This new model integrations are executed towards the Geophysical Liquid Figure Lab (GFDL) Atmospheric Design type 2

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This new model integrations are executed towards the Geophysical Liquid Figure Lab (GFDL) Atmospheric Design type 2

This new model integrations are executed towards the Geophysical Liquid Figure Lab (GFDL) Atmospheric Design type 2

1) Model works used

step one (Delworth ainsi que al. 2006) featuring a small-frequency dynamical key (Lin 2004) which have a horizontal resolution of around 2° latitude and 24 vertical levels. The brand new atmospheric model try coupled to help you an effective slab ocean having spatially uniform depth. Four outfit professionals which have recommended sea deepness from dos.4, 6, several, twenty-four, and you may 50 yards are examined within studies. The brand new design try pushed by seasonally different insolation that have no eccentricity and you can ° obliquity, and that is work at having 20 years, adequate to converge toward a steady climatology. The newest design climatology try taken from the final five years off the latest integrations.

2) Efficiency

The seasonal migration of the ITCZ off the equator has a larger amplitude for shallower ocean depths (Fig. 8) and PPenny reaches as far as 21° in the 2.4-m slab depth run as compared to 3° in the 50-m slab depth run. This behavior is expected because the adjustment time scale of a 50-m-deep ocean to solar heating is on the order of one year (Donohoe 2011) as compared to weeks for 2.4-m-deep ocean. Thus, the SSTs barely adjust to the seasonally varying insolation in the 50-m run while the maximum SST moves seasonally with the insolation in the 2.4-m run.

(top) Seasonal set of rain centroid and you can atmospheric heat transport across the equator regarding slab water aquaplanet simulations with every simulator (water depth) supplied by another type of colour. The new seasonal range was twice the new amplitude of your yearly harmonic of each varying in addition to slope of your own range is the regression coefficient of the monthly research. The brand new black colored asterisks would be the monthly observations as well as the strong black range ‘s the regular variety of brand new observations. (bottom) Just like the during the better, however for rain centroid and you will tropical SST gradient.

(top) Regular set of precipitation centroid and you will atmospheric temperature transport along side equator about slab ocean aquaplanet simulations with every simulation (ocean depth) provided by a special color. The regular variety is twice the fresh new amplitude of yearly harmonic of every varying therefore the slope of your line ‘s the regression coefficient of your own month-to-month studies. The brand new black asterisks are the month-to-month observations while the strong black line ‘s the seasonal listing of the new observations. (bottom) While the at finest, however for rain centroid and you will tropical SST gradient.

(top) Seasonal directory of precipitation centroid and you will atmospheric temperature transportation across the equator throughout the slab water aquaplanet simulations with each simulation (ocean breadth) provided by another colour. The brand new seasonal range try double the new amplitude of the annual harmonic each and every varying while the slope of the range is the regression coefficient of your month-to-month analysis. This new black asterisks may be the monthly observations while the good black range ‘s the seasonal a number of the new observations. (bottom) As the in the greatest, but for rain centroid and tropical SST gradient.

The seasonal amplitude of AHTEQ also decreases with increasing ocean depth, from 11.6 PW in the 2.4-m run to 0.5 PW in the 50-m run. In the shallow ocean run, the SSTs respond rapidly to the seasonally varying insolation, heating up over the summer hemisphere and subsequently fluxing energy upward (via turbulent and longwave fluxes) to the adjacent atmosphere to drive seasonal variations in AHTEQ; in the 2.4-m run ?SHF? is nearly in phase with the insolation (11-day lag) and has a seasonal amplitude of 11.6 PW. In contrast, the solar heating of the ocean makes a minimal impact on ocean temperatures in the deep ocean runs due to the large heat capacity of the ocean. In fact, SWABS is the only source of seasonal atmospheric heating in the 50-m run and the atmosphere loses energy to the ocean during the warm season; in the 50-m run ?SHF? is nearly antiphased with the insolation (192-day lag) and has a seasonal amplitude of 3.7 PW.

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