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NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
1 | P a g e
A Model for Correction Factors in GPS Signals
Mr. K. R. Desai
Department of Electronics, B.V.C.O.E, Kolhapur, India
Dr. R. H. Chile
Department of Instrumentation, S.G.G.S.C.O.E, Nanded, India
Dr. S. R. Sawant
Department of Technology, Shivaji University, Kolhapur, India
Abstract
The earth’s ionosphere acts as a perturbing medium on satellite-based navigational systems like GPS.
Variations in the ionosphere due to weather conditions caused by solar flares and coronal mass ejection can
scatter Trans - Ionosphere radio signals producing fluctuations in both amplitude and phase and GPS cycle
slips disrupting satellite communications and navigation. The ionosphere delay is one of the fundamental
reasons for inaccuracy in GPS positioning and routing. The Total Electron Content (TEC) along the radio
wave path from a GPS satellite to the ground receiver is directly proportional to the ionosphere delay. This
paper proposes a method allowing to calculate the TEC with a correctness of about 2–3 TECU and to sense
Travelling Ionosphere Disturbances using GPS measurements.
Index Terms— Epoch, GPS, Ionosphere, Satellite, TEC.
Introduction
Under the name of GPS, the compact radio navigation receivers have proliferated in the civilian market
place from past several years. The position calculated by a GPS receiver requires the current time, the
position of the satellite and the measured delay of the received signal and then by using the triangulation
rule the position of the receiver is determined.
The large sources of error in GPS are produced by the atmospheric effect (ionospheric, tropospheric), clock
errors of the satellite, multipath effect, satellite orbits errors and calculation-rounding errors. The satellite
signal slows as it passes through the atmosphere. The GPS framework utilizes an inherent model that
computes a normal measure of delay to in part right for this sort of mistake. Receiver’s inherent
timekeepers are not exact as the atomic clocks installed the GPS satellite. Along these lines, it may have
extremely slight timing errors. GPS error is a combo of clamor, inclination, and botches. Clamor mistakes
are the consolidated impact of PRN code disorder (around 1 meter) and clamor inside the receiver disorder
(around 1 meter). Inclination mistakes are the deliberate corruption of the SPS motions by a period shifting
inclination [1]. The primary goal of this work is to process the error correction factors in the GPS signals
and to create the information handling programming module to satisfy necessities. In this paper GPS
information is prepared and diagram is computed utilizing MATLAB tool. For this GPS equipmental setup
is carried out. A dual frequency GPS receiver can wipe out (to the first order) the ionospheric delay through
a direct mix of L1 and L2 observables [2]. The vast majority of the civilians utilizes low-cost single
frequency GPS receivers that can't utilize this alternative. Henceforth for precise navigation differential
GPS is chosen. Investigation of GPS position error and correcting method is done.
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
2 | P a g e
THE EFFECT OF SPHERES ON GPS SIGNAL
As radio signal pass through ionosphere and troposphere, they slow down based on the density of
atmosphere and they can be modeled as a bent path as in Fig. 2.1.
Figure 1 GPS signal distorted by spheres.
The Charged particles in the Ionosphere expel vitality from radio waves. Non – Uniform Electron thickness
alters course of propagation. The bearer stage is progressed and balance stage is impeded. The polarization
is rotated because of Faradays rotation. Ionosphere and Ionosphere Delays – The satellite Signal passes
through the atmosphere because of ionosphere changes generates delay [3]. Receiver Clock Errors –
Receiver Build in Clock is not exact as that of atomic clock. Orbital Error - Inaccuracy of the satellites
reported Locations. Geographic latitude, longitude, local time, season, geomagnetic activity and viewing
direction are the factors which decide the TEC [4] and it can be estimated by forming the linear
combination of the GPS measurement on L1 and L2 frequencies, either by using GPS carrier phase
or pseudo-ranges observables. The ionosphere compels the most unfavorable results for the radio wave
passing through it. Dispersive nature of the ionosphere and usage of two frequencies in GPS facilitate
estimation of ionospheric TEC which is a basic parameter in the examination of L-Band correspondence.
Rate of TEC (ROT) from GPS can illustrate the features of the ionospheric glimmers. Very irritated
ionosphere can result in cycle slips in GPS information. Very good correlation is found between the
ionospheric scintillations and the number of cycle slips in GPS data.
GPS EQUIPMENTAL SET-UP
The collector gear comprises of a receiving antenna, an accepting unit, a processor, a data/ yield gadget and
a force supply indicated in Fig.3.1. GPS receiving antenna can be single frequency or double frequency
receiving antenna. The physical configuration of the radio antenna can vary from helical to micro strip.
There are number of variables that need to be considered for receiving antenna choice, for example, radio
gain, mounting area, multipath execution, and stability of the electrical stage censer of the radio wire [5].
