U.S. patent number 3,774,224 [Application Number 05/267,755] was granted by the patent office on 1973-11-20 for radome.
This patent grant is currently assigned to Sumitomo Electric Industries Ltd.. Invention is credited to Tetsuo Hatano, Toshihiko Ohkura, Yoshizo Shibano, Shohachiro Yamashita.
United States Patent |
3,774,224 |
Shibano , et al. |
November 20, 1973 |
RADOME
Abstract
A one-half-wavelength radome is made of a corrugated plate of
ordinary dielectric material. The corrugated plate is made such
that the pitch of corrugation is smaller than the wavelength at the
operating frequency and the height of corrugation is effectively
equal to one-half the wavelength at the operating frequency. A
radome of this construction exhibits good electrical properties of
small reflection and low dielectric loss and high mechanical
strength.
Inventors: |
Shibano; Yoshizo (Osaka,
JA), Hatano; Tetsuo (Osaka, JA), Ohkura;
Toshihiko (Osaka, JA), Yamashita; Shohachiro
(Osaka, JA) |
Assignee: |
Sumitomo Electric Industries
Ltd. (Osaka, JA)
|
Family
ID: |
12786635 |
Appl.
No.: |
05/267,755 |
Filed: |
June 30, 1972 |
Foreign Application Priority Data
|
|
|
|
|
Jun 30, 1941 [JA] |
|
|
46/47843 |
|
Current U.S.
Class: |
343/872 |
Current CPC
Class: |
H01Q
1/42 (20130101) |
Current International
Class: |
H01Q
1/42 (20060101); H01q 001/42 () |
Field of
Search: |
;343/872,873 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Lieberman; Eli
Claims
What is claimed is:
1. A radome comprising a corrugated plate of dielectric material
wherein the pitch of corrugation is smaller than the wavelength at
the operating frequency, the height of corrugation is one-half of a
wavelength at the operating frequency, and the section thickness t
of said corrugated plate is equal to:
.lambda./2.sqroot..epsilon..sub.e ,
where .epsilon..sub.e = equivalent dielectric constant of said
corrugated plate as determined from the dielectric constant and
thickness of the plate material, and .lambda. = the wavelength at
the operating frequency.
Description
BACKGROUND OF THE INVENTION
This invention relates to a radome and more particularly to a
radome for the superhigh frequency band.
There are many kinds of radomes in the prior art, such as thin
plate radomes, one-half-wavelength radomes, etc. A thin plate
radome is made of a thin dielectric plate which is thin in
comparison with the wavelength at the operating frequency, thus
being simple to construct. It has been, therefore, used frequently
for the VHF band or the lower frequency bands. Where the wavelength
is shorter, however, it is necessary to make its thickness very
small in order to ensure the requisite electric properties.
Therefore, this type of radome is no longer practical because of
the difficulty with respect to mechanical strength.
A one-half-wavelength radome is made of a dielectric plate with the
thickness equivalent to one-half the wavelength at the operating
frequency. This eliminates the reflection of the wave by the
radome. In actuality, however, especially where the frequency is
high, there is a residual reflection due to the dielectric loss
produced in the interior of the dielectric material. Thus, the
desired properties may not be obtained. Moreover, the reflection
increases as the dielectric constant of the dielectric material
increases. It is, therefore, necessary to select dielectric
material having low dielectric constant and low dielectric loss as
the dielectric material for a one-half-wavelength radome.
SUMMARY OF THE INVENTION
It is a primary object of this invention to overcome the
disadvantages found in the prior art.
It is another object of this invention to provide a radome usable
for high frequency band, particularly for the SHF band.
Another object of this invention is to provide a
one-half-wavelength radome having good electrical properties of
small reflection and low dielectric loss.
Still another object of this invention is to provide a
one-half-wavelength radome made of ordinary dielectric material,
without the use of a dielectric material having an especially low
dielectric constant and low dielectric loss, thus having good
electrical properties of small reflection and low loss.
The radome according to this invention is composed of a corrugated
plate of dielectric material. The corrugated plate is constructed
such that the pitch of corrugation is smaller than the wavelength
at the operating frequency and the height of corrugation is
effectively equal to one-half of the wavelength at the operating
frequency. Such a corrugated plate has an effective low dielectric
constant, which is smaller than the dielectric constant of a flat
plate, and it may be substituted for a flat dielectric plate with
an equivalent dielectric constant. Moreover, the corrugated plate
shows low dielectric loss because of the existence of air between
the crests of corrugations.
