational Transition for Medium-/Long-Term Stability Enhancement Cheng Wang , Member, IEEE,XiangYi , Senior Member, IEEE, Mina Kim , Graduate Student Member, IEEE, Qingyu Ben Yang, and Ruonan Han , Senior Member, IEEE Abstract— Chip-scale molecular clocks (CSMCs) perform I. INTRODUCTION frequency stabilization by referencing to the rotational spectra IGHLY stable, miniaturized, power-efficient, and low- of polar gaseous molecules. With, potentially, the “atomic” clock grade stability, cm3-level volume, and <100-mW dc power, Hcost clocks are increasingly important for the emerg- CSMCs are highly attractive for the synchronization of the ing electronics. For instance, augmented/virtual reality high-speed radio access network (RAN), precise positioning, (AR/VR) devices, real-time multi-person online gaming, and and distributed array sensing. However, the medium-/long-term autonomous driving all require radio access networks (RANs) stability of CSMCs is hindered by the transmission baseline with high capacity (∼1-Gbit/s throughput per node), high den- tilting due to the uneven frequency response of the spectroscopic 2 ∼ system and the molecular cell. To enhance the medium-/long-term sity (one million nodes per km ), and low latency (1 10 ms) stability, this article presents a CSMC architecture locking to the [1], [2]. It leads to the stringent requirements for clock high-odd-order dispersion curve of the 231.061-GHz rotational synchronization. For example, the international telecommuni- spectral line of carbonyl sulfide (OCS) molecules, which is cation union (ITU) specifies a maximum relative timing error selected as the clock reference.
    [Show full text]
  • Middleware and Distributed Systems Time
    Middleware and Distributed Systems Time Martin v. Löwis Mittwoch, 22. Februar 12 Time In Distributed Systems • Time is important • Timestamp of electronic commerce transactions • Some distributed algorithms depend on global time (consistency, authenticity checking, duplicate elimination) • Time is problematic in distributed systems • Absence of global physical time • Local physical clock deviation • Order of event pairs from different nodes • E.g. distributed garbage collection Time | Middleware and Distributed Systems 2 MvL 2011 Mittwoch, 22. Februar 12 Time In Distributed Systems • Collection of N processes pi = p1, p2, ..., pN • Each process on a single processor, no shared memory, own state si • Only message communication - send and receive actions change state • Event as communication or state change action 0 1 2 • Single total ordering of events in one process: history(pi) = ei , ei , ei , ... • Timestamp for event • Physical computer clock: Counting of crystal oscillations, divide count and storage in register as hardware clock value Hi(t) • Clock drift: time is counted in different rates in the hardware clock • Drift rate: Change in Offset to perfect clock value (10-6 to 10-8, atom clock 10-13) • Drift rate may change over time (e.g. due to temperature changes) Time | Middleware and Distributed Systems 3 MvL 2011 Mittwoch, 22. Februar 12 Drift Rates Time Quartz Clock 1second 0,000001 seconds 1 minute 0,00006 seconds 1 hour 0,0036 seconds 1 day 0,0864 seconds 1 week 0,6048 seconds ~11.6 days 1 second Time | Middleware and Distributed
    [Show full text]
  • Time and Synchronization
    FYS3240- 4240 Data acquisition & control Time and synchronization Spring 2018– Lecture #11 Bekkeng, 02.04.2018 Why is time and synchronization so important? • Some examples: – In financial trading we must know the time accurately. – Important to reduce confusion in shared file systems. – Update databases (in parallel). – Tracking security breaches or network usage requires accurate timestamps in logs. – Used in electric power systems (fault recorders, billing meters, etc.). – Necessary in telecommunication networks. – Global Navigation Satellite Systems (GNSS), such as GPS, requires very accurate clock synchronization for position calculations. TU-artikkel : GPS mer enn bare navigasjon How good is a crystal oscillator (XO) ? • Interested in the long-term measurement stability and accuracy • Watch crystal oscillator: about 20 ppm, or worse – Error > 1.73 s in 24 hours (almost 1 minute drift in one month) • The accuracy can be improved using a: – Temperature compensated crystal oscillator (TCXO) – Oven controlled crystal oscillator (OCXO) • the oscillator is enclosed in a temperature controlled oven • Some DAQ card accuracy examples: – TCXO : 1 ppm – OCXO: 50 ppb Chip Scale Atomic Clock (CSAC) • Two orders of magnitude better accuracy than oven-controlled crystal oscillators (OCXOs). • Can keep track of the time if GPS-signals are lost (e.g. inside a building, or due to jamming). • Example: Microsemi CSAC – < 120 mW power consumption – < 17 cm3 volume – 35 g weight – two outputs; a 10 MHz square wave and 1 PPS (Pulse Per Second) The frequency of the TCXO is continuously – Maintains time-of-day (TOD) as a 32-bit compared and corrected to ground state hyperfine frequency of the cesium atoms, unsigned integer which is incremented contained in the “physics package”, which synchronously with the rising edge of the thereby improves the stability and 1 PPS output environmental sensitivity of the TCXO.
