25c. Constraints from Rhead vs. Rbullet—SL7A—mhead = 7 lb
For mhead = 7 lb
Increasing the mass of the head to the default case of 7
lb again shifts the pattern of constraints to the left and increases the
number of allowable solutions as the lower right part of the allowable zone
comes completely into the table. The boundaries of that zone are defined as
above. Again, the constraints imposed by vfrags
> 1100 ft s-1 coincide almost perfectly with those for PE
< 0. The two masks are again shown as one.
PE, ft-lb
The allowed values of PE range from 120 to 600 ft-lb, very similar to the two previous ranges. The number of acceptable values has increased from 18 to 30. This means that a 7-lb head is heavy enough to allow nearly half the solutions to be acceptable.
Rbullet, in ↓ Rhead, in → | 3.50 | 3.75 | 4.00 | 4.25 | 4.50 | 4.75 | 5.00 | 5.25 | 5.50 |
4.75 | 618 | 568 | 473 | 263 | -380 | -4585 | -146,400 | -2060 | -76 |
5.00 | 640 | 608 | 554 | 452 | 228 | -443 | -4585 | — | -2611 |
5.25 | 655 | 632 | 597 | 539 | 431 | 193 | -504 | -4585 | — |
5.50 | 665 | 649 | 624 | 587 | 524 | 409 | 159 | -564 | -4585 |
5.75 | 673 | 660 | 642 | 616 | 576 | 509 | 387 | 124 | -623 |
6.00 | 679 | 669 | 655 | 636 | 608 | 565 | 494 | 365 | 89 |
6.25 | 684 | 675 | 664 | 649 | 629 | 599 | 554 | 479 | 342 |
6.50 | 687 | 680 | 671 | 660 | 644 | 622 | 590 | 542 | 463 |
6.75 | 690 | 684 | 677 | 667 | 655 | 638 | 615 | 581 | 530 |
vfrags, ft s-1
The pattern of disallowed velocity of the fragments again coincided nearly perfectly with negative values for PE, and so did not add to the constraining process. The mask shown below represents vfrags and PE. The allowed values for vfrags ranged from 420 to 910 ft s-1, very similar to previous ranges.
Rbullet, in ↓ Rhead, in → | 3.50 | 3.75 | 4.00 | 4.25 | 4.50 | 4.75 | 5.00 | 5.25 | 5.50 |
4.75 | 390 | 471 | 593 | 802 | 1238 | 2710 | -14,260 | -1964 | -1055 |
5.00 | 348 | 407 | 491 | 617 | 831 | 1272 | 2710 | -20,770 | -2149 |
5.25 | 317 | 363 | 425 | 511 | 641 | 860 | 1305 | 2710 | -35,340 |
5.50 | 294 | 331 | 378 | 442 | 530 | 664 | 887 | 1337 | 2710 |
5.75 | 275 | 306 | 344 | 393 | 458 | 550 | 686 | 914 | 1367 |
6.00 | 260 | 286 | 317 | 357 | 407 | 475 | 568 | 708 | 940 |
6.25 | 248 | 270 | 297 | 329 | 370 | 422 | 491 | 587 | 730 |
6.50 | 237 | 257 | 280 | 307 | 341 | 382 | 436 | 507 | 605 |
6.75 | 228 | 245 | 265 | 289 | 317 | 352 | 395 | 450 | 523 |
tlurch, ms
As before, tlurch < 25 ms offers milder constraints than PE. The leftward shift of the patterns relative to mhead = 6 lb shrank the disallowed area at the lower left to only two points, but introduced a disallowed area at the upper right, where the values of tlurch became negative. Although this area was larger (six points), it still fell within a broader area of similar shape for PE. The values disallowed by tlurch are shown in boldface.
