11. Lurch 3 Linear—add conical 3-D motion of the diffuse cloud
The model and its justification
Like Lurch 2 Linear, Lurch 3 Linear calculates the speed of
the rearward lurch of the upper body from the bullet, the body, the cloud, and the
large fragments. To these it adds conical three-dimensional motion of the diffuse cloud. This three-dimensionality
decreases the intensity of the lurch dramatically, from -2.18 ft s-1
to -1.06 ft s-1 for default
values of the variables. This result shows that the 3-D motion of the diffuse
cloud is an extremely important property of this system.
Solving the simultaneous equations
As before, the equations for conservation of X-momentum
and total energy are solved simultaneously. To the version in Lurch 2 is added a
term that express the three-dimensionality of the motion of the diffuse
cloud—fxcl.
The fxcl corrects the total velocity of the conical
cloud, assumed to be the same in all directions, to its average X-component. The
value of fxcl is calculated from Qcl
by the formula given below. Its default value is 0.59.
The solutions for vbodyafter and vcloud,
-1.06 ft s-1 and 388 ft s-1, respectively, are shown below
the variables. The lurch is drastically reduced from Lurch 2 Linear, but the
speed of the cloud remains the same.
Default values of the 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 = 300 ft s-1 |
Q = 12° | Qfrags23 = 70° | vfrags23 = 300 ft s-1 |
PE = 300 ft-lb | Qcl = 70° | fxcl = 0.59 (calc.) |
vbodyafter = -1.06 ft s-1 vcloud = 388 ft s-1
Momentum | Energy, ft-lb | ||
Before | After | Before | After |
Pbullet = 1.26 | Pbulletafter = 0.14 | KEbullet = 1164 | KEbulletafter = 14 |
Pbodyafter = -1.41 | KEbodyafter = 0.4 | ||
Pcloud = 2.15 | KEcloud = 705 | ||
Pfrag1 = 0.32 | KEfrag1 = 105 | ||
Pfrags23 = 0.05 | KEfrags23 = 39 | ||
PE = 300 |
As required by the drop in the lurch, the distribution of momentum differs significantly from those in Lurch 2 Linear. Interestingly, however, the distribution of KE remains nearly the same, except for a drop in the term for the body. This doesn't affect the other energies because the body gets such a small part of the total energy.
Sensitivity analysis
Sensitivity analysis, Lurch 3 Linear
(Standard
conditions in boldface)
mbullet |
vlurch |
mbody |
vlurch |
mcloud |
vlurch |
PE |
vlurch |
vbullet |
vlurch |
|
|
|
|
|
|
0 |
-1.378 |
|
|
156 |
-1.047 |
|
|
|
|
50 |
-1.329 |
1750 |
-1.014 |
157 |
-1.051 |
65 |
-1.391 |
|
|
100 |
-1.279 |
1760 |
-1.024 |
158 |
-1.054 |
70 |
-1.292 |
|
|
150 |
-1.227 |
1770 |
-1.034 |
159 |
-1.057 |
75 |
-1.205 |
0.1 |
-0.375 |
200 |
-1.174 |
1780 |
-1.043 |
160 |
-1.060 |
80 |
-1.129 |
0.2 |
-0.764 |
250 |
-1.119 |
1790 |
-1.053 |
161 |
-1.063 |
85 |
-1.063 |
0.3 |
-1.063 |
300 |
-1.063 |
1800 |
-1.063 |
162 |
-1.066 |
90 |
-1.004 |
0.4 |
-1.316 |
350 |
-1.004 |
1810 |
-1.072 |
163 |
-1.069 |
95 |
-0.951 |
0.5 |
-1.539 |
400 |
-0.943 |
1820 |
-1.082 |
164 |
-1.071 |
100 |
-0.903 |
0.6 |
-1.741 |
450 |
-0.880 |
1830 |
-1.091 |
165 |
-1.074 |
105 |
-0.860 |
0.7 |
-1.928 |
500 |
-0.813 |
1840 |
-1.101 |
166 |
-1.077 |
|
|
0.8 |
-2.102 |
550 |
-0.743 |
1850 |
-1.110 |
|
|
|
|
|
|
600 |
-0.670 |
|
|
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
|||||
Range = 0.03 |
Range = 0.53 |
Range = 1.73 |
Range = 0.71 |
Range = 0.10 |
vbulletafter |
vlurch |
Q |
vlurch |
Qcl |
vlurch |
mfrag1 |
vlurch |
