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Kinneret

Karsten Bolding edited this page Jul 19, 2024 · 2 revisions

Simulations to investigate the annual temperature profile.

A correct evolution of the temperature field is essential as a proper basis for bio-geochemical simulations.

pyGETM contains some configuration settings that influences the structure of the temperature field. In the following simulations are carried out where these settings are changed. As a measure of the impact a Hovmöller diagram is produced at the deepest point of the lake - i.e. around 43 m. A very important process for the development of the temperature distribution is the distribution of the short wave radiation through the water column. As an illustration is below given the results of a 4 year GOTM simulation for the deepest point of Lake Kinneret where two different Jerlov water types are used. The meteo-forcing is ERA5.

jerlov_i

jerlov_iii

It is clear that the penetration depth os the short wave radiation has a strong impact on the temperature field.

An inherent issue with the sigma-coordinate models are the pressure-gradient

Run 1 - reference run

run1_temp

Run 2

  • Scale factor on wind is 0.75

run2_temp

Run 3

  • Jerlov type III - (A=0.78, g1=1.4, g2=7.9)

run3_temp

Run 4

  • Salt: 0.4 -> 0.1
  • Jerlov: II -> III
  • Read from gotm.yaml- instead of using GOTM defaults

run4_tmp

Run 5

  • As 4 - but with wind scaling of 0.75

run5_temp

Run 6

  • As 5 but with Dgamma=20

run6_temp

Run 7

  • As 6 but with Albedo according to Cogley (default is Payne)

run7_temp

Run 8

  • As 1 - but with 15 vertical layers

run8_temp

Run 9

  • As 1 - but with a minimum depth of 5 m

run9_temp

Run 10

  • As 1 - but with
  • Pure sigma coordinates
  • Minimum depth is set to 5 meter

run10_temp