[0001] The invention relates to radar reflectors comprising at least six corner reflectors
divided outwardly of a major axis and more particularly but not solely to such reflectors
for use on sea vessels.
[0002] Radar reflectors are employed to improve the radar echoing properties of objects
or land formations with a view to improving the detection of such objects or formation
by radar scanning equipment. Radar reflectors of this type to be fully efficient should
reflect radar waves back parallel to their initial direction.
[0003] Known radar reflections such as the standard octahedral provide a polar reflection
which exhibits a considerable reduction in response between reflector lobes and which
exhibits a particularly poor response when healed.
[0004] Similar disadvantages occur with the AGA reflector as described in British Patent
Number 681 666 in which reflectors are disposed along a single common helical path.
In many applications it is advantageous if the reflector is capable of providing reflection
of radar signals in any direction and in applications such as in sea vessels it is
advantageous if this capability is not badly affected upon heeling of the vessel.
[0005] Corner reflectors, constructed of three sheets of reflective material which are mutually
perpendicular, i.e., orthogonal re-entrant trihedrals, are known to provide effective
reflection over a range of angles of incidence, with the signal strength decreasing
as the obliquity increases, forming a lobe.
[0006] This invention has been arrived at by consideration of the above mentioned requirements
and seeks to provide a radar reflector which provides effective reflection of signals
received from any direction in a horizontal plane.
[0007] According to the invention there is provided a radar reflector comprising at least
six corner reflectors directed outwardly of and disposed helically about a major axis
of the reflector along two successive helical paths one of which paths is sinistrorse
and the other of which paths is dextrorse.
[0008] The location of the reflectors along two successive helical paths of opposite hand
results in a simple and particularly good response characteristic over a desired azimuth
and provides a reflector that is still effective when heeled. The corner reflectors
are preferably evenly distributed to cover the full 360
0 of horizon.
[0009] In one advantageous form of the invention ten corner reflectors are employed.
[0010] A reflector in accordance with the invention may be formed from a strip of radar
reflective sheet material folded in alternate directions along fold axes spaced apart
on the strip and extending transversely across the strip with two consecutive ones
of the fold axes disposed intermediately being substantially parallel and the remaining
folds being alternately convergent and divergent in a direction from one edge to the
opposite edge of the strip the folds dividing the strip into sections adjacent sections
being disposed at right angles and a separator plate being provided between and at
right angles to each pair of adjacent sections to form therewith two corner reflectors.
The separator plates may be rectangular but rectangular plates having one point cut
off are to be preferred, the plate being positioned such that the edge where the point
has been removed is remote from the adjecent sections. This cut away avoids interaction
with reflections from other ones of the corner reflectors.
[0011] The edge of the strip and/or the cut away point of the separator plates can be profiled
such that they have an edge profile conforming to part of the internal surface of
a cylindrical housing to permit slidable and secure location of the reflector within
the housing.
[0012] In order that the invention and its various other preferred features may be understood
more easily, two embodiments thereof will now be described, by way of example only,
with reference to the drawings, in which:-
Figure 1 is an elevational view of a radar reflector constructed in accordance with
the invention,
Figure 2 shows a blank strip for bending to form the reflector of Figure 1 illustrating
the bending axes,
Figure 3 shows horizontal projections of two adjacent sections of the target radar
reflector of Figure 1 illustrating angle of twist,
Figures 4a and 4b are circular and elliptical sections of a stepped helix,
Figures 5a and 5b are schematic elevational views of opposite sides of a stepped helix,
Figure 6a is a schematic elevational view of a corner reflector,
Figure 6b is a schematic plan view of the corner reflector of Figure 6a,
Figures 7a and 7b are schematic tilted corner views in plan and perspective respectively.
Figure 8 is a polar diagram showing schematically the construction viewed from above.
