This is a schematic representation of sound passing through the density-near-zero membrane.
Credit: Liu/Nanjing University
When a sound wave hits an obstacle and
is scattered, the signal may be lost or degraded. But what if you could
guide the signal around that obstacle, as if the interfering barrier
didn't even exist? Recently, researchers at Nanjing University in China
created a material from polyethylene membranes that does exactly that.
Their final product, described this week in the Journal of Applied Physics,
from AIP Publishing, was an acoustical "metamaterial" with an effective
density near zero (DNZ). This work could help to endow a transmission
network with coveted properties such as high transmission around sharp
corners, high-efficient wave splitting, and acoustic cloaking.
"It's as if the entire [interior] space is missing," said Xiaojun
Liu, a professor in the physics department at Nanjing University's
Collaborative Innovation Center of Advanced Microstructures.
"We were curious about whether we could make a simple but compact
density-near-zero metamaterial from just a few tiny membranes," Liu
said, "and, if so, can we further manipulate sound and make acoustic
invisibility cloaks and other strange functional devices?"
Previous prototypes had attempted to achieve density-near-zero by
using coiled structures and phononic crystals to create "Dirac cones,"
but required large physical dimensions, complex geometric structures,
and the difficult feat of slowing sound waves to extremely low
velocities within scattering cylinders to be effective -- limiting their
practical applications.
Their current paper proposes a physical, minimalist realization of
their original density-near-zero idea, consisting of 0.125 mm-thick
polyethylene membranes perforated with 9-millimeter-radius holes in a
square grid inside of a metal waveguide, a physical structure for
guiding sound waves. The intensive resonances of the membranes
significantly reduce the structure's effective mass density, which is a
measure of its dynamic response to incident sound waves. By Newton's
second law, this reduction causes the average acceleration of the
structure to approach infinity, which gives rise to sound tunneling.
When sound at a frequency of 990 Hz is then conducted and rapidly
accelerated through the material, the membranes act as a tunnel for
sound, encapsulating the waves into local subwavelength regions. This
arrangement allows the sound waves to pass through without accumulating a
phase change or distorting the wavefront -- analogous to the quantum
tunneling effect, in which a particle crosses through a potential energy
barrier otherwise insurmountable by classical mechanics.
For future applications, the metamaterial would likely be integrated
into acoustic circuits and structures. When implemented in a wave
splitter, the researchers found an 80 percent increase in the efficiency
of energy transmission, regardless of the wave's incident angle.
Additionally, the researchers are able to tune the frequency of the
metamaterial network by altering the membrane's tension and physical
dimensions, which they were unable to do in previous prototypes.
Liu and his colleagues have already used the membrane network to
fabricate a planar hyperlens, a device which magnifies one and
two-dimensional objects on the subwavelength scale to compensate for the
losses of acoustic waves carrying fine details of images as they pass a
lens. This can allow scientists to see fine features of objects such as
tumors, or minute flaws within airplane wings in industrial testing,
that may otherwise be unobservable due to an instrument's diffractive
limit. Additional planned applications include using smart acoustic
structures, such as logic gates that can control acoustic waves by
altering their propagation, for communication systems in environmental
conditions too extreme for conventional electronic devices and photonic
structures.
"The vanishing mass density we've demonstrated is definitely more than a mathematical trick," said Liu.
Story Source:
The above post is reprinted from
materials provided by
American Institute of Physics (AIP).
Note: Materials may be edited for content and length.
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