FIELD
[0001] The present invention relates to acoustic black holes and structures utilising the
same.
BACKGROUND
[0002] In product design, it is often desirable to design a product that is both lightweight
and low noise. However, this results in a conflict between reducing the weight and
increasing the sound radiation from the structure. It is known to use a structure
referred to as an acoustic black hole (ABH) to provide structural damping.
[0003] The acoustic black hole effect is typically achieved by introducing a power law taper
into a beam or plate that changes the thickness over a set distance. This change in
thickness profile causes the flexural waves propagating along the direction of the
ABH to decrease in wave speed. In the theoretical limit, there is no reflection of
the waves from the ABH. The ABH effect can also be achieved using other gradient functions,
including a power-cosine curve, for example.
[0004] However, the dimensionality/shape of existing ABHs make them inappropriate for use
in certain contexts. Hence an improved ABH which is more widely applicable is desirable.
SUMMARY
[0005] It is an aim of the present invention, amongst others, to provide a improved acoustic
black hole and/or structure and/or address one or more of the problems discussed above,
or discussed elsewhere, or to at least provide an alternative acoustic black hole
or structure.
[0006] According to an aspect of the present invention, there is provided an acoustic black
hole 'ABH', comprising a tapered body comprising an upstream end and a downstream
end, the tapered body tapering from a first characteristic towards the upstream end
to a second characteristic towards the downstream end, and comprising at least one
fold in between the upstream end and the downstream end, such that the downstream
end at least partly points towards the upstream end of the tapered body.
[0007] In an example, the first characteristic and second characteristics are thicknesses
of a cross section of the tapered body.
[0008] In an example, the at least one fold is closer to the downstream end of the tapered
body. Conversely, in an example, the at least one fold is closer to the upstream end
of the tapered body.
[0009] In an example, a first region may be considered proximate to the upstream end and
a second region proximate to the downstream end, the regions being separated by the
at least one fold.
[0010] In an example, the first region comprises a first material and the second region
comprises a second, different, material.
[0011] In an example, the first region comprises a first density and the second region comprises
a second, different, density.
[0012] In an example, the first region comprises a first rigidity and the second region
comprises a second, different, rigidity.
[0013] In an example, at least one of the first region and second region are actively controlled.
[0014] In an example, the tapered body may comprise at least two folds, and a be considered
to comprise a third region in between the at least two folds and spacing apart the
first region and the second region. Suitably, in an example, the first region and
second region may be arranged substantially parallel.
[0015] In an example, the third region comprises a third material different to the first
material and the second material.
[0016] In an example, the third region comprises a third density different to the first
density and the second density.
[0017] In an example, the third region comprises a third rigidity different to the first
rigidity and the second rigidity.
[0018] In an example, the third region is actively controlled.
[0019] In an example, a height of the third region in a y-axis does not exceed a height
of the upstream end in the y-axis.
[0020] In a related aspect of the present invention, there is provided a compound ABH comprising
a plurality of the aforementioned ABHs.
[0021] In an example the compound ABH comprises a first pair of ABHs abutting at their respective
at least one fold.
[0022] In an example, the compound ABH comprises a second pair of ABHs abutting at their
respective least one fold.
[0023] In an example, the first and second pair of ABHs may be arranged to form a cavity
in between the two pairs of ABHs.
[0024] In a related aspect of the present invention, there is provided a structural damper
comprising the aforementioned ABH.
[0025] In a related aspect of the present invention, there is provided a primary structure
comprising the aforementioned structural damper.
BRIEF DESCRIPTION OF THE FIGURES
[0026] Embodiments of the invention will now be described by way of example only with reference
to the figures, in which:
Figure 1 shows the principles of an acoustic black hole;
Figure 2 shows an example improved acoustic black hole - Fig. 2A shows a single fold
acoustic black hole and Fig. 2B shows a double fold acoustic black hole;
Figure 3 shows a graph of displacement magnitude with distance for a range of acoustic
black holes;
Figure 4 shows a graph of power dissipation for a range of acoustic black holes;
Figure 5 shows an example compound ABH - Fig. 5A shows a linear compound ABH while
Fig. 2B shows a circular compound ABH;
Figure 6 shows another example compound ABH;
Figure 7 shows an example of a damper structure with controlled ABH; and
Figure 8 shows examples of a controlled folded ABH.
