16 research outputs found

    ๋ถ€ํƒ„ํ…ŒํŠธ๋ผ์นด๋ฅด๋ณต์‹œ์‚ฐ์— ์˜ํ•œ ๋ฉด์ง๋ฌผ์˜ DP๊ฐ€๊ณต

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์„ฌ์œ ๊ณ ๋ถ„์ž๊ณตํ•™๊ณผ,1995.Maste

    ์ „๋‹จ๋†ํ™”์œ ์ฒด๋ฅผ ํ•จ์œ ํ•œ ์ง๋ฌผ์˜ ๊ณ ์† ์ถฉ๊ฒฉ ์ €ํ•ญ์„ฑ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์žฌ๋ฃŒ๊ณตํ•™๋ถ€, 2012. 8. ๊ฐ•ํƒœ์ง„.yarn pullout is dominant at lower impact velocity while stress localization is dominant at high impact velocity. The hybridization of STF treated fabrics improved both blunt trauma resistance and perforation resistance against deformable projectiles (e.g. 9mm full metal jacketed (FMJ) bullets) compared to an all neat fabric panel having the same areal density. The layering sequence of the neat and STF treated fabrics in a hybrid panel was found to play an important role in improving the ballistic performance, where the panel with neat fabric layers backed by STF impregnated fabric layers showed a better performance. Such superior ballistic performance is presumed to be due to the better coupling of yarn elongation in the frontal neat fabric layers and the rear STF treated fabric layers, and thus, increased bullet expansion. A conceptual analysis was carried out by adopting a method of accumulating successive line segments to present the energy dissipation route of each panel during the impact. For another series of hybrid ballistic materials (i.e. unidirectional (UD) and woven fabrics), the effect of layering sequence on the ballistic performance was further investigated with two different kinds of bulletsan unexpandable 5.56mm FSP and an easily expandable .44 Magnum semi-jacketed hollow point (SJHP) bullet. Some of the woven fabric layers were treated with STF to modify their properties. When the layers with smaller in-plane constraint (neat woven fabric) were laminated behind the layers with larger in-plane constraint (UD or STF treated woven fabric), an increase in perforation resistance against the FSP was observed due to the decreased out-of-plane constraint. When the layering sequence was reversed, an increase in both the blunt trauma resistance and