ILA 4-6 November 2003 Integrated GPS/Loran Sensor for Maritime Operations Wouter J. Pelgrum...
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Transcript of ILA 4-6 November 2003 Integrated GPS/Loran Sensor for Maritime Operations Wouter J. Pelgrum...
ILA 4-6 November 2003
Integrated GPS/Loran Sensor for Maritime Operations
Wouter J. Pelgrum
Reelektronika / Delft University of Technology / Gauss Research Foundation
ILA 2003 4-7 Nov 2003
Introduction
Two very challenging applications for LC
Aviation: The Seven Nines Maritime: The Eight to Twenty Meter
This presentation: Maritime- Focus on accuracy- Outline of error budget- Identification & elimination of potential threads
ILA 2003 4-7 Nov 2003
Loran-C TXGroundwave
+Skywave
+ Near Field + Antenna
Rx error
Error Budget
Loran-C TXGroundwave
+Skywave
+Skywave
Near Field + Antenna
Local O
bject
s
CWICRI
Local I
nterfe
rence
Equival
ent R
X nois
e+
CWI
CRI Local Objects
+
Antenna
Local InterferenceEquivalent RX noise
PFSF ASF
Groundwave
PFSF ASF
Tuning
E-fiel
d susc
eptib
ility
X-talk
Boat
Near Field
Ref S
tatio
n Erro
r
Rx errorSpatial decorrelation of Regional ASF
Loran-C TXGroundwave
+Skywave
+ Near Field + Antenna
+CWI
CRI Local Objects
+Local Interference
Equivalent RX noise
Rx error
ILA 2003 4-7 Nov 2003
H-field Antenna Design Issues
Why use a H-field antenna and not an E-field- ‘no’ P-static susceptibility- Less susceptible to near-field phenomena - no grounding needed- Low profile
H-field antenna challenges:- More difficult to make low-noise- Parasitic E-field susceptibility- Tuning- Cross-talk- Beam steering algorithm / 180 degrees phase ambiguity
ILA 2003 4-7 Nov 2003
Noise
Low effective height of an H-field antenna vs. E-field requires special attention to noise design
Given a well designed H-field antenna and the Loran-C coverage of the United States, the error due to H-field antenna noise is not (yet) a bottleneck in the total error-budget
ILA 2003 4-7 Nov 2003
+
-
Rotating a H-field antenna+
-
+-
LC 1
LC 2
We need 2 H-field antennas for an omni-directional radiation pattern
H-field antenna bias-errors are heading dependant So they are different for all tracked stations And therefore they degrade positioning accuracy
ILA 2003 4-7 Nov 2003
E-field Susceptibility
.
L
E
E
H
.
.
L
E
E
H
.
.
L
E
E
H
.
In the far field, the E-field has a 90 degrees, 120 pi relation with the H-field
Parasitic E-field pickup by a H-field antenna will result in a heading-dependant phase-error (range error)
H-f
ield
(S
dir
ect
)
E-field (SEfield)
Well designed shielding and/or balancing of the H-field antenna reduces the range error due to E-field susceptibility to the meter level
ILA 2003 4-7 Nov 2003
H-f
ield
(S
dir
ect
)
E-field (SEfield)
E-field Susceptibility (cont’d)
0.10
1.00
10.00
100.00
1000.00
0 10 20 30 40 50 60 70 80 90angle (degrees)
TO
A e
rro
r (m
ete
rs)
-25 dB
-30 dB
-40 dB
-50 dB
-60 dB
Single loop used up to 45 degrees. After that, the other loop effectively takes over
Maximum range errors of approximately 1 meter achievable with carefully designed shielding and / or balancing
Range error due to E-field susceptibility
ILA 2003 4-7 Nov 2003
H-field Antenna Tuning
Two modes of operation of H-field antennas: Resonance vs Wide-band+ Slightly better noise performance @ Q=3
+ Some off-band interference rejection
+ Anti-aliasing OK for Sigma-Delta ADCs
- Surrounding metal influences resonance freq- Temperature influence on resonance freq- Multiple LF-Rnav systems reception more difficult
Tuning / phase difference between antennas leads to a heading dependant error