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
3 | P a g e
Fig. 2 Overview of research work
GPS receivers can either track only C/A codes or both C/A and P(Y) codes. Most receivers have multiple
channels, where each channel tracks transmission from a single satellite. There can be a most extreme of 12
such channels. The receiving unit forwards the signals to the processor. The processor performs position,
velocity, and time estimation from the signals received from the receiving unit. The processor is
responsible for issuing commands to the receiving and input/output units.
The I/O device acts as an interface between the receiver equipment and other user equipment. By and large
the I/O devices is a basic showcase unit that shows the immediate position while in configurations where
the GPS is used along with other sensors, the interface could be a RS- 232, RS-422 or ARINC 429.
The power supply could be either external or integrated into the receiver. It may even be a combination of
both. Typically, alkaline or lithium batteries are used for integrated power supplies while external supplies
are generally AC adapters.
GRAPHICAL REPRESENTATION OF ERROR PROCESSED IN IONOSPHERE
All the data interpreted is taken from Indian Institute of Geomagnetism, Shivaji University, Kolhapur from
LICA Receiver.
The system designed has following objectives:
• Extraction of alpha, beta, GPS coordinates and GPS time for a epoch
• Evaluation of errors contributed by Ionosphere, Troposphere and satellite clock error is to be done.
To understand the system working, it needs to follow the steps mentioned in block diagram Fig. 3
Keeping the alpha, beta, GPS coordinates and GPS time available from ephemeris table as a reference, the
drifts in the values for known epochs has to be calculated. The meaning of drifts in the value is the delays
introduced by Ionosphere, troposphere and also the offset error in satellite clock values.
As per the diagram Ionosphere error model consists of evaluation of Slant delay using vertical delay at the
Ionosphere Pierce Point (IPP) [6]. Knowing the value of nα the Earth centered angle ϕ and hence φ the
geomagnetic latitude of the IPP can be calculated using Klobuchar algorithm.
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
4 | P a g e
Fig. 3 Overview of research work
Epoch Signal Information
An epoch means an instant in time chosen as the origin of a particular era .The "epoch" then serves as a
reference point from which time is measured. Time measurement units are counted from the epoch so that
the date and time of events can be specified unambiguously. The epoch moment or date is usually defined
by a specific clear event, condition, or criteria— the epoch event or epoch criteria —from which the period
or era or age is usually characterized or described.
The orbit Epoch indicates the time at which the satellite's position, orbit orientation and orbit shape were
last known. Knowing the satellite's position and the orbit orientation alone is not enough to know
the satellite's future position. It is also necessary to know WHEN the satellite's orbit was last known
accurately.
A two-line element set (TLE) is a data format used to convey sets of orbital elements that describe the
orbits of Earth-orbiting satellites. The determination of Epoch for a particular day is understood using a toy
example given in Fig.
Clock Bias, drift and drift rate
The estimation of the satellite ephemeris is explicitly determined as the GPS satellite clock bias, drift and
drift-rate. The offset, drift and drift-rate of the satellite clocks are available to all GPS users as clock error
coefficients broadcast in the Navigation Message. The behavior of each GPS satellite clock is monitored
with respect to GPS Time, as maintained by an ensemble of atomic clocks at the GPS Master Control
Station in Colorado Springs.
Starting with 50.28438588 days (Days = 50)
50.28438588 days - 50 = 0.28438588 days
0.28438588 days x 24 hours/day = 6.8253 hours (Hours = 6)
6.8253 hours - 6 = 0.8253 hours
0.8253 hours x 60 minutes/hour = 49.5157 minutes (Minutes = 49)
49.5157 - 49 = 0.5157 minutes
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
5 | P a g e
0.5157 minutes x 60 seconds/minute = 30.94 seconds (Seconds = 30.94)
In the algorithm shown in fig. 4, ‘.05o’ file is used which is extracted by processing ‘.dat’ file in Trimble
rinexe converter software, from set of receivers database of recordings. In this ‘.05o’ observation file’s
header, GPS time, alpha and beta parameters are recorded. These parameters are stored in ‘.mat’ file for
further use and for easy and fast processing. After header segment, epochs are recorded in observation file.
Each segment of epochs is recorded by number of satellites available. The number of available satellites,
out of total 32 satellites, is also indicated in starting string of each epoch segment. These epochs with
respect to their time of recording and with respect to their satellite number are extracted and stored as an
array in the same ‘.mat’ file for further use.
Epochs obtained here contains errors in terms of clock cycle shift and also posses’ impact of earth’s
atmospheric layers, which ultimately depends on solar activities. These changes can be observed and mean
position of receiver can be calculated on the basis of epochs.
From the data sets of Quiet and disturbed days epochs have been obtained. Using these, mean position of
the receiver have been calculated. Fig 3 shows the plot of receivers position for Quiet day. Fig 4 shows the
plot of receivers position for disturbed day.
