use of acoustic travel times for ocean model validation ... · abstract no 1534 use of acoustic...

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Use of acoustic travel times for ocean Abstract no 1534 Use of acoustic travel times for ocean Abstract no 1534 Poster session PS3 Friday 11 june 2010 S. A. Haugen 1 , H. Sagen, S.Sandven 1 , 1 Nansen Environmental and Re Data Treatment Data treatment for Ocean Acoustic Also the arrivals are t pulses such that multipl Data treatment for Ocean Acoustic Tomography primarily deals with the issues of mooring motion, clock drift and arrival time pulses such that multipl ms can be resolved. As FM sweep can hardly mooring motion, clock drift and arrival time estimation. Mooring Motion FM sweep can hardly noise at a distance of 60 is virtually impossible t the signals in the raw Mooring Motion Mooring motion is monitored using a 3 or 4 transponder “Long Baseline (LBL) positioning the signals in the raw receivers 130 km from figure 3 (left). After transponder “Long Baseline (LBL) positioning system. A scatter of the mooring position of the Fram Strait Acoustic Tomography System figure 3 (left). After multiple resolved recep on all 8 receiver depth the Fram Strait Acoustic Tomography System during the 2008/2009 experiment is shown in figure 1. By monitoring the position of the mooring instruments, all travel times can be on all 8 receiver depth (right). mooring instruments, all travel times can be corrected in post experimental analysis as if the moorings were in their nominal upright the moorings were in their nominal upright position. Figure 1 – Scatter of receiver mooring motion at 300m of depth throughout sept 2008- aug 2009. depth throughout sept 2008- aug 2009. Clock Drift Clock drift correction is carried out in several steps, with the most important one employing a dual clock system where the frequency of an a dual clock system where the frequency of an accurate but power hungry Rubidium oscillator is compared to the oscillation frequency of a Figure 3 – Acoustical raw d compression (right) on all 8 is compared to the oscillation frequency of a less accurate and less power hungry MXCO. Also, synchronization to GPS time before and compression (right) on all 8 979m of depth in 96 m incr Trave time predictions a after experiment is carried out. The timestamps provided by the continuously run MCXO oscillator clock can thus be corrected Trave time predictions a Having detected the mu introduced the correct MCXO oscillator clock can thus be corrected during post experimental data treatment. introduced the correct mooring motion and c for a nominal moor Arrival Time Estimation Accurate arrival time estimation is facilitated measured threoghou Correspondingly, trave predicted on the basis o using Frequency Modulated Sweeps for the Acoustic Tomography Transmissions, as shown in figure 2. Employing matched filtering for predicted on the basis o salinity fields of TOP model. in figure 2. Employing matched filtering for these types of signals makes the arrival to stand clearly out from the noise. model. stand clearly out from the noise. Figure 3 – FM sweep at source (left) and r=60km (right). Duration is 60 seconds and frequecies are from 190 to 290 Hz. Duration is 60 seconds and frequecies are from 190 to 290 Hz. Acknowledgement: This work has been sponsored bu EU (through the DAMOCLES an n model validation, and assimilation n model validation, and assimilation , L. Bertino 1 , P. Sakov 1 , F. Counillon 1 , emote Sensing Center, Norway; transformed to narrow le arrivals as close as 10 Ocean model validation The multiple travel times and the le arrivals as close as 10 s shown in figure 3, the be distinguished from The multiple travel times and the corresponding travel times predicted are shown in figure 4. In the beginning of the be distinguished from 0 km from the source. It to observe reception of w data at any of the shown in figure 4. In the beginning of the period the meassured and prediced travel times differ noticable, by ca 200 ms, while the correspondence improves after 2-3 months. w data at any of the the source as seen in matched filtering, the correspondence improves after 2-3 months. Comparison of mesured and predicted travel times provides a method for ocean model matched filtering, the ptions stand clearly out, hs as shown in figure 3 times provides a method for ocean model validation. hs as shown in figure 3 Figure 4 Measured (upper) and predicted (lower) travel Figure 4 Measured (upper) and predicted (lower) travel times throughout the experiment. The dots indicate individual arrivals. The color of the dots of measurements indicates the intensity of the arrival. For the predictions black indicates the intensity of the arrival. For the predictions black dots represent waterborne arrivals, while pink dots represent bottom intracting arrivals. The colored background of the predictions represent the sound speed field provided data (left) and pulse 8 channels (from 307 to of the predictions represent the sound speed field provided by TOPAZ3. Preparation for data assimilation Having measured and predicted the acoustic 8 channels (from 307 to rements). and measurements Having measured and predicted the acoustic travel times of several multipath arrivals, fetures of these arrival patterns will be used and measurements ultiple arrival times and tions terms related to fetures of these arrival patterns will be used for data assimilation. As a preprocessing step, the matched filter outputs of one week of tions terms related to clock drift, travel times ring position can be the matched filter outputs of one week of receptions have been averaged, to emphaize on the most stable of the arrivals . ut the experiment. el times have been of the temperature and Left: Predicted Travel times of all 100 TOPAZ3 ensemble embers of the temperature and PAZ3 numerical ocean ensemble embers Middle: Instant travel time measurements measurements Right: Averaged travel time mesurements TOPAZ 3 model system has a resolution of 3.5 km and 22 hybrid layers in the vertical. Upper: 01.10.2008 Lower:27.03.2009 hybrid layers in the vertical. The model does not resolve mesocale processes properly and does not include tides. There is a good overlap between TOPAZ3 member predictions and and does not include tides. 100 members and assimilation of satelite data and ARGO profiles using predictions and mesurements for 26.03.2009, while a bias is evident for 01.10.2008 and ARGO profiles using EnKF. evident for 01.10.2008 nd ACOBAR projects), The Norwegian Research Council, Statoil, Aker Solutions