ILA 2003 4-7 Nov 2003
Laptop (for monitoring,control & data recording)
‘7499Z’ (7499M + 45ms)
LORADD Loran-C receiver
signalout
Loran-C simulator
Std in
Std in
Sinle loop H-fieldrover antenna
Fixed single loop H-fieldreference antenna
NovAtel OEM4GPS receiver
1 PPS out
GPS Disciplined Rb Oscillator
10 MHz
1 PPS in
Channel 2
Channel 1
H-field Antenna Tuning Error Compensation
ILA 2003 4-7 Nov 2003
0 10 20 30 40 50 60 70 80 90
-12
-10
-8
-6
-4
-2
0
2
4
6
8
Time [minutes]
Dif
fere
nti
al
TD
[n
s]
7499M Double Difference Measurement
Not calibrated
0 10 20 30 40 50 60 70 80 90
-12
-10
-8
-6
-4
-2
0
2
4
6
8
Time [minutes]
Dif
fere
nti
al
TD
[n
s]
7499M Double Difference Measurement
Not calibrated
Calibrated
H-field Antenna Tuning Error Compensation (cont’d)
ILA 2003 4-7 Nov 2003
+
-
+-
+
-
+-
X-talk: Introduction
Xtalk causes a heading dependant error Solve Xtalk-problem by:
Prevent Xtalk by electrical and mechanical construction of the antenna
Measure Xtalk and apply feed-forward correction Auto-calibration by feed-back correction
ILA 2003 4-7 Nov 2003
X-talk: some formulas…
sin2
cos1
loop
loop
1sin2
2cos1
122
211
loopAGloop
loopAGloop
Heading Relative
antenna y x toantenna fromXtalk A
xantenna of Tuning & Gain
xy xG
Ideal dual loop H-field antenna response:
Approximation of actual dual loop H-field antenna response:
G1 & G2: Gain and tuning
mismatch
A21 & A12
Xtalk
Model of X-talk and Tuning
ILA 2003 4-7 Nov 2003
X-talk: Measurement of parameters (cont’d)
130
cm
The H-field antenna (yellow box) is rotated inside a measurement loop. The field at the centre of the loop is quite homogeneous due to the large diameter of the loop (1.30m)
Computer controlled antenna rotor
H-field antenna
Cross-section of measurement setup
Measurement Setup
ILA 2003 4-7 Nov 2003
0 50 100 150 200 250 300 350
0.5
1
1.5
2
2.5x 10
4 Measured Antenna Gain Response
ga
in
0 50 100 150 200 250 300 350
-2
0
2
4
Measured Antenna Phase Response
Heading (degrees)
Ph
as
e [
us
]
Capacitive coupling from antenna 1 to antenna 2
Measured Antenna Response
Antenna 1
Antenna 2
X-talk: Measurement of parameters (cont’d)
ILA 2003 4-7 Nov 2003
0 50 100 150 200 250 300 350
0.5
1
1.5
2
2.5x 10
4 Curve-Fitting to Antenna Gain Response
ga
in
0 50 100 150 200 250 300 350
-2
0
2
4
Curve-Fitting to Antenna Phase Response
Heading (degrees)
Ph
as
e [
us
]
Antenna 1
Antenna 2
1sin2
2cos1
122
211
loopAGloop
loopAGloop
Curve-Fitting to find antenna parametersG1, G2, A21 and A12
X-talk: Measurement of parameters (cont’d)
ILA 2003 4-7 Nov 2003
X-talk: Feed Forward Correction
0 50 100 150 200 250 300 3500
0.5
1
1.5
2
x 104 Corrected antenna gain
ga
in
0 50 100 150 200 250 300 350
-1
0
1
2
3
Corrected antenna Phase
Ph
as
e [
us
]
Heading (degrees)
signal
Feed-ForwardCorrection
usingG1,A21G2,A12
Digitized Antenna signals
Feed Forward Correction of Antenna
ILA 2003 4-7 Nov 2003
0 50 100 150 200 250 300 350-25
-20
-15
-10
-5
0
5
10
15
20
Phase response of Beam-Steered Antenna
Heading (degrees)
rang
e er
ror
[m]
Uncorrected
Corrected45 m
Comparison of Uncorrected and Feed-Forward Corrected Response after Beam-Steering
X-talk: Feed Forward Correction (cont’d)
ILA 2003 4-7 Nov 2003
50 100 150 200 250 300 350
-1
-0.5
0
0.5
1
Phase response of Beam-Steered Antenna
Heading (degrees)
ran
ge
err
or
[m]
Corrected
(zoomed in)
1.5 m
Comparison of Uncorrected and Feed-Forward Corrected Response after Beam-Steering
X-talk: Feed Forward Correction (cont’d)
ILA 2003 4-7 Nov 2003
Not Only The Antenna Matters…
Attenuators Cables …
ILA 2003 4-7 Nov 2003
Xtalk: Work Continues….
