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Description  |
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BACKGROUND OF THE INVENTION
This invention relates to a system for the accumulation of heat from solar
radiant energy. More particularly this invention relates to a system for
the accumulation of heat from solar radiant energy adapted to have solar
energy absorbed by absorbing means and transferred therefrom to a
heat-transfer medium, which system is improved by having said
heat-transfer medium divided into a few stages for thereby enabling the
heating thereof to be effected in the sequence of said stages.
Of the electromagnetic wave energies, typical is the solar radiant energy.
In the orbit of the earth, the mean intensity of solar radiation is about
0.1 W/cm.sup.2 (equivalent to 1,000,000 KW per kilometer), the spectral
curve of solar radiant energy has the highest value in the neighborhood of
0.5.mu. of wavelength and the color temperature thereof is 5900.degree.K.
Incidentally, the solar radiant energy may as well be regarded as
inexhausible. If such solar radiant energy can be efficiently and directly
harnessed and converted into heat, then the system will serve as a
permanent energy source which entails no environmental pollution.
Heretofore various types of solar energy collectors have been proposed
(examples being those disclosed in U.S. Pat. Nos. 1,880,938; 2,917,817;
3,176,678; 3,176,679 and 3,227,153).
The present inventors pursued a research and have consequently proposed a
system for absorbing solar radiant energy which enables the solar radiant
energy to be absorbed at a high percentage and minimizes possible loss of
absorbed energy through radiation (U.S. patent application Ser. No.
402,918 abandoned). The proposed system for the absorption of solar
radiant energy comprises a highly conductive basal member, a heat
absorption member disposed in close contact with the external surface of
said basal member, a selectively penetrating membrane permitting passage
of only desired wavelengths of the electromagnetic wave energies and
disposed on said heat absorption member and a heat-transfer medium
circulated inside said highly conductive basal member, whereby the sun's
rays are concentratedly irradiated upon the heat absorption member to have
the energies absorbed in the form of heat by said heat absorption member,
the absorbed heat is conveyed through said highly conductive basal member
to said coolant to elevate the temperature thereof and the coolant which
now has an elevated temperature is withdrawn and put to use. Said
selectively penetrating membrane permits penetration of electromagnetic
wave having only wavelengths (about 0.3 to 2.0.mu.m) contemplated for
absorption by the present apparatus and reflects electromagnetic waves of
all the other wavelengths. Accordingly, electromagnetic wave energies
which have penetrated the membrane are absorbed by the heat absorption
member and radiant energies radiated by the heat absorption member are
again reflected back to the heat absorption member by the membrane, with
the result that electromagnetic energies are absorbed with high
efficiency. When it is desired to obtain heat of a high temperature by use
of the solar radiant energy absorption system of the one-stage
construction described above, it will suffice for this system to be
provided with a reflector of a parabolic profile or other similar device
designed to concentrate the solar radiant energy impinging upon a wide
area into one point. It is actually difficult, however, to obtain heat
energies of a high temperature as expected, because the heat-transfer
medium fails to effect the desired heat-exchange to a sufficient extent
even if it is delivered at once to this focus. The output by the device
under discussion will sharply decline when the actual point at which the
solar energy are concentrated deviates, though to the slightest extent,
from the fixed focus of the parabolic reflector. Also in this respect, it
proves difficult to obtain heat of a sufficiently high intensity as the
output. Since the angle at which the solar radiant energy impinge upon a
given area changes constantly with lapse of time, it is essential that the
system be provided with a sun-chasing device adapted for the solar radiant
energy to be accurately focused at one fixed point of the reflector at all
times. An attempt to obtain heat energies of a high temperature with such
one stage system of the aforementioned description is difficult to
accomplish and proves disadvantageous from the economic point of view.
The inventors pursued a further study on devices for the absorption of
solar energies. They have, consequently, arrived at a discovery that a
system in which heating is effected at a few stages of successively
elevated temperatures by use of heat-absorption members optimum for
respective temperature ranges fixed for said stages so as to obtain heat
energies of a desired high temperature finally in the last of said stages
is simpler in mechanism, suffers less from possible temperature dispersion
and attains the object more easily than the system wherein the
heat-transfer medium is heated immediately to a high temperature in one
stage.
It is, therefore, an object of this invention to provide a system for the
accumulation of heat from the solar energy which permits said energy of a
high temperature to be obtained economically.