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Page 1: Use of acoustic travel times for ocean model validation ... · Abstract no 1534 Use of acoustic travel times for ocean model validation, and assimilation Poster session PS3 Friday

Use of acoustic travel times for ocean model validation, and assimilationAbstract no 1534

Use of acoustic travel times for ocean model validation, and assimilationAbstract no 1534

Poster session PS3

Friday 11 june 2010

S. A. Haugen1, H. Sagen, S.Sandven1, L. Bertino1Nansen Environmental and Remote Sensing Nansen Environmental and Remote Sensing

Data Treatment

Data treatment for Ocean Acoustic

Also the arrivals are transformed

pulses such that multipleData treatment for Ocean Acoustic

Tomography primarily deals with the issues of

mooring motion, clock drift and arrival time

pulses such that multiple

ms can be resolved. As

FM sweep can hardlymooring motion, clock drift and arrival time

estimation.

Mooring Motion

FM sweep can hardly

noise at a distance of 60

is virtually impossible to

the signals in the rawMooring Motion

Mooring motion is monitored using a 3 or 4

transponder “Long Baseline (LBL) positioning

the signals in the raw

receivers 130 km from

figure 3 (left). Aftertransponder “Long Baseline (LBL) positioning

system. A scatter of the mooring position of

the Fram Strait Acoustic Tomography System

figure 3 (left). After

multiple resolved receptions

on all 8 receiver depthsthe Fram Strait Acoustic Tomography System

during the 2008/2009 experiment is shown in

figure 1. By monitoring the position of the

mooring instruments, all travel times can be

on all 8 receiver depths

(right).

mooring instruments, all travel times can be

corrected in post experimental analysis as if

the moorings were in their nominal uprightthe moorings were in their nominal upright

position.

Figure 1 – Scatter of receiver mooring motion at 300m of

depth throughout sept 2008- aug 2009.depth throughout sept 2008- aug 2009.

Clock DriftClock Drift

Clock drift correction is carried out in several

steps, with the most important one employing

a dual clock system where the frequency of ana dual clock system where the frequency of an

accurate but power hungry Rubidium oscillator

is compared to the oscillation frequency of a

Figure 3 – Acoustical raw data (left) and pulse

compression (right) on all 8 channels (from 307 to is compared to the oscillation frequency of a

less accurate and less power hungry MXCO.

Also, synchronization to GPS time before and

compression (right) on all 8 channels (from 307 to

979m of depth in 96 m increments).

