12. Lurch 4 Linearadd 3-D motion of the large fragments

The model and its justification
    Like Lurch 3 Linear, Lurch 4 Linear calculates the speed of the rearward lurch of the upper body from the bullet, the body, the cloud, the large fragments, and three-dimensional motion of the cloud. To these it adds three-dimensional motion of the large fragments. This addition hardly changes the answer (from -0.88 ft s-1 to -0.87 ft s-1 for default values of the variables). This shows that the 3-D motion of the large fragments is not an important consideration.

Solving the simultaneous equations
    As before, the equations for conservation of X-momentum and total energy are solved simultaneously. To the version in Lurch 3 are added two terms that express the three-dimensionality of the motion of the two large fragmentsfkefrag1 and fkefrags23. These terms are roughly analogous to the earlier fkecl, and range upward from 1 because the the kinetic energy of a fragment will always be greater than the value calculated from the X- and Z-components of its velocity that are derived from the Zapruder film. To this must be added a component perpendicular to the film, which we can call the Y-component. A fkefrag of 2 would mean that the fragment has twice the kinetic energy of that calculated from its X- and Z-velocities.
    There is no reliable way to tell how much more kinetic energy the two large fragments had than is shown in the film's XZ plane, because we can't determine their velocities perpendicular to the film. Thus we can only estimate values for fkefrag1 and fkefrags23. To be conservative, we use default values of 1.25 for both and ranges of 1 to 1.5 It turns out not to matter much, for the speed of the lurch is very insensitive to both terms.

Conservation of X-momentum

 

Conservation of total energy

 

Preset 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 = 17°  Qfrags23 = 70°  vfrags23 = 300 ft s-1
PE = 200 ft-lb fxcl = 0.7 fkefrag1 = 1.25
  fkecl = 2 fkefrags23 = 1.25

Default solutions to the simultaneous equations

vbodyafter = -0.87 ft s-1  vcloud = 307 ft s-1

Distributions of momentum and energy

Momentum Energy, ft-lb
Before After Before After
Pbullet = 1.24 Pbulletafter = 0.14 KEbullet = 1164  KEbulletafter = 14
  Pbodyafter = -1.15   KEbodyafter = 0.2
  Pcloud = 2.02   KEcloud = 885
  Pfrag1 = 0.19   KEfrag1 = 47
  Pfrags23 = 0.03    KEfrags23 = 18
      PE = 200

Sensitivity analysis
    This sensitivity analysis is practically identical to the one for Lurch 3 Linear. The two new terms, fkefrag1 and fkefrags23, have minimal sensitivities and minimal effects on the lurch. Thus they are unimportant variables.

Sensitivity analysis, Lurch 4 linear
(Standard conditions in boldface)

mbullet

vlurch

mbody

vlurch

mcloud

vlurch

PE

vlurch

vbullet

vlurch

156

-0.863

 

 

 

 

 

 

1750

-0.838

157

-0.864

65

-1.137

 

 

0

-1.032

1760

-0.844

158

-0.865

70

-1.055

 

 

50

-0.992

1770

-0.85

159

-0.866

75

-0.984

0.1

-0.224

100

-0.952

1780

-0.856

160

-0.867

80

-0.923

0.2

-0.588

150

-0.911

1790

-0.862

161

-0.868

85

-0.868

0.3

-0.868

200

-0.868

1800

-0.868

162

-0.869

90

-0.82

0.4

-1.105

250

-0.825

1810

-0.874

163

-0.87

95

-0.776

0.5

-1.314

300

-0.78

1820

-0.88

164

-0.871

100

-0.738

0.6

-1.504

350

-0.733

1830

-0.886

165

-0.872

105

-0.702

0.7

-1.679

400

-0.685

1840

-0.892

166

-0.873

 

 

0.8

-1.842

 

 

1850

-0.898

Sensitivity = 
[(-0.869 + 0.867)/2]/
[0.868/161] = -0.19

Sensitivity = 
[(-0.82 + 0.923)/10]/
[0.868/85] = 1.01

Sensitivity = 
[(-1.105 + 0.588)/0.2]/
[0.868/0.3] = -0.89

Sensitivity = 
[(-0.825 + 0.911)/100]/
[0.868/200] = 0.20

Sensitivity = 
[(-0.874 + 0.862)/20]/
[0.868/1800] = -1.24

Range = 0.01

Range = 0.43

Range = 1.62

Range = 0.35

Range = 0.05

vbulletafter

vlurch

Q

vlurch

mfrag1

vlurch

mfrags23

vlurch

vfrag1

vlurch

 

 

12

-0.847

0.022

-0.849

0.005

-0.864

 

 