DETAILED DESCRIPTION
[0027] Figure 1 shows an example of an acoustic black hole (ABH) 1 on a beam 2. The ABH
1 may be provided with a layer of damping material 3. The flexural wave speed c
f (x), decreases as the taper height decreases as:

where E is the Young's modulus of the ABH material, h(x) is the height of the taper,
ρ
s is the density of the ABH material and ω is the angular frequency.
[0028] From Equation 1 it can be seen that if the tip of the ABH reduces to zero thickness,
i.e. h(x)=0, then the flexural wave speed at the tip will be c
f (x)=0. In this ideal, theoretical case, the incident wave will not be reflected from
the end of the tapered beam and will therefore, be effectively attenuated.
[0029] In this respect, acoustic black holes are known in the art. For example,
'Higher-order WKB analysis of reflection from tapered elastic wedges' Journal of Sound
and Vibration 449 (2019) 368-388 (Angelis Karlos, Stephen J. Elliot, Jordan Cheer), the contents of which are incorporated herein, provides examples of different types
of 'one-dimensional' acoustic black holes. The thickness variations, of these acoustic
black holes, are according to the expressions provided in Table 1 below:
Table 1
| Thickness profile type |
Thickness variation |
Length of ideal wedge |
Decay parameter |
| Power-law |

|

|
- |
| Exponential |
h = h0e-βx |
∞ |

|
| Power-cosine |

|

|
- |
| Gaussian |
h = h0e-γx2 |
∞ |

|
| Compound power-law |

|

|
- |
where:
'x' is the distance, in the length direction, from the upstream end of the acoustic
black hole (i.e. at the start of the taper);
'x1' is the length of the acoustic black hole;
'h' is the thickness of the acoustic black hole (at position (x));
'h0' is the thickness of the acoustic black hole at the upstream end of the acoustic
black hole (i.e. at position (x = 0));
'h1' is the thickness of the acoustic black hole at the downstream end of the acoustic
black hole (i.e. at position (x = x1));
'n' is power coefficient of the shape function (which must be greater or equal to
2).
[0030] In the description which follows, acoustic black holes, structural dampers, structurally
damped structures, and methods, are described. The term "acoustic black hole" is used
to refer to an element, member, or structure, which, in use, exhibits the acoustic
black hole effect.
[0031] In the description herein, acoustic black holes comprise regions of taper. In the
examples shown and described, the taper is a thickness taper. That is, the thickness
of the acoustic black hole tapers (i.e., reduces or diminishes in thickness in a direction
and along a line toward a point, line or region). Additionally, or alternatively,
tapering may be in shape. A thickness or shape may be referred to generally as a "spatial
property". Conventional ABHs incorporate tapers in thickness, from a first thickness
to a second thickness. The first thickness is typically a non-zero thickness. The
second thickness is, in the ideal case, a zero thickness. A thickness or shape taper
may be advantageous in that it may be simpler to manufacture than, for example, a
taper in material and/or material property.
[0032] However, in contrast to a thickness taper, the taper could also be a "functional
taper" or a "functional grading". That is, the tapering could be a tapering function
of the acoustic black hole, rather than a tapering thickness. For example, the tapering
may be a tapering of material and/or material property. The material property may
be, for example, density and/or rigidity. This may be achieved by use of additive
layer manufacturing (e.g. 3D printing) to form an acoustic black hole having a tapering,
graded, or varying, material property. A tapering in material and/or material property
may be advantageous in that thin ABH regions need not be provided, which may improve
the structural strength, and operational lifetime, of the ABH.
[0033] In this way, it is appropriate to refer to ABH tapers as tapering of a "characteristic".
Tapering may be from a "first characteristic" to a "second characteristic". A similar
or identical effect to a thickness tapering may be achieved by a tapering in material
and/or material property. For example, a tapering from a region of high rigidity to
a region of low rigidity may provide a reduction of the flexural wave speed to c
f (x)=0, as described above, thereby to provide the ABH effect. A variation from a
first characteristic to a second characteristic includes a variation in a magnitude
of a specific characteristic from a first to a second value, or a variation in a type
of characteristic from a first to a second (different) type.
[0034] The term "structural damper" may be used to refer to an arrangement, assembly or
kit of acoustic black holes and optionally active control components (e.g., comprising
a sensor, an actuator, and a controller).