Trave time predictions and measurementsAlso, synchronization to GPS time before and

after experiment is carried out. The

timestamps provided by the continuously run

MCXO oscillator clock can thus be corrected

Trave time predictions and measurements

Having detected the multiple

introduced the correctionsMCXO oscillator clock can thus be corrected

during post experimental data treatment.

introduced the corrections

mooring motion and clock

for a nominal mooring

Arrival Time Estimation

Accurate arrival time estimation is facilitated

for a nominal mooring

measured threoghout

Correspondingly, travel

predicted on the basis ofusing Frequency Modulated Sweeps for the

Acoustic Tomography Transmissions, as shown

in figure 2. Employing matched filtering for

predicted on the basis of

salinity fields of TOPAZ

model.in figure 2. Employing matched filtering for

these types of signals makes the arrival to

stand clearly out from the noise.

model.

stand clearly out from the noise.

Figure 3 – FM sweep at source (left) and r=60km (right).

Duration is 60 seconds and frequecies are from 190 to 290 Hz.Duration is 60 seconds and frequecies are from 190 to 290 Hz.Acknowledgement: This work has been sponsored bu EU (through the DAMOCLES and

Use of acoustic travel times for ocean model validation, and assimilationUse of acoustic travel times for ocean model validation, and assimilation

, L. Bertino1, P. Sakov1, F. Counillon1,

Nansen Environmental and Remote Sensing Center, Norway;Nansen Environmental and Remote Sensing Center, Norway;

transformed to narrow

multiple arrivals as close as 10

Ocean model validation

The multiple travel times and themultiple arrivals as close as 10

As shown in figure 3, the

be distinguished from

The multiple travel times and the

corresponding travel times predicted are

shown in figure 4. In the beginning of thebe distinguished from

60 km from the source. It

to observe reception of

raw data at any of the

shown in figure 4. In the beginning of the

period the meassured and prediced travel

times differ noticable, by ca 200 ms, while the

correspondence improves after 2-3 months.raw data at any of the

the source as seen in

matched filtering, the

correspondence improves after 2-3 months.

Comparison of mesured and predicted travel

times provides a method for ocean modelmatched filtering, the

receptions stand clearly out,

depths as shown in figure 3

times provides a method for ocean model

validation.

depths as shown in figure 3

Figure 4 – Measured (upper) and predicted (lower) travelFigure 4 – Measured (upper) and predicted (lower) travel

times throughout the experiment. The dots indicate

individual arrivals. The color of the dots of measurements

indicates the intensity of the arrival. For the predictions blackindicates the intensity of the arrival. For the predictions black

dots represent waterborne arrivals, while pink dots

represent bottom intracting arrivals. The colored background

of the predictions represent the sound speed field provided

Acoustical raw data (left) and pulse

compression (right) on all 8 channels (from 307 to

of the predictions represent the sound speed field provided

by TOPAZ3.

Preparation for data assimilation

Having measured and predicted the acousticcompression (right) on all 8 channels (from 307 to

979m of depth in 96 m increments).

time predictions and measurements

Having measured and predicted the acoustic

travel times of several multipath arrivals,

fetures of these arrival patterns will be usedtime predictions and measurements

multiple arrival times and

corrections terms related to

fetures of these arrival patterns will be used

for data assimilation. As a preprocessing step,

the matched filter outputs of one week ofcorrections terms related to

clock drift, travel times

mooring position can be

the matched filter outputs of one week of

receptions have been averaged, to emphaize

on the most stable of the arrivals .mooring position can be

threoghout the experiment.

travel times have been

of the temperature and

Left: Predicted Travel times

of all 100 TOPAZ3

ensemble embersof the temperature and

TOPAZ3 numerical ocean

ensemble embers

Middle: Instant travel time

measurements measurements

Right: Averaged travel time

mesurements

TOPAZ 3 model system has a

resolution of 3.5 km and 22

hybrid layers in the vertical.

mesurements

Upper: 01.10.2008

Lower:27.03.2009hybrid layers in the vertical.

The model does not resolve

mesocale processes properly

and does not include tides.

Lower:27.03.2009

There is a good overlap

between TOPAZ3 member

predictions and and does not include tides.

100 members and

assimilation of satelite data

and ARGO profiles using

predictions and

mesurements for

26.03.2009, while a bias is

evident for 01.10.2008and ARGO profiles using

EnKF.evident for 01.10.2008

and ACOBAR projects), The Norwegian Research Council, Statoil, Aker Solutions