SUMMARY OF THE INVENTION
To accomplish the object described above, the present invention provides a
system for the accumulation of the solar radiant energy adapted to have
the solar radiant energy absorbed by heat-absorption means and transferred
therefrom to a heat-transfer medium, which system incorporates a few
heat-absorption members arranged at different stages in a series
connection and provided with selectively penetrating membranes capable of
reflecting electromagnetic wave energies optimum for successively elevated
temperatures of the heat-transfer medium at said stages, with said
heat-absorption members connected in the increasing order ot optimum rated
temperature ranges in their respective selectively penetrating membranes.
Having the heat-transfer medium divided into a few stages and heated under
conditions optimum for the respective rated temperature ranges at said
stages as described above, the system according to this invention can
obtain heat energies at a desired high temperature with high efficiency.
Other objects and other characteristic features of the present invention
will become apparent from the description to be given in further detail
hereinbelow with reference to the accompanying drawings.
BRIEF EXPLANATION OF THE DRAWINGS
FIG. 1 represents spectral distributions of the solar radiant energy.
FIG. 2 represents an enlarged view of the cardinal portion of a
heat-absorption member used for absorbing the solar radiant energy.
FIG. 3 is a graph illustrating the properties, indices of penetration and
reflection, of a selectively penetrating membrane for use in said
heat-absorption member.
FIG. 4 is an explanatory diagram indicating the condition in which the
solar radiant energy are absorbed.
FIG. 5 is an explanatory diagram indicating the pattern of heat
accumulation according to the present invention.
FIG. 6 represents a sectional view of one preferred embodiment of the
system for heat accumulation according to the present invention.
FIG. 7 is a graph indicating the properties, i.e. wavelength and index of
reflection, of the selectively penetrating membrane for use in the present
invention.
FIG. 8 is a perspective view illustrating another preferred embodiment of
the system for heat accumulation according to this invention.
FIGS. 9 through 11 are explanatory diagrams indicating devices for the
concentration of the solar radiant energy for the purpose of the present
invention.
FIG. 12 is a schematic diagram illustrating a complete system for
practicing the heat accumulation contemplated by the present invention.
DETAILED DESCRIPTION OF THE INVENTION
The spectrum of solar energy which is representative of electromagnetic
wave energies is shown in FIG. 1 (Curve I). In the graph, the vertical
axis represents the relative intensity of energy and the horizontal axis
the wavelength.
Solar energy has its peak intensity in the neighborhood of a wavelength of
0.5.mu.m and has a color temperature of 5,900.degree.K. In said graph, the
characteristic of a black body at a color temperature of 700.degree.K is
shown as Curve II. This Curve II indicates that the fraction of the solar
energy corresponding to the color temperature of 700.degree.K has a
wavelength of about 4.5.mu.m and that the intensity of energy at this
wavelength is extremely small compared with that at a wavelength of about
0.5.mu.m. The greater part of the solar energy is concentrated in the
range of wavelengths between 0.3 and 2.mu.m. The solar energy showered
upon every square 1Km of the earth's surface lying perpendicularly to the
sun's rays is close to about 1,000,000 KW. If this electromagnetic wave
energy is efficiently absorbed in the form of heat of high temperature, it
can be utilized as an infinite pollution-free energy source requiring no
fuel.
In view of the foregoing state of affairs, the inventors have proposed a
solar energy absorption device which absorbs the solar radiant energy at a
high percentage and suffers very little loss of the absorbed energy
through radiation. FIG. 2 is an enlarged sectional view of a selectively
penetrating membrane 1 which is used in said absorption device. The upper
side of this selectively penetrating member 1 is covered with a glass
sheet 2. When the solar energy absorption device of such construction is
irradiated with the solar radiant energy E, a substantial part of the
energy penetrates through the selectively penetrating membrane 1. The
energy which has penetrated the membrane is absorbed by the
heat-absorption member 3 disposed inside. The heat-absorption member 3
which has consequently gained in temperature is then cooled as it releases
the heat to a coolant 4 flowing thereunder and, thereupon, radiates a
radiant energy of a greater wavelength than that of the incoming energy.
