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SeaSonde Overview O C E A N S E N S O R S Tuesday, October 8, 13
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CODAR SeaSonde Principles

Feb 21, 2022

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Page 1: CODAR SeaSonde Principles

SeaSonde Overview

O C E A N S E N S O R S

Tuesday, October 8, 13

Page 2: CODAR SeaSonde Principles

HF RADAR Definition and Uses

• What Is HF RADAR?• RADAR = RAdio Detection And Ranging

• HF = High Frequency: 3 - 30 MHz or 100 - 10 m wavelength

• VHF = Very High Frequency: 30 - 300 MHz or 10 - 1 m wavelength

• What Can Be Observed/Detected?• Currents

• Most robust environmental data product from HF RADAR systems

• First-order effect - sea echo from Bragg scattering

• Waves• Second-order effect

• Subject to perturbation theory limits - upper waveheight limitation

• Ionosphere Layers• Can cause interference with current measurements

• Discrete “Targets”• Ships: dual use w/ current mapping (under development)

• Ice Packs/Bergs (work done in 70’s - more being done currently)

Tuesday, October 8, 13

Page 3: CODAR SeaSonde Principles

monopole (A3)

radial whips

loop box(A1 & A2)

Computer and Monitor TransmitterReceiver

What does an HF RADAR consist of?

loop 1 (A1)loop 2 (A2)

receive antenna

loop box

Transmit Antenna

Receive Antenna

electronics

Tuesday, October 8, 13

Page 4: CODAR SeaSonde Principles

RF Modes of Propagation

Ionosphere

Earth

Line-of-sight (Horizon Limited)

Over-The-Horizon (OTH)

Ground Wave (Beyond Horizon)

Tuesday, October 8, 13

Page 5: CODAR SeaSonde Principles

λ/2λ/2

λλ

Bragg Sea Echo

A B C

Freq mhz

λmeters

λ/2meters

Tseconds

5 60 30.0 4.4

13 23 11.5 2.7

25 12 6.0 2.0

42 7 3.6 1.5

SeaSonde PrinciplesSeaSonde Principles

Tuesday, October 8, 13

Page 6: CODAR SeaSonde Principles

λ/2λ/2

λλ

Bragg Sea Echo

A B C

Freq mhz

λmeters

λ/2meters

Tseconds

5 60 30.0 4.4

13 23 11.5 2.7

25 12 6.0 2.0

42 7 3.6 1.5

SeaSonde PrinciplesSeaSonde Principles

Tuesday, October 8, 13

Page 7: CODAR SeaSonde Principles

λ/2λ/2

λλ

Bragg Sea Echo

A B C

Freq mhz

λmeters

λ/2meters

Tseconds

5 60 30.0 4.4

13 23 11.5 2.7

25 12 6.0 2.0

42 7 3.6 1.5

SeaSonde PrinciplesSeaSonde Principles

Tuesday, October 8, 13

Page 8: CODAR SeaSonde Principles

λ/2λ/2

λλ

Bragg Sea Echo

A B C

Freq mhz

λmeters

λ/2meters

Tseconds

5 60 30.0 4.4

13 23 11.5 2.7

25 12 6.0 2.0

42 7 3.6 1.5

SeaSonde PrinciplesSeaSonde Principles

Tuesday, October 8, 13

Page 9: CODAR SeaSonde Principles

λ/2λ/2

λλ

Bragg Sea Echo

A B C

Freq mhz

λmeters

λ/2meters

Tseconds

5 60 30.0 4.4

13 23 11.5 2.7

25 12 6.0 2.0

42 7 3.6 1.5

SeaSonde PrinciplesSeaSonde Principles

Tuesday, October 8, 13

Page 10: CODAR SeaSonde Principles

λ/2λ/2

λλ

Bragg Sea Echo

A B C

Freq mhz

λmeters

λ/2meters

Tseconds

5 60 30.0 4.4

13 23 11.5 2.7

25 12 6.0 2.0

42 7 3.6 1.5

SeaSonde PrinciplesSeaSonde Principles

Tuesday, October 8, 13

Page 11: CODAR SeaSonde Principles

λ/2λ/2

λλ

Bragg Sea Echo

A B C

Freq mhz

λmeters

λ/2meters

Tseconds

5 60 30.0 4.4

13 23 11.5 2.7

25 12 6.0 2.0

42 7 3.6 1.5

SeaSonde PrinciplesSeaSonde Principles

Tuesday, October 8, 13

Page 12: CODAR SeaSonde Principles

λ/2λ/2

λλ

Bragg Sea Echo

A B C

Freq mhz

λmeters

λ/2meters

Tseconds

5 60 30.0 4.4

13 23 11.5 2.7

25 12 6.0 2.0

42 7 3.6 1.5

SeaSonde PrinciplesSeaSonde Principles

Tuesday, October 8, 13

Page 13: CODAR SeaSonde Principles

Doppler Spectrum

Doppler Frequency (Hz)

