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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

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