The radiated energy, however, is reflected by said selectively penetrating
membrane 1 to be absorbed again by the heat-absorption member 3. A typical
condition of said radiation and subsequent reabsorption is represented by
the curve II in the diagram of FIG. 1. In this manner, absorption of the
solar radiant energy can be effected efficiently. The selectively
penetrating membrane 1 may be constructed in a single layer or in a
multiplicity of layers. Alternatively, it may be made in the shape of a
metallic lattice like mesh, with the size of meshes selected so as to suit
the wavelength of the electromagnetic wave energy desired to be passed.
The selectively penetrating membrane of this construction will permit
passage of electromagnetic wave energies of a specific wavelength only. As
the material for the metallic mesh, there can be used various metals such
as, for example, gold, tin, aluminum and antimony. The selectively
penetrating membrane 1 having any of the properties shown in FIG. 3 can be
obtained by combining films of different metals or by selecting the
thickness of such films suitably. In FIG. 3, the horizontal axis
represents the wavelength (in .mu.m) and the vertical axis the index of
penetration and reflection (in %). In the graph, the curve I indicates the
relative distribution of the solar radiant energy, the curve II the index
of penetration in the selectively penetrating membrane, the curve IIIa the
index of reflection of the selectively penetrating membrane of Sn-1% Sb
system satisfying nh = 0.68.mu.m (n : index of diffraction and h :
thickness), the curve IIIb the index of reflection of the selectively
penetrating membrane of Sn-30% F satisfying nh = 0.83.mu.m, the curve IV
the index of penetration of glass and the curve V the index of reflection
of glass respectively.
Now, a description will be made of the heat-absorption member to be used in
said device.
As the heat-absorption member, there may be used what is obtained by
depositing blackbody or some other substance having an equal index of
absorption on the surface of a basal metal such as of copper or stainless
steel. The desired heat absorption can be attained more efficiently by
using heat-absorption members especially designed to provide improved
absorption efficiency. Examples are a light-heat conversion cell whereby
the incident solar radiant energy is caused to fall on a junction of n and
p semiconductors to generate heat through the phenomenon of thermal
oscillation and, in the case of a short wavelength, to liberate secondary
photons and the electrons excited by said photons cause a flow of
short-circuit electric current in the conductor to bring about generation
of Joule's heat which is accumulated directly in its unmodified form of
heat and a modulation type light-heat conversion system which is obtained
by conferring upon said light-heat conversion cell an additional function
to obtain harmony with the electromagnetic wave energy expected to be
absorbed.
A typical apparatus for the absorption of the solar radiant energy which is
composed of the selectively penetrating membrane and the heat-absorption
member described above is illustrated in FIG. 4. In the diagram, 1 denotes
the selectively penetrating membrane disposed on the internal wall of the
glass cylinder 2 whose interior is maintained under vacuum (of the order
of 10.sup.-.sup.3 to 10.sup.-.sup.4 Torr., for example). The
heat-absorption member 3 is disposed inside the cylinder. In the interior
of the heat-absorption member 3, a gaseous or liquid heat-transfer medium
4 flows to conduct the heat accumulated by the heat-absorption member 3
out of the member. As the heat-transfer medium there is used CO.sub.2,
H.sub.2 O, Na, NaK or other similar substance. Denoted by 5 is a
converging lens such as a convex lens or fresnel lens. By the apparatus of
this construction, the solar radiant energy E is converged, passed through
the selectively penetrating membrane 1 and allowed to impinge upon the
heat-absorption member 3 to be absorbed thereby. And a part of the solar
radiant energy which has escaped being absorbed and the energy which has
been radiated by the heat-absorption member 3 are both reflected by the
selectively penetrating membrane 1 to impinge upon the heat-absorption
member 3 again. Since this cycle of radiation and reabsorption is
repeated, the greater part of the solar radiant energy E is finally
absorbed by the heat-absorption member 3.
A study of the process of temperature elevation which occurs in the
heat-transfer medium 4 of the aforementioned apparatus for the absorption
of the solar radiant energy shows that the heat-transfer medium 4 which
has entered the heat-absorption member 3 at one end thereof gradually
gains in temperature as it flows through said member and it is discharged
at an elevated temperature from the other end. It follows as a consequence
that the temperature of the heat-transfer medium 4 is fairly different at
the inlet and at the outlet and, for this reason, the heat-absorption
member 3 itself has a temperature gradient. This means that the wavelength
of the solar radiant energy to be radiated from the heat-absorption member
3 similarly differs at the first part and at the last part of the member
3. As is evident from the foregoing explanation, if the properties of the
selectively penetrating membrane 1 are rendered uniform throughout the
entire length of the heat-absorption member 3, then there may be entailed
a disadvantage that the amount of the solar radiant energy lost through
radiation will increase to an extent of inpairing the overall efficiency
of the apparatus.
