19. Lurch 4 Angular—add 3-D motion of large fragments
The model and its justification
Lurch 4 Angular is the rotational analog of Lurch 4 Linear.
As with Lurch 3 Angular, it calculates the speed of the rearward lurch from the bullet,
the body, the conical cloud, large fragments, and the large fragments. To this
it adds 3-D motion of the large fragments. This addition barely changes the
results, with the rearward lurch decreasing in strength from 1.44 ft s-1
to 1.38 ft s-1. This change amounts to only 4%, and means that the 3-D
motion of the large fragments is an unimportant part of the solution. A similar
result was found for the linear calculations.
Solving the simultaneous equations
Default values of variables
mbullet = 161 gr |
vbullet = 1800 ft s-1 |
mfrag1 = 0.027 gr |
mbody = 85 lb |
vbulletafter = 200 ft s-1 |
mfrags23 = 0.01 gr |
mcloud = 0.3 lb |
Qfrag1 = 40° |
vfrag1 = 500 ft s-1 |
Q = 17° |
Qfrags23 = 70° |
vfrags23 = 500 ft s-1 |
PE = 200 ft-lb |
Qcl = 70° |
fkefrag1 = 1.25 |
fI = 1.11 |
|
fkefrags23 = 1.25 |
vbodyafter = -1.38 ft s-1 vcloud = 378 ft s-1
Angular momentum |
Energy, ft-lb |
||
Before |
After |
Before |
After |
Ωbullet = 3.80 |
Ωbulletafter = 0.43 |
KEbullet = 1164 |
KEbulletafter = 14 |
|
Ωbodyafter = -4.05 |
|
KEbodyafter = 1 |
|
Ωcloud = 6.28 |
|
KEcloud = 668 |
|
Ωfrag1 = 0.97 |
|
KEfrag1 = 132 |
|
Ωfrags23 = 0.16 |
|
KEfrags23 = 49 |
|
|
|
PE = 300 |
Sensitivity analysis
Sensitivity analysis, Lurch 4 angular
(Standard
conditions in boldface)
mbullet |
vlurch |
mbody |
vlurch |
mcloud |
vlurch |
PE |
vlurch |
vbullet |
vlurch |
|
|
|
|
|
|
0 |
-1.813 |
|
|
156 |
-1.356 |
|
|
|
|
50 |
-1.746 |
1750 |
-1.310 |
157 |
-1.361 |
65 |
-1.804 |
|
|
100 |
-1.677 |
1760 |
-1.324 |
158 |
-1.365 |
70 |
-1.675 |
|
|
150 |
-1.606 |
1770 |
-1.337 |
159 |
-1.370 |
75 |
-1.563 |
0.1 |
-0.474 |
200 |
-1.532 |
1780 |
-1.351 |
160 |
-1.374 |
80 |
-1.465 |
0.2 |
-0.985 |
250 |
-1.457 |
1790 |
-1.365 |
161 |
-1.378 |
85 |
-1.378 |
0.3 |
-1.378 |
300 |
-1.378 |
1800 |
-1.378 |
162 |
-1.383 |
90 |
-1.301 |
0.4 |
-1.710 |
350 |
-1.297 |
1810 |
-1.392 |
163 |
-1.387 |
95 |
-1.233 |
0.5 |
-2.003 |
400 |
-1.212 |
1820 |
-1.405 |
164 |
-1.391 |
100 |
-1.171 |
0.6 |
-2.269 |
450 |
-1.124 |
1830 |
-1.418 |
165 |
-1.395 |
105 |
-1.115 |
0.7 |
-2.513 |
500 |
-1.031 |
1840 |
-1.432 |
166 |
-1.399 |
|
|
0.8 |
-2.742 |
550 |
-0.933 |
1850 |
-1.445 |
|
|
|
|
|
|
600 |
-0.828 |
|
|
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
|||||
Range = 0.04 |
Range = 0.69 |
Range = 2.27 |
Range = 0.98 |
Range = 0.14 |
vbulletafter |
vlurch |
Q |
vlurch |
Qcl |
vlurch |
mfrag1 |
vlurch |
mfrags23 |
vlurch |
|
|
7 |
-1.359 |
20 |
-2.704 |
0.022 |
-1.356 |
0.005 |
-1.390 |
0 |
-1.255 |
8 |
-1.362 |
30 |
-2.531 |
0.023 |
-1.360 |
0.006 |
-1.387 |
50 |
-1.290 |
9 |
-1.366 |
40 |
-2.301 |
0.024 |
-1.365 |
0.007 |
-1.385 |
100 |
-1.322 |
10 |
-1.369 |
50 |
-2.023 |
0.025 |
-1.369 |
0.008 |
-1.383 |
150 |
-1.352 |
11 |
-1.374 |
60 |
-1.701 |
0.026 |
-1.374 |
0.009 |
-1.381 |
200 |
-1.378 |
12 |
-1.378 |
70 |
-1.378 |
0.027 |
-1.378 |
0.010 |
-1.378 |
250 |
-1.402 |
13 |
-1.383 |
80 |
-1.038 |
0.028 |
-1.383 |
0.011 |
-1.376 |
300 |
-1.423 |
14 |
-1.389 |
90 |
-0.705 |
0.029 |
-1.387 |
0.012 |
-1.374 |
350 |
-1.440 |
15 |
-1.394 |
100 |
-0.391 |
0.030 |