Figure 9 is a predicted polar diagram showing the response of the radar reflector,
and
Figure 10 is a side view of a demountable reflector constructed in accordance with
the invention and folded into a flat condition.
[0013] In the drawings Figure 1 shows a particularly advantageous form of the invention
hauled up to the cross tree of a mast. The radar reflector indicated generally at
10 is formed of a strip 10a of radar reflective material e.g. 18 s.w.g. sheet duraluminium
or stainless steel. The strip is folded along axes lla, 12a, 12b which extend transversely
across the strip in concertina fashion. The folds divide the strip into a series of
sections 11, 12 and 13 adjacent ones of which are disposed at right angles.
[0014] A flat strip suitable for folding to form in this case triangular divisions is shown
in Figure 2. The chain lines indicate axes at which the fold is to be forwards and
the dot and chain lines indicate axes at which the fold is to be backwards. It will
be apparent from the drawing that the fold axes in this case are all of the same length.
[0015] The fold axes (12 12b) defining the centre section 12 of the strip are parallel,
the centre section being of parallelogram form. The other fold axes (lla) are alternately
convergent in a direction from one edge to the opposite edge of the strip and divide
the strip into triangular sections 11 and end sections 13 of basically trapezium form
which end sections are cut away to one side of an axis extending at right angles to
their adjacent fold axis to leave only the portion with the shorter side at the edge
of the strip.
[0016] The folded strip forms a spine having seven sections adjacent ones of which are disposed
at right angles. Each pair of adjacent surfaces of the sections is provided with a
sheet metal divider 14 which is affixed thereto by for example rivetting or welding
at right angles to both surfaces to form a pair of corner reflectors 14a, 14b in the
form of orthogonal re-entrant trihedrals which are capable of acting as elementary
reflectors.
[0017] The radar reflector can be hung from one end from a point adjacent the axis at which
the end section is cut away or can be hoisted by a similar connection at each end
as shown in Figure 1. The reflector hangs normally by its own weight with the surfaces
of the sections inclined, alternately at 4So above and below the horizontal.
[0018] The maximum reflecting capability of a corner reflector occurs along an axis extending
equiangularly between the faces of the corner and this axis may be termed the directional
axis of the reflector. When the reflector is hung as previously described the directional
axes are inclined above or below the horizontal at a constant angle.
[0019] The folding of the strip to form the spine results in an effective twist or change
in azimuth of each fold relative to its adjacent one. Figure 3 shows only two adjacent
sections to facilitate illustration of the twist which occurs. It will be seen that
bisectors of the two sections are disposed at horizontal angles 2 γo to each other.
It has been discovered that if the twist is arranged such that the reflectors on adjacent
folds are directed with an azimuthal displacement of about 36° then a most efficient
"all round" reflection coverage results. The reflected signal strength at a lobe width
of 36°, i.e. + 18° from the directional axis, is sufficiently low that overlap of
the lobes of different ones of the reflective corners at this level have been found
to introduce an acceptably narrow deterioration of the polar response of the radar
target reflector due to phase cancellation. Accordingly ten elemental reflectors evenly
disposed around a polar axis have been found to give a particularly good polar response.
To provide this displacement the angle "γo" should be about 18°. It will be appreciated
that in view of the twist the solid angles of the elemental reflectors all diverge
radially from two helical axes one of which is sinistrorse and the other of which
is dextrorse.
[0020] The sections 11 need not be triangular but can be of truncated triangular form that
is of trapezium shape.
[0021] There now follows a mathematical analysis of the construction.
Stepped Helix Dimensions
[0022] The circle in Figure 4a represents a right section of a cylinder in which are contained
the stepped helices of a reflector. The trapezium shown is the projection of an actual
trapezium of construction on to the circular plane which is normally horizontal. All
intersections, dimensions and angles in this plane will bear a zero suffix. The actual
trapezium of construction is at 45 deg to the circular plane. Its plane will be an
ellipse. 0, W and W' are in both planes because they are on the axis of rotation.
[0023] Note Q
oP
o is parallel to S
oN
o (and parallel to OV0