The present invention has been developed with a view to eliminating the
disadvantages described above. The present invention will be described
specifically hereinbelow.
FIG. 5 represents a block diagram indicating the principle of the layout of
the temperature-elevation system for the purpose of this invention. In the
diagram, A denotes a heat-absorption unit of the preheating stage which
possesses a selectively penetrating membrane capable of reflecting
electromagnetic wave energy of a low temperature, B a second-stage
heat-absorption unit which serves the purpose of elevating to a heat
energy of an increased temperature the heat-transfer medium received in a
preheated state from the heat-absorption unit and which, for tbat purpose,
possesses a selectively penetrating membrane capable of reflecting
electromagnetic wave energy of a higher temperature than that of the
heat-absorption unit A. C denotes a heat-absorption unit which functions
to elevate the heat-transfer medium to a heat energy of the high
temperature desired to be attained and, for this purpose, possesses a
selectively penetrating membrane capable of reflecting electromagnetic
wave energy of a still higher temperature than that of the heat-absorption
unit B. These heat-absorption units A, B and C are arranged in a series
connection. While the heat-transfer medium is sent through the three
units, it is preheated to 200.degree.C, for example, during its travel
through the unit A, then to 600.degree. C during its passage through the
unit B and finally to 1,200.degree. C during its flow through the unit C.
FIG. 6 illustrates one preferred embodiment of the present invention,
wherein A, B and C denote heat-absorption capsules similar in
construction. Selectively penetrating membranes 12A, 12B and 12C are
formed on the inner faces of transparent vacuum containers 11A, 11B and
11C respectively and heat-absorption members 13A, 13B and 13C are disposed
respectively inside said vacuum containers 11A, 11B and 11C. Inside the
heat-absorption members 13A, 13B and 13C, there are concentrically
disposed pipes 14A, 14B and 14C. The interior of the heat-absorption
member 13A and the pipe 14B are connected via a pipe 15A and the interior
of the heat-absorption member 13B and the pipe 14C are connected via a
pipe 15B.
What is important in this connection is the fact that the selectively
penetrating membranes 12A, 12B and 12C disposed in the different
heat-absorption capsules be not possessed of equal properties but capable
of reflecting electromagnetic wave energies of successively shorter
wavelengths. Specifically, as the heat-transfer medium 16 is supplied
through the pipe 14A, it reverses the direction of its flow at the
extremity of the pipe 14A to advance through the opening between the
heat-absorption member 13A and the pipe 14A and gradually gain in
temperature, then departs from the heat-absorption member 13A and enters
the pipe 14B through the pipe 15A. In much the same way, it is heated
during its travel through the heat-absorption capsule B and further heated
during its flow through the heat-absorption capsule C eventually to be
elevated to the temperature desired to be attained. The heat-transfer
medium thus elevated to the target temperature is discharged as the
output. As described above, the heat-transfer medium 16 has different
degrees of temperature in the heat-absorption capsules A, B and C. If the
selectively penetrating membranes 12A, 12B and 12C are possessed of equal
properties, the solar radiant energy cannot efficiently be entrapped
inside the heat-absorption capsules A, B and C, with the result that some
of the absorbed solar radiant energy escapes from the system through
radiation.
To preclude this possibility, therefore, the properties of the selectively
penetrating mambranes 12A, 12B and 12C are differentiated as indicated in
FIG. 7. In this diagram, the horizontal axis represents the wavelength and
the vertical axis the index of reflection and the curves 12A, 12B and 12C
indicate the properties of the selevtively penetrating membranes 12A, 12B
and 12C respectively. This diagram clearly indicates that the selectively
penetrating membrane 12B is capable of reflecting and entrapping
electromagnetic wave energies of a shorter wavelength than that of
electromagnetic wave energies reflected and entrapped by the membrane 12A
and, by the same token, the membrane 12C is capable of reflecting and
entrapping electromagnetic wave energies of a shorter wavelength than that
of electromagnetic wave energies reflected and entrapped by the membrane
12B.