-1.391 |
0.013 |
-1.371 |
400 |
-1.455 |
16 |
-1.401 |
110 |
-0.106 |
0.031 |
-1.396 |
0.015 |
-1.369 |
|
|
17 |
-1.407 |
120 |
+0.142 |
0.032 |
-1.400 |
0.015 |
-1.366 |
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
|||||
Range = 0.20 |
Range = 0.05 |
Range = 2.85 |
Range = 0.04 |
Range = 0.02 |
vfrag1 |
vlurch |
vfrags23 |
vlurch |
Qfrag1 |
vlurch |
Qfrags23 |
vlurch |
fkefrag1 |
vlurch |
250 |
-1.366 |
250 |
-1.409 |
|
|
|
|
1.00 |
-1.420 |
300 |
-1.377 |
300 |
-1.406 |
20 |
-1.453 |
50 |
-1.426 |
1.05 |
-1.412 |
350 |
-1.384 |
350 |
-1.401 |
25 |
-1.439 |
55 |
-1.415 |
1.10 |
-1.403 |
400 |
-1.387 |
400 |
-1.395 |
30 |
-1.421 |
60 |
-1.403 |
1.15 |
-1.395 |
450 |
-1.385 |
450 |
-1.388 |
35 |
-1.401 |
65 |
-1.391 |
1.20 |
-1.387 |
500 |
-1.378 |
500 |
-1.378 |
40 |
-1.378 |
70 |
-1.387 |
1.25 |
-1.378 |
550 |
-1.367 |
550 |
-1.367 |
45 |
-1.353 |
75 |
-1.365 |
1.30 |
-1.370 |
600 |
-1.349 |
600 |
-1.355 |
50 |
-1.325 |
80 |
-1.351 |
1.35 |
-1.361 |
650 |
-1.327 |
650 |
-1.340 |
55 |
-1.295 |
85 |
-1.338 |
1.40 |
-1.353 |
700 |
-1.297 |
700 |
-1.324 |
60 |
-1.264 |
90 |
-1.324 |
1.45 |
-1.344 |
700 |
-1.261 |
750 |
-1.306 |
|
|
|
|
1.50 |
-1.336 |
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity
= |
Sensitivity = |
|||||
Range = 0.10 |
Range = 0.10 |
Range = 0.19 |
Range = 0.10 |
Range = 0.08 |
fkefrags23 |
vlurch |
fI |
vlurch |
1.00 |
-1.394 |
1.06 |
-1.443 |
1.05 |
-1.391 |
1.07 |
-1.430 |
1.10 |
-1.388 |
1.08 |
-1.417 |
1.15 |
-1.384 |
1.09 |
-1.404 |
1.20 |
-1.381 |
1.10 |
-1.391 |
1.25 |
-1.378 |
1.11 |
-1.378 |
1.30 |
-1.375 |
1.12 |
-1.366 |
1.35 |
-1.372 |
1.13 |
-1.354 |
1.40 |
-1.369 |
1.14 |
-1.342 |
1.45 |
-1.366 |
1.15 |
-1.330 |
1.50 |
-1.363 |
1.16 |
-1.319 |
Sensitivity = |
Sensitivity = |
||
Range = 0.03 |
Range = 0.12 |
Ordered summary of sensitivities
Variable | Sensitivity of vlurch | Range of vlurch, ft s-1 | Magnitude |
Positive effect on lurch (reduces rearward velocity) | |||
mfrags23 | 0.02 | 0.02 | Small |
fkefrags23 | 0.05 | 0.03 | Small |
fkefrag1 | 0.15 | 0.08 | Small |
vfrags23 | 0.08 | 0.10 | Small |
vfrag1 | 0.06 | 0.10 | Small |
Qfrags23 | 0.13 | 0.10 | Small |
fI | 1.01 | 0.12 | Small |
Qfrag1 | 0.14 | 0.19 | Small |
mbody | 1.01 | 0.69 | Medium |
PE | 0.35 | 0.98 | Medium |
Qcl | 1.71 | 2.85 | Large |
Negative effect on lurch (increases rearward velocity) | |||
mbullet | -0.53 | 0.04 | Small |
mfrag1 | -0.09 | 0.04 | Small |
Q | -0.04 | 0.05 | Small |
vbullet | -1.76 | 0.14 | Small |
vbulletafter | -0.07 | 0.20 | Small |
mcloud | -0.79 | 2.27 | Large |
As expected from the fact that the addition of three-dimensionality to the large fragments didn't change the lurch perceptibly, the basic pattern of sensitivities remained nearly unchanged, although the minor terms mfrags23 and vfrag1 moved from negative to positive. The two new parameters, fkefrag1 and fkefrags23, also had extremely small sensitivities. The two dominant sensitivities remained Qcl and mcloud, both properties of the cloud.
Summary
The addition of three-dimensionality to the motion of
the large fragments changed the solution by only a few percent, and left the
basic pattern of sensitivities unchanged. The variables of the cloud remained by
far the most important.
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