[0035] The term "primary structure" may be used to refer to a structure that a damper device,
or structural damper, is arranged to provide structural damping to. The primary structure
is a structure that, in use, has a vibration applied to it. The primary structure
may be a structure that is vibrated, directly or indirectly, by a source of vibration
(e.g., an engine, fluid flow, etc.).
[0036] An acoustic black hole may be formed in or on the primary structure. For example,
the acoustic black hole may be embedded in the primary structure. Alternatively, or
additionally, the acoustic black hole may be coupled to the primary structure. That
is, the acoustic black hole may be manufactured separately and coupled, or connected,
to the primary structure.
[0037] A structural damper may be formed in or on the primary structure. For example, the
structural damper may be integral to the primary structure. Alternatively, or additionally,
the structural damper may be coupled to the primary structure. That is, the structural
damper may be manufactured separately and coupled, or connected, to the primary structure.
[0038] The term "structurally damped structure" may be used to refer to a structure, arrangement,
assembly or kit comprising an acoustic black hole and a primary structure. The structurally
damped structure may also comprise active control components (e.g., comprising a sensor,
an actuator, and a controller). That is, the structurally damped structure may comprise
a primary structure and a structural damper. As above, whilst in the exemplary embodiments
described herein the structurally damped structure comprises a structural damper comprising
a single compound ABH, the structurally damped structure may comprise a plurality
of compound ABHs and associated control components (e.g., a plurality of actuators,
sensors and/or controllers).
[0039] The term "damper structure" may be used to refer to a structure that is coupled to
an ABH (e.g., mechanically coupled) such that it can transmit vibration and/or flexural
waves through its structure to and from an ABH. The ABH may be formed in or on the
damper structure. The damper structure may be coupled, or connected to, the primary
structure, or the damper structure may be formed in or on the primary structure.
[0040] In examples herein, the acoustic black hole may be said to have a first axis and
a second axis, and the primary structure may be said to have a first axis and a second
axis. Throughout, the first axis of the primary structure is parallel to the first
axis of the acoustic black hole, and the second axis of the primary structure is parallel
to the second axis of the acoustic black hole. The first axis of the primary structure
may be the same as the first axis of the acoustic black hole, and the second axis
of the primary structure may be the same as the second axis of the acoustic black
hole.
[0041] In some examples, the first axis and second axis are perpendicular. In this way,
the acoustic black hole may comprise tapering (or variation) in directions parallel
to, for example, the first axis, and no tapering (or variation), or tapering (or variation),
in the second axis, the first and second axis being perpendicular. This may simplify
construction, by avoiding construction or formation of tapering/varying features at
relative angles. Nevertheless, in other embodiments, the first axis and second axis
need not be perpendicular, which may lead to improvements in structural damping where
vibrations emanate from multiple angles relative to the acoustic black hole.
[0042] In some examples a structurally damped structure may be said to comprise a primary
structure having a "region of curvature" in at least one of the first axis and second
axis, the region of curvature may be about the acoustic black hole, surrounding the
acoustic black hole and/or in proximity of the acoustic black hole. It will be appreciated
that the whole of the primary structure may comprise curvature in at least one of
the first axis and second axis. Thus, it may be appropriate to refer to the primary
structure comprising "at least a region" of curvature.
[0043] Figure 2 shows an example of an improved acoustic black hole 100. In particular,
the acoustic black hole has been designed to save space compared to prior art ABHs,
as well as allow for flexibility in length and height. Fig. 2A shows one example implementation.
Fig. 2B shows another example implementation. Each of the example ABHs in Fig. 2 may
be considered linear, or 1-D, ABHs.
[0044] Here the ABH comprises a body 102 having an upstream end 104 and a downstream end
106. The body 102 is tapered such that the body 102 tapers from a first characteristic
at, or proximate to, the upstream end 104 to a second characteristic at, or proximate
to, the downstream end 106.
[0045] In the example shown the tapering is a shape wise tapering, such that the first characteristic
and second characteristics are thicknesses of a cross section of the body 102 in a
x-z plane. That is, the first characteristic is a thickness greater than a thickness
of the second characteristic.
[0046] It will however be appreciated from the discussion above that other approaches to
tapering the body 102 consistent with ABH principles may be utilised.
