DEVICE AND METHOD FOR FABRICATING LOCALLY HETEROGENEOUS COMPOSITE MATERIAL BASED ON TIME-FREQUENCY REGULATED SURFACE ACOUSTIC WAVES (SAWS)

Abstract

A device and method for preparing a locally heterogeneous smart composite material based on time-frequency regulated SAWs are provided. The method includes: mixing functional particles, a photosensitive liquid and a photoinitiator evenly; inputting periodic time-frequency regulated sinusoidal signals defined by a frequency, a duration, an interval time and a time difference to a pair of slanted-finger interdigital transducers, such that the pair of slanted-finger interdigital transducers are excited to produce corresponding standing SAWs; coupling and allowing the standing SAWs to enter a liquid tank to form a local sound field in the photosensitive liquid; forming, by the functional particles in the photosensitive liquid, a stable array distribution under the action of an acoustic radiation force of the local sound field; and turning on an UV light source for curing, thereby completing the preparation.

Claims

1. A device for fabricating a locally heterogeneous composite material based on time-frequency regulated surface acoustic waves, wherein: a pair of slanted-finger interdigital transducers are distributed on two side surfaces of a lithium niobate wafer; a liquid tank is placed on a central surface of the lithium niobate wafer between the pair of slanted-finger interdigital transducers; the liquid tank is filled with a mixture of a photosensitive liquid, functional particles and a photoinitiator; and an ultraviolet light source is provided directly under the lithium niobate wafer.

2. The device for fabricating the locally heterogeneous composite material based on the time-frequency regulated SAWs according to claim 1, wherein the pair of slanted-finger interdigital transducers are interdigital transducers, a finger width of the interdigital transducers changes continuously in a finger length direction; and the interdigital transducers are straight-line or circular-arc in the finger length direction to correspondingly define a slanted-finger interdigital transducer or a circular-arc interdigital transducer.

3. The device for fabricating the locally heterogeneous composite material based on the time-frequency regulated SAWs according to claim 2, wherein the pair of slanted-finger interdigital transducers are respectively excited by sinusoidal signals to generate SAWs of different frequencies in a direction perpendicular to the finger length direction on a surface of the lithium niobate wafer; the SAWs are superimposed in a central region of the lithium niobate wafer between the pair of slanted-finger interdigital transducers to form standing SAWs; and the liquid tank is located above the central region.

4. The device for fabricating the locally heterogeneous composite material based on the time-frequency regulated SAWs according to claim 1, wherein the UV light source emits an UV light into the liquid tank through the lithium niobate wafer to photocure the photosensitive liquid in the liquid tank.

5. The device for fabricating the locally heterogeneous composite material based on the time-frequency regulated SAWs according to claim 1, wherein the functional particles comprise a metal powder, an organic particle, and a cell.

6. A method for fabricating a locally heterogeneous composite material based on time-frequency regulated SAWs, applied to the device according to claim 1, and comprising the following steps: step 1: mixing the functional particles, the photosensitive liquid and the photoinitiator evenly to obtain the mixture, and adding the mixture into the liquid tank by a pipette; step 2: inputting periodic time-frequency regulated sinusoidal signals defined by a frequency, a duration, an interval time, and a time difference to the pair of slanted-finger interdigital transducers, such that the pair of slanted-finger interdigital transducers are excited to produce corresponding standing SAWs; coupling and allowing the standing SAWs to enter the liquid tank to form a localized acoustic field in the photosensitive liquid; and forming, by the functional particles in the photosensitive liquid, a stable array distribution under an acoustic radiation force inside the localized acoustic field; and step 3: turning on the UV light source to photocure the photosensitive liquid and fabricate the locally heterogeneous composite material, wherein the functional particles are fixedly distributed in an array within a localized acoustic field.

7. The method for preparing the locally heterogeneous composite material based on the time-frequency regulated SAWs according to claim 6, wherein the functional particles comprise a metal powder, an organic particle, and a cell.

8. The method for fabricating the locally heterogeneous composite material based on the time-frequency regulated SAWs according to claim 6, wherein the periodic time-frequency regulated sinusoidal signals input into the pair of slanted-finger interdigital transducers are exactly the same in each cycle; each cycle is defined by a sinusoidal signal duration connected to a zero input signal duration; a sinusoidal signal frequency within the sinusoidal signal duration is f.sub.1; and there is the time difference t.sub.c between the periodic time-frequency regulated sinusoidal signals input into the pair of slanted-finger interdigital transducers.

9. The method for preparing the locally heterogeneous composite material based on the time-frequency regulated SAWs according to claim 6, wherein the pair of slanted-finger interdigital transducers are interdigital transducers, a finger width of the interdigital transducers changes continuously in a finger length direction; and the interdigital transducers are straight-line or circular-arc in the finger length direction to correspondingly define an oblique interdigital transducer and a circular-arc interdigital transducer.

