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METHOD OF USE OF ULTRASOUND TO STUDY DETAILS The immersion fluid

机译:使用超声波研究细节的方法浸入液

摘要

1.method u0438u0441u043fu043eu043bu044cu0437u043eu0432u0430u043du0438u00a0 ultrasound u0434u043bu00a0 u0438u0441u0441u043bu0435u0434u043eu0432u0430u043du0438u00a0 details in u0438u043cu043cu0435u0440u0441u0438u043eu043du043du043eu0439 fluid involves the use of a u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u0442u0435u043bu00a0 emitting focused p u0443u0447u043eu043a ultrasonic waves and a receiver echo signals formed by the u043eu0442u0440u0430u0436u0435u043du0438u00a0 focused beam of any defects in the u0443u043fu043eu043cu00a0u043du0443u0442u043eu0439 details in the axis of the focused beam on the surface of the u043fu0435u0440u043fu0435u043du0434u0438u043au0443u043bu00a0u0440u043du0430 detailsmethod u0437u0430u043au043bu044eu0447u0430u0435u0442u0441u00a0 using u043cu043du043eu0433u043eu044du043bu0435u043cu0435u043du0442u043du043eu0433u043e circular ultrasonic u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u0442u0435u043bu00a0, u0441u0432u00a0u0437u0430u043du043du043eu0433u043e with electronic means for automatic focusing, and if the axis of siberian federal district u043au0443u0441u0438u0440u043eu0432u0430u043du043du043eu0433u043e beam close to the edge details and passes through the zone of the shadows, u043au043eu0442u043eu0440u0430u00a0 can mask the presence of a defect in u0443u043fu043eu043cu00a0u043du0443u0442u043eu0439 zone, at least in the part of the volume.then u043eu0441u0443u0449u0435u0441u0442u0432u043bu00a0u044eu0442 slant axis of focused beam in the direction of u043au0440u0430u00a0 details on u043du043eu0440u043cu0430u043bu0438 surface details on the corner, which is quite small u0434u043bu00a0 u0438u0437u0431u0435u0436 u0430u043du0438u00a0 u0438u0437u043cu0435u043du0435u043du0438u00a0 amplitude reflected defect waves and high u0434u043bu00a0 u0438u0441u043au043bu044eu0447u0435u043du0438u00a0 lateral shadow zone on all, or substantially all over the depth of detail.;2. method for 1, which contains the original use of the calibration details u0434u043bu00a0 u0438u0437u043cu0435u0440u0435u043du0438u00a0 first values of the angle, beyond which the shadow suit u043bu044eu0447u0430u0435u0442u0441u00a0 u0434u043bu00a0 different depths within the details, and the choice of u0437u043du0430u0447u0435u043du0438u00a0 angle u0434u043bu00a0 u0438u0441u0441u043bu0435u0434u043eu0432u0430u043du0438u00a0, less than, or slightly more than the maximum value first of u0443u043fu043eu043cu00a0u043du0443u0442u044bu0445 measured values.;3. method for 2, which also contains additional details on the calibration of the second u0437u043du0430u0447u0435u043du0438u00a0 angle, beyond which the amplitude of the reflected u0434u0435u0444u0435u043au0442u043e m wavelength is u0443u043cu0435u043du044cu0448u0430u0442u044cu0441u00a0 with increase of angle, and the inclination of the axis of u0434u043bu00a0 u0438u0441u0441u043bu0435u0434u043eu0432u0430u043du0438u00a0 focused beam, the value of which lies between the first u0443u043fu043eu043cu00a0u043du0443u0442u044bu043cu0438 a u0437u043du0430u0447u0435u043du0438u00a0u043cu0438 and the