[0047] The body 102 comprises at least one fold 112 in between the upstream end 104 and
the downstream end 106 such that the downstream end 106 at least partly points back
towards the upstream end 104.
[0048] In the examples shown, the downstream end 106 does not reach the upstream end 104
- i.e., the at least one fold 112 is closer to the downstream end 106 than the upstream
end 104. In some alternative examples the downstream end 106 may instead extend past
the upstream end 104 - i.e., the at least one fold 112 is closer to the upstream end
104 than the downstream end 106.
[0049] Put another way, given a Euclidian coordinates system in which the upstream end 104
starts at x=0, in examples where the at least one fold 112 is closer to the downstream
end 106, a termination point 107 of the downstream end 106 may have an a positive
x value, whereas in examples where the at least one fold 112 is closer to the upstream
end 104, the termination point 107 of the downstream end 106 may have a negative x
value.
[0050] Suitably, the at least one fold 112 may be considered to divide the body 102 into
a plurality of regions comprising a first region 108 and a second region 110. The
first region may be considered proximate to the upstream end 104 of the body 102 and
the second region 110 proximate to the downstream end 106 of the body 102. Suitably
the second region 110 may be considered at least partly oriented back towards the
first region 108 as a result of the at least one fold 112. In this way an overall
length of the AHB 100 may be reduced (in the direction of the first (x) axis).
[0051] More specifically, in the example of Fig. 2A, exactly one fold 112 is provided which
separates the body 102 into the first and second regions 108, 110. Suitably, the downstream
end 106 points back towards the upstream end 106 at an angle defined by the fold 112.
[0052] In the example of Fig. 2B, two folds 112 are provided which separates the body 102
into the aforementioned first and second regions 108, 110 and also a third region
114. Suitably, the third region 114 spaces apart the first and second regions 108,
110. In particular, in the present example the third region 114 allows for the first
region 108 and second region 110 to be substantially parallel. That is, the third
region 114 may be substantially orthogonal to the first region 108 and second region
11. Or put anther way, the first and second regions 108, 110 may be considered to
have major (first) axes in an x direction, while the third region 110 may be considered
to have major (first) axis in a z direction.
[0053] Suitably, a length of the third region 114 (i.e., the degree to which it separates
the first and second regions 108, 110) controls a height (in a z direction) of the
AHB 100. In the example shown, the size of the third region 114 is set such that a
total height of the AHB 100 does not exceed the height of the upstream end 104; thus
the example of Fig. 2B has advantages not only for overall length but also for height
of the AHB 100.
[0054] Although the above has focused on tapering shape as the variable characteristic,
it will however be appreciated that other characteristics can also be applied to the
ABH 100 instead of or in addition to tapering shape. Also, it will be appreciated
that other aspects of ABHs may be applied to the presently described ABH.
[0055] For example, the first region 108 may comprise a first material while the second
region 110 may comprise a second material. The first region 108 may have a first density
while the second region 110 has a second density. The first region 108 may have a
first rigidity while the second region 110 has a second rigidity. The first region
108 may be actively controlled while the second region 110 is not actively controlled
- or vice-versa - or indeed both the first region 108 and second region 110 may be
both actively controlled.
[0056] Similarly, in examples where the body 102 also comprises the third region 114, the
third region 114 may be the same material as one of the first or second regions 108,
110, or may be a different material to both of the first and second regions 108, 110.
The third region 114 may have the same, or substantially similar, density to either
the first or second regions 108, 110 or may have a different density to both the first
and second regions 108, 110. The third region 114 may have the same or different rigidity
to one or both of the first and second regions 108, 110. The third region 114 may
be actively controlled in addition to both the first and second regions 108, 110 or
instead of the second and third regions 108, 110.
[0057] Figure 3 shows an example of the space savings that can be achieved using an ABH
designed as above. Here there is shown sound propagation through a standard bar 10,
a standard ABH 20, an ABH 100 as above, and a coiled ABH 30. Versus the standard ABH
20 the improved ABH 100 has the same height (as in, how much vertical space it would
take up in a structure) but much reduced length. Versus the coiled ABH 30, that device
can be utilised in much shorter spaces, but similarly only in spaces with much greater
height in order to account for the coil.
