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Induced stress wave on the materials surface irradiated by high-intensity pulsed ion beam

机译:高强度脉冲离子束辐照在材料表面的感应应力波

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The induced stress wave in pure metal Al and Ti, and thermal barrier coating (TBC) on heat-resistant steel irradiated by high-intensity pulsed ion beam (HIPIB) with ion current density of 200 and 350 A/cm2 and shot number of 1–10 at accelerating voltage of 350 kV with a pulse width of 75 ns (full width at half maximum) has been dynamically measured using lead–zirconte–titanate (PZT) piezoelectric sensor. The measured waveform showing a process of loading, unloading and oscillating is detected as a series of positive–negative pulses, in which the peak value of the first negative pulse represents the maximal intensity of the stress wave. For Al sample the intensity of stress wave is about 40 MPa at 200 A/cm2 and about 78 MPa at 350 A/cm2. At 350 A/cm2, the intensity of stress wave for Ti sample is about 36 MPa. During ablation, the intensity of stress wave for Al irradiated at 200 A/cm2 is similar to that of Ti at 350 A/cm2, due to the different melting and vaporizing behavior. For TBC sample, its high melting temperature and porous structure cause the decreasing intensity to 18 MPa. At 350 A/cm2, the peak intensity of stress wave for the pure Al and Ti irradiated during 10 shots is in the range of 70–90 MPa and 27–40 MPa, respectively, and for the TBC is 15–20 MPa. The fluctuation of stress wave intensity is attributed to the selective ablation caused by the micro-non-uniformity on the sample surface with different mass loss per shot. It is found that the structure and properties of materials have an effect on the formation and transmission of the induced stress wave in the materials under the irradiation conditions.
机译:高强度脉冲离子束(HIPIB)以200和350 A / cm2的离子电流密度和1的发射数照射纯金属Al和Ti中的感应应力波以及耐热钢上的热障涂层(TBC)在350 kV的加速电压下,脉冲宽度为75 ns(半峰全宽)时的–10已使用锆钛酸铅(PZT)压电传感器进行了动态测量。测得的波形显示了加载,卸载和振荡的过程,被检测为一系列正负脉冲,其中第一个负脉冲的峰值代表应力波的最大强度。对于铝样品,应力波强度在200 A / cm2时约为40 MPa,在350 A / cm2时约为78 MPa。在350 A / cm2时,Ti样品的应力波强度约为36 MPa。在烧蚀期间,由于不同的熔化和汽化行为,以200 A / cm2辐射的Al的应力波强度与以350 A / cm2辐射的Ti的应力波强度相似。对于TBC样品,其高熔点温度和多孔结构导致强度降低至18 MPa。在350 A / cm2时,在10次发射中照射的纯Al和Ti的应力波的峰值强度分别在70–90 MPa和27–40 MPa的范围内,而TBC为15–20 MPa。应力波强度的波动归因于样品表面的微观不均匀性导致的选择性烧蚀,且每次发射的质量损失不同。发现材料的结构和性能对在辐照条件下材料中的感应应力波的形成和传递有影响。

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