Method of designing high-power energy-gathered reflex housing
An energy-concentrating reflector and a design method technology, which are applied in computing, special data processing applications, instruments, etc., can solve the problem that the energy-concentrating reflector cannot obtain the best reflection efficiency, the installation error and transient dynamic response are not considered, and there is no Considering the nonlinear effects of acoustic pulses and other issues, the effects of improving structural stress safety margin and energy gathering effect, improving design efficiency, and facilitating installation and formation are achieved.
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Embodiment 1
[0042] The structure of the ellipsoid energy-gathering reflector to be designed in this embodiment is as follows: figure 1 As shown, its surface equation can be expressed as: . In the figure, c is the half focal length of the reflector, c is 0.15~15m, w is the aperture of the reflector, w is 0.1~1m, h is the depth of the reflector, by installing the discharge electrode at the first focal point F1, it can Converge the energy reflection to the second focal point F2. The position of the second focal point F2 is set according to application requirements.
[0043] The acquisition of the processing data of the energy-concentrating reflector mainly includes three processes, and its flow chart is as follows: figure 2 shown.
[0044] Step 1: Generate ideal surface type value table
[0045] According to the requirements of the best cost-effective ratio, the gain function method is used to calculate the relationship between the energy-gathering gain and the depth h of the reflecto...
Embodiment 2
[0061] The structure of the energy-gathering reflector in this embodiment is as follows: Figure 7 As shown, its surface equation can be expressed as: . By placing the discharge electrode at the focus F of the parabola, the beamforming can be reflected to generate parallel waves. For example, for a parabolic reflector with a diameter of w'=1m and a concave depth of h'=0.5m, placing the discharge electrode at F=0.25m can form an acoustic pulse impact beam with a diameter of 1m. Also adopt the design method adopted in embodiment 1 to obtain the ideal surface type value table, the revised surface type value table and the processed surface type value table, finally according to Figure 6 The specific implementation process is processed to obtain the parabolic energy-concentrating reflector with the best cost-effectiveness ratio and the best reflection efficiency characteristics.
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