[0058] Figure 4 shows a graph demonstrating the attenuation of vibrations in the objects
of Fig. 3. Line 11 shows dissipated power for a solid standard shaped bar 10 which
has little to no attenuation of vibration. Line 21 shows dissipated power for a standard
ABH 20. Line 101 shows dissipated power for an improved ABH 100. Line 31 shows dissipated
power for a coiled ABH 30.
[0059] Figure 5 shows an example of a compound ABH 200 based on the principles above. Here,
the compound ABH 200 comprises a plurality a folded ABHs 100. The compound ABH is
particularly suited for damping vibrations from multiple angles.
[0060] As shown in Fig. 5A, two ABHs 100 are arranged back to back. That is, each ABH 100
is arranged with its upstream end 106 pointing (in the direction of taper) at the
other ABH 100. Suitably, each ABH 100 abuts the other ABH 100 where the ABHs 100 are
folded. Put another way, where the ABHs comprise the third region 114, the third region
114 of one ABH 100 may abut the third region 114 of the other ABH. Here the compound
ABH 200 is assumed to have a substantially linear, or 1-D, geometry.
[0061] Fig. 5B shows an example of a compound ABH 200 as per Fig. 5A in a circular, or cylindrical,
geometry as from a top down view. That is, in the context of Fig. 5B, Fig. 5A may
be taken to represent a cross sectional slice through a cylindrical compound ABH 200.
The cylindrical compound ABH may also be considered a 2-D ABH.
[0062] Put another way, it may be envisaged that the ABH 200 comprises a cylindrical symmetry
about an axis defined by the third region 114. Suitably, in one example, the upstream
end 204 of the compound ABH 200 may be taken to correspond to an outer circumference
of the ABH 200, while the downstream end 206 has a radius less than the radius of
the upstream end 204. In another example, the radius of the downstream end 206 may
be greater than the radius of the upstream end 204.
[0063] The compound ABH 200 may form part of a structurally damped structure. For example,
there may be provided a substantially two-dimensional primary structure in the form
of a relatively thin flat plate. The plate may comprise a plurality of compound ABHs
that are embedded in the plate; that is each compound ABH 200 may take the form of
a generally circular indentation in a surface of the plate.
[0064] Figure 6 shows another example compound ABH 200 comprising a plurality of ABHs 100.
Here the compound ABH 200 comprises two pairs of back-to-back ABHs analogous to Fig.
5A. The plurality of ABHs 100 are arranged to form a cavity 216 which separates the
second regions 110a of the first pair of ABHs 100a and the second regions 110b of
the second pair of ABHs 100b.
[0065] More specifically, a first pair of ABHs 100a are arranged abutting at the third regions
114a to form a lower housing 218, while a second pair of ABHs 100b are arranged abutting
at the third regions 114b to form an upper housing. Suitably the two pairs of ABHs
100a,b are arranged to abut at the upstream ends 104a,b. It will also be appreciated
that the present arrangement can be achieved in 3-D, or cylindrical, form analogous
to Fig. 5B.
[0066] Figure 7 shows an example of an actively controlled acoustic black hole 300 as part
of a structurally damped structure 30. The structurally damped structure 30 comprises
a primary structure 32 in the form of a rectangular beam 32 and a structural damper
14, at the end of the beam 32, configured to provide structural damping of the beam
32.
[0067] In this respect, the beam 32 is attached, at one end, to a vibration source 36. The
vibration source 36 produces a vibratory excitation force (V) at that end of the beam
32, which induces vibration and flexural waves in the beam 32. This also causes the
beam 32 to emit acoustic radiation, i.e. noise.
[0068] In general, the structural damper 14 has a damper structure 38, that comprises an
acoustic black hole 300, provided at the opposite end of the beam 32 to the vibration
source 36. The damper structure 38 (and the acoustic black hole 300) may be considered
embedded in the end of the beam 32. It will however be appreciated that in the example
shown the damper structure 38 is the same as the ABH 300; or put another way, the
ABH 100 is the damper structure. It will be appreciated that in other examples the
damper structure may comprise other components in addition to the ABH 300.
[0069] The ABH 300 may be substantially the same as described with reference to the previous
Figures for ABH 100 above. That is, the ABH 300 comprises a body 302 having an upstream
end 304 and a downstream end 106 and a tapered body 302 tapering from a first characteristic
at the upstream end 104 to a second characteristic at the downstream end 306. Suitably,
the upstream end is proximate to the vibration source 36. The body 302 may comprise
at least one fold 316 in between the upstream end 304 and the downstream end 306 (not
shown in Fig. 7; shown in Fig. 8).