    [Show full text]
  • Product Support Notice © 2016 Avaya Inc
    Product Support Notice © 2016 Avaya Inc. All Rights Reserved. PSN # PSN004915u Original publication date: 23-Dec-16. This is Issue #01, published date: 23-Dec-16. Severity/ Medium Urgency When convenient risk level Name of problem Leap second issue with Avaya Meeting Exchange Products affected Avaya Meeting Exchange Audio Bridge (S6200) Avaya Meeting Exchange Web Portal Problem description A leap second insertion to the Coordinated Universal Time (UTC) shall occur on December 31, 2016 at 23:59:60 UTC. There are possible known issues in Red Hat Enterprise Linux due to Leap Second adjustments. For servers running Bridge or Web Portal synchronized to Network Time Protocol (NTP) servers, when Leap Second occurs the RHEL kernel will print a message to the system log. Depending on the version of RHEL kernel, there is a chance the printing of this message could cause the kernel to crash. For additional information see the following RHEL Leap Second KB article: https://access.redhat.com/articles/15145. Resolution Releases 5.2 and lower are End of Manufacturer Support (EOMS) and therefore only covered by the information provided in the Workaround or alternative remediation section of this document. Note: 1. Only 5.2.x and earlier software versions of Meeting Exchange are vulnerable to Leap second issue. 2. In rare instances, insertion of a Leap Second can cause a system to hang or high CPU usage. These issues are documented in the RHEL Leap Second KB article: https://access.redhat.com/articles/15145 Refer to the following chart for actions recommended, the workaround column suggests any actions required.
    [Show full text]
  • Relativity in the Global Positioning System
    Relativity in the Global Positioning System Neil Ashby Dept. of Physics, University of Colorado Boulder, CO 80309–0390 U.S.A. [email protected] http://physics.colorado.edu/faculty/ashby_n.html Published on 28 January 2003 www.livingreviews.org/Articles/Volume6/2003-1ashby Living Reviews in Relativity Published by the Max Planck Institute for Gravitational Physics Albert Einstein Institute, Germany Abstract The Global Positioning System (GPS) uses accurate, stable atomic clocks in satellites and on the ground to provide world-wide position and time determination. These clocks have gravitational and motional fre- quency shifts which are so large that, without carefully accounting for numerous relativistic effects, the system would not work. This paper dis- cusses the conceptual basis, founded on special and general relativity, for navigation using GPS. Relativistic principles and effects which must be considered include the constancy of the speed of light, the equivalence principle, the Sagnac effect, time dilation, gravitational frequency shifts, and relativity of synchronization. Experimental tests of relativity ob- tained with a GPS receiver aboard the TOPEX/POSEIDON satellite will be discussed. Recently frequency jumps arising from satellite orbit adjust- ments have been identified as relativistic effects. These will be explained and some interesting applications of GPS will be discussed. c 2003 Max-Planck-Gesellschaft and the authors. Further information on copyright is given at http://www.livingreviews.org/Info/Copyright/. For permission to reproduce the article please contact [email protected]. Article Amendments On author request a Living Reviews article can be amended to include errata and small additions to ensure that the most accurate and up-to-date informa- tion possible is provided.
    [Show full text]