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

CODAR SeaSonde Principles

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SeaSonde Overview

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

Tuesday, October 8, 13

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

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

RF Modes of Propagation

Ionosphere

Earth

Line-of-sight (Horizon Limited)

Over-The-Horizon (OTH)

Ground Wave (Beyond Horizon)

Tuesday, October 8, 13

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

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

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

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

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

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

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

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

Doppler Spectrum

Doppler Frequency (Hz)

Echo

Str

engt

h (d

Bm)

0 +fB-fB

Tuesday, October 8, 13

Doppler Spectrum

Doppler Frequency (Hz)

Echo

Str

engt

h (d

Bm)

0 +fB-fB

Tuesday, October 8, 13

Doppler Spectrum

Doppler Frequency (Hz)

Echo

Str

engt

h (d

Bm)

0 +fB-fB

Tuesday, October 8, 13

Doppler Spectrum

Doppler Frequency (Hz)

Echo

Str

engt

h (d

Bm)

0 +fB-fB

Tuesday, October 8, 13

1 2 3 4 5

Radial Currents

Tuesday, October 8, 13

1 2 3 4 5

Doppler Frequency (Hz)Ec

ho S

tren

gth

(dBm

)0 +fB-fB

RadialCurrents

Tuesday, October 8, 13

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

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

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

Tuesday, October 8, 13

Tuesday, October 8, 13

Loop 1

Tuesday, October 8, 13

Loop 1

Loop

2

Tuesday, October 8, 13

Loop 1

Loop

2

Tuesday, October 8, 13

Tuesday, October 8, 13

Tuesday, October 8, 13

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

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

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

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

New Jersey

Long Island

Nested Ranges & Resolutions

Tuesday, October 8, 13

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

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

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

Combining Radials into Totals

Tuesday, October 8, 13

Combining Radials into Totals

Tuesday, October 8, 13

Combining Radials into Totals

Tuesday, October 8, 13

Combining Radials into Totals

Tuesday, October 8, 13

Combining Radials into Totals

Tuesday, October 8, 13

Surface Current Maps

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

Tuesday, October 8, 13

Applications

Tuesday, October 8, 13

Nyhamna Gas Terminal

Tuesday, October 8, 13

Improving Search & Rescue

ModelDrifter

CODAR

Tuesday, October 8, 13

Data courtesy of Japan Coast Guard

Vessel Traffic Safety

TextKurushio

Tokyo Bay

Typical Current = 170 cm/s

Tuesday, October 8, 13

Planning Coastal Development

Tuesday, October 8, 13

South North

Chevron’s Genesis Platform

Loop Current Detection

Tuesday, October 8, 13

Loop Current Detection

Tuesday, October 8, 13

Operational Oceanography in Norway

Tuesday, October 8, 13

Data Assimilation

Tuesday, October 8, 13

Fisheries Management

Tuesday, October 8, 13

Washington State to Rosarita, Mexico

~2000 km of coastline

Continuous SeaSonde coverage

Nested grid resolutions

COCMP

Tuesday, October 8, 13

Tuesday, October 8, 13

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