0

-0.772

13

-0.851

0.023

-0.852

0.006

-0.864

100

-0.806

50

-0.798

14

-0.854

0.024

-0.856

0.007

-0.865

150

-0.825

100

-0.823

15

-0.859

0.025

-0.86

0.008

-0.866

200

-0.842

150

-0.846

16

-0.863

0.026

-0.864

0.009

-0.867

250

-0.856

200

-0.868

17

-0.868

0.027

-0.868

0.010

-0.868

300

-0.868

250

-0.888

18

-0.873

0.028

-0.872

0.011

-0.869

350

-0.878

300

-0.907

19

-0.879

0.029

-0.876

0.012

-0.87

400

-0.885

350

-0.924

20

-0.884

0.03

-0.88

0.013

-0.871

450

-0.889

400

-0.939

21

-0.89

0.031

-0.884

0.014

-0.872

500

-0.891

 

 

22

-0.897

0.032

-0.888

0.015

-0.873

 

 

Sensitivity = 
[(-0.888 + 0.846)/100]/
[0.868/200] = -0.097

Sensitivity = 
[(-0.873 + 0.863)/2]/
[0.868/17] = -0.098

Sensitivity = 
[(-0.872 + 0.864)/0.002]/
[0.868/0.027] = -0.124

Sensitivity = 
[(-0.869 + 0.867)/0.002]/
[0.868/0.01] = -0.012

Sensitivity = 
[(-0.878 + 0.856)/100]/
[0.868/300] = -0.076

Range = 0.17

Range = 0.04

Range = 0.04

Range = 0.01

Range = 0.08

 

vfrags23

vlurch

Qfrag1

vlurch

Qfrags23

vlurch

fxcl

vlurch

fkecl

vlurch

100

-0.865

20

-0.901

50

-0.889

 

 

1

-1.499

150

-0.867

25

-0.895

55

-0.885

0.4

-0.215

1.25

-1.272

200

-0.868

30

-0.887

60

-0.879

0.5

-0.433

1.5

-1.104

250

-0.869

35

-0.878

65

-0.874

0.6

-0.651

1.75

-0.973

300

-0.868

40

-0.868

70

-0.868

0.7

-0.868

2

-0.868

350

-0.867

45

-0.857

75

-0.862

0.8

-1.086

2.25

-0.781

400

-0.864

50

-0.845

80

-0.856

0.9

-1.303

2.5

-0.707

450

-0.861

55

-0.831

85

-0.85

1

-1.521

2.75

-0.644

500

-0.857

60

-0.817

90

-0.844

 

 

3

-0.589

Sensitivity = 
[(-0.867 + 0.869)/100]/
[0.868/300] = 0.007

Sensitivity = 
[(-0.857 + 0.868)/10]/
[0.868/40] = 0.097

Sensitivity = 
[(-0.862 + 0.874)/10]/
[0.868/70] = 0.097

Sensitivity = 
[(-1.086 + 0.651)/0.2]/
[0.868/0.7] = -1.75

Sensitivity = 
[(-0.781 + 0.973)/0.5]/
[0.868/2] = 0.88

Range = 0.01

Range = 0.08

Range = 0.04

Range = 1.31

Range = 0.91

fkefrag1

vlurch

fkefrags23

vlurch

 

1

-0.876

1

-0.871

 

1.1

-0.873

1.1

-0.87

 

1.25

-0.868

1.25

-0.868

 

1.4

-0.863

1.4

-0.866

 

1.5

-0.86

1.5

-0.865

 

Sensitivity = 
[(-0.863 + 0.873)/0.3]/
[0.868/1.25] = 0.048

Sensitivity = 
[(-0.866 + 0.87)/0.3]/
[0.868/1.25] = 0.019

Range = 0.02

Range = 0.01

 

Ordered summary of sensitivities

Variable Sensitivity of vlurch Range of vlurch, ft s-1 Magnitude
Positive effect on lurch (reduces rearward velocity)
vfrags23 0.007 0.01 Small
fkefrags23 0.019 0.01 Small
fkefrag1 0.048 0.02 Small
 Qfrags23 0.097 0.04 Small
Qfrag1  0.097 0.08 Small
PE 0.20 0.35 Small
mbody 1.01 0.43 Small
fkecl 0.88 0.91 Medium
Negative effect on lurch (increases rearward velocity)
mfrags23 -0.012 0.01 Small
mbullet -0.19 0.01 Small
mfrag1 -0.124 0.04 Small
Q  -0.098 0.04 Small
vbullet -1.24 0.05 Small
vfrag1 -0.076 0.08 Small
vbulletafter -0.097 0.17 Small
fxcl -1.75 1.31 Large
mcloud -0.89 1.62 Large

    The two additional variables from the three-dimensionality of the fragments changed the solution imperceptibly and had the smallest effects of any of the seven intensifying variables.

Summary
    Adding three-dimensional effects for the two large fragments hardly changed anything about the solution, presumably because these variables were minor to begin with.

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