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
6 | P a g e
Fig 4 Flow chart for processing observation File Quiet Day (6th
Sept., 2005) signal Data output
Fig 5: Receiver position over time Disturbed day (7th
Sept., 2005) signal Data output
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
7 | P a g e
Fig 6: Receiver position over time disturbed day signal Data output
1. The graph of X, Y and Z coordinates variations indicates the impact on epochs recorded due to changes
in earth’s atmospheric layer. The deviations from x-axis indicate deviations obtained in receivers position.
2. In case of Quiet day 6th
September 2005 receiver position is not so affected that is why very little
deviations have been observed.
3. In Case of disturbed day 7th
September 2005 deviations in X, Y and Z coordinates of receiver position
appear to be significant due to impact of Ionosperic and tropospheric impacts.
A. Calculation of ionosphere error for normal day
X-Co-ordinate ionosphere error initially starts to increase from a negative value and crosses zero level. It
then increases in more fraction amount. At an instant it gradually reduces to an intermediate fraction value.
Further it approaches approximately 0.5 values very slowly. Now it suddenly falls to -1 and after -1 it tries
approaching zero level and further some positive value Y & Z co-ordinates show similar fluctuations at
different interval which is calculated by Fig. 7
Sequence of satellites connected to the receiver dependent on signal strength and line of site basis hence
epoch of first satellite forms the basis of detection in position. Connected satellites are at distance and may
involve more delays in connections. But on disturbed days satellites connected initially also posses more
errors in position and are observed in processing of quiet and disturbed days data sets. Ionospheric errors
are detected for satellite position error.
INTERNATIONAL JOURNAL OF INNOVATIONS IN
Fig 7 : Flow chart for ionospheric error detection using Klobuchar method
1. Satellites positions are calculated from
Ionosperic delays in received signal.
2. Klobuchar equation is used for detecting these Ionosperic effects and errors are indicated in figure 1
and figure 3 for quiet and disturbed day respectively.
3. Figure 4.1 indicates the error in satellite position in meters for some of satellites. X
ionosphere error initially starts to increase from a negative value and crosses zero level. It then
increases in more fraction amount. At an instant it gradually r
value.
4. Figure 1 shows many irregularities around zero level. X
suddenly falls sharply at particular points. From there it rises suddenly, approaches zero and
gradually falls again at nearly. It continues to fall gradually and finally reaches at negative level.
Similarly Y co-ordinates, Z co
gradually.
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
VOLUME 2, ISSUE 3 MARCH2015
Flow chart for ionospheric error detection using Klobuchar method
Satellites positions are calculated from epochs. The coordinates calculated posses effect of
Ionosperic delays in received signal.
Klobuchar equation is used for detecting these Ionosperic effects and errors are indicated in figure 1
and figure 3 for quiet and disturbed day respectively.
.1 indicates the error in satellite position in meters for some of satellites. X
ionosphere error initially starts to increase from a negative value and crosses zero level. It then
increases in more fraction amount. At an instant it gradually reduces to an intermediate fraction
Figure 1 shows many irregularities around zero level. X-co-ordinate is initially at zero level, but it
suddenly falls sharply at particular points. From there it rises suddenly, approaches zero and
again at nearly. It continues to fall gradually and finally reaches at negative level.
ordinates, Z co-ordinates show complex fluctuations Y
NOVATEUR PUBLICATIONS
ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
8 | P a g e
Flow chart for ionospheric error detection using Klobuchar method
epochs. The coordinates calculated posses effect of
Klobuchar equation is used for detecting these Ionosperic effects and errors are indicated in figure 1
.1 indicates the error in satellite position in meters for some of satellites. X-Co-ordinate
ionosphere error initially starts to increase from a negative value and crosses zero level. It then
educes to an intermediate fraction
ordinate is initially at zero level, but it
suddenly falls sharply at particular points. From there it rises suddenly, approaches zero and
again at nearly. It continues to fall gradually and finally reaches at negative level.
ordinates show complex fluctuations Y-co-ordinate moves
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
9 | P a g e
Fig. 4 Two line element set coordinate system
Where F = Slant Factor
߶௠ = Geometric Latitude
Fig. 4 Ionosphere error for normal day
B. Calculation of ionosphere error for abnormal day
Fig. 5 Ionosphere error for abnormal day
The graph is quite self explanatory. It shows many irregularities around zero level. X-co-ordinate is initially
at zero level, but it suddenly falls sharply at -2.5. From there it rises suddenly, approaches zero and
gradually falls again at nearly -0.2.
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
10 | P a g e
It continues to fall gradually and finally reaches -3. Similarly Y co-ordinates, Z co-ordinates show complex
fluctuations Y-co-ordinate gradually moves from -1.5 and ascends to 2.5. It then falls linearly to -3.2 and
again increases to 0.4. Z co-ordinate declines down continuously from 2.2 to -0.9 and finally step by step
approaches -1.2 values.