Rbullet, in ↓ Rhead, in → | 3.50 | 3.75 | 4.00 | 4.25 | 4.50 | 4.75 | 5.00 | 5.25 | 5.50 |
4.75 | 15.4 | 12.8 | 10.1 | 7.5 | 4.8 | 2.2 | -0.4 | -3.1 | -5.7 |
5.00 | 17.2 | 14.7 | 12.2 | 9.7 | 7.2 | 4.7 | 2.2 | -0.3 | -2.8 |
5.25 | 18.9 | 16.5 | 14.1 | 11.7 | 9.4 | 7.0 | 4.6 | 2.2 | -0.2 |
5.50 | 20.4 | 18.1 | 15.9 | 13.6 | 11.3 | 9.0 | 6.8 | 4.5 | 2.2 |
5.75 | 21.8 | 19.6 | 17.4 | 15.3 | 13.1 | 10.9 | 8.7 | 6.6 | 4.4 |
6.00 | 23.1 | 21.0 | 18.9 | 16.8 | 14.7 | 12.6 | 10.6 | 8.5 | 6.4 |
6.25 | 24.2 | 22.2 | 20.2 | 18.2 | 16.2 | 14.2 | 12.2 | 10.2 | 8.2 |
6.50 | 25.3 | 23.4 | 21.5 | 19.5 | 17.6 | 15.7 | 13.8 | 11.8 | 9.9 |
6.75 | 26.3 | 24.5 | 22.6 | 20.8 | 18.9 | 17.0 | 15.2 | 13.3 | 11.5 |
vbodyafter, ft s-1
The speed of the lurch ranged from -2.6 to +10.4 ft s-1, much more here than with the 6-lb head. The acceptable speeds, all rearward, were 0.9–1.3 ft s-1, very close to previous ranges and to the observed -0.8 ft s-1.
Rbullet, in ↓ Rhead, in → | 3.50 | 3.75 | 4.00 | 4.25 | 4.50 | 4.75 | 5.00 | 5.25 | 5.50 |
4.75 | -0.85 | -0.92 | -1.01 | -1.17 | -1.51 | -2.64 | 10.42 | 0.96 | 0.26 |
5.00 | -0.82 | -0.87 | -0.93 | -1.03 | -1.19 | -1.53 | -2.64 | — | 1.10 |
5.25 | -0.80 | -0.83 | -0.88 | -0.95 | -1.05 | -1.22 | -1.56 | -2.64 | — |
5.50 | -0.78 | -0.81 | -0.84 | -0.89 | -0.96 | -1.06 | -1.24 | -1.58 | -2.64 |
5.75 | -0.77 | -0.79 | -0.82 | -0.86 | -0.91 | -0.98 | -1.08 | -1.26 | -1.60 |
6.00 | -0.75 | -0.77 | -0.80 | -0.83 | -0.87 | -0.92 | -0.99 | -1.10 | -1.28 |
6.25 | -0.74 | -0.76 | -0.78 | -0.81 | -0.84 | -0.88 | -0.93 | -1.00 | -1.12 |
6.50 | -0.74 | -0.75 | -0.77 | -0.79 | -0.82 | -0.85 | -0.89 | -0.94 | -1.02 |
6.75 | -0.73 | -0.74 | -0.76 | -0.78 | -0.80 | -0.82 | -0.86 | -0.90 | -0.96 |
vsnap, ft s-1
These results show that the snap of a 7-lb head is constrained to speeds between 4.0 and 4.8 ft s-1, a range consistent with the observed vsnap > 3.3 ft s-1 and practically identical to the previous range.
Rbullet, in ↓ Rhead, in → | 3.50 | 3.75 | 4.00 | 4.25 | 4.50 | 4.75 | 5.00 | 5.25 | 5.50 |
4.75 | 4.97 | 4.64 | 4.35 | 4.09 | 3.89 | 3.66 | 3.48 | 3.31 | 3.16 |
5.00 | 5.23 | 4.88 | 4.58 | 4.31 | 4.07 | 3.86 | 3.66 | 3.49 | 3.33 |
5.25 | 5.49 | 5.13 | 4.81 | 4.52 | 4.27 | 4.05 | 3.85 | 3.66 | 3.50 |
5.50 | 5.76 | 5.37 | 5.04 | 4.74 | 4.48 | 4.24 | 4.03 | 3.84 | 3.66 |
5.75 | 6.02 | 5.62 | 5.26 | 4.96 | 4.68 | 4.43 | 4.21 | 4.01 | 3.83 |
6.00 | 6.28 | 5.86 | 5.49 | 5.17 | 4.88 | 4.63 | 4.40 | 4.19 | 4.00 |
6.25 | 6.54 | 6.10 | 5.72 | 5.39 | 5.09 | 4.82 | 4.58 | 4.36 | 4.16 |
6.50 | 6.80 | 6.35 | 5.95 | 5.60 | 5.29 | 5.01 | 4.76 | 4.54 | 4.33 |
6.75 | 7.06 | 6.59 | 6.18 | 5.82 | 5.49 | 5.20 | 4.94 | 4.71 | 4.50 |
Ahead to Constraints for mhead = 8 lb
Back to Constraints for mhead = 6 lb
Back to Constraints from Rhead and Rbullet
Back to Physics of the Head Shot