European Journal of Scientific Research - EuroJournals
European Journal of Scientific Research - EuroJournals
European Journal of Scientific Research - EuroJournals
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<strong>European</strong> <strong>Journal</strong> <strong>of</strong> <strong>Scientific</strong> <strong>Research</strong><br />
ISSN 1450-216X Vol.14 No.3 (2006), pp. 417-425<br />
© Euro<strong>Journal</strong>s Publishing, Inc. 2006<br />
http://www.eurojournals.com/ejsr.htm<br />
<strong>Research</strong> <strong>of</strong> the Characteristics <strong>of</strong> a Solar Panel Radiated with<br />
Со2 Laser, as Means for Injection on Fading Satellites<br />
M. Zamfirov<br />
Department <strong>of</strong> Aerospace Control Systems, Space <strong>Research</strong> Institute<br />
Bulgarian Academy <strong>of</strong> Sciences<br />
E-mail: mzamfirov@space.bas.bg<br />
Abstract<br />
The article discusses the results achieved after a radiation <strong>of</strong> a solar panel with СО2<br />
laser and covers the short circuit, the floating voltage, and the efficiency. Theoretical<br />
deduction <strong>of</strong> the most appropriate laser wavelength, referred to the maximum <strong>of</strong><br />
transformation <strong>of</strong> the laser energy in electrical energy for the mono crystal silicon is<br />
presented. The volt-ampere characteristics <strong>of</strong> the photo receiver are described.<br />
Keywords: Satellites, Laser radiation, CO2 – laser, Solar panel<br />
Introduction<br />
The research <strong>of</strong> the influence <strong>of</strong> the laser radiation on photo voltage systems is important, providing<br />
energy for existing satellites in the end <strong>of</strong> their life, due to reduction <strong>of</strong> the energy system [1]. This<br />
type <strong>of</strong> radiated laser energy has a great commercial value [2]. The laser radiation is preferable because<br />
<strong>of</strong> the high efficiency <strong>of</strong> the silicon cells under monochromatic lightening [3], and the possibility <strong>of</strong><br />
increasing the energy, in order to produce more energy outcome per area [4].<br />
Exposition<br />
For calculating the most appropriate laser wavelength, relevant to the maximum <strong>of</strong> the transformation<br />
<strong>of</strong> the laser energy to electric energy, we use the following formula:<br />
c<br />
Е = Ћ.ν = Ћ (1)<br />
λ<br />
where<br />
Е – еV 1,610 -19 С (coulomb); 1 V = 1,6.10 -19 J.<br />
Hence:<br />
Е [eV] = 6,6.10 -19 J.s/1,6.10 -19 J. 3.10 8 m/s/ λ [nm] = 1,2375// λ [nm] =<br />
1,<br />
24<br />
=<br />
(2)<br />
λ[<br />
nm]<br />
Consequently:<br />
1,<br />
24 1,<br />
24<br />
Е = = λ =<br />
(3)<br />
λ E[<br />
eV ]<br />
Where Е is the width <strong>of</strong> the forbidden area <strong>of</strong> the semi-conductor.<br />
For silicon Е = 1,11 eV