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marine macro-litter in the Bay of Bengal between 1st June 208 – 30th 
September 2019, saved as NetCDF files. The model incorporated advection due to 
ocean, wind, and Stokes drift velocities, horizontal diffusion, and particle 
beaching behaviours. Two different hydrodynamic data sets were used to force 
the particles’ trajectories: a high-resolution ocean velocity hindcast (ROMS – 
Regional Oceanic Modelling System) and a lower-resolution dataset which 
included data assimilation (CMEMS - Copernicus Marine Environment Monitoring 
Service). Sensitivity tests were run to determine whether hourly or daily 
forcing resulted in significantly different particle end locations and 
validation simulations were run to compare with undrogued drifter tracks for 
the same period and region. All model output is stored in NetCDF files. This 
is data to accompany a manuscript submitted to Ocean Science entitled 
‘Monsoonal influence on floating marine litter pathways in the Bay of Bengal’ 
(Preprint: `EGUsphere - Monsoonal influence on floating marine litter 
pathways in the Bay of Bengal`_). These experiments aimed to determine 
source-to-sink connectivity between countries surrounding the Bay of Bengal.


.. _`egusphere - monsoonal influence on floating marine litter pathways in the bay of bengal`:
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 – Please note the applicable attribution statement is as follows: ‘includes 
Crown copyright, Cefas 2024'


.. _`https://www.nationalarchives.gov.uk/doc/open-government-licence/version/3/)`:
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            <gco:CharacterString>The transport of marine litter was modelled using the OceanParcels v2.3.1** 
**Lagrangian particle tracking model (Delandmeter and van Sebille, 2019; 
Lange and van Sebille, 2017). The model includes several processes which 
influence the movement of floating, buoyant particles around the domain. 
Advection of particles via surface ocean currents (detailed below) was 
included using an inbuilt OceanParcels kernel which uses a fourth-order 
Runge-Kutta advection scheme. Stokes drift velocities were added to surface 
currents to account for the movement of particles resulting from wave motions. 
To account for sub-grid scale processes, diffusion is implemented as a random 
walk, with a diffusion coefficient of 100 m2/s, chosen based on grid cell 
size (Peliz et al., 2007), as detailed below. Windage is implemented in the 
model by applying 1% of the wind velocity to the particles’ trajectories, 
following analysis of observations of the wind’s effect on drifters by Pereiro 
et al. (2018), which should account for all but very large items of litter. 
The final process implemented here was beaching. At the end of each timestep, 
after advancing each particle’s position, ocean velocities were checked at 
this new position. If the velocity was less than 10-14 m/s, the particle was 
considered to be beached (after Delandmeter and van Sebille (2019)) and was no 
longer tracked. There is no resuspension of particles that have beached; the 
beached location is considered the final sink location.

The advection of particles depends on surface ocean currents taken from two 
different models which were used to evaluate the transport of particles and 
help quantify uncertainty in the results. The NEMO-based CMEMS Global Ocean 
Physics Analysis and Forecast hydrodynamic model (E.U. Copernicus Marine 
Service Information (CMEMS), Marine Data Store (MDS), 2022a) has a resolution 
of 1/12°, which is roughly 9.2 km at the latitudes of the Bay of Bengal, and 
includes data assimilation (Lellouche et al., 2018). Also included was the 
ROMS-based high-resolution model, configured for the North Indian Ocean as a 
part of the High-Resolution Operational Ocean Forecast and Reanalysis System 
(known as NIO-HOOFS) by INCOIS for the Indian Ocean (Francis et al., 2020), 
which has a much higher resolution of 1/48°, corresponding to approximately 
2.3 km at these latitudes, but does not include data assimilation. Additional 
datasets from CMEMS Global Ocean Wave Analysis and Forecasting model (Ardhuin 
et al., 2010; E.U. Copernicus Marine Service Information (CMEMS). Marine Data 
Store (MDS), 2022b) and ERA5 global atmospheric reanalysis (Hersbach et al., 
2023) were used to provide Stokes drift velocities and wind fields at a height 
of 10 m above land, respectively.

Particle release locations were uniformly spaced around all major coastlines 
in the Bay of Bengal. Particles were released on average 6 km from the 
coastline, with a maximum distance of 18 km in some locations. A particle was 
released from each of the 500 coastal locations every day for a year, with 
182,500 particles released in total.

Model simulations covered 1st June 2018 – 30th September 2019 for each 
case (CMEMS and ROMS). Following some sensitivity tests detailed below, 
particles were forced with daily-mean ocean, Stokes drift, and wind 
velocities. A model time step of 15 minutes was used (following Delandmeter 
and van Sebille (2019)) and particle positions were output daily.

We ran separate simulations for each season, with particles released over a 
season-specific, four-month period: monsoon = 1st June – 30th September 2018; 
post-monsoon = 1st October 2018 – 31st January 2019; pre-monsoon = 1st 
February – 30th May 2019 (Anoop et al., 2015). Regardless of the release 
period, all particles were tracked until the end of September 2019.

To assess model performance, the simulated trajectories of floating litter 
were compared with paths of drifters which had lost their drogues in the Bay 
of Bengal between June 2018 – September 2019. Within the Global Drifter 
Program’s quality-controlled 6-hour interpolated dataset (Lumpkin and 
Centurioni, 2019), five drifters were identified that met these criteria 
within the spatial and temporal limits of the model. As the separation between 
the particles and drifter location is expected to increase with time (Tamtare 
et al., 2021), each drifter trajectory was separated into week-long segments.

