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Ground vibrations produced by surface and near-surface explosions

机译:地面和近地爆炸产生的地面振动

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Measurements of seismic signatures produced by airborne, near-surface detonations of explosive charges over a variety of ground types show two distinct ground vibration arrivals. In all cases, the earlier arrival (precursor), has a time of arrival consistent with a predominantly underground path and coupling of blast sound to the ground close to the source and is always much smaller than the later vibration, the time of arrival of which is consistent with coupling from the air blast arrival at the receiver. The ratio of the seismic particle velocity to the acoustic pressure at the surface for the air-coupled seismic wave is constant with respect to distance and maximum pressure at a given location, but varies from site to site, with values usually between 1 and 13 μms~(-1)Pa~(-1). For the precursor seismic wave, a coupling coefficient of 0.16 μm s~(-1) Pa~(-1) was measured. A numerical code enabling calculations of the fields due to an impulsive source above a layered poro-elastic ground is described. Predictions of the air pressure spectrum above ground and the vertical and radial components of solid particle velocity near the ground surface are found to compare tolerably well with the measured spectra and waveforms of acoustic and seismic pulses at about 100 m range in seis-mically-hard and -soft soils and with a snow cover present. The predicted seismic responses in 'soft' soil confirm that the existence of a near-surface S-wave speed less than that in air is responsible for the observed 'ringing', i.e. a long low-frequency wavetrain associated with coupling to the dispersive Ray-leigh wave. The predicted seismic pulses in the presence of the shallow snow cover explain the observed phenomenon whereby a high frequency ground vibration is modulated by a lower frequency layer resonance. An empirical equation relating ground vibration from explosions to distance predicts that the commonly-used vibrational damage peak velocity criterion of 12 or 25 mm s~(-1) will be exceeded when the peak positive pressure exceeds 480 Pa (147.6 dB) or 1 kPa (154.0dB), respectively. Either of these levels is much higher than the current U.S. Army overpressure damage criterion of 159 Pa (138 dB). Thus in most situations damage from blast overpressure will occur long before damaging levels of ground vibration are reached, so it is likely that civilian perceptions of vibration are produced by coupling from the airblast.
机译:对各种类型地面上的炸药的机载近地爆炸产生的地震信号的测量结果表明,有两种不同的地面振动到达。在所有情况下,较早到达(前体)的到达时间与主要是地下路径以及爆炸声与靠近源头的地面的耦合相一致,并且总是比较晚到达的振动小得多。与鼓风到达接收器的耦合是一致的。对于空气耦合地震波,地震粒子速度与表面声压之比相对于给定位置处的距离和最大压力而言是恒定的,但因位置而异,通常在1到13μms之间〜(-1)Pa〜(-1)。对于前体地震波,测量的耦合系数为0.16μms〜(-1)Pa〜(-1)。描述了一种数字代码,该数字代码能够计算由于层状孔隙弹性地面上方的脉冲源引起的场。发现地面上的气压谱以及地表附近固体颗粒速度的垂直和径向分量的预测与在地震硬的约100 m范围内测得的声波和地震脉冲的频谱和波形具有很好的耐受性和-软土,并有积雪。在“软”土壤中的预测地震响应证实,近地表S波的存在速度比空气中的慢,这是观测到的“振铃”的原因,即与耦合到色散射线相关的长低频波列-瑞波。在浅雪覆盖的情况下预测的地震脉冲解释了所观察到的现象,由此高频地面振动由低频层共振调制。将爆炸引起的地面振动与距离相关联的经验公式预测,当峰值正压超过480 Pa(147.6 dB)或1 kPa时,将超过12或25 mm s〜(-1)的常用振动损伤峰值速度准则。 (154.0dB)。这些水平中的任何一个都远高于当前美国陆军159 Pa(138 dB)的超压损坏标准。因此,在大多数情况下,由于爆炸超压造成的损害会在达到破坏性的地面振动水平之前很久就发生,因此,平民的振动感觉很可能是由空气冲击产生的。

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