A cambered acoustic waveguide device suitable for the field of ultrasonic thickness measurement
An ultrasonic wave and sound-focusing technology, which is applied in the field of arc-shaped sound-focusing waveguide devices, can solve the problems of the influence of receiving position and angle, the inability to guarantee the incident angle, and the unoptimized receiving angle, etc., and achieve the effect of reducing reflection
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Embodiment 1
[0098] image 3 It is one of the examples described in accordance with the present invention. In practice, an arc-shaped acoustic waveguide device is used, which is divided into left and right parts, a transmitting waveguide 1 and a receiving waveguide 2 . Between the A section and the B section is a regular bar with a rectangular section shape, and all sections parallel to the A section have the same shape and size as the A and B sections. The size of the section A is adapted to the size of the circular surface of the transducer 5. In order to maximize the contact area between the incident surface of the waveguide and the circular surface of the transducer 5, it can also be made into a square section inscribed with the circular surface of the transducer 5. As shown in the figure, the diameter of the circular surface of the transducer 5 is Φ18, and the rectangular size of the A section is 12X15 (mm).
[0099] The H surface is an arc surface, which starts to bend from the B s...
Embodiment 2
[0104] In order to adapt the installation between the waveguide and the instrument, the image 3 Based on the curved surface waveguide shown, it can also be extended to such as Figure 4 The waveguide shape shown. The waveguide expands upwards from the A section, and the section shape of the extension section 7 is still a regular bar, which is the same as the A section. After the second bending, it reaches the D section. On the slope E, it is reflected by the E surface to the F surface, and after being reflected by the F surface, it becomes vertically downward and enters the A section. It is guaranteed that after the second reflection of the full-wave sound wave incident from the D surface, all the sound rays just translate to the A section, and all the sound ray travels from the D section to the A section are equal. The situation after the sound wave passes through the A section is consistent with the above-mentioned arc waveguide. The E plane and the F plane are parallel,...
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