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The mine rises to a height of 0.3 to 1.7 meters [1] before one or both of the pyrotechnic delays detonates the main charge of the mine, which sprays high-speed metal fragments 360° around the point of detonation. These metal fragments have an expected casualty radius of 27 meters for the M16 and M16A1 mines, and out to 30 meters for the M16A2 ...
The final prototype featured an upper and lower receiver with the now-familiar hinge and takedown pins, and the charging handle was on top of the receiver placed inside of the carry handle. [38] For a 7.62 mm NATO rifle, the AR-10 was incredibly lightweight at only 6.85 lb (3.11 kg) empty. [ 42 ]
M16A1 carbine/CAR15: 2nd Generation Short Ribbed S-1-F A1 No No .223 REM 14.5 in. A1 1:12 Yes A1 Birdcage 655: M16A1 Special High Profile: A1 Triangular S-1-F A1 (used with special raised carry handle scope mount) Yes No .223 REM 20 in. HBAR 1:12 Yes A1 656: M16A1 Special Low Profile: A1 Triangular S-1-F Flattop Yes No .223 REM 20 in. HBAR 1:12 Yes
Eugene Morrison Stoner (November 22, 1922 – April 24, 1997) was an American machinist and firearms designer who is most associated with the development of the ArmaLite AR-15 rifle that was redesigned and modified by Colt's Patent Firearm Company for the United States military as the M16 rifle.
M16, XM16E1, and M16A1 – M16 was issued in 1964, but due to reliability issues, it was replaced by the M16A1 in 1967 which added the forward assist and chrome-lined barrel to the rifle for increased reliability. [42] CAR-15 – carbine variant of the M16 produced in very limited numbers, fielded by special operations early on. Later ...
M16A1, a version of the American M16 rifle; M1903A1, a variant of the American M1903 Springfield rifle; M4A1, a variant of the M4 Carbine; M82A1, M82A1A and M82A1M, three variants of the American Barrett M82 rifle; M96-A1, a variant of the American Robinson Armaments M96 Expeditionary rifle; PSG1A1, a variant of the German Heckler & Koch PSG1 ...
The detonation velocity values presented here are typically for the highest practical density which maximizes achievable detonation velocity. [ 1 ] The velocity of detonation is an important indicator for overall energy and power of detonation, and in particular for the brisance or shattering effect of an explosive which is due to the ...
David Chapman [3] and Émile Jouguet [4] originally (c. 1900) stated the condition for an infinitesimally thin detonation. A physical interpretation of the condition is usually based on the later modelling (c. 1943) by Yakov Borisovich Zel'dovich, [5] John von Neumann, [6] and Werner Döring [7] (the so-called ZND detonation model).