perforation resistance against the .44 Magnum round was observed due to the better coupling of yarn elongation in the frontal and rear layers. The effect of fabric count and shot location on the ballistic performance of hybrid panels containing STF impregnated layers was also investigated. The panels with higher fabric count dissipated a higher fraction of the given impact energy through tensile dissipation and this led to a lower BFS. The decrease in BFS value by the hybridization of neat and STF impregnated fabrics was smaller for panels of densely woven fabric due to a larger difference in the warp and weft crimp ratios. Shot location affected the V50 value as well as the BFS value of the panels, where both values increased as the shot location approached the edge. Finally, the amount of energy transferred to the backing material of oil-based clay (i.e. kinetic dissipation) in ballistic tests of soft body armor panels was assessed. To determine the relationship between penetration depth (or dent volume) and impact velocity (or energy), weight dropping test with a series of steel spheres was carried out at low impact velocities, and direct shooting with a 5.56mm FSP was carried out at high impact velocities. At both high and low impact velocities, the volume of the dent made in the oil-based clay was proportional to the velocity of the impactor. The change in dent volume per the change in impact velocity was found to be proportional to the 1.5th power of the mass of the impactor, while the energy absorption per unit dent volume increased linearly with the impact velocity. The relationship between trauma depth (or dent volume) and kinetic dissipation of a soft body armor panel subjected to a 9mm bullet at 436 m/s is presented, where the trauma diameter approached that of a 1.043 kg steel ball. Keywords: high velocity impact, soft body armor, shear thickening fluid, laminating sequence, fabric count, crimp, shot location, ballistic limit, backface signature, kinetic dissipation์ „๋‹จ๋†ํ™”์œ ์ฒด๋ฅผ ํ•จ์œ ํ•œ ๋ฐฉํƒ„์ง๋ฌผ(์—ฐ์งˆ๋ฐฉํƒ„์žฌ)์˜ ๊ณ ์† ์ถฉ๊ฒฉ ์ €ํ•ญ์„ฑ์— ๊ด€ํ•œ ์—ฐ๊ตฌ๋ฅผ ์ˆ˜ํ–‰ํ•˜์˜€๋‹ค. ์—ฐ๊ตฌ์— ์‚ฌ์šฉ๋œ ์ „๋‹จ๋†ํ™”์œ ์ฒด๋Š” ์•ก์ƒ์˜ ํด๋ฆฌ์—ํ‹ธ๋ Œ๊ธ€๋ฆฌ์ฝœ์— ๊ณ ์ƒ์˜ ๊ฒฝ์งˆ ์‹ค๋ฆฌ์นด ๋‚˜๋…ธ์ž…์ž๊ฐ€ ์ž„๊ณ„์น˜์— ๊ทผ์ ‘ํ•˜๊ฒŒ ์ถฉ์ „๋œ ์—ฐ์งˆ์˜ ํ˜ผํ•ฉ์‘์ถ•์ƒ ๋ฌผ์งˆ๋กœ์„œ ์ž„๊ณ„์น˜ ๋ถ€๊ทผ์˜ ์ „๋‹จ๋ณ€ํ˜•์†๋„์—์„œ ์ „๋‹จ์‘๋ ฅ์ด ๊ฐ€์—ญ์ ์œผ๋กœ ๊ธ‰๊ฒฉํžˆ ๋ณ€ํ•˜๋Š” ๊ฑฐ๋™์„ ๋ณด์ธ๋‹ค. ์ „๋‹จ๋†ํ™”์˜ ๊ฐœ์‹œ์ ์€ ์ž…์ž์˜ ํฌ๊ธฐ์— ์˜์กดํ•˜๋ฉฐ ๊ธ€๋กœ๋ฒŒํ•œ ํ•ญ๋ณต์‘๋ ฅ์€ ์ž…์ž์˜ ํฌ๊ธฐ ๋ฐ ๋ถ€ํ”ผ๋ถ„์œจ์— ์˜์กดํ•œ๋‹ค. ์ „๋‹จ๋†ํ™”์œ ์ฒด๋ฅผ ์•„๋ผ๋ฏธ๋“œ์ง๋ฌผ์— ํ•จ์นจํ•˜์—ฌ ๊ตฌ์„ฑ์‚ฌ์˜ ๋ฝ‘ํž˜์„ฑ์งˆ ๋ฐ ์ธ์žฅ์„ฑ์งˆ์„ ์กฐ์‚ฌํ•œ ๊ฒฐ๊ณผ ์ด ๋ฌผ์งˆ์ด ์ง๋ฌผ๋‚ด๋ถ€์˜ ๊ณต๊ทน์„ ์ ์œ ํ•˜๋Š” ํšจ๊ณผ ๋ฐ ์ „๋‹จ๋†ํ™” ํšจ๊ณผ๊ฐ€ ๋ณตํ•ฉ์ ์œผ๋กœ ์ž‘์šฉํ•˜์—ฌ ๊ตฌ์„ฑ์‚ฌ์˜ ๋ฝ‘ํž˜์ €ํ•ญ์„ฑ์ด ์ฆ๊ฐ€ํ•˜๊ณ , ์ธ์žฅ ์‹œ ํฌ๋ฆผํ”„์— ์˜ํ•œ ์ธ์žฅ์ง€์—ฐ ํ˜„์ƒ์„ ์–ต์ œํ•˜๋ฉฐ ๋‹จ์ผ์ธต์—์„œ ๊ฒฝ์œ„์‚ฌ ํฌ๋ฆผํ”„์œจ ์ฐจ์ด์— ์˜ํ•œ ๊ฒฝ์œ„์‚ฌ๊ฐ„ ์žฅ๋ ฅ๋ถˆ๊ท ์ผ ํ˜„์ƒ์„ ํ•ด์†Œํ•˜๋Š” ๊ธ์ •์ ์ธ ์ธก๋ฉด์„ ๋ณด์ด๋Š” ๋ฐ˜๋ฉด ์‘๋ ฅ์ง‘์ค‘์˜ ๋ถ€์ •์ ์ธ ์ธก๋ฉด๋„ ๋™์‹œ์— ๋ณด์˜€๋‹ค. ์ด๋Ÿฌํ•œ ํšจ๊ณผ๋“ค์˜ ํฌ๊ธฐ๋Š” ์ด ๋ฌผ์งˆ์˜ ์œ ๋ณ€ํŠน์„ฑ ๋ฐ ์ง๋ฌผ์— ํ•จ์นจ๋˜๋Š” ์–‘์— ์˜ํ•ด ๊ฒฐ์ •๋œ๋‹ค. ์ „๋‹จ๋†ํ™”์œ ์ฒด๊ฐ€ ํ•จ์นจ๋œ ์•„๋ผ๋ฏธ๋“œ์ง๋ฌผ์„ ํ•จ์œ ํ•˜๋Š” ์—ฐ์งˆ ๋ฐฉํƒ„์žฌ์˜ ๊ด€ํ†ต์ €ํ•ญ์„ฑ๊ณผ ๋‘”์ƒ์–ต์ œ๋ ฅ์„ ์กฐ์‚ฌํ•˜์˜€๋‹ค. ๋‹จ์ผ์„ฑ๋ถ„์œผ๋กœ ๊ตฌ์„ฑ๋œ ๋ฐฉํƒ„์žฌ๊ฐ„์˜ ์„ฑ๋Šฅ์„ ๋น„๊ตํ•œ ๊ฒฐ๊ณผ ๋น„๊ต์  ์ €์†์˜ ์˜์—ญ์—์„œ๋Š” ์ „๋‹จ๋†ํ™”์œ ์ฒด๋ฅผ ํ•จ์œ ํ•œ ์•„๋ผ๋ฏธ๋“œ์ง๋ฌผ๋กœ ์ด๋ฃจ์–ด์ง„ ๋ฐฉํƒ„์žฌ์˜ ๋ชจ์˜ํŒŒํŽธํƒ„ ๋ฐฉํ˜ธ์„ฑ๋Šฅ์ด ์ƒ๋Œ€์ ์œผ๋กœ ์šฐ์ˆ˜ํ•˜์˜€์œผ๋‚˜, ์†๋„์˜ ์ฆ๊ฐ€์— ๋”ฐ๋ผ ์„ฑ๋Šฅ์˜ ์šฐ์—ด์ด ๋ฐ”๋€Œ๋Š” ํ˜„์ƒ์„ ๊ด€์ฐฐํ•  ์ˆ˜ ์žˆ์—ˆ์œผ๋ฉฐ ์ด๋Š” ๋ฐฉํƒ„์žฌ์˜ ์ฃผ์š” ํŒŒ๋‹จ๊ฑฐ๋™์ด ์†๋„์— ๋”ฐ๋ผ ๋ณ€ํ•˜๋Š” ๋ฐ์„œ ๊ธฐ์ธํ•œ๋‹ค. ๋ฏธ์ฒ˜๋ฆฌ์ง๋ฌผ๊ณผ ์ „๋‹จ๋†ํ™”์œ ์ฒด ํ•จ์นจ ์ง๋ฌผ์„ ํ˜ผ์šฉํ•œ ๋ฐฉํƒ„์žฌ์˜ ๊ฒฝ์šฐ ๋ฏธ์ฒ˜๋ฆฌ์ง๋ฌผ์„ ์•ž์ชฝ์— ์ ์ธตํ•œ ๊ฒฝ์šฐ 9๋ฐ€๋ฆฌ ๋ณผํƒ„์— ๋Œ€ํ•œ ๊ด€ํ†ต์ €ํ•ญ์„ฑ๊ณผ ๋‘”์ƒ์–ต์ œ๋ ฅ์ด ๋™์‹œ์— ์ฆ๊ฐ€ํ•˜๋Š” ํ˜„์ƒ์„ ๊ด€์ฐฐํ•  ์ˆ˜ ์žˆ์—ˆ์œผ๋ฉฐ, ์ด๋Š” ์•ž์ชฝ์— ์œ„์น˜ํ•œ ๋ฏธ์ฒ˜๋ฆฌ์ง๋ฌผ๊ณผ ๋’ค์ชฝ์— ์œ„์น˜ํ•œ ์ „๋‹จ๋†ํ™”์œ ์ฒด ํ•จ์นจ ์ง๋ฌผ์ค‘์˜ ํƒ„์ž์™€ ๋งˆ์ฃผ์น˜๋Š” ๊ตฌ์„ฑ์‚ฌ๋“ค๊ฐ„์˜ ์žฅ๋ ฅ๊ฒฐํ•ฉ์ด ์ข€ ๋” ํšจ์œจ์ ์œผ๋กœ ์ผ์–ด๋‚˜๋Š” ์ ์œผ๋กœ ์ธํ•œ ํƒ„์ž์˜ ๋ญ‰๊ฐœ์ง ์ฆ๊ฐ€์—์„œ ๊ธฐ์ธํ•˜๋Š” ๊ฒƒ์œผ๋กœ ๋ณด์—ฌ์ง„๋‹ค. ๊ต์ฐจ ์ผ๋ฐฉํ–ฅ ์ง๋ฌผ์„ ๋ณดํ†ต์˜ ์ œ์ง๋ฌผ๊ณผ ํ˜ผ์šฉํ•œ ๋ฐฉํƒ„์žฌ์— ๋Œ€ํ•ด์„œ๋„ 44๊ตฌ๊ฒฝ ๋งค๊ทธ๋„˜ ํƒ„์ž๋กœ ์‹คํ—˜ํ•œ ๊ฒฐ๊ณผ 9๋ฐ€๋ฆฌ ๋ณผํƒ„๊ณผ ์œ ์‚ฌํ•œ ๊ฒฐ๊ณผ๋ฅผ ๋ณด์ธ ๋ฐ˜๋ฉด ๋ชจ์˜ํŒŒํŽธํƒ„๊ณผ ๊ฐ™์ด ๋ญ‰๊ฐœ์ง์ด ์—†๋Š” ํƒ„์ž์˜ ๊ฒฝ์šฐ๋Š” ์ •๋ฐ˜๋Œ€์˜ ๊ฒฐ๊ณผ๋ฅผ ๋ณด์˜€์œผ๋ฉฐ, ๊ทธ ์ด์œ ๋Š” ๋‹ค์ธต์ ์ธต๋ฌผ์˜ ์ธต๊ฐ„ ๊ฐ„์„ญ์˜ ์ฆ๊ฐ€๋กœ ์ธํ•œ ํŒŒ๋‹จ๊ฑฐ๋™์˜ ๋ณ€ํ™”์— ์˜ํ•œ ๊ฒƒ์œผ๋กœ ๋ณด์—ฌ์ง„๋‹ค. ์ œ์ง๋ฐ€๋„๊ฐ€ ๋†’์€ ์ง๋ฌผ๋กœ ๋™์ผํ•œ ์‹œํ—˜์„ ์ˆ˜ํ–‰ํ•œ ๊ฒฐ๊ณผ ๊ฒฝ์œ„์‚ฌ๊ฐ„์˜ ํฌ๋ฆผํ”„์œจ์˜ ๊ฒฉ์ฐจ๊ฐ€ ์ƒ๋Œ€์ ์œผ๋กœ ์ฆ๊ฐ€ํ•˜์—ฌ ํ˜ผ์„ฑํ™”์— ์˜ํ•œ ์„ฑ๋Šฅํ–ฅ์ƒ์˜ ์ •๋„๋Š” ๊ฐ์†Œํ•œ ๋ฐ˜๋ฉด ์ ˆ๋Œ€์ ์ธ ์„ฑ๋Šฅ์— ์žˆ์–ด์„œ๋Š” ๋‘”์ƒ์–ต์ œ๋ ฅ ์ธก๋ฉด์—์„œ ์ œ์ง๋ฐ€๋„๊ฐ€ ๋‚ฎ์€ ์ง๋ฌผ์— ๋น„ํ•ด ์ข€ ๋” ๋‚˜์€ ๊ฒฐ๊ณผ๋ฅผ ๋ณด์˜€๋‹ค. ๋”ฐ๋ผ์„œ ์ œ์ง๋ฐ€๋„๋Š” ๋†’์ด๋˜ ๊ฒฝ์œ„์‚ฌ ํฌ๋ฆผํ”„์œจ์˜ ๊ด€๋ฆฌ (๊ฒฝ์œ„์‚ฌ๊ฐ„ ํฌ๋ฆผํ”„ ๊ฒฉ์ฐจ๋ฅผ ์ค„์ด๊ณ  ํฌ๋ฆผํ”„์œจ ์ž์ฒด๋ฅผ ๋‚ฎ๊ฒŒํ•จ)์— ์ข€ ๋” ์„ธ์‹ฌํ•œ ๋…ธ๋ ฅ์„ ๊ธฐ์šธ์ผ ํ•„์š”๊ฐ€ ์žˆ์Œ์„ ํ™•์ธํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๋˜ํ•œ ๋ฐฉํƒ„๋ณต์— ์ ์šฉํ•  ๊ฒฝ์šฐ ์œ ํšจ ๋ฐฉํ˜ธ๋ฉด์ ๊ณผ ์ง์ ‘ ๊ด€๋ จ๋˜๋Š” ์‚ฌ๊ฒฉ์œ„์น˜์— ๋”ฐ๋ฅธ ์˜ํ–ฅ์„ ์‚ดํŽด๋ณธ ๊ฒฐ๊ณผ ๋ณ€๋ถ€์—์„œ ๊ฐ€๊นŒ์šด ์œ„์น˜์ผ์ˆ˜๋ก ๊ด€ํ†ต์ €ํ•ญ์„ฑ์€ ์ฆ๊ฐ€ํ•˜๋Š” ๋ฐ˜๋ฉด ๋‘”์ƒ์–ต์ œ๋ ฅ์€ ๊ฐ์†Œํ•จ์„ ํ™•์ธํ•  ์ˆ˜ ์žˆ์—ˆ๊ณ , ์ „๋‹จ๋†ํ™”์œ ์ฒด ์ ์šฉ ์‹œ ๋‚˜ํƒ€๋‚˜๋Š” ํ˜„์ƒ๋“ค์€ ์‚ฌ๊ฒฉ์œ„์น˜์— ๋ฌด๊ด€ํ•จ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋์œผ๋กœ ์—ฐ์งˆ ๋ฐฉํƒ„์žฌ์˜ ๋ฐฉํƒ„์‹œํ—˜ ์‹œ ํ›„๋ฉด์žฌ๋กœ ์ „๋‹ฌ๋˜๋Š” ์—๋„ˆ์ง€๋ฅผ ์ •๋Ÿ‰ํ™” ํ•˜๊ธฐ ์œ„ํ•ด ๊ฐ•๊ตฌ์˜ ์ž์œ ๋‚™ํ•˜์‹คํ—˜๊ณผ ๋ชจ์˜ํŒŒํŽธํƒ„์„ ์œ ์ ํ† ์— ์ง์ ‘ ์‚ฌ๊ฒฉํ•˜๋Š” ๋ฐฉ๋ฒ•์„ ๋ณ‘ํ–‰ํ•˜์—ฌ ์ถฉ๊ฒฉ์ž์˜ ์น˜์ˆ˜(์ค‘๋Ÿ‰)์— ๋”ฐ๋ฅธ ์‹คํ—˜์‹์„ ์–ป๊ณ , ์šด๋™๋ฐฉ์ •์‹๊ณผ ํƒ„์„ฑํ•œ๊ณ„์น˜๋ฅผ ์ด์šฉํ•˜์—ฌ ์–ป์–ด์ง„ ์‹คํ—˜์‹์˜ ๋ฌผ๋ฆฌ์  ์˜๋ฏธ๋ฅผ ํŒŒ์•…ํ•จ์œผ๋กœ์จ ์ด์˜ ํ™•์žฅ์‘์šฉ ๊ฐ€๋Šฅ์„ฑ์„ ์ œ์‹œํ•˜์˜€๋‹ค. ์ฃผ์š”์–ด: ๊ณ ์† ์ถฉ๊ฒฉ, ์—ฐ์งˆ ๋ฐฉํƒ„์žฌ, ์ „๋‹จ๋†ํ™”์œ ์ฒด, ์ ์ธต์ˆœ์„œ, ์ œ์ง๋ฐ€๋„, ํฌ๋ฆผํ”„, ์‚ฌ๊ฒฉ์œ„์น˜, ๊ด€ํ†ต์ €ํ•ญ์„ฑ, ๋‘”์ƒ์–ต์ œ๋ ฅ, ํ›„๋ฉด์ „๋‹ฌ ์—๋„ˆ์ง€The high velocity impact properties of p-aramid fabrics treated with shear thickening fluid (STF) was investigated for soft body armor application. The STF used in this study was a mixed soft condensed matter which was composed of solid phase hard silica nanoparticles and liquid