By Michael J P Cullen

This publication counteracts the present type for theories of "chaos" and unpredictability through describing a concept that underpins the superb accuracy of present deterministic climate forecasts, and it means that extra advancements are attainable. The ebook does this by way of creating a particular hyperlink among an exhilarating new department of arithmetic referred to as "optimal transportation" and present classical theories of the large-scale surroundings and ocean move. it truly is then attainable to resolve a collection of straightforward equations proposed a long time in the past via Hoskins that are asymptotically legitimate on huge scales, and use them to derive quantitative predictions approximately many large-scale atmospheric and oceanic phenomena. a specific function is that the easy equations used have hugely predictable recommendations, therefore suggesting that the bounds of deterministic predictability of the elements would possibly not but were reached. it's also attainable to make rigorous statements concerning the large-scale behaviour of the ambience and ocean through proving effects utilizing those uncomplicated equations and using them to the true procedure making an allowance for the error within the approximation. there are many different titles during this box yet they don't deal with this large-scale regime.

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**Additional info for A Mathematical Theory of Large-scale Atmosphere/ocean Flow**

**Example text**

6). We will see later that such a conservation law does hold for the deep atmosphere version of the equations. Much of this book is taken up with analysing the semi-geostrophic equations. However, some key points are noted at the outset: (i) The only approximations made are to the horizontal momentum. We will see that this ensures large-scale validity. In [Hoskins (1975)] additional approximations are made. These are not valid on large scales, but allow the equations to be solved relatively easily.

Such behaviour is illustrated by exact solutions in [Majda (2003)] and in the experiments of [Fincham et al. (1996)]. This means that the vertical scale of the flow will reduce in time. 97) will no longer be an accurate approximation to the full governing equations. As discussed by [Majda (2003)], the vertical scale can be controlled by 48 Large-scale atmosphere flow viscosity, in which case the small value of Fr can be maintained. 5 become appropriate. 5 Quasi-geostrophic solutions In this section we assume Ro = Fr <§C 1.

Define the region of integration V as B x (0, H), where B = ( ( — | i , \V) x {—\L, \L)). Write Tz for the horizontal cross-section Large-scale atmosphere flow 50 B x {z}. Since the solution is unaltered by adding an arbitrary constant to the geopotential