The overall efficiency of the system under discussion can be notably
improved by using the selectively penetrating membranes 12A, 12B and 12C
which have properties optimum for the respective rated degrees of
temperature of the heat-transfer medium 16 in the different capsules as
illustrated in FIG. 6. The individual properties for the selectively
penetrating membranes 12A, 12B and 12C can be determined in accordance
with the principle set forth with reference to FIG. 3.
One example of the method followed for the manufacture of selectively
penetrating membranes of the aforementioned description will be cited:
Indium or tin is uniformly deposited on the inner surface of a glass pipe
in accordance with the vacuum evaporation coating method. The glass pipe
is introduced into an electric furnace, heated to a temperature in the
range of from 320.degree. to 350.degree. C and subjected to gradual forced
oxidation. Accordingly, an indium oxide membrane, tin oxide membrane or
membrane composed of a mixture of these substances is formed on the inner
surface of the glass pipe.
Electromagnetic wave energy having a temperature above 150.degree. C is
reflected by a membrane having a thickness of about 1,000A. When a
membrane of such thickness produced in the manner described above is
applied to the heat-absorption apparatus A as a selectively penetrating
membrane, the heat-transfer medium can be heated up to about 130.degree.
C. If the thickness of the membrane is made 2,000A, electromagnetic wave
energy having a temperature above 300.degree. C is reflected by the
membrane. Accordingly, when such a membrane is applied to the
heat-absorption apparatus B as a selectively penetrating membrane the
heat-transfer medium can be heated up to about 250.degree. C. Similarly,
if the width of the membrane is 3,200A, electromagnetic wave energy having
a temperature above 600.degree. C is reflected by the membrane.
Accordingly, when such a membrane is applied to the heat-absorption
apparatus C as a selectively penetrating membrane the heat-transfer medium
can be heated up to about 550.degree. C.
In this way, it is possible to effectively obtain heat energy of a high
temperature.
FIG. 8 illustrates another preferred embodiment of the present invention,
wherein selectively penetrating membranes 12A, 12B and 12C are formed
continuously in the order mentioned on the inner face of a transparent
vacuum container 11 and heat-absorption member 13 is disposed inside said
vacuum container 11, with the interior of said member 13 adapted to permit
flow of the heat-transfer medium 16. And 17 denotes a curved reflecting
mirror of a parabolic cross section and 18 denotes a prop for supporting
the mirror in position. As the heat-transfer medium 16 travels upwardly
through the heat-absorption member 13, it gains in temperature
increasingly more in the upward direction. Thus, the properties of the
selectively penetrating membranes 12A, 12B and 12C have only to be
selected in the similar relationship as described above with reference to
FIG. 5.
The selectively penetrating membranes used in the preferred embodiments
cited above invariably have their properties varied stepwise. If there are
used those membranes whose properties are continuously varied in
conformity with the gradient of temperature elevation, then the system may
be expected to perform with much more improved efficiency.
When heat-absorption devices provided with selectively penetrating
membranes which are capable of reflecting electromagnetic wave energies
optimum for the respective rated degrees of temperature of the
heat-transfer medium at the different stages are arranged in a series
connection as described above, the desired accumulation of the heat
energies of high temperature can be attained with enhanced efficiency by
differentiating the individual heat-absorption devices in terms of the
method for absorption of the solar radiant energy.
Where heat energies of high temperature are to be obtained by efficient
absorption of the solar radiant energy, for example, it will suffice for
the purpose to utilize parabolic reflecting mirrors each adapted to
concentrate the solar radiant energy at one point and allow the foci to
fall on the respective heat-absorption devices in use.
In such point-focussing type heat-absorption devices, the points at which
the solar radiant energy is concentrated tend to deviate from the fixed
foci of the reflecting mirrors and, consequently, cause the absorption
efficiency of the solar radiant energy to be impaired to an extreme
extent. Thus, the point-focussing type heat-absorption device should be
possessed of a chasing mechanism of high precision enough for the solar
radiant energy to be focussed at a fixed point at all times. Moreover, it
requires the highest technical level and is limited in terms of dimensions
on account of the precision of curvature achievable at all. Where the
heat-absorption in a fixed area is considered, therefore, this method of
absorption of the solar radiant energy proves to be most expensive. In
addition, this method has no sufficient reliability from the long range of
view and entails difficulty from the standpoint of mechanical performance
or maintenance. It is, therefore, wise to adopt a plane-focussing type
light-absorption device for the preheating-stage unit which suffers a
relatively small loss of energy for the whole system, a line-focussing
type light-absorption device for the second-stage heat-absorption unit,
and a point-focussing type light-absorption device for the last-stage
heat-absorption unit.