phase polyethylene glycol (PEG) where the volume fraction of the solid phase was just below the critical packing fraction. The matter showed a reversible shear thickening behavior in which the shear stress jumps dramatically (i.e. discontinuous shear thickening) as the shear rate was increased. The onset stress of shear thickening of the matter was found to be dependent mainly upon particle size, while the global failure stress of the shear thickened matter was dependent upon both particle volume fraction and particle size. The pullout and elongational properties of a single yarn within p-aramid fabrics that were treated with STF were investigated. The occupation of the interstitial volume within the fabrics by the impregnated STF resulted in an increase in yarn pullout force. Additional increase in yarn pullout force was observed above the critical pullout rate, which is presumed to be due to shear thickening of the impregnated matter. Furthermore, the occupation of the interstitial volume within the fabrics by STF also less retarded the tension increase upon elongation (i.e. less retardation of the propagation of the elongational wave). Otherwise, upon elongation, the increase in tension would have been more retarded due to the yarn crimp. Both the single yarn pullout and elongational properties of the fabrics were affected by the rheological property of the STF, the add-on of the matter as well as the fabric count. The ballistic performance of p-aramid fabrics treated with STF was investigated using the two most widely adopted methods, the ballistic limit (V50) test and the backface signature (BFS) test. For single component ballistic panels (i.e. all neat fabrics or all STF treated fabrics), STF treatment improved the impact resistance of the panels against an undeformable projectile such as 5.56mm fragment simulating projectile (FSP) at low velocity (< 250 m/s), but at increased velocity, the V50 performance decreased even with the same number of layers. This is presumed to be due to the different failure mechanisms involved at each impact velocity rangeAbstract 1. Introduction 