SIGNIFICANCE OF RESEARCH WORK
There are numerous purposes behind error correction factors considered in GPS signal however some
major point that influence the GPS signal altogether are clarified as follows (1) GPS errors are combination
of noise, bias and blunders. (2) Noise errors are the consolidated impact of PRN code noise (around 1
meter) and noise inside the receiver noise (around 1 meter). (3) Selective Ability (SA) is the intentional
degradation of the SPS signals by a time varying bias. SA is controlled by the DOD to farthest point
precision for non-U. S. military and government clients. The potential exactness of the C/A code of around
30 meters is reduced to 100 meters (two standard deviations). The SA bias on each one satellite signal is
diffrent, along these lines the ensuing position arrangement is a capacity of the consolidated SA inclination
from every SV utilized as a part of the route arrangement [7]. Since SA is a changing predisposition with
low recurrence terms in overabundance of a couple of hours, position arrangements alternately individual
SV pseudo-ranges can't be viably found the middle value of over periods shorter than a couple of hours.
Differential revisions must be redesigned at a rate short of what the relationship time of SA (and different
inclination blunders). (4) Troposphere defers: 1 meter. The troposphere is the lower part (ground level to
from 8 to 13 km) of the environment that encounters the changes in temperature, weight, and moistness
connected with climate changes [8]. Complex models of Troposphere deferral oblige evaluations or
estimations of these parameters. (5) Ionospheres defers: 10 meters. The ionosphere is the layer of the
environment from 50 to 500 km that comprises of ionized air. The transmitted model can just evacuate
about a large portion of the conceivable 70 ns of deferral leaving a ten meter unmodelled lingering.
FUTURE SCOPE
The results obtained so far are simulation dependent. Also error detection and corrections are post
processing dependent. The simulation results have shown considerable error correction capabilities in post
processing. These algorithms of error correction can be implemented with valid real time error detection
and correction capabilities and experimentations and can be implemented in hardware of receivers, where
errors will be corrected while writing data itself in real time.
CONCLUSION
The signals from the GPS Satellites will be picked up by receiving antenna. The GPS receiver might
contain the inbuilt information recording and storage facility however this recorded information again
reformatted and transferred in the PC (for case Navigation and Observation Data). This information
contains all the terms of the navigational and observational structures of the guidelines utilized as a part of
the GPS framework. The computational assignment for the algorithm and software for information
handling will be executed. At long last the obtained results will be investigated and the execution of the
framework will be observed. The computed error correction factors may be used to rectify different GPS
parameters which will be useful to acquire the error free corrected GPS information.
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 3 MARCH2015
11 | P a g e
REFERENCES
[1] A. D. Sharma ‘Ionospheric Time Delay Variation Over Low Lattitude Station at Hyderabad’ osmania
University, Hydrabad.
[2] Lao-Sheng LIN. ‘Quality Control Issues on Real-time Estimation of Ionospheric Delay Using GPS
Measurements’. Taipei ACRS (2002)
[3] Norbert Jakowski, Leitinger R., Ciraolo L. ‘Behaviour of Large Scale Structures of the Electron
Content as a Key Parameter for Range Errors in GNSS Applications’. INGV 2004, 47(2/3)
[4] Ren´e Warnant and Eric Pottiaux. ‘The increase of the ionospheric activity as measured by GPS’. Earth
Planets Space(2000), 52, 1055–1060
[5] Filjar, R.; Kos, T.; Markezic, I. ‘GPS Ionospheric Error Correction Models’Multimedia Signal
Processing and Communications, 48th International Symposium
[6] A. Araujo-Pradere. ‘GPS-derived total electron content response for the Bastille Day magnetic Storm of
2000 at a low mid-latitude station’. Geofísica Internacional (2005), Vol. 44, Num. 2, pp. 211-218.
[7] Bracewell, R. N., K. G. Budden, J. A. Radcliffe, T. W. Straker,and K. Weekes, ‘The ionospheric
propagation of long and very long radio waves over distances less than 1000 km, Proc. Instn. Elect.
Engrs.,98,p. 221,1951. E. Yizengaw and E. A. Essex, Dept. of Physics Brook, M.,N. Kitagawa, and E. J.
Workman, ‘Use of GPS Study Total Electron Content of the Ionosphere during the Geomagnetic Storm on
22 September.
[8] Michael A. Lombardi, Lisa M. Nelson, Andrew N. Novick, Victor S. Zhang, “Time and Frequency
Measurements Using the Global Positioning System” presented at the Measurement Science Conference,
January 2001.
[9] Vsevolod B. Ivanov, Oleg A. Gorbachev, Dmitry.V. Khazanov, Andrey A.Kholmogorov, “Some
Peculiarities of Positioning in Satellite Radio Navigation Systems” Apr. 2013, Vol. 2 Iss. 2, PP. 96-100.