10. The method for preparing the locally heterogeneous composite material based on the time-frequency regulated SAWs according to claim 9, wherein the pair of slanted-finger interdigital transducers are respectively excited by sinusoidal signals to generate SAWs of different frequencies in a direction parallel to the finger length direction on a surface of the lithium niobate wafer; the SAWs are superimposed in a central region of the lithium niobate wafer between the pair of slanted-finger interdigital transducers to form standing SAWs; and the liquid tank is located above the central region.

11. The method for preparing the locally heterogeneous composite material based on the time-frequency regulated SAWs according to claim 6, wherein the UV light source emits an UV light into the liquid tank through the lithium niobate wafer to photocure the photosensitive liquid in the liquid tank.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0024] FIG. 1 is a schematic view of a device for fabrication a locally heterogeneous composite material according to the present disclosure;

[0025] FIG. 2 shows a characteristic range of standing SAWs formed by frequency-regulated SAWs;

[0026] FIG. 3 shows input signals for time-regulated SAWs;

[0027] FIG. 4 shows a characteristic range of standing SAWs formed by time-regulated SAWs; and

[0028] FIG. 5 shows an arrangement of functional particles in a locally heterogeneous composite material fabricated based on time-frequency regulated SAWs.

[0029] Reference Numerals: (1) lithium niobate wafer; (2) a pair of slanted-finger interdigital transducers; (3) liquid tank; (4) UV light source; (5) mixture; and (6) localized acoustic field range.

DETAILED DESCRIPTION OF THE EMBODIMENTS

[0030] The present disclosure will be described in further detail below with reference to the drawings and examples, but the embodiments of the present disclosure are not limited thereto.

[0031] As shown in FIG. 1, in an experimental fabrication device of the present disclosure, a pair of slanted-finger interdigital transducers 2 are fabricated on two sides of a lithium niobate wafer 1 by a micro-electromechanical systems (MEMS) process. The pair of slanted-finger interdigital transducers 2 are usually made of aluminum or gold, with a pattern determined by a mask in the MEMS process, and a thickness determined by a sputtering time, usually 50 nm to 200 nm. A finger width of the pair of slanted-finger interdigital transducers 2 is equal to a finger spacing thereof. A liquid tank 3 is used to hold a mixture 5 of photosensitive liquid, photoinitiator and functional particles, and is provided between the pair of slanted-finger interdigital transducers 2. The liquid tank is usually made of an organic polymer material with low acoustic impedance, such as polydimethylsiloxane (PDMS), to reduce the reflection of SAWs between the lithium niobate wafer 1 and the liquid tank 3. An UV light source 4 is provided under the lithium niobate wafer 1.

[0032] In order to realize the fabrication of a locally heterogeneous composite material, the pair of slanted-finger interdigital transducers 2 may be slanted-finger interdigital transducers or circular-arc interdigital transducers. If the pair of slanted-finger interdigital transducers 2 are slanted-finger interdigital transducers, as shown in FIG. 1, the pair of variable-frequency interdigital transducers are symmetrically distributed along the lithium niobate wafer 1. If the pair of slanted-finger interdigital transducers 2 are circular-arc, centers of curvature radii of the pair of variable-frequency interdigital transducers 2 coincide at a point, and the pair of variable-frequency interdigital transducers are centrally symmetrically distributed about this point. Through the above structural design, the pair of slanted-finger interdigital transducers 2 can generate SAWs of different frequencies after being excited, and the SAWs can be superimposed in a central region of the pair of slanted-finger interdigital transducers 2 to form standing SAWs. The liquid tank 3 is located above the region where the standing SAWs are formed. In order to realize the fabrication of the locally heterogeneous composite material, the UV light source 4 emits UV light to the liquid tank through the transparent lithium niobate wafer 1 so as to perform photocuring of the photosensitive liquid in the liquid tank.

[0033] The fabrication process of the locally heterogeneous composite material of the present disclosure includes three steps:

[0034] Step 1: The functional particles, the photosensitive liquid and the photoinitiator are mixed evenly to form the mixture 5, and the mixture is added into the liquid tank 2 through a pipette. The functional particles are indicated by black dots in FIG. 2.

[0035] The functional particles include but are not limited to metal powder, organic particles and cells.

[0036] The maximum size of the functional particles is less than 1/10 of a wavelength of the SAWs, so as to avoid the influence of the functional particles on the acoustic field distribution. The photosensitive liquid is preferably a substance with a low dynamic viscosity, such as low-molecular-weight PEGDA. After the functional particles, the photosensitive liquid and the photoinitiator are mixed, an ultrasonic vibration process is performed such that the functional particles are evenly dispersed in the photosensitive liquid.