2. Literature review 2.1 Shear thickening fluid (STF) 2.1.1 Proposed mechanisms of shear thickening phenomenon 2.1.2 Dense particle suspension system and interactions acting on the system 2.1.3 Interactions and related parameters 2.2 High velocity impact studies on shear thickening fluid and STF-assisted high-strength fabrics 2.3 Ballistic impact on high-strength fabrics 2.3.1 Research methods of ballistic impact on fabrics 2.3.2 Factors influencing ballistic performance of fabric armors 2.4 Ballistic tests of soft body armor, test standards and behind armor blunt trauma (BABT) 2.4.1 Ballistic limit (V50) test 2.4.2 Backface signature (BFS) test 2.4.3 The NIJ (National Institute of Justice) ballistic standard 2.4.4 Behind armor blunt trauma (BABT) 3. Experimental 3.1 Materials 3.1.1 Shear thickening fluids 3.1.2 Ballistic fabrics 3.2 Characterization 3.2.1 Preparation of STFs and characterization of their rheological properties 3.2.2 Preparation of STF impregnated fabrics and characterization of their mechanical properties 3.2.3 Ballistic impact tests of STF-assisted fabric panels 3.2.4 Assessment of kinetic dissipation in ballistic tests 4. Results and discussion 4.1 Rheological properties of dense colloidal suspensions 4.2 Mechanical properties of STF impregnated fabrics 4.2.1 Yarn pullout properties 4.2.2 Tensile properties (elongation of a single yarn in the fabric) 4.2.3 Representation of the change in the mechanical properties of aramid fabrics by STF impregnation 4.3 High velocity impact resistance of STF-assisted fabric panels 4.3.1 Ballistic impact resistance against 5.56mm FSP 4.3.2 Effect of laminating sequence (9mm FMJ) 4.3.3 Effect of fabric count and crimp (9mm FMJ) 4.3.4 Effect of shot location (9mm FMJ) 4.3.5 Effect of bullet expandability and laminating sequence 4.4 Kinetic dissipation in ballistic tests of soft body armor 4.4.1 The weight dropping test 4.4.2 The direct shooting test 4.4.3 Determination of the energy transferred to backing clay in ballistic tests 5. Conclusions 6. References Appendix Korean AbstractDocto
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