Improved measurement loop for better quality and repeatability of factory calibration
Separate measurement of X-talk and tuning
Extensive testing of calibration-quality
Automatic Calibration Investigate influence of
cables, attenuators, etc..
160 cm
Computer controlled antenna rotor
DUT
ILA 2003 4-7 Nov 2003
H-field Antennas Seem Troublesome, Why Again Are We Using Them?
Pstatic No grounding needed Low profile Less susceptible to local effects
And…
True Heading Reradiation Detection
ILA 2003 4-7 Nov 2003
Now We Can Rotate the Antenna…
… rotate the vessel
ILA 2003 4-7 Nov 2003
Loran-C TXGroundwave
+Skywave
+Skywave
Near Field + Antenna
Local O
bject
s
CWICRI
Local I
nterfe
rence
Equival
ent R
X nois
e+
CWI
CRI Local Objects
+
Antenna
Local InterferenceEquivalent RX noise
PFSF ASF
Groundwave
PFSF ASF
Tuning
E-fiel
d susc
eptib
ility
X-talk
Boat
Near Field
Ref S
tatio
n Erro
r
Rx errorSpatial decorrelation of Regional ASF
Error Budget
ILA 2003 4-7 Nov 2003
Influence of Vessel on Received Phase
+
-
+-
ILA 2003 4-7 Nov 2003
Rotating the Vessel…
+
-
+-
ILA 2003 4-7 Nov 2003
Influence of the Measurement Vehicle
Range error due to influence ship might be in the order of the ships size. Effect is most likely larger on E-field than on H-field.
Heading dependant error relative constant as long as the antenna orientation with respect to the vessel is fixed.
Apply correction method similar to Xtalk correction Develop auto calibration similar as a ship-compass:
take a spin and measure the response.
ILA 2003 4-7 Nov 2003
Loran-C TXGroundwave
+Skywave
+Skywave
Near Field + Antenna
Local O
bject
s
CWICRI
Local I
nterfe
rence
Equival
ent R
X nois
e+
CWI
CRI Local Objects
+
Antenna
Local InterferenceEquivalent RX noise
PFSF ASF
Groundwave
PFSF ASF
Tuning
E-fiel
d susc
eptib
ility
X-talk
Boat
Near Field
Ref S
tatio
n Erro
r
Rx errorSpatial decorrelation of Regional ASF
Reradiation by Local Objects
ILA 2003 4-7 Nov 2003
Reradiation by Local Objects (cont’d)
ILA 2003 4-7 Nov 2003
12 14 16 18 20 22 24-20
0
20
40
60
80
TOA Lessay (6731M)[n
s]
time [h]
H-field
E-field
Reradiation By Local Effects: E-field vs H-field
ILA 2003 4-7 Nov 2003
+
-
+-Direct (primary) signal
Reradiated (secondary) signal
EP+HP
ES+HS
, ,
0 0,
Reradiation By Local Objects (cont’d)
Reradiation is a near-field effect Detect reradiation by looking at the relation between E-field
and H-field (ASF survey / reference site) Detect reradiation by looking at the difference between two
(ideal) loops (user Rx)
ILA 2003 4-7 Nov 2003
Reradiation By Local Objects (cont’d)
Reradiation causes a heading dependant error
The effect of reradiation on the range- and position error depends on the beam-steering algorithm and is therefore RX dependant
Therefore, ASF mapping is only allowed in a reradiation free environment
By detecting reradiation, the problem shifts from accuracy/integrity to availability
ILA 2003 4-7 Nov 2003
Conclusions
Heading dependant antenna challenges solvable Reelektronika antenna available 2004 Q1 Influence vessel can be (auto) calibrated ASF is a far field phenomenon and has to be
measured as such
Loran-C: 20 meter of a 3000 meter wavelength = 2.4ºGPS: 2.4º of a 20 cm wavelength = 1.3 mm
The challenge of getting the accuracy of Loran better than 20 meters is somewhat comparable
with GPS better than 1 mm.