This volume is a collection of lectures given at the two colloquia on atmospheric flows over complex terrain with applications to wind energy and air pollution, organized and sponsored by ICTP in Trieste, Italy. The colloquia were the result of the recognition of the importance of renewable energy sources, an important aspect which grows yearly as the environmental problems become more pronounced and their effects more direct and intense, while at the same time, the wise management of the Earth's evidently limited resources becomes imperative.
It is divided into two main parts. The first, which comprises Chaps. 1 to 4, presents the structure of the atmospheric boundary layer with emphasis in the region adjacent to the ground. The second, Chaps. 5 to 10, discusses methods for the numerical computation of the wind field on an arbitrary terrain. The unique feature of this book is that it does not stop at the theoretical exposition of the analytical and numerical techniques but includes a number of codes, in a diskette, where the mechanisms and techniques presented in the main part are implemented and can be run by the reader. Some of the codes are of instructional value while others can be utilized for simple operational work.
Some of the lecturers are: D N Asimakopoulos, C I Aspliden, V R Barros, A K Blackadar, G A Dalu, A de Baas, D Etling, G Furlan, D P Lalas, P J Mason, C F Ratto and F B Smith.
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In the following, the expressions in italics within a definition are the subject of a definition themselves.
ADIABATIC LAPSE-RATE – The rate of temperature decrease with height of a parcel displaced vertically in the atmosphere adiabatically. The parcel becomes cooler with lifting as it expands upon encountering less pressure; conversely, the parcel becomes warmer with descent as it is compressed due to higher pressures. The adiabatic lapse rate is a decrease of 0.98 °C per 100 m of ascent, assuming no condensation occurs. See also dry adiabatic and saturated adiabatic lapse rate…
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For computer demonstrations we choose a simple 1-D model for neutrally stratified boundary layer…
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This one–dimensional time dependent model simulates the atmospheric boundary layer up to a height of three kilometers (only the lowest two kilometers are displayed). The vertical distributions of temperature, dew point and wind speed are displayed on a color screen, and this display is updated every ten minutes of model time (or every two minutes if desired) to provide a dynamically changing profiles of wind speed, temperature, and dew point. In addition, layers containing liquid water are indicated. An inset panel is provided so that the diurnal course of the terms in the surface heat balance equation can be followed graphically.
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The code is designed in order to evaluate the horizontal velocity field induced by a simple isolated topography on an incoming boundary layer.
As input, the code requires some specification of the unperturbed boudary layer and of the shape of the topography. It estimates the perturbation velocity field according th the simplified model described in chapter… To do that, thefourier transform of the topography is computed first, based on an input matrix which specifies the topography height on the domain, at gridded points (the same points where the velocity will be computed)…
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The model Breeze solves a system of equations which include the continuity equation, the horizontal equations of motion, the non–hydrostatic non–elastic form of the vertical equation of motion, the thermodynamic equation and a K-theory turbulence scheme. The details of the theory on which the numerical model Breeze is based, are discussed in detail in the corresponding chapter in the main text. Typical results are also presentedx dthere and especially in the figures…
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Note from Publisher: This article contains the errata to pages 250–257 of the above article.
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