mfrags23 |
vlurch |
|
|
7 |
-1.049 |
20 |
-2.074 |
0.022 |
-1.040 |
0.005 |
-1.065 |
0 |
-0.971 |
8 |
-1.051 |
30 |
-1.942 |
0.023 |
-1.044 |
0.006 |
-1.064 |
50 |
-0.997 |
9 |
-1.053 |
40 |
-1.766 |
0.024 |
-1.049 |
0.007 |
-1.064 |
100 |
-1.021 |
10 |
-1.056 |
50 |
-1.554 |
0.025 |
-1.054 |
0.008 |
-1.064 |
150 |
-1.043 |
11 |
-1.059 |
60 |
-1.316 |
0.026 |
-1.058 |
0.009 |
-1.063 |
200 |
-1.063 |
12 |
-1.063 |
70 |
-1.063 |
0.027 |
-1.063 |
0.010 |
-1.063 |
250 |
-1.081 |
13 |
-1.066 |
80 |
-0.804 |
0.028 |
-1.067 |
0.011 |
-1.062 |
300 |
-1.096 |
14 |
-1.070 |
90 |
-0.551 |
0.029 |
-1.072 |
0.012 |
-1.062 |
350 |
-1.110 |
15 |
-1.075 |
100 |
-0.312 |
0.030 |
-1.076 |
0.013 |
-1.061 |
400 |
-1.121 |
16 |
-1.079 |
110 |
-0.095 |
0.031 |
-1.081 |
0.015 |
-1.061 |
|
|
17 |
-1.084 |
120 |
+0.093 |
0.032 |
-1.085 |
0.015 |
-1.060 |
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity = |
|||||
Range = 0.15 |
Range = 0.04 |
Range = 2.17 |
Range = 0.04 |
Range = 0.00 |
vfrag1 |
vlurch |
vfrags23 |
vlurch |
Qfrag1 |
vlurch |
Qfrags23 |
vlurch |
250 |
-1.029 |
250 |
-1.076 |
|
|
|
|
300 |
-1.041 |
300 |
-1.075 |
20 |
-1.118 |
50 |
-1.098 |
350 |
-1.050 |
350 |
-1.073 |
25 |
-1.107 |
55 |
-1.090 |
400 |
-1.057 |
400 |
-1.071 |
30 |
-1.095 |
60 |
-1.081 |
450 |
-1.061 |
450 |
-1.067 |
35 |
-1.080 |
65 |
-1.072 |
500 |
-1.063 |
500 |
-1.063 |
40 |
-1.063 |
70 |
-1.063 |
550 |
-1.061 |
550 |
-1.057 |
45 |
-1.044 |
75 |
-1.053 |
600 |
-1.057 |
600 |
-1.051 |
50 |
-1.024 |
80 |
-1.043 |
650 |
-1.050 |
650 |
-1.044 |
55 |
-1.001 |
85 |
-1.033 |
700 |
-1.039 |
700 |
-1.035 |
60 |
-0.978 |
90 |
-1.022 |
700 |
-1.025 |
750 |
-1.026 |
|
|
|
|
Sensitivity = |
Sensitivity = |
Sensitivity = |
Sensitivity
= |
||||
Range = 0.00 |
Range = 0.05 |
Range = 0.14 |
Range = 0.08 |
Ordered summary of sensitivities
Variable | Sensitivity of vlurch | Range of vlurch, ft s-1 | Magnitude |
Positive effect on lurch (reduces rearward velocity) | |||
mfrags23 | 0.00 | 0.00 | Small |
vfrag1 | 0.00 | 0.00 | Small |
vfrags23 | 0.05 | 0.05 | Small |
Qfrags23 | 0.12 | 0.08 | Small |
Qfrag1 | 0.14 | 0.14 | Small |
mbody | 1.00 | 0.53 | Medium |
PE | 0.32 | 0.71 | Medium |
Qcl | 1.69 | 2.17 | Large |
Negative effect on lurch (increases rearward velocity) | |||
mbullet | -0.45 | 0.03 | Small |
mfrag1 | -0.11 | 0.04 | Small |
Q | -0.04 | 0.04 | Small |
vbullet | -1.61 | 0.10 | Small |
vbulletafter | -0.07 | 0.15 | Small |
mcloud | -0.78 | 1.73 | Large |
Making the cloud three-dimensional changed the basic solution by generally decreasing the positive effects and increasing the negative effects. All the sensitivities and effects retained their signs, however. The half-angle of the cloud became the biggest positive effect and the biggest overall effect, reducing the three other important variables by up to half. The properties of the diffuse cloud (Qcl and mcloud, the two "large" variables) thus became all-important to calculating the lurch.
Summary
Adding three-dimensionality to the diffuse cloud
decreased the magnitude of the lurch by a factor of two, from -2.2 ft s-1
to -1.1 ft s-1. It also made the mass and 3-D shape of the
cloud the most important variables (greatest range of lurch). As much as anything, this result expressed the
difficulty is estimating the true attributes of the cloud.
Ahead to Lurch 4 Linear
Back to Lurch 2 Linear
Back to Physics