[0037] Step 2: High-frequency sinusoidal signal regulated by frequency and time are input to the slanted-finger interdigital transducers 2, so as to excite the corresponding standing SAWs. The SAWs are coupled and enter the liquid tank to form a local acoustic field in the photosensitive liquid. The functional particles in the photosensitive liquid are affected by acoustic radiation force to form a stable array arrangement in a local region 6.

[0038] Step 3: The UV light source is turned on to cure the photosensitive liquid, thereby completing the fabrication of the locally heterogeneous composite material. During the curing process, the photosensitive liquid is protected by nitrogen gas, so as to avoid the contact between the surface of the photosensitive liquid and the oxygen to cause the curing of the surface liquid to fail. After curing, the position of the functional particles remains unchanged, and the functional particles are still distributed within localized acoustic field range 6.

[0039] A method for preparing a locally heterogeneous composite material provided by the present disclosure will be described below through specific examples.

[0040] Example 1: Distribution range characteristic of standing SAWs formed by frequency-regulated SAWs

[0041] FIG. 2 shows a pair of slanted-finger interdigital transducers, and it can be seen as a top view of the device in FIG. 1 without the liquid tank 3 and the mixture 5. According to the principle of the SAW transducers, the excitation frequency of the transducers corresponds to the finger width thereof, which is f=c/4 m, wherein c is an acoustic speed in a direction of a lithium niobate wafer 1 parallel to a finger width direction of the slanted-finger interdigital transducers 2, and m is a finger width (or a finger spacing) of the pair of slanted-finger interdigital transducers. Since the finger width of the slanted-finger interdigital transducers varies, the adjustment range of the excitation frequency is f.sub.min<f<f.sub.max, and the minimum frequency f.sub.min corresponds to the maximum finger width. Similarly, the maximum frequency f.sub.max corresponds to the minimum finger width.

[0042] In an application process, due to the influence of the quality factor of the pair of slanted-finger interdigital transducers, the resonance frequency has a certain bandwidth. Therefore, when the sinusoidal signal with a specific excitation frequency of f.sub.1 (f.sub.min<f.sub.1<f.sub.max) are input, standing SAWs with a width of a.sub.1 will be formed on both sides of the finger width corresponding to the specific frequency f.sub.1, as indicated by the dotted line in FIG. 2. a.sub.1 can be calculated by an approximate formula a.sub.1=1/n*f/(f.sub.max−f.sub.min)*d, wherein n is the interdigital pair number of the slanted-finger interdigital transducers 2, d is the acoustic aperture, that is, the total width of the electrodes, as shown in FIG. 2.

[0043] Meanwhile, the position b.sub.1 of the SAWs generated by inputting the specific frequency relative to the slanted-finger interdigital transducers 2 can be calculated from the excitation frequency f.sup.1 and the design parameters of the slanted-finger interdigital transducers. For the slanted-finger interdigital transducers 2 with the finger width changing evenly, the calculation formula of the position is b.sub.1=(f.sub.max−f)/(f.sub.max−f.sub.min)*d.

[0044] Example 1 shows that the selectivity of the region and position of the SAWs in the width direction can be achieved by frequency regulation of the input sinusoidal signals.

[0045] Example 2: Distribution range characteristic of standing SAWs formed by time-regulated SAWs

[0046] For the sake of convenience, a two-dimensional (2D) situation is analyzed, that is, the SAW propagation characteristics of the slanted-finger interdigital transducers 2 along a horizontal midline section in FIG. 2 after being input with the time-regulated sinusoidal signals. The time-regulated input signals are shown in FIG. 3, wherein V.sub.1 and V.sub.2 are the input signals into the pair of SAW transducers respectively. t.sub.1 corresponds to a sinusoidal signal and t.sub.2 corresponds to a zero input signal. V.sub.1 and V.sub.2 are exactly the same in each cycle but there is a relative time difference t.sub.c. The cycle of the sinusoidal signals corresponds to the excitation frequency of the slanted-finger interdigital transducers 2 at a specific position. t.sub.m is assumed to be a time it takes for the SAWs to be completely absorbed from excitation to propagation to the two sides of the lithium niobate wafer. To avoid superimposition of the signals at other positions, (t.sub.1+t.sub.2)>t.sub.m. However, in an actual process, in order to ensure the maximum energy, t.sub.1+t.sub.2 is slightly greater than t.sub.m.