second value.;4. method for 1, in which the angle of inclination of the focused beam on the surface of u0441u043eu0441u0442u0430u0432u043bu00a0u0435u0442 u043du043eu0440u043cu0430u043bu0438 details about 3 u0434u043bu00a0 parts made of ti zeng.;5. method for p.1, in which u0434u043bu00a0 u043eu043fu0440u0435u0434u0435u043bu0435u043du0438u00a0 u043fu0440u043eu0442u00a0u0436u0435u043du043du043eu0441u0442u0438 zone shadows from u043au0440u0430u00a0 details u043eu0441u0443u0449u0435u0441u0442u0432u043bu00a0u044eu0442 displacement element u043eu0442u043au043bu043eu043du0435u043du0438u00a0 u0434u043bu00a0 u043eu0442u043au043bu043eu043du0435u043du0438u00a0 focused beam in dc motors u0435u0449u0435u043du0438u0438 on surface parts along an axis crossing the axis of the focused ultrasonic beam; and the identification of the elements u043eu0442u043au043bu043eu043du0435u043du0438u00a0, to u043eu0442u043eu0440u043eu043c amplitude echo signalformed by the focused beam from the defect u0438u0437u043cu0435u043du00a0u0435u0442u0441u00a0 between minimum and maximum u0437u043du0430u0447u0435u043du0438u00a0u043cu0438.;6. method according to clause 5, in which the element u043eu0442u043au043bu043eu043du0435u043du0438u00a0 u043fu0440u0435u0434u0441u0442u0430u0432u043bu00a0u0435u0442 a u043fu0440u0435u0434u043eu0441u0442u0430u0432u043bu00a0u044eu0449u0443u044e prism, at least one u043eu0442u0440u0430u0436u0430u0442u0435u043bu044cu043du0443u044e line, bowed, for example, under 45 to tu. u0435u0440u0445u043du043eu0441u0442u0438 details and to the axis of the focused beam.;7. method for p.6, in addition to containing the identification of the two diametrically opposed about the axis of the prism focused ultrasonic beam, u0434u043bu00a0 which ila u043bu0438u0442u0443u0434u0430 echo signal formed by a focused beam of defectstarts to drop from the maximum u0437u043du0430u0447u0435u043du0438u00a0 in advance and to the axis of the focused beam; and the calculation of u0440u0430u0441u0441u0442u043eu00a0u043du0438u00a0 between the u0434u0432u0443u043cu00a0 based on u0438u00a0u043cu0438 u0434u043bu00a0 u043fu043eu043bu0443u0447u0435u043du0438u00a0 u043fu0440u043eu0442u00a0u0436u0435u043du043du043eu0441u0442u0438 shadow zone.
机译:1.方法 u0438 u0441 u043f u043e u043b u044c u0437 u043e u0432 u0430 u043d u0438 u00a0超声 u0434 u043b u00a0 u0438 u0441 u0441 u043b u0435 u0434 u0434 u0438 u043c u043c u0435 u0440 u0441 u0438 u043e u043e u043d u043d u043d u043e u0439流体中的 u0432 u0430 u043d u0438 u00a0详细信息涉及使用 u043f u0440 u0435 u043e u0431 u0440 u0430 u0437 u043e u0432 u0430 u0442 u0435 u043b u00a0发射聚焦的 u0443 u0447 u043e u043a超声波和由 u043e u0442 u0440 形成的接收器回波信号u0430 u0436 u0435 u043d u0438 u00a0 u0443 u043f u043e u043c u00a0 u043d u0443 u0442 u0432 u043e u0439聚焦光束在表面上的任何缺陷的细节 u043f u0435 u0440 u043f u0435 u043d u0434 u0438 u043a u0443 u043b u00a0 u0440 u043d u0430详细信息方法 u0437 u0430 u0430 u043a u043b u043b u044e u0447 u0430 u04330 u0441 u00a0使用 u043c u043d u043e u0433 u043e u044d u043b u0435 u043c u0435 u043d u0442 u043d u043e u0433 u043e圆形ultras onic u043f u0440 u0435 u043e u0431 u0440 u0430 u0437 u043e u043e u0432 u0430 u0442 u0435 u043b u00a0, u0441 u0432 u00a0 u0437 u0430 u043d u043d u043d u043 u043e具有电子装置自动聚焦,并且西伯利亚联邦区的轴 u043a u0443 u0441 u0438 u0440 u043e u0432 u0430 u043d u043d u043d u043e u0433 u043e光束靠近边缘细节并且通过阴影区域 u043a u043e u0442 u043e u0440 u0430 u00a0可以掩盖 u0443 u043f u043e u043e u043c u00a0 u043d u0443 u0443 u0442 u043e u0439区域,至少在体积的一部分中。