[10]Ryan Monaghan,“GPS Satellite Position Estimation from
Ephemeris Data by Minimum Mean Square Error
Filtering Under Conditions of Selective
Availability” IEEE March 13th, 2006.

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GPS signal correction factors

  • 1. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 1 | P a g e A Model for Correction Factors in GPS Signals Mr. K. R. Desai Department of Electronics, B.V.C.O.E, Kolhapur, India Dr. R. H. Chile Department of Instrumentation, S.G.G.S.C.O.E, Nanded, India Dr. S. R. Sawant Department of Technology, Shivaji University, Kolhapur, India Abstract The earth’s ionosphere acts as a perturbing medium on satellite-based navigational systems like GPS. Variations in the ionosphere due to weather conditions caused by solar flares and coronal mass ejection can scatter Trans - Ionosphere radio signals producing fluctuations in both amplitude and phase and GPS cycle slips disrupting satellite communications and navigation. The ionosphere delay is one of the fundamental reasons for inaccuracy in GPS positioning and routing. The Total Electron Content (TEC) along the radio wave path from a GPS satellite to the ground receiver is directly proportional to the ionosphere delay. This paper proposes a method allowing to calculate the TEC with a correctness of about 2–3 TECU and to sense Travelling Ionosphere Disturbances using GPS measurements. Index Terms— Epoch, GPS, Ionosphere, Satellite, TEC. Introduction Under the name of GPS, the compact radio navigation receivers have proliferated in the civilian market place from past several years. The position calculated by a GPS receiver requires the current time, the position of the satellite and the measured delay of the received signal and then by using the triangulation rule the position of the receiver is determined. The large sources of error in GPS are produced by the atmospheric effect (ionospheric, tropospheric), clock errors of the satellite, multipath effect, satellite orbits errors and calculation-rounding errors. The satellite signal slows as it passes through the atmosphere. The GPS framework utilizes an inherent model that computes a normal measure of delay to in part right for this sort of mistake. Receiver’s inherent timekeepers are not exact as the atomic clocks installed the GPS satellite. Along these lines, it may have extremely slight timing errors. GPS error is a combo of clamor, inclination, and botches. Clamor mistakes are the consolidated impact of PRN code disorder (around 1 meter) and clamor inside the receiver disorder (around 1 meter). Inclination mistakes are the deliberate corruption of the SPS motions by a period shifting inclination [1]. The primary goal of this work is to process the error correction factors in the GPS signals and to create the information handling programming module to satisfy necessities. In this paper GPS information is prepared and diagram is computed utilizing MATLAB tool. For this GPS equipmental setup is carried out. A dual frequency GPS receiver can wipe out (to the first order) the ionospheric delay through a direct mix of L1 and L2 observables [2]. The vast majority of the civilians utilizes low-cost single frequency GPS receivers that can't utilize this alternative. Henceforth for precise navigation differential GPS is chosen. Investigation of GPS position error and correcting method is done.
  • 2. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 2 | P a g e THE EFFECT OF SPHERES ON GPS SIGNAL As radio signal pass through ionosphere and troposphere, they slow down based on the density of atmosphere and they can be modeled as a bent path as in Fig. 2.1. Figure 1 GPS signal distorted by spheres. The Charged particles in the Ionosphere expel vitality from radio waves. Non – Uniform Electron thickness alters course of propagation. The bearer stage is progressed and balance stage is impeded. The polarization is rotated because of Faradays rotation. Ionosphere and Ionosphere Delays – The satellite Signal passes through the atmosphere because of ionosphere changes generates delay [3]. Receiver Clock Errors – Receiver Build in Clock is not exact as that of atomic clock. Orbital Error - Inaccuracy of the satellites reported Locations. Geographic latitude, longitude, local time, season, geomagnetic activity and viewing direction are the factors which decide the TEC [4] and it can be estimated by forming the linear combination of the GPS measurement on L1 and L2 frequencies, either by using GPS carrier phase or pseudo-ranges observables. The ionosphere compels the most unfavorable results for the radio wave passing through it. Dispersive nature of the ionosphere and usage of two frequencies in GPS facilitate estimation of ionospheric TEC which is a basic parameter in the examination of L-Band correspondence. Rate of TEC (ROT) from GPS can illustrate the features of the ionospheric glimmers. Very irritated ionosphere can result in cycle slips in GPS information. Very good correlation is found between the ionospheric scintillations and the number of cycle slips in GPS data. GPS EQUIPMENTAL SET-UP The collector gear comprises of a receiving antenna, an accepting unit, a processor, a data/ yield gadget and a force supply indicated in Fig.3.1. GPS receiving antenna can be single frequency or double frequency receiving antenna. The physical configuration of the radio antenna can vary from helical to micro strip. There are number of variables that need to be considered for receiving antenna choice, for example, radio gain, mounting area, multipath execution, and stability of the electrical stage censer of the radio wire [5].