are constructed right angles Let







the half-twist angle
[0024] Problem: Given r
o, γ
o and x
(i) Calculate po, q , so, t etc, then
(ii) Calculate p, q, s, t etc in the tilted plane formed by a 45 deg rotation about
axis WW'.
[0026] Combining (2) and (3)

Now, in the tilted plane,
q = qo √2
s = so √2 (see Figure 5a)
[0028] Because planes QQ
oP
oP and SS
oN
oN are parallel

[0029] Examining the plane SS
oN
oN (Figure 5b), Q will be directly above T, distance t


[0031] Finally note in ΔS
oQ
oT
o (Figure 4a)

and in Δ OQW
Q
[0032] Definition of the unit trapezium is now complete.
[0033] The position of the separator plates must now be defined. In the circular plane of
Figure 4a each is defined by the line U
oO
oY
o. U is at the apex of the two reflecting corners. (Note however U = U , because both
are in the circular and tilted planes). O
o is on the cylinder axis (midway) between the intersections of the axis with adjacent
trapezia. Y
o is located arbitrarily on the U
oO
o axis at some point within the cylinder envelope.
[0034] Because QS is tilted at angle ε from the horizontal, so the plane of the separator
plate will be tilted at angle ε from the vertical. Thus the separator plate will be
situated on the tilted plane QSNP at UX where X is on PN (see Figure 4b). On the next
PN fold above XYZ, P'N' say, there will be another point X' where the plane of the
separator intersects P'N'. However, P'N' will not be in the vertical plane of PN,
but another, also vertical but rotated through the twist angle. In fact UX = UX' by
symmetry.

[0035] Now calculate the dimensions of the individual reflectors. They are QXX' which has
edges UQ, UX, UX' and SXX' which has edges US, UX, UX'.
Of these edges UQ - US (bisected chord of an ellipse, and so constructed )
and UX = UX' (see above)

[0036] Consider Δ XJP in Figure 4b


[0037] A hypotenuse length can now be calculated using the smallest of the edges (15) or
(18) and multiplying by √2.
Ellipse Dimensions
[0038] It has been assumed this far that the stepped helix has been constructed of trapezia
with sides QP and SN straight and parallel. In fact they could be extended to the
wall of the enclosing cylinder when they would assume an elliptical curvature.
[0039] It can be simply shown that the smaller semi-diameter is on the axis WW' and is r
, the radius of cylinder. The major semi diameter is then √2 r .
Lobe Elevations and Azimuths
[0040] Let ε be the angle of tilt of the fold to the horizontal. This is angle SQS
T described in association with Figure 5b.

[0041] Thus, in Figure 4a direction US is inclined upwards at ε deg " UQ " downwards at
ε deg " UO
o" " horizontally Each lobe will therefore be inclined at a characteristic elevation,
between 0 and ε deg, up or down as appropriate, as determined by its azimuth between
the face and edge of the corner (see Figure 6a).
[0042] Recall that the lobe azimuth is at tan

from the face of the corner,
Recall that the lobe azimuth is at tan

from the edge of the corner,
provided the plane of edge-to-face-centre is in the plane of the incident radiation
(ss Figure 6b). But it is not, S tilted upwards ε deg about axis FU (and Q is tilted
down), see Figure 7a.
[0043] If S is the projection of S in the horizontal plane, note
(i) FUS being 90 deg, FUS0 < 90 deg,
(ii) the angle between the lobe peak and the fold US (LUS in Figure 7b), which was
formerly tan

must now be less. Call this angle K (= LoUSo in Figure 7b).
[0044] First calculate the lobe elevation. As it is a concomitant of heel (Ψ) it can usefully
be called Ψ
o (=

in Figure 7b). Note in Figure 7b that

,

,

,

,

, and

are all 90 deg.




Now find K =

, the angle between the azimuths of the directional axis of the lobe and the fold.