[0047] After the time-regulated signals are input, the frequency-variable interdigital transducers 2 form two traveling SAWs, as shown in FIG. 4. The two SAWs propagate in opposite directions (indicated by the black arrows in the upper part of FIG. 4) and then form standing SAWs (indicated by the dotted region). The width of the standing SAW region is the same as the width of a single traveling SAW, expressed as a.sub.2=t.sub.1*c, as indicated by the dotted line in FIG. 4, wherein c is the acoustic speed of the lithium niobate wafer 1 in the direction parallel to the width direction of the slanted-finger interdigital transducers 2. The position b.sub.2 of the standing SAW forming region relative to the center of the lithium niobate wafer 1 is determined by the time difference t.sub.c of the sinusoidal signals of the two transducers, specifically, b.sub.2=t.sub.c*c. If t.sub.c=0, the two SAWs meet exactly in the center of the lithium niobate wafer 1, and b.sub.2 is equal to 0. Meanwhile, the position b.sub.2 of the standing SAWs can be changed by adjusting the time difference t.sub.c of the periodic signals.

[0048] Example 2 shows that the selectivity of the region and position of the SAWs in the length direction can be achieved by the time regulation of the input sinusoidal signals.

[0049] Example 3: Movement and photocuring of the functional particles under the action of the acoustic field

[0050] In Example 1 and Example 2, the range of the standing SAWs formed by the slanted-finger interdigital transducers under the excitation of the time-frequency regulated signals can be calculated. After the SAWs are formed on the lithium niobate wafer, the SAWs will couple along a Rayleigh angle and enter the photosensitive liquid to form nodes and antinodes of the same cycle. However, in the actual process, affected by the propagation loss and the level of the photosensitive liquid, the final range of the acoustic pressure field may be slightly smaller than the region of the standing SAWs, which can be calculated in the time domain by a finite element (FE) method. Specifically, under the premise of ignoring the effect of the functional particles on the acoustic field, the acoustic field distribution p(x,y,z,t) inside the photosensitive liquid is obtained in the time domain through piezoelectric coupling and acoustic-structure coupling. The final acoustic pressure distribution range p(x,y,z) is obtained by calculating the integral of 1/(t.sub.1+t.sub.2)*(∫p(x,y,z,t)dt) over one input signal cycle (t.sub.1+t.sub.2).

[0051] Within the calculated acoustic pressure distribution range, there will be periodic nodes and antinodes with a distribution cycle the same as that of the operating SAWs. Meanwhile, the acoustic pressure will exert acoustic radiation force on the functional particles inside the photosensitive liquid, such that it moves to an acoustic pressure node and finally converge at the node. That is, the cycle of the final particle arrangement is equal to half of the cycle of the operating SAWs. At this time, if the UV light source 4 is turned on, the photosensitive liquid will be cross-linked under the driving of the photoinitiator to form a macromolecular material from small molecules, and then change from liquid to solid to form the heterogeneous composite material. Since the photocuring time is usually very short, the functional particles will not move significantly during the photocuring process, so the final arrangement position of the functional particles is the same as that before curing.

[0052] Example 4: Fabrication of a locally heterogeneous composite material based on time-frequency regulated SAWs

[0053] FIG. 5 is a top view of a locally heterogeneous composite material prepared by inputting time-frequency regulated SAW signals to a pair of slanted-finger interdigital transducers 2. In this example, in this view, the lithium niobate wafer 1 is 5 mm long and 3 mm wide. The length direction of the lithium niobate wafer 1 coincides with a Y-cut 128° X-direction, then c=3940 m/s, t.sub.m=1.27 μs. The slanted-finger interdigital transducers 2 are straight-line oblique in the finger length direction. The finger width ranges from 25 μm to 50 μm, corresponding to f.sub.max and f.sub.min of 39.4 MHz and 19.7 MHz, respectively. The total electrode width d=2 mm, and there are 4 pairs of electrodes. In order to clearly represent the oblique interdigital transducer, the slanted-finger interdigital transducers 2 in FIG. 5 are for illustration only, and are not drawn to the scale.

[0054] The input frequency of the pair of slanted-finger interdigital transducers 2 is 30 MHz, and the corresponding SAW wavelength is 131 μm. The duration of the sinusoidal signals is t.sub.1=0.33 μs (10 sinusoidal cycles), and the interval time t.sub.2=1 μs (30 sinusoidal cycles), which meets the requirement that t.sub.1+t.sub.2 is slightly greater than t.sub.m. In addition, there is a time difference t.sub.c=0.2 between the input signals of the pair of slanted-finger interdigital transducers 2. The size of the localized acoustic field distribution range 6 is a.sub.1=0.6 mm, a.sub.2=1.3 mm. The position of the localized acoustic field distribution range 6 is b.sub.1=0.96 mm, b.sub.2=0.76 mm.

[0055] The functional particles (indicated by the black dots) are distributed in an array within the localized acoustic field range 6 with a cycle of half the wavelength of the input SAWs (66 μm in this example). Affected by Rayleigh radiation, the specific arrangement range is slightly smaller than the localized acoustic field range 6, which can be accurately calculated by the FE method. Outside the localized acoustic field range 6, the functional particles are randomly arranged.