  • 3. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 3 | P a g e Fig. 2 Overview of research work GPS receivers can either track only C/A codes or both C/A and P(Y) codes. Most receivers have multiple channels, where each channel tracks transmission from a single satellite. There can be a most extreme of 12 such channels. The receiving unit forwards the signals to the processor. The processor performs position, velocity, and time estimation from the signals received from the receiving unit. The processor is responsible for issuing commands to the receiving and input/output units. The I/O device acts as an interface between the receiver equipment and other user equipment. By and large the I/O devices is a basic showcase unit that shows the immediate position while in configurations where the GPS is used along with other sensors, the interface could be a RS- 232, RS-422 or ARINC 429. The power supply could be either external or integrated into the receiver. It may even be a combination of both. Typically, alkaline or lithium batteries are used for integrated power supplies while external supplies are generally AC adapters. GRAPHICAL REPRESENTATION OF ERROR PROCESSED IN IONOSPHERE All the data interpreted is taken from Indian Institute of Geomagnetism, Shivaji University, Kolhapur from LICA Receiver. The system designed has following objectives: • Extraction of alpha, beta, GPS coordinates and GPS time for a epoch • Evaluation of errors contributed by Ionosphere, Troposphere and satellite clock error is to be done. To understand the system working, it needs to follow the steps mentioned in block diagram Fig. 3 Keeping the alpha, beta, GPS coordinates and GPS time available from ephemeris table as a reference, the drifts in the values for known epochs has to be calculated. The meaning of drifts in the value is the delays introduced by Ionosphere, troposphere and also the offset error in satellite clock values. As per the diagram Ionosphere error model consists of evaluation of Slant delay using vertical delay at the Ionosphere Pierce Point (IPP) [6]. Knowing the value of nα the Earth centered angle ϕ and hence φ the geomagnetic latitude of the IPP can be calculated using Klobuchar algorithm.
  • 4. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 4 | P a g e Fig. 3 Overview of research work Epoch Signal Information An epoch means an instant in time chosen as the origin of a particular era .The "epoch" then serves as a reference point from which time is measured. Time measurement units are counted from the epoch so that the date and time of events can be specified unambiguously. The epoch moment or date is usually defined by a specific clear event, condition, or criteria— the epoch event or epoch criteria —from which the period or era or age is usually characterized or described. The orbit Epoch indicates the time at which the satellite's position, orbit orientation and orbit shape were last known. Knowing the satellite's position and the orbit orientation alone is not enough to know the satellite's future position. It is also necessary to know WHEN the satellite's orbit was last known accurately. A two-line element set (TLE) is a data format used to convey sets of orbital elements that describe the orbits of Earth-orbiting satellites. The determination of Epoch for a particular day is understood using a toy example given in Fig. Clock Bias, drift and drift rate The estimation of the satellite ephemeris is explicitly determined as the GPS satellite clock bias, drift and drift-rate. The offset, drift and drift-rate of the satellite clocks are available to all GPS users as clock error coefficients broadcast in the Navigation Message. The behavior of each GPS satellite clock is monitored with respect to GPS Time, as maintained by an ensemble of atomic clocks at the GPS Master Control Station in Colorado Springs. Starting with 50.28438588 days (Days = 50) 50.28438588 days - 50 = 0.28438588 days 0.28438588 days x 24 hours/day = 6.8253 hours (Hours = 6) 6.8253 hours - 6 = 0.8253 hours 0.8253 hours x 60 minutes/hour = 49.5157 minutes (Minutes = 49) 49.5157 - 49 = 0.5157 minutes
  • 5. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 5 | P a g e 0.5157 minutes x 60 seconds/minute = 30.94 seconds (Seconds = 30.94) In the algorithm shown in fig. 4, ‘.05o’ file is used which is extracted by processing ‘.dat’ file in Trimble rinexe converter software, from set of receivers database of recordings. In this ‘.05o’ observation file’s header, GPS time, alpha and beta parameters are recorded. These parameters are stored in ‘.mat’ file for further use and for easy and fast processing. After header segment, epochs are recorded in observation file. Each segment of epochs is recorded by number of satellites available. The number of available satellites, out of total 32 satellites, is also indicated in starting string of each epoch segment. These epochs with respect to their time of recording and with respect to their satellite number are extracted and stored as an array in the same ‘.mat’ file for further use. Epochs obtained here contains errors in terms of clock cycle shift and also posses’ impact of earth’s atmospheric layers, which ultimately depends on solar activities. These changes can be observed and mean position of receiver can be calculated on the basis of epochs. From the data sets of Quiet and disturbed days epochs have been obtained. Using these, mean position of the receiver have been calculated. Fig 3 shows the plot of receivers position for Quiet day. Fig 4 shows the plot of receivers position for disturbed day.