Lobe Azimuth Array
[0045] Considering the construction of Figures 1 and 2, which I call an ambiorse construction,
with the sinistrorse folds Nos: 1, 2 and 3 on top, and No: 1 topmost. The spine before
folding is shown in Figure 2. Let us start at fold No: 3 for (ultimate) simplicity.
Fold No: 3 defines the azimuth datum, 0°, in the horizontal projection shown in Figure
8, where the construction is viewed from above. Each fold is tangential to the circle,
radius x
o which is the locus of the corners U. The face of the plate shown in Figure 2 is defined
as its 'front' face, and the odd-numbered folds (which are shown as chain lines in
Figure 2 and dotted in Figure 8, and which have reference numerals encircled in Figures
2 and 8) are produced by folding the plate forwards for example see fold No: 3, i.e.
the front is the face on which the corners 3L and 3R will be situated. The other face
is the 'back', and the(even-numbered) backwards folds are shown as dot and chain lines
in Figure 2 and as solid lines in Figure 8 and with reference numerals not circled
in Figures 2 and 8.
[0046] Adjacent folds are folded in opposite senses (Figure 2), i.e. the plate is folded
from top to bottom alternately forwards and backwards, with odd-numbered folds forwards
(encircled) and even-numbered folds backwards.
[0047] Going from ("start" in Figure 8) Fold No: 3 to Fold No: 2 up the sinistrorse helix
causes a right-hand turn through the twist angle 2γ
o= 35.8° in this example). Similarly going from Fold No: 2 to Fold No: 1 causes the
same 35.8° right-handed turn. These are shown in Figure 8.
[0048] Fold No: 4 is parallel to Fold No: 3, and is of opposite sense. It is the uppermost
of the three (Nos: 4, 5 and 6) dextrorse folds forming the bottom half of the whole
construction. Going from Fold No: 4 to Fold No: 5 down the dextrorse helix causes
a right-hand turn through the twist angle, and similarly again from Fold No: 5 to
Fold No: 6 ("Finish").
[0049] The horizontal projection of each pair of corners for each fold is shown in Figure
8 following the construction described above. In the following Table 1 are shown the
fold azimuths (left and right, when viewing from behind the reflector, i.e. towards
the central axis). Hence the lobe azimuths (left and right) for each fold are given,
being K degrees (see Eqn. 22) into each corner from each fold azimuth. The lobe azimuths
for the dextrorse helix are exactly at 180° to those for the enantiomorphic sinistrorse
helix. The lobe azimuths are shown around Figure 8.
* 9.77 deg above (+) or below (-) the horizon.
[0050] Thus the whole 360 degrees of azimuth are covered by 12 corners with two overlapping
pairs, one corner of each of which can be eliminated as they are at opposite ends
of the construction (1L and 6L, bracketted in the Table), leaving 10 lobes.
[0051] So the azimuthal sequence of the remaining lobes is as in Table 2.