[0070] Here the ABH 300 comprises an actuator 308 configured to apply an actuating force
to the ABH 300. The actuator 308 causes the ABH 300 to deform (i.e. through expansion
or contraction) due to the application of the actuating force. Put another way, energy
is input from the actuator 308 into the acoustic black hole 300.
[0071] In the present example, the actuating force is applied parallel to the plane of the
flexural waves that travel along the beam 32 due to excitation by the vibration source
36. In other examples, the actuating force may be applied in a different direction
with or without a component parallel to the flexural waves. The actuator 308 may be
located remote from the ABH 300 such as on the beam 32, or a fold of the beam 218.
[0072] The ABH 300 also comprises a first sensor 310 configured to detect a deformation
of the ABH 300. A signal from the sensor 310 is provided to a controller 312 which
generates a control signal, based on the received sensor signal, for controlling the
actuator 308. The control signal is suitably transmitted to the actuator 308 in order
to attenuate the vibration of the primary structure / beam 32.
[0073] In the present example, the actuator 308 may comprise a piezo-electric transducer
(PZT) patch 308 which is provided on at least one of the upper and lower surface of
the ABH 300; shown on the upper surface in Fig. 7. The actuating PZT patch 108 may
be provided on a partial area of a surface of the ABH or substantially covering an
entire surface of the ABH 300.
[0074] Likewise, the sensor 310 may also comprise a PZT patch 310 provided on at least one
of the upper and lower surface of the ABH 300; here shown on the lower surface in
Fig. 7.
[0075] The upper and lower PZT patches 308, 310 are each of a material that has an intrinsic
level of damping and so provide a passive damping of the ABH 300.
[0076] Suitably, the movement of the ABH 300 acts to deform the sensing PZT patch 310, which
causes a voltage to be induced across the sensing PZT patch 310 that is representative
of the deformation. The sensing PZT patch 310 is connected to the controller 312 such
that the voltage induced across the sensing PZT patch 310 is passed to the controller
312 as a feedback signal. The output of the controller 312 is connected to the actuating
PZT patch 308 such that the control signal, here in the form of a voltage, is applied
across the actuating PZT patch 308 in dependence on the feedback signal.
[0077] It will of course be appreciated that any suitable type and arrangement of sensors
and actuators may be used. It will also be appreciated that the upper and lower PZT
patches could be reversed, i.e. the actuator provided on the lower surface and the
sensor provided on the upper surface.
[0078] As shown, the structurally damped structure 30 may comprise a second sensor 314,
mounted on the primary structure 32, which is configured to sense the vibration of
the beam 32. As above, the second sensor 314 may be a PZT sensor, however any suitable
type of sensor may be used. It will be appreciated that the second sensor 314 may
be embodied as a set of sensors.
[0079] The second sensor 314 may be located upstream of the actuator 308. The second sensor
314 is connected to the controller 312 so as to provide a feed forward reference signal
(r) to the controller 32 that corresponds to the vibrating movement of the beam 32
at the location of the sensor 34. In this way the controller 312 may better generate
a signal to minimise the vibration of the beam 32. Where the second sensor 314 is
embodied as a set of sensors, such sensors may be distributed in different locations
across the primary structure 32 or indeed vibration source 36.
[0080] Figure 8 shows example arrangements of the actuator 308 and first sensor 310 specific
to a folded ABH arrangement.
[0081] In the example of Fig. 8A, the actuator 308 is provided on an upper surface of the
first region 318 on the side of the fold 316 proximate to the upstream end 304. Suitably,
the first sensor 310 may be provided on the opposite surface of the first region 318
to the actuator 308. It will of course be appreciated that the sensor 310 and actuator
308 may be disposed the other way around.
[0082] In the example of Fig. 8B, the actuator 308 is disposed on an upper surface of the
second region 320 on the side of the fold 316 proximate to the downstream end 306.
Here "upper" is defined relative to the tapered shape, so that upper corresponds to
the surface of the body 302 which is angled, or has curvature (compared to the opposite
surface which may be flat). That is, here the "upper" surface of the second region
320 corresponds to the surface which faces the upper surface of the first region 318.