Heat-absorption apparatuses utilizing such methods of light-absorption will
be described with reference to FIGS. 9 through 12.
FIGS. 9(a) and (b) are a perspective view and a sectional side view
respectively of a flat type of plane-focussing type heat-absorption
apparatus A' for use in the preheating stage. In FIG. 9(b), 2 denotes each
of two glass plates and 1 each of two selectively penetrating membranes
formed on the inner faces of said glass plates. The interior of the glass
plates is maintained under a low pressure to prevent release of thermal
energy. Denoted by 3 is a heat-absorption member serving to absorb the
solar radiant energy E. In the illustrated embodiment, there is used a
heat-absorption member capable of a temperature elevation to the level of
150.degree. - 200.degree. C suitable for use in the preheating stage. As
the selectively penetrating membrane, there is used a membrane capable of
reflecting radiant energies of a temperature of 200.degree. C. The
temperature of the heat-transfer medium 4 is elevated by the heat energy
which is absorbed by this heat-absorption member 3. Reference numeral 6
denotes a heat-insulation material.
Since the heat-absorption member 3 which is used in the heat-absorption
apparatus A' is in the shape of a flat plate, the area on which the solar
radiant energy E impinges is large and the selectively penetrating
membrane 1 is also large proportionally. The loss of output per unit area
increases with the increasing area of the selectively penetrating membrane
1. Therefore, this heat-absorption apparatus A' has inferior efficiency
and cannot be expected to provide any temperature elevation beyond a
certain level. Thus, it is proposed to be used as the first-stage
preheating unit. The output of this unit is then forwarded to the
heat-absorption apparatus B' for the second stage.
FIG. 10 represents a perspective view of the heat-absorption apparatus B'
having a curved reflecting mirror for use in the second stage, wherein 7
denotes a reflecting mirror which is utilized in lieu of a convex lens or
fresnel lens 5 of the type to be used in the heat-absorption device
described previously with reference to FIG. 4. As the solar radiant energy
E impinges upon the reflecting mirror 7, the portion of the solar radiant
energy which is reflected on the mirror surface is absorbed by the
heat-absorption member 3. The absorbed heat energy is transferred to the
heat-transfer medium 4 flowing inside the heat-absorption member 3 and
consequently conveyed to the subsequent stage. Since the reflecting mirror
7 of this heat-absorption apparatus B' has a cylindrical reflecting
surface, the heat-absorption member 3 is disposed in the shape of a line
in the axial direction (namely, the direction of the length). In other
words, this is a line-focussing type heat-absorption apparatus B'. In this
apparatus, any deviation of the focus due to possible day-after-day change
in the angle to elevation of the direction of the solar radiant energy E
occurs in the axial direction of the reflecting mirror. Thus, the
apparatus does not require daily adjustment but suffices with weekly or
monthly adjustment for the elimination of such change. It does not suffer
from decline of efficiency. Thus, the heat-transfer medium 4 can be
elevated to a higher degree of temperature. For use as the heat-absorption
unit in the second stage, it is essential that the apparatus be provided
with a sun-chasing mechanism designed to warrant the fullest utilization
of the solar radiant energy E. The heat-transfer medium 4 which has been
elevated to said higher temperature is now forwarded to the
heat-absorption apparatus C' in the final stage. It goes without saying
that the reflecting mirror 7 in the heat-absorption apparatus B' is not
necessarily limited to such cylindrical shape as described above but may
be in the shape of a flat plate insofar as it enables the solar radiant
energy to be focused in a line.
FIG. 11 represents a perspective view of the final-stage heat-absorption
apparatus C' adapted to obtain the heat energy of the desired high
temperature. It may be in the shape of a convex lens or fresnel lens 5
like the one used in the heat-absorption apparatus illustrated in FIG. 4.
Alternatively, it may be formed in the shape of a flat plate so far as the
reflecting mirror produces a point focus. In the illustrated embodiment, a
parabolic reflecting mirror 8 is disposed as a typical example.