Echo

Str

engt

h (d

Bm)

0 +fB-fB

Tuesday, October 8, 13

Page 14: CODAR SeaSonde Principles

Doppler Spectrum

Doppler Frequency (Hz)

Echo

Str

engt

h (d

Bm)

0 +fB-fB

Tuesday, October 8, 13

Page 15: CODAR SeaSonde Principles

Doppler Spectrum

Doppler Frequency (Hz)

Echo

Str

engt

h (d

Bm)

0 +fB-fB

Tuesday, October 8, 13

Page 16: CODAR SeaSonde Principles

Doppler Spectrum

Doppler Frequency (Hz)

Echo

Str

engt

h (d

Bm)

0 +fB-fB

Tuesday, October 8, 13

Page 17: CODAR SeaSonde Principles

1 2 3 4 5

Radial Currents

Tuesday, October 8, 13

Page 18: CODAR SeaSonde Principles

1 2 3 4 5

Doppler Frequency (Hz)Ec

ho S

tren

gth

(dBm

)0 +fB-fB

RadialCurrents

Tuesday, October 8, 13

Page 19: CODAR SeaSonde Principles

The Doppler Spectrum

Loop 1 (A1)

Loop 2 (A2)

Monopole (A3)

0 HzDoppler Offset

a.k.a. “DC”

Positive Doppler:Targets moving

towards Antennas

Negative Doppler:Targets moving

away from Antennas

Positive Bragg peaks(Waves approaching)

Negative Bragg peaks(Waves receding)

Noise Floor

Tuesday, October 8, 13

Page 20: CODAR SeaSonde Principles

First Order Regions are convolution of spectral energy from all velocities at a given range cell

+30 cm/s-45 cm/s

Compare Phase, Amplitude of all three antennas to determine

direction of velocity

Loop 1 (A1)

Loop 2 (A2)

Monopole (A3)

0 cm/s

Tuesday, October 8, 13

Page 21: CODAR SeaSonde Principles

monopole (A3)

radial whips

loop box(A1 & A2)

Computer and Monitor TransmitterReceiver

What does an HF RADAR consist of?

loop 1 (A1)loop 2 (A2)