然后 u043e u0441 u0443 u0449 u0435 u0441 u0442 u0432 u043b u00a0 u044e u0442聚焦光束的倾斜轴沿 u043a u0440 u043d u043e u0440 u043c u0430 u043b u0438上的u0430 u00a0详细信息角落上的表面细节非常小 u0434 u043b u00a0 u0438 u0437 u0431 u0431 u0435 u0436 u0430 u043d u0438 u00a0 u0438 u0437 u043c u0435 u043d u0435 u043d u0438 u00a0振幅反射缺陷wa ves以及所有或几乎整个细节深度上的高阴影区域和高阴影区域。2。方法1,其中包含原始使用的校准详细信息 u0434 u043b u00a0 u0438 u0437 u043c u0435 u0440 u0435 u043d u0438 u00a0角度的第一个值,超出此范围的阴影套装 u043b u044e u0447 u0430 u0435 u0442 u0441 u00a0 u0434 u043b u00a0细节内的不同深度,以及 u0437 u043d u0430 u0447 u0435 u043d u043d u0438 u00a0角度 u0434 u043b u00a0 u0438 u0441 u0441 u043b u0435 u0434 u043e u0432 u0430 u043d u0438 u00a0,小于或稍大于 u0443 u043f u043e u043c u00c0 u043d u0443 u0442 u044b u0445测量值; 3。 2的方法,其中还包含有关第二个 u0437 u043d u0430 u0447 u0435 u043d u0438 u00a0角度的校准的其他详细信息,超出的部分反射的 u0434 u0435 u0444 u0435 u043a u0442 u043e m波长为 u0443 u043c u0435 u043d u044c u0448 u0430 u0442 u044c u0441 u00a0随着角度的增加,以及 u0434 u043b u00a0 u0438 u0441 u0441 u043b u0435 u0434 u043e u0432 u0430 u043d u0438 u00a0聚焦光束的值位于第一个 u0443 u043f u043e u043c u00a0 u043d u0443 u0442 u044b u043c u0438 u0437 u043d u0430 u0447 u0435 u043d u0438 u00a0 u043c u0438和第二个值; 4。 1的方​​法,其中聚焦光束在 u0441 u043e u0441 u0442 u0430 u0432 u043b u00a0 u0435 u0442 u043d u043e u0440 u043c u0430 u043b的表面上的倾斜角度 u0438详细介绍3个由ti zeng制成的零件; 5。第1页的方法,其中 u0434 u043b u00a0 u043e u043f u0440 u0435 u0434 u0434 u0435 u043b u0435 u043d u043d u0438 u00a0 u043f u0440 u04340 u043e u0442 u00a0 u0436 u0435 u043d u043d u043e u0441 u0442 u0438来自 u043a u0440 u0430 u00a0详细信息的区域阴影 u043e u0441 u0443 u0449 u0435 u0441 u0442 u0432 u0432 u043b u00a0 u044e u0442 u043e u0442 u043a u043b u043e u043d u0435 u043d u0438 u00a0 u0434 u043b u00b0 u043e u0442 u043a u043b u043e u043e u043d u0435 u043d u0438 u00c0沿与聚焦超声束的轴相交的轴在表面部分上驱动电机 u0435 u0449 u0435 u043d u0438 u0438;并识别由缺陷束聚焦束形成的振幅回波的元素 u043e u0442 u043a u043b u043e u043d u0435 u043d u0438 u00a0至 u043e u0442 u043e u0440 u043e u043c u0438 u0437 u043c u0435 u043d u00a0 u0435 u0442 u0441 u00a0在最大值和最小值之间 u0437 u043d u0430 u0447 u0435 u043d u0438 u00a0 u043c u0438。; 6。根据条款5的方法,其中元素 u043e u0442 u043a u043b u043e u043d u0435 u043d u043d u0438 u00a0 u043f u0440 u0435 u0434 u0441 u0442 u042 u0430 u0432 u043b u0040 u0435 u0442 u043f u0440 u0435 u0434 u043e u0441 u0442 u0430 u0432 u043b u00a0 u044e u0449 u0443 u044e棱镜,例如至少45弯弓形的 u043e u0442 u0440 u0430 u0436 u0430 u0442 u0435 u043b u044c u043d u0443 u044e线。 u0435 u0440 u0445 u043d u043e u0441 u0442 u0438详细信息并指向聚焦光束的轴; 7。 p.6的方法,除了包含两个围绕着棱镜聚焦的超声波束沿直径方向相对的标识外,还形成了回波信号 u043b u0438 u0442 u0443 u0434 u0430通过聚焦的缺陷束开始从最大 u0437 u043d u0430 u0447 u0435 u043d u0438 u00a0预先下降到聚焦束的轴;并基于 u0438 u00a0 u043c u0438 u0434 u0432 u0443 u043c u00a0之间的 u0440 u0430 u0441 u0441 u0442 u043e u00a0 u0432 u0443 u043c u00a0计算 u00a0 u043f u043e u043b u0443 u0447 u0435 u043d u043e u0442 u00a0 u0436 u0435 u043d u043d u043d u043e u0441 u0442 u043d u043d u043d u043d u043e u0441 u0442 u0435

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