CMEMS and ROMS simulations were run, using the same input data and parameters 
described for the main simulations. Starting at midday on the first full day 
after each drifter lost its drogue, 100 particles were released at the same 
location as the drifter. For each subsequent week, a further 100 particles 
were released from the location of the drifter at that time. Each particle was 
then followed for one week to compare to the relevant drifter trajectory 
during that time.

To decide the required temporal resolution necessary to simulate particle 
trajectories across the Bay of Bengal, simulations were run to test the 
sensitivity of sink locations to temporal forcing. Simulations were forced 
with either CMEMS or ROMS hydrodynamic forcing at either hourly or daily 
temporal resolution. All four simulations used the same parameters as well as 
wind and Stokes drift data as detailed above and were run for the month of 
July 2020 with particles released for the first two weeks only.

This study has been conducted using E.U. Copernicus Marine Service 
Information: `10.48670/moi-00016`_`10.48670/moi-00017`_

Anoop, T. R., Kumar, V. S., Shanas, P. R., and Johnson, G.: Surface Wave 
Climatology and Its Variability in the North Indian Ocean Based on ERA-Interim 
Reanalysis, Journal of Atmospheric and Oceanic Technology, 32, 1372–1385, 
`https://doi.org/10.1175/JTECH-D-14-00212.1`_, 2015.

Ardhuin, F., Rogers, E., Babanin, A. V., Filipot, J.-F., Magne, R., Roland, 
A., Westhuysen, A. van der, Queffeulou, P., Lefevre, J.-M., Aouf, L., and 
Collard, F.: Semiempirical Dissipation Source Functions for Ocean Waves. Part 
I: Definition, Calibration, and Validation, Journal of Physical Oceanography, 
40, 1917–1941, `https://doi.org/10.1175/2010JPO4324.1`_, 2010.

Delandmeter, P. and van Sebille, E.: The Parcels v2.0 Lagrangian framework: 
new field interpolation schemes, Geoscientific Model Development, 12, 
3571–3584, `https://doi.org/10.5194/gmd-12-3571-2019`_, 2019.

Francis, P. A., Jithin, A. K., Effy, J. B., Chatterjee, A., Chakraborty, K., 
Paul, A., Balaji, B., Shenoi, S. S. C., Biswamoy, P., Mukherjee, A., Singh, 
P., Deepsankar, B., Reddy, S. S., Vinayachandran, P. N., Kumar, M. S. G., 
Bhaskar, T. V. S. U., Ravichandran, M., Unnikrishnan, A. S., Shankar, D., 
Prakash, A., Aparna, S. G., Harikumar, R., Kaviyazhahu, K., Suprit, K., Shesu, 
R. V., Kumar, N. K., Rao, N. S., Annapurnaiah, K., Venkatesan, R., Rao, A. S., 
Rajagopal, E. N., Prasad, V. S., Gupta, M. D., Nair, T. M. B., Rao, E. P. R., 
and Satyanarayana, B. V.: High-Resolution Operational Ocean Forecast and 
Reanalysis System for the Indian Ocean, Bulletin of the American 
Meteorological Society, 101, E1340–E1356, 
`https://doi.org/10.1175/BAMS-D-19-0083.1`_, 2020.

Hersbach, H., Bell, B., Berrisford, P., Biavati, G., Horányi, A., Muñoz 
Sabater, J., Nicolas, J., Peubey, C., Radu, R., Rozum, I., Schepers, D., 
Simmons, A., Soci, C., Dee, D., and Thépaut, J.-N.: ERA5 hourly data on single 
levels from 1940 to present. Copernicus Climate Change Service (C3S) Climate 
Data Store (CDS), `https://doi.org/10.24381/cds.adbb2d47`_, 2023.

Lange, M. and van Sebille, E.: Parcels v0.9: prototyping a Lagrangian ocean 
analysis framework for the petascale age, Geoscientific Model Development, 10, 
4175–4186, `https://doi.org/10.5194/gmd-10-4175-2017`_, 2017.

Lellouche, J.-M., Greiner, E., Le Galloudec, O., Garric, G., Regnier, C., 
Drevillon, M., Benkiran, M., Testut, C.-E., Bourdalle-Badie, R., Gasparin, F., 
Hernandez, O., Levier, B., Drillet, Y., Remy, E., and Le Traon, P.-Y.: Recent 
updates to the Copernicus Marine Service global ocean monitoring and 
forecasting real-time 1∕12° high-resolution system, Ocean Science, 14, 
1093–1126, `https://doi.org/10.5194/os-14-1093-2018`_, 2018.

Lumpkin, R. and Centurioni, L.: Global Drifter Program quality-controlled 
6-hour interpolated data from ocean surface drifting buoys. June 
2018-September 2019. NOAA National Centers for Environmental Information. 
[Dataset.] `https://doi.org/10.25921/7ntx-z961`_, 2019, (Accessed 07 July 
2023).

Peliz, A., Marchesiello, P., Dubert, J., Marta-Almeida, M., Roy, C., and 
Queiroga, H.: A study of crab larvae dispersal on the Western Iberian Shelf: 
Physical processes, Journal of Marine Systems, 68, 215–236, 
`https://doi.org/10.1016/j.jmarsys.2006.11.007`_, 2007.

Pereiro, D., Souto, C., and Gago, J.: Calibration of a marine floating litter 
transport model, Journal of Operational Oceanography, 11, 125–133, 
`https://doi.org/10.1080/1755876X.2018.1470892`_, 2018.

Tamtare, T., Dumont, D., and Chavanne, C.: Extrapolating Eulerian ocean 
currents for improving surface drift forecasts, Journal of Operational 
Oceanography, 14, 71–85, `https://doi.org/10.1080/1755876X.2019.1661564`_, 
2021.


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