  • 6. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 6 | P a g e Fig 4 Flow chart for processing observation File Quiet Day (6th Sept., 2005) signal Data output Fig 5: Receiver position over time Disturbed day (7th Sept., 2005) signal Data output
  • 7. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 7 | P a g e Fig 6: Receiver position over time disturbed day signal Data output 1. The graph of X, Y and Z coordinates variations indicates the impact on epochs recorded due to changes in earth’s atmospheric layer. The deviations from x-axis indicate deviations obtained in receivers position. 2. In case of Quiet day 6th September 2005 receiver position is not so affected that is why very little deviations have been observed. 3. In Case of disturbed day 7th September 2005 deviations in X, Y and Z coordinates of receiver position appear to be significant due to impact of Ionosperic and tropospheric impacts. A. Calculation of ionosphere error for normal day X-Co-ordinate ionosphere error initially starts to increase from a negative value and crosses zero level. It then increases in more fraction amount. At an instant it gradually reduces to an intermediate fraction value. Further it approaches approximately 0.5 values very slowly. Now it suddenly falls to -1 and after -1 it tries approaching zero level and further some positive value Y & Z co-ordinates show similar fluctuations at different interval which is calculated by Fig. 7 Sequence of satellites connected to the receiver dependent on signal strength and line of site basis hence epoch of first satellite forms the basis of detection in position. Connected satellites are at distance and may involve more delays in connections. But on disturbed days satellites connected initially also posses more errors in position and are observed in processing of quiet and disturbed days data sets. Ionospheric errors are detected for satellite position error.
  • 8. INTERNATIONAL JOURNAL OF INNOVATIONS IN Fig 7 : Flow chart for ionospheric error detection using Klobuchar method 1. Satellites positions are calculated from Ionosperic delays in received signal. 2. Klobuchar equation is used for detecting these Ionosperic effects and errors are indicated in figure 1 and figure 3 for quiet and disturbed day respectively. 3. Figure 4.1 indicates the error in satellite position in meters for some of satellites. X ionosphere error initially starts to increase from a negative value and crosses zero level. It then increases in more fraction amount. At an instant it gradually r value. 4. Figure 1 shows many irregularities around zero level. X suddenly falls sharply at particular points. From there it rises suddenly, approaches zero and gradually falls again at nearly. It continues to fall gradually and finally reaches at negative level. Similarly Y co-ordinates, Z co gradually. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] VOLUME 2, ISSUE 3 MARCH2015 Flow chart for ionospheric error detection using Klobuchar method Satellites positions are calculated from epochs. The coordinates calculated posses effect of Ionosperic delays in received signal. Klobuchar equation is used for detecting these Ionosperic effects and errors are indicated in figure 1 and figure 3 for quiet and disturbed day respectively. .1 indicates the error in satellite position in meters for some of satellites. X ionosphere error initially starts to increase from a negative value and crosses zero level. It then increases in more fraction amount. At an instant it gradually reduces to an intermediate fraction Figure 1 shows many irregularities around zero level. X-co-ordinate is initially at zero level, but it suddenly falls sharply at particular points. From there it rises suddenly, approaches zero and again at nearly. It continues to fall gradually and finally reaches at negative level. ordinates, Z co-ordinates show complex fluctuations Y NOVATEUR PUBLICATIONS ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 8 | P a g e Flow chart for ionospheric error detection using Klobuchar method epochs. The coordinates calculated posses effect of Klobuchar equation is used for detecting these Ionosperic effects and errors are indicated in figure 1 .1 indicates the error in satellite position in meters for some of satellites. X-Co-ordinate ionosphere error initially starts to increase from a negative value and crosses zero level. It then educes to an intermediate fraction ordinate is initially at zero level, but it suddenly falls sharply at particular points. From there it rises suddenly, approaches zero and again at nearly. It continues to fall gradually and finally reaches at negative level. ordinates show complex fluctuations Y-co-ordinate moves
  • 9. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 9 | P a g e Fig. 4 Two line element set coordinate system Where F = Slant Factor ߶௠ = Geometric Latitude Fig. 4 Ionosphere error for normal day B. Calculation of ionosphere error for abnormal day Fig. 5 Ionosphere error for abnormal day The graph is quite self explanatory. It shows many irregularities around zero level. X-co-ordinate is initially at zero level, but it suddenly falls sharply at -2.5. From there it rises suddenly, approaches zero and gradually falls again at nearly -0.2.