Suitably, the sensor 310 may be provided on the opposite (e.g., flat) surface of the
second region 320. It will also be appreciated that the arrangement of the actuator
308 and sensor 310 could be reversed.
[0083] Fig. 8C shows an example whereby the actuator 308 is provided on the upper surface
of the third region 322. Here the upper surface of the third region may be the surface
which faces the upper surfaces of the first and second regions 318, 320. Again the
sensor may be on the opposite surface and optionally the arrangement of the actuator
and sensor 308, 310 may be reversed.
[0084] Although the above examples have focussed on arranging the (PZT) actuators and sensors
on specific regions of the body 302 with respect to the fold 316, it should be appreciated
that the examples are non-limiting.
[0085] For example, a set of actuators 308 may be provided with each actuator in the set
corresponding to a surface of one of the regions of the body 302; here some regions
may also be left without an actuator 308. A corresponding set of sensors may be provided
on the opposite surfaces, with control of each of the actuators 308 being independent
based on a feedback from each corresponding sensor 310. For example, much like a basic
example of a controlled ABH, an entirety of a surface of the folded ABH may be covered
with PZT patches.
[0086] In some examples only one sensor 310 may be provided and the feedback signals suitably
averaged before sending a common control signal to the actuators 308, or a plurality
of sensors 310 may be used to generate a control signal for only one actuator 308
as either a sole actuator or an isolated member of a set of actuators.
[0087] In some examples, one or more actuators may be provided on one or more surfaces of
the ABH 300, while the first sensor 310 is not provided on an opposite surface but
elsewhere on the ABH 300. For example, an actuator may be provided on a surface of
the first region 318 or the second region 320 (or both) and a sensor on the third
region 322, as shown in Fig. 8D.
[0088] In summary, the above has described a new technique for acoustic black holes that
achieves space savings compared to existing techniques.
[0089] Where, in the foregoing description, integers or elements are mentioned that have
known, obvious, or foreseeable equivalents, then such equivalents are herein incorporated
as if individually set forth. Reference should be made to the claims for determining
the true scope of the present disclosure, which should be construed so as to encompass
any such equivalents. It will also be appreciated by the reader that integers or features
of the disclosure that are described as optional do not limit the scope of the independent
claims. Moreover, it is to be understood that such optional integers or features,
while of possible benefit in some embodiments of the disclosure, may not be desirable,
and can therefore be absent, in other embodiments.
1. An acoustic black hole 'ABH', comprising:
a tapered body comprising an upstream end and a downstream end, the tapered body tapering
from a first characteristic towards the upstream end to a second characteristic towards
the downstream end;
the tapered body comprising at least one fold in between the upstream end and the
downstream end, such that the downstream end at least partly points towards the upstream
end of the tapered body.
2. The ABH of claim 1, wherein the first characteristic and second characteristics are
thicknesses of a cross section of the tapered body.
3. The ABH of claim 1 or 2, wherein the at least one fold is closer to the downstream
end of the tapered body.
4. The ABH of claim 1 or 2, wherein the at least one fold is closer to the upstream end
of the tapered body.
5. The ABH of any preceding claim, comprising a first region proximate to the upstream
end and a second region proximate to the downstream end separated by the at least
one fold.
6. The ABH of claim 5, wherein the first region comprises a first material and the second
region comprises a second, different, material.
7. The ABH of claim 5 or 6, wherein the first region comprises a first density and the
second region comprises a second, different, density.
8. The ABH of any of claims 5 to 7, wherein the first region comprises a first rigidity
and the second region comprises a second, different, rigidity.
9. The ABH of any of claims 5 to 8, wherein at least one of the first region and second
region are actively controlled.
10. The ABH of any of claims 5 to 9, comprising at least two folds, and a third region
in between the at least two folds and spacing apart the first region and the second
region.
11. The ABH of claim 10, wherein the first region and second region are arranged substantially
parallel.
12. The ABH of claim 10 or 11, wherein a height of the third region in a y-axis does not
exceed a height of the upstream end in the y-axis.
13. A compound ABH comprising a plurality of ABHs according to any preceding claim, comprising
a first pair of ABHs abutting at their respective at least one fold.
14. The compound ABH of claim 13, comprising a second pair of ABHs abutting at their respective
least one fold.
15. The compound ABH of claim 14, wherein the first and second pair of ABHs are arranged
to form a cavity in between the two pairs of ABHs.