I did some calculations for a 6 pdr. 1840's field gun to see how the program results would stack up to what's in the book.
First, from the table of fire in the book:
solid shot
Elevation, deg. ___________ Range, ft.
0° _______________________954
1 ________________________2,022
2 _______________________2,601
3 ______________________ 3,414
4 _______________________3,768
5 _______________________4,569
Calculated with RoundShot:
using
6.1 lbs., V0 1439 ft./sec., 196,000 ft.-lbs.
LgSphere drag function C 0.522
Elevation*_ Ymax _____Range ______ Vel. ____Time ___kE
deg.______ft._________ft.________ft./sec.____sec.___ft.-lbs.
0.3_____4.8________944________1,025____0.787____99 ,712
1.3_____16.5_______1,928_______809_____1.880____62 ,130
2.3_____38.2_______2,729_______719_____2.937____49 ,057
3.3_____67.4_______3,406_______672_____3.918____42 ,825
4.3____103________4,007_______641_____4.843____39, 009
5.3____144________4,555_______619_____5.727____36, 383
10.3___420_______6,833_______562______9.767____29, 939
15.3___794_______8,636_______530_____13.467____26, 673
*Note the above was calculated on the basis of the barrel being 4 ft. above ground level, and recoil producing a 0.3 degree 'jump'.
One can see that while the shot slows quickly at the start, drag becomes much less, and velocity loss occurs very slow around 600 or so. This corresponds to the graph of the drag function I used for the large sphere, so it is not really a surprise.
I consider these results to be in good agreement.
I have no idea, offhand what kind of kinetic energy would be required for a 6 lb. shot to breach a wood hulled ship, a stone wall, or ricochet, but certainly the shot would be lethal to personnel, even at long range.
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