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Tracer timestep selection criteria #733

@minghangli-uni

Description

@minghangli-uni

Hi all,

As highlighted in Lecture: MOM6 time stepping, the tracer advection timestep does not necessarily need to be shortened to match the horizontal grid resolution. Instead, it can capture the natural timescale of tracers, such as the diurnal cycle (~hourly resolution), regardless of the grid size. In both GFDL OM4 and the more recent GFDL OM5, the tracer timestep was set to 7200s (2 hours). Inspired by this, we did similar tests using the ACCESS-OM3 (MOM6-CICE6) 0.25deg RYF configuration, starting from initial conditions and running the model for 5 years. The results are summarised below,

Experiment details

  1. Control (run0): (red line in line plots)
    • baroclinic timestep = coupling timestep = tracer timestep = 1350s
    • DIABATIC_FIRST=True
    • configuration available at: here
  2. Perturbation (run1): (green line in line plots)
    • baroclinic timestep = coupling timestep = tracer timestep = 1350s
    • DIABATIC_FIRST=False
  3. Perturbation (run2): (blue line in line plots)
    • baroclinic timestep = coupling timestep = 1350s
    • tracer timestep = 10800s (3 hours)
    • DIABATIC_FIRST=False

1. line plots

1.1 Global mean ocean potential temperature (thetaoga)

The DIABATIC_FIRST parameter did not significantly impact this diagnostic. However, run2 with the 3-hour tracer timestep shows a slower increase in global mean temperature compared to the control and run1.
thetaoga_compare

  • difference compared to the control run (red)
    thetaoga_compare_diff

1.2 Global mean ocean salinity (soga)

The salinity values are consistent across all three runs, with minimal differences between them.
soga_compare

  • difference compared to the control run (red)
    soga_compare_diff

2. 2D snapshots comparisons

We compared snapshots of various fields for the first month (1900-02-01) and after 5 years (1905-01-01).
Note:

  • The differences represent the perturbation runs subtracted from the control run, highlighting impacts of the perturbations.
  • The top-left figure in each set shows the control run difference with itself, which is blank intentionally.

After 5 years, the differences between runs increase, suggesting that the tracer timestep significantly affects field evolution. While the DIABATIC_FIRST parameter had minimal impact, increasing the tracer timestep led to slower changes in global temperature and larger discrepancies in field distributions over time. We’re now curious to understand the criteria GFDL uses to evaluate if a tracer timestep is optimal.

2.1 Vertically Integrated Advective Zonal Flux of Heat T_adx_2d

  • 1900-02-01
    T_adx_2d_diff
  • 1905-01-01
    T_adx_2d_diff_2

2.2 Sea Surface Temperature (tos)

  • 1900-02-01
    tos_diff
  • 1905-01-01
    tos_diff_2

2.3 Potential Temperature (thetao) Depth vs Latitude (Averaged over all longitudes)

  • 1900-02-01
    thetao_diff
  • 1905-01-01
    thetao_diff_2

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