receive antenna

loop box

Transmit Antenna

Receive Antenna

electronics

Tuesday, October 8, 13

Page 22: CODAR SeaSonde Principles

Tuesday, October 8, 13

Page 23: CODAR SeaSonde Principles

Tuesday, October 8, 13

Page 24: CODAR SeaSonde Principles

Loop 1

Tuesday, October 8, 13

Page 25: CODAR SeaSonde Principles

Loop 1

Loop

2

Tuesday, October 8, 13

Page 26: CODAR SeaSonde Principles

Loop 1

Loop

2

Tuesday, October 8, 13

Page 27: CODAR SeaSonde Principles

Tuesday, October 8, 13

Page 28: CODAR SeaSonde Principles

Tuesday, October 8, 13

Page 29: CODAR SeaSonde Principles

Direction Finding

AmplitudesAmplitudes PhasesPhases

A1/A3 A2/A3 P1-P3 P2-P3

0 0.707 0.707 0 0

15 0.866 0.5 0 0

45 1 0 0

75 0.866 0.5 0 180

90 0.707 0.707 0 180

120 0.259 0.966 0 180

180 0.707 0.707 180 180

Tuesday, October 8, 13

Page 30: CODAR SeaSonde Principles

Direction Finding

AmplitudesAmplitudes PhasesPhases

A1/A3 A2/A3 P1-P3 P2-P3

0 0.707 0.707 0 0

15 0.866 0.5 0 0

45 1 0 0

75 0.866 0.5 0 180

90 0.707 0.707 0 180

120 0.259 0.966 0 180

180 0.707 0.707 180 180

Tuesday, October 8, 13

Page 31: CODAR SeaSonde Principles

Direction Finding

AmplitudesAmplitudes PhasesPhases

A1/A3 A2/A3 P1-P3 P2-P3

0 0.707 0.707 0 0

15 0.866 0.5 0 0

45 1 0 0

75 0.866 0.5 0 180

90 0.707 0.707 0 180

120 0.259 0.966 0 180

180 0.707 0.707 180 180

Tuesday, October 8, 13

Page 32: CODAR SeaSonde Principles

Output of MUSIC processing:radial vectors

Vectors are in polar coordinate system centered at receive

antenna

1 radial map per averaged cross spectra file

Typically, seven radial maps “merged” into one hourly map

Angular resolutions are 1 - 5˚

Radial Vector Output of MUSIC Processing

Tuesday, October 8, 13

Page 33: CODAR SeaSonde Principles

New Jersey

Long Island

Nested Ranges & Resolutions

Tuesday, October 8, 13

Page 34: CODAR SeaSonde Principles

Two (or more) Sites Used to Produce Total Current Vector Maps from

Single-Site Radials Where Coverages Overlap

Angle of incidenceGreater than 15°or less than 165°

Tuesday, October 8, 13

Page 35: CODAR SeaSonde Principles

Two (or more) Sites Used to Produce Total Current Vector Maps from

Single-Site Radials Where Coverages Overlap

Angle of incidenceGreater than 15°or less than 165°

Tuesday, October 8, 13

Page 36: CODAR SeaSonde Principles

Two (or more) Sites Used to Produce Total Current Vector Maps from

Single-Site Radials Where Coverages Overlap

Angle of incidenceGreater than 15°or less than 165°

Tuesday, October 8, 13

Page 37: CODAR SeaSonde Principles

Combining Radials into Totals

Tuesday, October 8, 13

Page 38: CODAR SeaSonde Principles

Combining Radials into Totals

Tuesday, October 8, 13

Page 39: CODAR SeaSonde Principles

Combining Radials into Totals

Tuesday, October 8, 13

Page 40: CODAR SeaSonde Principles

Combining Radials into Totals

Tuesday, October 8, 13

Page 41: CODAR SeaSonde Principles

Combining Radials into Totals

Tuesday, October 8, 13

Page 42: CODAR SeaSonde Principles

Surface Current Maps

[Paduan, J.D. and L.K. Rosenfeld, Journal of Geophysical Research, vol. 101, 1996]

Tuesday, October 8, 13

Page 43: CODAR SeaSonde Principles

Applications

Tuesday, October 8, 13

Page 44: CODAR SeaSonde Principles

Nyhamna Gas Terminal

Tuesday, October 8, 13

Page 45: CODAR SeaSonde Principles

Improving Search & Rescue

ModelDrifter

CODAR

Tuesday, October 8, 13

Page 46: CODAR SeaSonde Principles

Data courtesy of Japan Coast Guard

Vessel Traffic Safety

TextKurushio

Tokyo Bay

Typical Current = 170 cm/s

Tuesday, October 8, 13

Page 47: CODAR SeaSonde Principles

Planning Coastal Development

Tuesday, October 8, 13

Page 48: CODAR SeaSonde Principles

South North

Chevron’s Genesis Platform

Loop Current Detection

Tuesday, October 8, 13

Page 49: CODAR SeaSonde Principles

Loop Current Detection

Tuesday, October 8, 13

Page 50: CODAR SeaSonde Principles

Operational Oceanography in Norway

Tuesday, October 8, 13

Page 51: CODAR SeaSonde Principles

Data Assimilation

Tuesday, October 8, 13

Page 52: CODAR SeaSonde Principles

Fisheries Management

Tuesday, October 8, 13

Page 53: CODAR SeaSonde Principles

Washington State to Rosarita, Mexico

~2000 km of coastline

Continuous SeaSonde coverage

Nested grid resolutions

COCMP

Tuesday, October 8, 13

Page 54: CODAR SeaSonde Principles

Tuesday, October 8, 13

Page 55: CODAR SeaSonde Principles

Ground Wave Propagation & Depth of Measurement

• Requires interface between free space (air) and highly conductive medium (>8 ppt salinity sea water)

• Ocean surface exists as a free boundary allowing surface molecules freedom to conduct EM energy, much like a waveguide

• Allows vertically polarized EM energy to propagate w/ reduced energy loss for greater distances and beyond horizon

• Radar wave does not penetrate surface at all - depth of measurement comes from effective depth-averaged current “felt” by ocean wave

• 25 MHz measures to < .5 m, 5 MHz measures to 2 m deep

D ∝ λ

Depth of measurement is related to ocean wavelength(Can be linear or logarithmic)Seawater is conductive

Air is almost like free space

Tuesday, October 8, 13