Accordingly, it is possible to obtain a radome having good
electrical properties of small reflection and low dielectric loss,
using an ordinary dielectric material. Furthermore, the radome has
good mechanical properties of high mechanical strength and high
flexibility because of the corrugated structure.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a cross sectional view of the radome embodying this
invention.
FIGS. 2 and 3 are the drawings for illustrating the operation of
the radome according to this invention.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
Referring to FIG. 1, a corrugated plate 1 is made by corrugating a
dielectric plate of FRP (fiber-reinforced plastic) or the like. The
pitch P of the corrugations of the corrugated plate 1 is made
smaller than the wavelength at the operating frequency and the
height t of the corrugation is made effectively to be one-half the
wavelength at the operating frequency. The form of the corrugations
of the corrugated plate 1 may be as desired, such as a triangular
wave, sine wave, continuation of arcs, etc.
Now the operation of the radome according to this invention will be
explained with reference to FIGS. 2 and 3. SInce the pitch P of the
corrugations of the corrugated plate 1 is smaller than the
wavelength at the operating frequency, if the cross section of the
corrugated plate 1 is observed along any desired line A-A' parallel
to the plane of the corrugated plate 1 as shown in FIG. 1, it is
noted that there are two pieces of dielectric layers 2 having a
thickness .DELTA. t in every pitch P of the corrugations as shown
in FIG. 2. Even though the distance between these two pieces of
dielectric layers 2 varies depending on the position of the cross
section line A-A', the distance between them is constant in every
cycle of the pitch. Consequently, the equivalent dielectric
constant of the corrugated plate 1 is equal to the equivalent
dielectric constant of a model which is composed of two pieces of
dielectric layers 2 having a thickness .DELTA. t in every pitch P
as shown in FIG. 3.
When the incident direction of the wave is parallel to the normal
line of the plane of the corrugated plate 1 and the direction of
the electric field thereof is perpendicular to the plane of the
paper, the equivalent dielectric constant of this model is:
.epsilon..sub.e = 1 + ( .epsilon..sub..gamma. - 1) 2 .DELTA. t/P
(1)
when the direction of the electric field is parallel to the plane
of the paper, the formula is: ##SPC1##
Suppose that P = 10 mm and .DELTA. t = 1 mm in the case the
wavelength is 25 mm and that the dielectric material is FRP and its
dielectric constant .epsilon..sub..gamma. is 4. Then, from the
formula (1)
.epsilon..sub.e = 1.6 . (3)
Also, from the formula (2)
.epsilon..sub.e = 1.177 . (4)
In both cases, the dielectric constant is considerably lower than a
flat plate of the same material.
Comparing the formulas (3) and (4), the formula (4) shows a smaller
dielectric constant. Therefore, since it is possible to select the
relationship between the corrugated plate 1 and the direction of
polarization of the wave, it is advantageous to select such a
relationship wherein the direction of the electric field is
parallel to the plane of the paper.
It is apparent from the formulas (1) and (2) that the corrugated
plate 1 shown in FIG. 1, which is made of dielectric material
having dielectric constant .epsilon..sub..gamma., may be
substituted by a uniform dielectric plate having dielectric
constant .epsilon..sub.e given by the formula (1) or (2).
In consequence, if the thickness t of the corrugated plate 1 shown
in FIG. 1 is effectively to be one-half a wavelength then using
formulas (1) and (2)
t = .lambda./2.sqroot..epsilon..sub.e
where .lambda. is the wavelength of the operating frequency. Thus,
it is possible to decrease the effective dielectric constant as can
be seen from the figures of the formulas (3) and (4).
Moreover, since there are only two pieces of dielectric layer in
every pitch P of the corrugations of the corrugated plate 1 and the
remainder of the space is filled with air, the dielectric loss, as
well as the dielectric constant, is also decreased.
As described above, the radome according to this invention shows
good electrical properties of a low dielectric constant and loss,
though an ordinary dielectric material is used instead of special
dielectric materials having especially low dielectric constants and
losses.
Furthermore, the radome of this invention has superior mechanical
strength in the direction of the ridges of the corrugations of the
corrugated plate. It is therefore advantageous to design the radome
to bear the load in that direction. Also, it has flexibility with
respect to bending deformation in the direction normal to the
ridges of the corrugations, so that it is easy to make cylindrical
or other shaped radomes with the corrugated plate.
* * * * *