Open Access Journal of Biomedical Engineering and Biosciences

Mini Review(ISSN: 2637-4579)

Optical and Geometrical Characteristics of Secondary
Conic Concentrators Volume 3 - Issue 4

Akbarov R Yu and Nurmatov Sh R*

Institute of Materials Science of the Uzbek Academy of Sciences, Uzbekistan

Received: October 01, 2019; Published: October 10, 2019

*Corresponding author: Nurmatov Sh R, Institute of Materials Science of the Uzbek Academy of Sciences, Tashkent city, Yunusabad
district, Chingiz Aitmatov St., Building 2B, Uzbekistan

In this work the task of increasing the efficiency of solar collectors using secondary conical concentrators is considered. The
article presents the analytical and numerical analysis of the optical-geometrical characteristics of the secondary conic concentrators.

Keywords: Solar concentrator; collector; secondary concentrator; radiation; flux density; focon; parabolic; conical; reflector;
parametric angle; critical angle; length; radius; large solar furnace

In solar engineering, secondary concentrators are commonly
used to increase the density of concentrated energy flux generated
from the primary solar concentrators. They can also be used, for
example, to change the location of the focal area of the concentrator
or the shape of the distribution of concentrated flux density, etc.
Note that the modules of secondary concentrators can be used
without a primary concentrator, but with a lower concentration
ratio.

The types of secondary concentrators are very
different, typically they are parabolic concentrators,
various types of focons (parabolotoric, conical, wedge-shaped,
prism etc.), lenses, parabolic through concentrators, flat reflectors,
fragments of conical sections - cassegrain system, gregoria system
etc.

For certain categories of concentrators used as secondary
concentrators, their optical-geometric properties have been
studied in enough detail.

The achieved positive effect using secondary concentrators
depends on the particular optical scheme, which includes the
secondary concentrator. Therefore, despite the well-known general
optical-geometrical properties of several types of concentrators,
for the “primary concentrator + secondary concentrator” optical
system, a detailed analysis of the output characteristics of such
systems is difficult or evaluative. Therefore, in these cases a detailed
optical- geometrical calculation of specific system is separately
performed based on the developed mathematical models [1,2].

This paper investigates the optical and geometrical properties
of conical concentrators.

Figure 1: Optical scheme of the focon.

We introduce the notations as shown in Figure 1. The geometry
of the conical focon is defined by two radii (R and r), angles γ
(parametric angle) and θ (critical angle), and length L, and three
parameters are needed to uniquely determine the focon geometry.
We have

And for these angles

Let φ will be the angle of incidence and reflection at point D (the
vector DN is the normal to the surface), and β the angle between
the reflected beam 1 and the direct CD. Then it is easy to see the
correctness of the following relations:

Let us determine such parameters of the focon, for which all
the rays with an angle of incidence greater than θ come back. A
necessary condition for this case is the equality β = 0 at the point D
(that is, the reflected beam begins go to back). For this case we have

It’s obvious that, in this case, the focon geometry is determined
by two parameters for the given θ.

We have

(It is easy to see that for the case of multiple reflection i, we
have γ = (90-θ/ 2i).

Figure 2: Change interval of the angle γ.

For such conditions, the angles cannot be arbitrary. Figure 2
presents a graph in which a possible interval of angles is highlighted.
Thus, the values of the angle γ must be less than 30 degrees.

Now we define the output radius r and the length L of the focon.
From equation (1) we have

or

from here

And, in turn,

From equation (1) we define r

Since r>0, therefore 1-3tg^{2}γ > 0 or tgγ <
, and hence we have γ <30^{0}, i.e. as mentioned above.

Thus, it can be noted that the value of the critical focal angle
determines such a focal configuration (θ = 90 − 2γ ) that rays with
an incidence angle greater than θ always return back. In this case, if
the angle of incidence of the rays is less than θ, then after a single or
multiple reflection, they can pass through the focon or come back.

Figure 3: Focon options for the LSF.

Based on the obtained relations the calculations were carried
out to determine the parameters of the conical focon in the case of its use in the optical scheme of the thousand kWt Large Solar
Furnace of the Institute of Materials Science (Uzbekistan, LSF) [3,4].
In Figure 3 the dependence of the output radius and the length of
the focon on its parametric angle is shown. Based on these data, it
is possible to determine the optimal geometry of the conical focon
for the LSF.

R Winston, JC Miсano, P Benitez (2005) “Nonimaging Optics”, Elsevier-
Academic Press, New York, USA.

Zakhidov RA, Weiner AA, Umarov G (1992) Theory and Calculation
of Applied Solar Energy Concentrating Systems (English Ed). Gujarat
Energy Development Agency, Vadodara, India, pp. 146.