14. Lurch 6 Linear—Set vfrags = vcloud and solve for mcloud
The model and its justification
This version of the simulation tries to directly get values
for mcloud, one of the hardest variables to estimate, by
solving for it directly. In order to do that, some other variable must take on
an assumed value, because only two variables can be solved for by the two
equations. Since vcloud was coming out to values very similar
to those assumed for vfrags, I decided to set vfrags23
= vfrag1 and vfrags (really vfrag1)
= vcloud in order to free up a degree of freedom that could then be
used to solve for mcloud. I was gratified to see that the
value of mcloud, at least for the default conditions, came out
very similar to the default value I had previously taken (0.32 lb vs. 0.30 lb
previously used). Of course, the other variable solved for remained vbodyafter.
Just to be clear, this version of the equations calculated the speed of the
rearward lurch of JFK's upper body from the bullet, the body, the cloud, and the
large fragments, with 3-D motion of cloud, large fragments, and body.
Solving the simultaneous equations
Since no new variables were introduced here, the form of the
two equations remained the same as in Lurch 5 Linear. Since the assumed value
for vcloud was very close to the value solved for there, the
default solution for vbodyafter (-0.90 ft s-1) was
very similar to the previous value of -0.87 ft s-1.
vfrag1 = vcloud
vfrags23 = vcloud
fkefrags23 = fkefrag1
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 | vcloud = 300 | fkefrag1 = 1.25 |
Q = 17° | Qfrag1 = 40° | fkebody = 1.2 |
PE = 200 ft-lb | Qfrags23 = 70° | fxcl = 0.7 |
fkecl = 2 |
vbodyafter = -0.90 ft s-1 mcloud = 0.32 lb
Momentum | Energy, ft-lb | ||
Before | After | Before | After |
Pbullet = 1.24 | Pbulletafter = 0.14 | KEbullet = 1164 | KEbulletafter = 14 |
Pbodyafter = -1.20 | KEbodyafter = 0.3 | ||
Pcloud = 2.06 | KEcloud = 885 | ||
Pfrag1 = 0.19 | KEfrag1 = 47 | ||
Pfrags23 = 0.03 | KEfrags23 = 18 | ||
PE = 200 |
Sensitivity analysis
Linking the speed of the cloud to the speed of the fragments
made the speed of the lurch considerably more sensitive to the mass of the
bullet (7 times) and to the potential energy (2 times) and the initial speed of
the bullet (3 times). Sensitivities to the other variables remained about the
same.
Sensitivity analysis, Lurch 6 Linear
(Standard conditions in boldface)
mbullet |
vlurch |
mbody |
vlurch |
PE |
vlurch |
vbullet |
vlurch |
vbulletafter |
vlurch |
156 |
-0.867 |
|
|
|
|
1750 |
-0.818 |
|
|
157 |
-0.875 |
65 |
-1.184 |
0 |
-1.258 |
1760 |
-0.835 |
0 |
-0.822 |
158 |
-0.882 |
70 |
-1.099 |
50 |
-1.17 |
1770 |
-0.852 |
50 |
-0.847 |
159 |
-0.89 |
75 |
-1.026 |
100 |
-1.081 |
1780 |
-0.87 |
100 |
-0.87 |
160 |
-0.897 |
80 |
-0.962 |
150 |
-0.993 |
1790 |
-0.887 |
150 |
-0.889 |
161 |
-0.905 |
85 |
-0.905 |
200 |
-0.905 |
1800 |
-0.905 |
200 |
-0.905 |
162 |
-0.912 |
90 |
-0.854 |
250 |
-0.816 |
1810 |
-0.922 |
250 |
-0.918 |
163 |
-0.92 |
95 |
-0.809 |
300 |
-0.728 |
1820 |
-0.94 |
300 |
-0.927 |
164 |
-0.927 |
100 |
-0.769 |
350 |
-0.64 |
1830 |
-0.958 |
350 |
-0.934 |
165 |
-0.935 |
105 |
-0.732 |
400 |
-0.552 |
1840 |
-0.976 |
400 |
-0.937 |
166 |
-0.942 |
|
|
|
|
1850 |
-0.995 |
|
|
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
|||||
Range = 0.075 |
Range = 0.45 |
Range = 0.71 |
Range = 0.18 |
Range = 0.12 |
vcloud |
vlurch |
Q |
vlurch |
