13.07.2015 Views

Advanced Ocean Modelling: Using Open-Source Software

Advanced Ocean Modelling: Using Open-Source Software

Advanced Ocean Modelling: Using Open-Source Software

SHOW MORE
SHOW LESS
  • No tags were found...

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

3.11 Exercise 6: Kelvin-Helmholtz Instability 513.11.2 Task DescriptionConsider a vertical ocean slice of 500 m in length and 100 m in depth with cycliclateral boundaries (see below) and grid spacings of Δx = 5 m and Δz = 2m.The density interface of two superimposed layers of different densities is locatedat a depth of 50 m. The density of the top layer is set to ρ 1 = 1,027.0kg/m 3 .The bottom layer has a density of ρ 2 = 1,029.0kg/m 3 , yielding a density differenceof Δρ = 2kg/m 3 . Density diffusion is included in the model. Horizontaland vertical density diffusivities are set to small uniform values of K h = K z = 1 ×10 −4 m 2 /s.The initial lateral flow in the top layer has an average speed of 1 m/s, whereasthe lower layer is at rest. Randomly generated values of ±0.01 m/s are added tothe upper-layer flow. This technique promotes the initial growth of disturbances atrandom locations. The random-number generator was taken from Press et al. (1989).With a difference in layer speeds of Δu = 1m/s, Eq. (3.62) suggests that the transitionmixing zone attains a thickness of around 13 m. Equation (3.56) predicts thatmixing is initiated by disturbances of

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!