Dual-frequency ultrasonic transducer for scanning imaging
An ultrasonic transducer, scanning imaging technology, applied in the direction of fluids, piezoelectric/electrostrictive/magnetostrictive devices, electrical components, etc. using vibration, can solve problems such as resonance interference, reduce resonance interference, reduce Small approach angle blind spot, improving imaging resolution
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Embodiment 1
[0034] As a preferred embodiment, such as Figure 4 As shown, the large transducers 2 are distributed in a uniform array, and the small transducers 3 are installed on the midpoint of the line connecting the centers of two adjacent large transducers 2 and on the diagonal of the two large transducers 2 At the midpoint, 8×8=64 large transducers 2 distributed in a uniform array are installed on the substrate 1 , and 161 small transducers 3 are installed between the large transducers 2 .
[0035] In this embodiment, the center-to-center distance ds between the large transducers 2 is relatively large. At this time, the interference between the large transducers 2 is significantly reduced, but the reflected signal strength is insufficient, and the blind area of the approach angle is relatively large. Since the center distance ds of the transducer unit is designed strictly according to ds=λ / 2, the use area of the entire transducer array is seriously wasted, such as Figure 5 As s...
Embodiment 2
[0038] As a preferred embodiment, such as Figure 6 As shown, the large transducers 2 are distributed in a staggered array, and the relative positions of the large transducers 2 in two adjacent rows differ by λ / 4. The number of large transducers 2 in two adjacent columns is 8 and 7 respectively.
[0039]Since the large transducer 2 plays a decisive role in the function of the device, the small transducer 3 is complementary and optimized. For the arrangement of large transducers 2, the overall sound pressure distribution is not uniform enough. Based on this, Figure 6 exist Figure 4 On the basis of the staggered arrangement, the positions of two adjacent large transducers 2 are staggered by λ / 4, and the staggered vacancies are filled by small transducers 3 . Such dislocation design makes the sound pressure distribution everywhere more uniform under the layout of the large transducer 2, such as Figure 7 shown.
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