mfrag1 |
vlurch |
mfrags23 |
vlurch |
Qfrag1 |
vlurch |
0 |
- |
|
|
|
|
|
|
|
|
50 |
-10.231 |
12 |
-0.883 |
0.022 |
-0.893 |
0.005 |
-0.908 |
|
|
100 |
-4.319 |
13 |
-0.887 |
0.023 |
-0.895 |
0.006 |
-0.907 |
20 |
-0.938 |
150 |
-2.575 |
14 |
-0.891 |
0.024 |
-0.898 |
0.007 |
-0.907 |
25 |
-0.932 |
200 |
-1.73 |
15 |
-0.895 |
0.025 |
-0.9 |
0.008 |
-0.906 |
30 |
-0.924 |
250 |
-1.232 |
16 |
-0.9 |
0.026 |
-0.902 |
0.009 |
-0.905 |
35 |
-0.915 |
300 |
-0.905 |
17 |
-0.905 |
0.027 |
-0.905 |
0.01 |
-0.905 |
40 |
-0.905 |
350 |
-0.674 |
18 |
-0.91 |
0.028 |
-0.907 |
0.011 |
-0.904 |
45 |
-0.893 |
400 |
-0.504 |
19 |
-0.915 |
0.029 |
-0.909 |
0.012 |
-0.903 |
50 |
-0.881 |
450 |
-0.374 |
20 |
-0.921 |
0.03 |
-0.912 |
0.013 |
-0.903 |
55 |
-0.868 |
500 |
-0.272 |
21 |
-0.927 |
0.031 |
-0.914 |
0.014 |
-0.902 |
60 |
-0.854 |
550 |
-0.19 |
22 |
-0.933 |
0.032 |
-0.916 |
0.015 |
-0.901 |
|
|
600 |
-0.123 |
|
|
|
|
|
|
|
|
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
|||||
Range = 4.20 |
Range = 0.05 |
Range = 0.023 |
Range = 0.007 |
Range = 0.084 |
Qfrags23 |
vlurch |
fxcl |
vlurch |
fkecl |
vlurch |
fkefrag1 |
vlurch |
fkebody |
vlurch |
50 |
-0.926 |
|
|
1 |
-2.467 |
|
|
|
|
55 |
-0.921 |
0.4 |
-0.236 |
1.25 |
-1.842 |
|
|
|
|
60 |
-0.916 |
0.5 |
-0.459 |
1.5 |
-1.426 |
1 |
-0.928 |
1.0 |
-0.905 |
65 |
-0.91 |
0.6 |
-0.682 |
1.75 |
-1.128 |
1.1 |
-0.919 |
1.1 |
-0.905 |
70 |
-0.905 |
0.7 |
-0.905 |
2 |
-0.905 |
1.25 |
-0.905 |
1.2 |
-0.905 |
75 |
-0.899 |
0.8 |
-1.127 |
2.25 |
-0.731 |
1.4 |
-0.891 |
1.3 |
-0.905 |
80 |
-0.893 |
0.9 |
-1.35 |
2.5 |
-0.592 |
1.5 |
-0.882 |
1.4 |
-0.905 |
85 |
-0.887 |
1.0 |
-1.572 |
2.75 |
-0.479 |
|
|
|
|
90 |
-0.881 |
|
|
3 |
-0.384 |
|
|
|
|
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
|||||
Range = 0.045 |
Range = 1.34 |
Range = 2.08 |
Range = 0.046 |
Range = 0.000 |
Ordered summary of sensitivities
Variable | Sensitivity of vlurch | Range of vlurch, ft s-1 | Magnitude |
Positive effect on lurch (reduces rearward velocity) | |||
fkebody | 0.000 | 0.00 | Small |
mfrags23 | 0.006 | 0.03 | Small |
Qfrags23 | 0.085 | 0.04 | Small |
fkefrag1 | 0.129 | 0.05 | Small |
Qfrag1 | 0.097 | 0.08 | Small |
mbody | 1.01 | 0.45 | Small |
PE | 0.39 | 0.71 | Medium |
fkecl | 1.75 | 2.08 | Large |
vcloud | 1.85 | 4.20 | Large |
Negative effect on lurch (increases rearward velocity) | |||
mbullet | -0.13 | 0.01 | Small |
mfrag1 | -0.075 | 0.02 | Small |
Q | -0.094 | 0.05 | Small |
vbulletafter | -0.064 | 0.12 | Small |
vbullet | -3.48 | 0.18 | Small |
fxcl | -1.72 | 1.34 | Large |
The sensitivities of the variables in Lurch 6 Linear are very similar to those in Lurch 5 Linear, although with some minor rearrangements attributable to equating some of the variables and solving for mcloud instead of vcloud. The most important variables remained those of the diffuse cloud.
Summary
Linking the speed of the cloud to the speed of the fragments
allowed us to solve for the mass of the cloud, which was nearly the same as that
previously assumed. The default speed of the lurch was also very similar to
previous calculations. Sensitivities to the incoming bullet increased by factors
of two to seven, however. As in previous cases, the greatest sensitivities and
effects were to properties of the diffuse cloud such as its speed and its
spatial properties.
Ahead to Lurch 7 Linear
Back to Lurch 5 Linear
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