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Tidal Current Energy

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228 D. Infield<br />

Spectral irradiance (W m �2 �m �1 )<br />

2000<br />

1500<br />

1000<br />

500<br />

Figure 13.4 . The AM1.5G solar spectrum.<br />

Incident on earth’s surface<br />

Outside atmosphere<br />

0<br />

0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5<br />

Wavelength/�m<br />

AM1 represents the shortest path through the atmosphere, i.e. normal to the<br />

earth’s surface, and AM x refers to x times this shortest path. Formally this is calculated<br />

as 1/cos ( θ ), with θ the angle between the path in question and the normal<br />

to the surface. Also by convention, the European standard air mass value<br />

used for cell and module testing is AM1.5. After adding the diffused light intensity<br />

this becomes AM1.5G (where G stands for global). Spectra corresponding to<br />

this and AM0 are shown in Figure 13.4 .<br />

A comprehensive account of the solar resource can be found in Ref. [1] ,<br />

together with the formulae for undertaking calculations of the radiation falling<br />

on differently oriented surfaces at different times of day and year, and at different<br />

locations.<br />

3 . Outline of the Conversion Process<br />

All photovoltaic devices convert incident photons to free charge carriers through<br />

the process of absorption. The heart of a photovoltaic device is a p–n junction<br />

made from the doping of semiconductors, explained later in the section. In semiconductors,<br />

which are by far the most common PV materials, the process starts<br />

with an incoming photon promoting a valence electron to the conduction band of<br />

the semiconductor in question, thus creating electron–hole pairs. These electrons<br />

and holes are then separated by the existing electric field at the p–n junction<br />

and get collected at the end contacts to deliver open circuit voltage. This process<br />

is called photovoltaics. In dye cells and organic polymer devices the process<br />

is more complicated. The solar cell action contrasts to free carrier transport in<br />

a conventional semiconductor p–n junction in that the charge transfer is mediated<br />

via excitons or polarons, which are a kind of bound form of electron–hole<br />

pair as a neutral entity or particle. The so-called exciton that results from photon<br />

absorption in a conjugated polymer or in a dye system then dissociates into free

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