  • 10. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 10 | P a g e It continues to fall gradually and finally reaches -3. Similarly Y co-ordinates, Z co-ordinates show complex fluctuations Y-co-ordinate gradually moves from -1.5 and ascends to 2.5. It then falls linearly to -3.2 and again increases to 0.4. Z co-ordinate declines down continuously from 2.2 to -0.9 and finally step by step approaches -1.2 values. SIGNIFICANCE OF RESEARCH WORK There are numerous purposes behind error correction factors considered in GPS signal however some major point that influence the GPS signal altogether are clarified as follows (1) GPS errors are combination of noise, bias and blunders. (2) Noise errors are the consolidated impact of PRN code noise (around 1 meter) and noise inside the receiver noise (around 1 meter). (3) Selective Ability (SA) is the intentional degradation of the SPS signals by a time varying bias. SA is controlled by the DOD to farthest point precision for non-U. S. military and government clients. The potential exactness of the C/A code of around 30 meters is reduced to 100 meters (two standard deviations). The SA bias on each one satellite signal is diffrent, along these lines the ensuing position arrangement is a capacity of the consolidated SA inclination from every SV utilized as a part of the route arrangement [7]. Since SA is a changing predisposition with low recurrence terms in overabundance of a couple of hours, position arrangements alternately individual SV pseudo-ranges can't be viably found the middle value of over periods shorter than a couple of hours. Differential revisions must be redesigned at a rate short of what the relationship time of SA (and different inclination blunders). (4) Troposphere defers: 1 meter. The troposphere is the lower part (ground level to from 8 to 13 km) of the environment that encounters the changes in temperature, weight, and moistness connected with climate changes [8]. Complex models of Troposphere deferral oblige evaluations or estimations of these parameters. (5) Ionospheres defers: 10 meters. The ionosphere is the layer of the environment from 50 to 500 km that comprises of ionized air. The transmitted model can just evacuate about a large portion of the conceivable 70 ns of deferral leaving a ten meter unmodelled lingering. FUTURE SCOPE The results obtained so far are simulation dependent. Also error detection and corrections are post processing dependent. The simulation results have shown considerable error correction capabilities in post processing. These algorithms of error correction can be implemented with valid real time error detection and correction capabilities and experimentations and can be implemented in hardware of receivers, where errors will be corrected while writing data itself in real time. CONCLUSION The signals from the GPS Satellites will be picked up by receiving antenna. The GPS receiver might contain the inbuilt information recording and storage facility however this recorded information again reformatted and transferred in the PC (for case Navigation and Observation Data). This information contains all the terms of the navigational and observational structures of the guidelines utilized as a part of the GPS framework. The computational assignment for the algorithm and software for information handling will be executed. At long last the obtained results will be investigated and the execution of the framework will be observed. The computed error correction factors may be used to rectify different GPS parameters which will be useful to acquire the error free corrected GPS information.
  • 11. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 3 MARCH2015 11 | P a g e REFERENCES [1] A. D. Sharma ‘Ionospheric Time Delay Variation Over Low Lattitude Station at Hyderabad’ osmania University, Hydrabad. [2] Lao-Sheng LIN. ‘Quality Control Issues on Real-time Estimation of Ionospheric Delay Using GPS Measurements’. Taipei ACRS (2002) [3] Norbert Jakowski, Leitinger R., Ciraolo L. ‘Behaviour of Large Scale Structures of the Electron Content as a Key Parameter for Range Errors in GNSS Applications’. INGV 2004, 47(2/3) [4] Ren´e Warnant and Eric Pottiaux. ‘The increase of the ionospheric activity as measured by GPS’. Earth Planets Space(2000), 52, 1055–1060 [5] Filjar, R.; Kos, T.; Markezic, I. ‘GPS Ionospheric Error Correction Models’Multimedia Signal Processing and Communications, 48th International Symposium [6] A. Araujo-Pradere. ‘GPS-derived total electron content response for the Bastille Day magnetic Storm of 2000 at a low mid-latitude station’. Geofísica Internacional (2005), Vol. 44, Num. 2, pp. 211-218. [7] Bracewell, R. N., K. G. Budden, J. A. Radcliffe, T. W. Straker,and K. Weekes, ‘The ionospheric propagation of long and very long radio waves over distances less than 1000 km, Proc. Instn. Elect. Engrs.,98,p. 221,1951. E. Yizengaw and E. A. Essex, Dept. of Physics Brook, M.,N. Kitagawa, and E. J. Workman, ‘Use of GPS Study Total Electron Content of the Ionosphere during the Geomagnetic Storm on 22 September. [8] Michael A. Lombardi, Lisa M. Nelson, Andrew N. Novick, Victor S. Zhang, “Time and Frequency Measurements Using the Global Positioning System” presented at the Measurement Science Conference, January 2001. [9] Vsevolod B. Ivanov, Oleg A. Gorbachev, Dmitry.V. Khazanov, Andrey A.Kholmogorov, “Some Peculiarities of Positioning in Satellite Radio Navigation Systems” Apr. 2013, Vol. 2 Iss. 2, PP. 96-100. [10]Ryan Monaghan,“GPS Satellite Position Estimation from Ephemeris Data by Minimum Mean Square Error Filtering Under Conditions of Selective Availability” IEEE March 13th, 2006.