Journal of Engineering Science and Technology Review 5 (4) (2012) 35 -37
Special Issue on Renewable Energy Systems
Research Article
The Wireless Albedometer
D. T. Cotfas* and P. A. Cotfas
Transilvania University of Brasov, Romania
Received 5 August 2012; Revised 25 September 2012; Accepted 10 October 2012
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Abstract
The wireless albedemeter as a new solution for the measurement of the albedo is presented in this paper. The classica
pyranometers which are used to build the albedometers were replaced with two small monocrystalline silicon
photovoltaic cells. The mobility and applicability of the albedometer increase using the device called Tag4m instead of
the classical acquisition board.
Keywords: Albedometer, photovoltaic cells, wireless, Tag4m, router.
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1. Introduction
The solar radiation has several components. The global
horizontal solar radiation is composed of the diffuse
horizontal solar radiation and the direct solar radiation. If the
surface is tilted the third component appears - the reflected
solar radiation.
The reflected solar radiation is very important for the
energy balance. A new size - albedo has to be introduced if
this type of solar radiation is taken into account.
There are many definitions for the albedo in function of
the reflecting surface and the research domain: ground
albedo, crop albedo, etc. In general the definition for the
albedo is the ratio between the reflected radiation of surface
R and the global horizontal solar radiation G, see Eq. 1.
G
R
a =
(1)
The albedo is an important parameter for different
research domains, such as: the atmospheric sciences, the
agriculture, the bio-geo engineering, the photovoltaic
domain, climatology, the forestry and the building energy
science. Taking into account the climatic changes and not
only, albedo becomes a crucial parameter [1]. There are
many researchers who claim that by controlling the crop
canopy albedo, the warming can be averted. Increasing the
crop albedo with ~ 0.04 can lead to a cooling effect with
~1oC for Europe in summer [2-5].
2. Methodology
There are three methods to measure the albedo: from the top
of the atmosphere using planes, meteorological balloons or
satellites [6,7], in the lab [8] and in the field conditions [9].
The first method is suitable to measure the albedo for the
large area and homogenous surfaces. This method is not
recommended for small surfaces. The influence of the
atmospheric factors should be taken into account in this
case.
In the lab the albedo can be measured only for small
samples. In this case the light source can be a problem. In
the lab the light source must be a solar simulator to assure a
very good matching between the spectrum of the light source
and the solar spectrum. The price of the solar simulator is
very high and it grows with the increase of the illuminated
area. Another problem for the lab measurement is the area of
the albedometer. The area of classical pyranometers which
are used for albedometers is high and the shadow can cover
the entire illuminated area. A good solution can be using the
two small photovoltaic cells.
The third method is the most widely used because the
measurements are performed in the real conditions.
The albedometers can be realized using one or two back to
back pyranometers. In the first case the cost is lower than in
the second when two pyranometers should be used. The
measurements for the albedometer with one pyranometer are
performed step by step. The reflected radiation of the target
surface is measured first, and the global horizontal solar
radiation is measured after the pyranometer rotation with
180o. There is a big disadvantage; the two radiations are not
measured simultaneously. If the level of radiation is changed
due to the clouds, the measurements are not accurate. In this
case the measurements should be performed in clear sky
conditions. Using the two pyranometers positioned back to
back can eliminate the disadvantages above raising the
measurements’ accuracy but the costs become considerably
higher. To reduce costs pyranometers of inferior class can be
chosen if the measurements accuracy allows it [1].
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* E-mail address: dtcotgas@unitbv.ro
ISSN: 1791-2377 © 2012 Kavala Institute of Technology. All rights reserved.