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ChaAter26 <br />mined based on the kind of mck surrounding the explosive and at <br />receiving site where the particle motion is measured. (Experi¢ <br />has shown that differences in vibration levels caused by differ <br />kinds of commercial explosives are usually small compazed to <br />variations caused by other factors.) <br />• m and n are empirical constants based primarily on the ova <br />geology between the explosion and receiving sites. <br />• R is the distance between the explosion and receiving sites. <br />Work by the U.S. Bureau of Mines in ground motion transmis~~ <br />produced two particularly significant results for the typical chi <br />weights and distances found in surface blasting: <br />• The constant m is equal to one-half of the constant n. <br />The power law equation then has only two unknowns and asst <br />the following form: <br />where the quantity A/W"= is known as the scaled distance. <br />• The peak particle velocity depends on the maximum charge- <br />weight-per-delay and not on the total charge weight, providing the <br />delay interval is eight milliseconds or more. <br />These results, combined with a large number of field measure. <br />menu, have shown that the propagation equation can typically be <br />expressed as follows: <br />R l-~ s <br />V = 160 W" / <br />where <br />Scaled Distance - ft./Ib.'r2 <br />V =peak particle velocity in ips <br />(inches per second) <br />R =distance between explosion and <br />recording sites in feet <br />W =maximum pounds-per-delay-period <br />of eight milliseconds or more <br />Blasters can use this equation to estimate the peak particle velocity <br />oC a seismic wave or they can use the graph shown in Figure 26-B. For <br />example: Determine the typical peak particle velocity from a nor <br />molly confined blast with a maximum charge-weight-per-delay-period <br />of 400 pounds at a distance of 1,000 feet from the receiving site. The <br />scaled distance, R/W"'. = 1,000/400"': = 50 corresponds [o a peak <br />particle velocity of 0.31 ips on the graph. <br />It should be emphasized that the expression given in the above <br />equation relating the peak pazticle velocity, charge-weigh Lper- <br />delay-period, and distance provides typical values only Tor planning <br />blasting projects in the absence of seismic data. Modification may be <br />426 <br />Vibration and Air Blast <br />9 <br />C <br />O <br />to <br />d <br />a <br />d <br />a <br />a <br />d <br />L <br />v <br />C <br />r <br />.. <br />V <br />O <br />d <br />d <br />v <br />m <br />a <br />Y <br />m <br />o. <br />t.l <br />0~ <br />0.1 <br />0: <br />O.i <br />0.! <br />0. <br />0. <br />Flgure 26-B. Typical values of peak panicle velocity es a function of scaled distance for <br />6leeting to s Iree lace. Charge weight Is per-delay-period of eight milliseconds or more. <br />Blasts made under tight confinement such es the opening of holes In headings or In <br />presplltting may give values Ilve times more then typical under normal conllnament. <br />427 <br />\J <br />• <br />10 15 20 25 30 40 50 80 70 80 ev i 00 <br />