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SOLWEIG 1.0 – Modelling spatial variations of 3D radiant fluxes and ...

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698 Int J Biometeorol (2008) 52:697<strong>–</strong>713<br />

sky the upper hemisphere, both with an angle factor <strong>of</strong> 0.5<br />

(e.g. Jendritzky et al. 1990; Pickup<strong>and</strong>deDear1999).<br />

Although easier to use, this method is only reliable for<br />

unobstructed open spaces, <strong>and</strong> obstruction effects should<br />

be added using sky view factors.<br />

Over the years, several different s<strong>of</strong>tware have been<br />

developed to simulate Tmrt in outdoor urban settings.<br />

TOWNSCOPE (Teller <strong>and</strong> Azar 2001) is a CAD-based<br />

s<strong>of</strong>tware which, among other things, simulates <strong>spatial</strong><br />

<strong>variations</strong> <strong>of</strong> solar access <strong>and</strong> Tmrt in complex urban<br />

environments. Thermal comfort can only be calculated on<br />

a daily, monthly or annual basis <strong>and</strong>, since vector data are<br />

utilised, the <strong>spatial</strong> extension is limited. The RayMan<br />

s<strong>of</strong>tware (Matzarakis 2000; Matzarakis et al. 2000, 2007)<br />

is a tool which, along with Tmrt, simulates different thermal<br />

indices. RayMan is a stationary model <strong>and</strong> can be run on<br />

very few input meteorological parameters. RayMan is very<br />

user-friendly <strong>and</strong> thus a popular tool for researchers, urban<br />

planners <strong>and</strong> practitioners. Although commonly used,<br />

RayMan has some principal shortcomings regarding the<br />

calculation <strong>of</strong> the three-dimensional radiation flux densities<br />

<strong>and</strong> surface temperatures <strong>and</strong>, consequently, the resulting<br />

Tmrt (Thorsson et al. 2007). The three-dimensional ENVImet<br />

model (Bruse 1999, 2006) simulates radiation <strong>fluxes</strong>,<br />

temperature, wind flow, turbulence <strong>and</strong> humidity, as well as<br />

Tmrt with high <strong>spatial</strong> <strong>and</strong> temporal resolution. The model is<br />

grid-based. Because <strong>of</strong> its complexity, the model’s domain<br />

size is restricted to 250×250×25 grids. It can be run on a<br />

regular PC. Like the other models mentioned above, ENVImet<br />

calculates Tmrt according to Fanger (1972); the<br />

surrounding environment is divided into building surfaces,<br />

the free atmosphere (sky) <strong>and</strong> the ground surface for which<br />

the direct, diffuse <strong>and</strong> diffusely reflected shortwave <strong>and</strong> the<br />

total longwave radiation components are taken into account.<br />

At street level, the total longwave radiation <strong>fluxes</strong><br />

are assumed to originate from the upper hemisphere (sky<br />

<strong>and</strong> buildings) <strong>and</strong> from the ground (lower hemisphere).<br />

ENVI-met is still under development. To date, the model<br />

has only been evaluated with respect to Tmrt for an east<strong>–</strong>west<br />

oriented urban canyon (H/W=1) in Freiburg, Germany,<br />

during a hot summer’s day (Ali Toudert 2005). The<br />

evaluation showed good agreement between simulated<br />

shortwave radiation <strong>fluxes</strong> <strong>and</strong> field data. However, the<br />

simulated longwave radiation <strong>fluxes</strong> revealed discrepancies<br />

with the field data by up to 50 Wm −2 , which played the main<br />

role in the differences observed in T mrt, (<strong>–</strong>8°C in daytime)<br />

(Ali Toudert 2005).<br />

In this paper, the development <strong>of</strong> a new radiation model,<br />

<strong>SOLWEIG</strong> <strong>1.0</strong> (solar <strong>and</strong> longwave environmental irradiance<br />

geometry-model), which simulates three-dimensional<br />

daytime radiation <strong>fluxes</strong> <strong>and</strong> Tmrt in complex urban settings<br />

is presented. The first part <strong>of</strong> the paper presents the features<br />

<strong>of</strong> the <strong>SOLWEIG</strong> <strong>1.0</strong> model <strong>and</strong> is followed by an<br />

evaluation <strong>of</strong> the model using three-dimensional integral<br />

radiation measurements.<br />

Materials <strong>and</strong> methods<br />

Model structure<br />

The framework theory for Tmrt calculations used in this<br />

study is based on the measuring procedure proposed by<br />

Höppe (1992), in which each <strong>of</strong> the six longwave <strong>and</strong><br />

shortwave radiation <strong>fluxes</strong> (upward, downward <strong>and</strong> from<br />

the four cardinal points) is considered. The meteorological<br />

input parameters are direct, diffuse <strong>and</strong> global shortwave<br />

radiation, air temperature <strong>and</strong> relative humidity. Spatial<br />

<strong>variations</strong> <strong>of</strong> urban geometry are represented by a highresolution<br />

urban digital elevation model (DEM) covering<br />

the central parts <strong>of</strong> Göteborg (Fig. 1). <strong>SOLWEIG</strong> <strong>1.0</strong> is a<br />

2.5-dimensional model in the sense that it applies a 2.5dimensional<br />

DEM (i.e. x <strong>and</strong> y coordinates with height<br />

attributes) in the calculation <strong>of</strong> Tmrt. However, the output<br />

from the current version <strong>of</strong> <strong>SOLWEIG</strong> is represented in two<br />

dimensions (x <strong>and</strong> y). The model was evaluated by using<br />

three-dimensional radiation data from two different locations<br />

within the centre <strong>of</strong> Göteborg, Sweden (57°N), during<br />

different weather conditions <strong>and</strong> at different times <strong>of</strong> the<br />

year. Radiation data obtained from the Swedish Meteorological<br />

<strong>and</strong> Hydrological Institute (SMHI) are used as<br />

parameterisation data in the cloudiness calculations. Sur-<br />

Fig. 1 A DEM covering the central parts <strong>of</strong> Göteborg. The two<br />

locations where integral radiation measurements were conducted are<br />

marked (SITE 1 <strong>and</strong> SITE 2)

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