The illustrated design is characterized in that the solar radiant energy E
which is reflected by the parabolic reflecting mirror 8 is focussed to one
small point. Since only the forward end of the heat-absorption member 3 is
exposed to serve as the surface for heat absorption and the remaining
portion thereof is covered with a heat-insulation material, the area of
the heat-absorption member 3 is notably limited. The heat-absorption
member 3 of this construction can obtain heat energy of still higher
temperature because the heat-transfer medium 4 is delivered to said
surface for heat-absorption and the reflected solar radiant energy E is
concentrated at this point. On the other hand, however, the
point-focussing type heat-absorption apparatus is inevitably required to
be provided with a sun-chasing mechanism of high precision enough to
prevent said point focus from deviating from the fixed point on said
surface for heat-absorption owing to the change in the angle to elevation
of the direction of the solar radiant energy E with lapse of time. While
the focus formed in the heat-absorption apparatus B' for use in the second
stage is tolerated to deviate in the axial direction of the reflecting
mirror, the focus formed in the case of the heat-absorption apparatus C'
is not allowed to deviate from the fixed point in any direction. This
means that this apparatus requires the sun-chasing to be effected in the
three dimensions of X, Y and Z. As already described, the selectively
penetrating membranes for use in these heat-absorption apparatuses are
required to be capable of reflecting radiant electromagnetic energies of
magnitudes corresponding to the respective degrees of temperature rated
for the different stages concerned.
FIG. 12 is one preferred embodiment of the present invention, illustrating
the layout of a multi-stage system. In the diagram, A', B', and C' stand
respectively for the heat-absorption apparatuses described above, 21 and
22 for heat accumulators, 23 for a heat accumulator and exchanger, 24 for
a turbine, 25 for a generator, 26 for a condenser, 27 and 28 for pumps, 29
and 30 for heat-absorption members composing the point-focussing type
heat-absorption apparatus C', 31 for a convex lens or fresnel lens and 32
for a parabolic reflecting mirror adapted to form a point focus.
The operation of this system will be explained. The heat-transfer medium 4
is preheated by the heat-absorption apparatus A' and forwarded to the
heat-absorption apparatus B' in the subsequent stage, wherein it is
further heated. At this time, part of the heat energy is stored in the
heat accumulator 21 for the purpose of precluding possible variation of
the output due to temporary clouding of the sky. There are installed two
heat-absorption apparatuses B'. The heat-transfer medium 4 which has
flowed through the heat accumulator 21 advances via the latter
heat-absorption apparatus B' into the heat accumulator 22. To the heat
accumulator 22 are delivered the heat energy which the heat-absorption
member 29 has obtained from the heat-absorption apparatus C' using the
convex lens or fresnel lens 31 and the heat energy which the
heat-absorption member 30 has acquired from the parabolic reflecting
mirror 22. In this heat accumulator 22, the heat-transfer medium 4 reaches
the highest degree of temperature and it is forwarded to the subsequent
heat accumulator and exchanger 23. Inside the heat accumulator and
exchanger 23, the water delivered by the pump 27 is converted into steam
of high temperature and high pressure. The steam rotates the turbine 24 to
cause the generator 25 to produce electric power. The steam which has
worked the turbine 24 is condensed to water in the condenser 26 and is
recycled to the heat accumulator and exchanger 23. On the other hand, the
heat-transfer medium 4 which has departed from the heat exchanger 23 is
again returned to the heat-absorption apparatus A'. Then, the
heat-transfer medium 4 is put to circulation by the pump 28.
It should be noted that the system illustrated in FIG. 12 is only
representative, and not in the last limitative, of the present invention.
Needless to say, it is permissible to adopt line-focussing heat-absorption
devices for the apparatuses A' and B' or to select and combine suitable
quantities and types of heat-absorption apparatuses A', B' and C' to suit
the occasion.
As described in detail above, in the solar radiant energy absorption system
utilizing selectively penetrating membranes, the present invention
contemplates using selectively penetrating membranes the properties of
which are varied so as to be optimum for the respective extents of
temperature elevation rated for the heat-transfer medium at different
stages of heat absorption, so that the energy which constantly attempts to
escape to the exterior of the system can be reflected by said membranes to
entrapped within the system. Thus, the system according to this invention
enables the solar radiant energy to be converted quite efficiently into
heat by means of the heat-transfer medium.
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