[0052] That is to say, the 10 corners are disposed substantially evenly around the azimuth,
as indicated in Figure 9.
[0053] An alternative collapsible version of a reflector in accordance with the invention
is shown in Figure 10. In this embodiment sections 21 and 22 of radar reflective sheet
material are hingedly interconnected in edge to edge relationship to form a strip
by means of hinges 23. The portions 21 are of similar shaping to the portions 11 and
the portion 22 is of similar shaping to the portion 12 of Figure 2. The hinges permit
the strip to be folded backwards and forwards in concerting fashion into a small space.
The opposite edges of the portion 22 which are hingedly connected to adjacent portions
21 are substantially parallel. The hingedly connected edges of the other portions
21 are alternately divergent and convergent in a direction from one edge to the other
edge of the sectional strip.
[0054] Each of the portions 21 and 22 except the top portion is provided with a separator
plate 24 which are hingedly connected to their respective portion alternately to opposite
faces of the plate. The separator plates are shaped and positioned so as to be movable
into a position at right angles to their respective portion and to permit the adjacent
portion to be hinged into contact therewith at which position the adjacent portions
are mutually at right angles. A clip 25 is provided which engages the edge of the
separator plate and secures the plate in position. The two adjacent portions and the
separator plate form a pair of orthogonal re-entrant trihedrals in the same form as
Figure 1.
[0055] It will be appreciated that this version of the reflector can be folded down for
storage in a confined space yet is quickly reassembled for use.
[0056] It is believed that the constructions described fully meet the stringent performance
requirements of the Department of Trade Marine Radar Reflector Performance Specification
1977. In particular, since the response for the vertical plane is also extremely good
the vertical angle response, so important to maintain reflection during heeling in
rough seas, meets the requirement that the vertical coverage, ± 15° to the horizontal,
shall not remain below -6dB relative to the 10m
2 value over any single angle of more than 1.5°.
[0057] It will be appreciated that more or less reflective corners could be employed and
that provided at least six are distributed around a 360 arc, a useful construction
may be obtained. Reflectors employing more than 10 reflective corners in which overlapping
of lobes at higher signal strengths occurs may well provide useful constructions and
such constructions are at present being analysed as their usefulness is influenced
by their response at different heeling angles as well as by several other complex
factors.
[0058] Although the spine and dividers of the described reflector are formed from a single
sheet of material the invention is not restricted to such a construction and any other
radar reflective material can be employed. For example, the whole could be moulded
in plastics e.g. by injection moulding. Such a moulding could be effected with a moulding
material containing particles of radar reflective material so that these particles
are embedded in the moulded reflector. Another possibility is the provision of facings
of radar reflective material on a plastics moulded construction e.g. by metal plating
or metalization. A radar reflector as previously described may be encapsulated or
hermetically sealed in a container of for example glass reinforced plastics material.
1. A radar reflector having a major axis and comprising at least six corner reflectors
directed outwardly of said major axis characterized in that the corner reflectors
(14a, 14b) are disposed along two successive helical paths one of which paths is sinistrorse
and the other of which paths is dextrorse.
2. A radar reflector as claimed in Claim 1, wherein the reflectors (14a, 14b) are
evenly distributed within an angle of 360°.
3. A radar reflector as claimed in Claim 1 or 2, wherein the corner reflectors (14a,
14b) are orthogonal re-entrant trihedrals.
4. A radar reflector as claimed in Claim 3, comprising a strip (10a) of radar reflective
sheet material folded in alternate directions along fold axes (lla, 12a, 12b) spaced
apart on the strip and extending transversely across the strip with two consecutive
ones of the fold axes (12a,12b) disposed intemediately being substantially parallel
and the remaining folds (lla) being alternately convergent and divergent in a direction
from one edge to the opposite edge of the strip the folds dividing the strip into
sections (11,12)adjacent sections being disposed at right angles and a separator plate
(14) being provided between and at right angles to each pair of adjacent sections
to form therewith two corner reflectors (14a, 14b).
5. A radar reflector as claimed in Claim 3, comprising a strip of radar reflective
sheet material formed by a multiplicity of sheet sections (21, 22) having edges in
edge to edge relationship extending across the strip, said edges of an intermediate
one of the sections (22) being substantially parallel and the remaining ones of said
edges being alternately convergent and divergent in a direction from one edge to the
opposite edge of the strip, and for each pair of adjacent sections hinge means (23)
coupled between said sections and adapted to permit hinged movement of said sections
into a position where they are mutually at right angles and a separator plate 24 hingedly
connected to one of said sections adapted to permit hinged movement into a position
at right angles to each of said pair of adjacent sections to form therewith two corner
reflectors.
6. A radar reflector as claimed in Claim 4 or 5, wherein the separator plates (14,
24) are rectangular.
7. A radar reflector as claimed in Claim 4 or 5, wherein the separator plates (14,
24) are rectangular with one point cut off to provide an edge and are each positioned
such that said edge is remote from adjacent sections.
8. A radar reflector as claimed in Claim 4, 5, 6 or 7 wherein the strip (10a) or sheet
sections (21, 22) is/are profiled to provide an edge profile conforming to part of
the internal surface of a cylinder.
9. A radar reflector as claimed in Claim 8, wherein the separator plates (14,24) are
profiled to provide an edge profile conforming to part of the internal profile of
said cylinder.
10. A radar reflector as claimed in any one of the preceding claims contained within
a cylindrical housing.
11. A radar reflector as claimed in anyone of the preceding claims comprising ten
corner reflectors.