19. Lurch 4 Angularadd 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 1.30 ft s-1 to 1.28 ft s-1. This change is negligible, and means that the 3-D motion of the large fragments is an unimportant part of the solution. The same result was found in the linear calculations.
    

Solving the simultaneous equations
    

 

 

Conservation of angular X-momentum

 

Conservation of total energy

 

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 = 300 ft s-1

Q = 17°

Qfrags23 = 70°

vfrags23 = 300 ft s-1

PE = 200 ft-lb

Qcl = 45°

fkefrag1 = 1.25

fI = 1.11

 

fkefrags23 = 1.25

Solutions to simultaneous equations

vbodyafter = -1.28 ft s-1  vcloud = 279 ft s-1

Distributions of momentum and energy

Angular momentum

Energy, ft-lb

Before

After

Before

After

Ωbullet = 3.71

Ωbulletafter = 0.43

KEbullet = 1164

KEbulletafter = 14

 

Ωbodyafter = -3.77

 

KEbodyafter = 0.8

 

Ωcloud = 6.37

 

KEcloud = 884

 

Ωfrag1 = 0.58

 

KEfrag1 = 47

 

Ωfrags23 = 0.10

 

KEfrags23 = 18

 

 

 

PE = 200

 

Sensitivity analysis
    

Sensitivity analysis, Lurch 4 angular

(Standard conditions in boldface)

mbullet

vlurch

mbody

vlurch

mcloud

vlurch

PE

vlurch

vbullet

vlurch

156

-1.274

 

 

 

 

 

 

1750

-1.239

157

-1.276

65

-1.680

 

 

0

-1.516

1760

-1.248

158

-1.278

70

-1.560

 

 

50

-1.460

1770

-1.257

159

-1.280

75

-1.455

0.1

-0.366

100

-1.403

1780

-1.266

160

-1.282

80

-1.364

0.2

-0.885

150

-1.344

1790

-1.275

161

-1.284

85

-1.284

0.3

-1.284

200

-1.284

1800

-1.284

162

-1.285

90

-1.212

0.4

-1.621

250

-1.221

1810

-1.292

163

-1.287

95

-1.148

0.5

-1.918

300

-1.157

1820

-1.301

164

-1.289

100

-1.091

0.6

-2.187

350

-1.091

1830

-1.310

165

-1.291

105

-1.038

0.7

-2.436

400

-1.023

1840

-1.319

166

-1.292

 

 

0.8

-2.668

 

 

1850

-1.327

Sensitivity = 
[(-1.287 + 1.280)/4]/
[1.284/161] = -0.22

Sensitivity = 
[(-1.364 + 1.212)/10]/
[1.284/85] = 1.01

Sensitivity = 
[(-1.621 + 0.885)/0.2]/
[1.284/0.3] = -0.86

Sensitivity = 
[(-1.221 + 1.344)/100]/
[1.284/200] = 0.19

Sensitivity = 
[(-1.301 + 1.266)/40]/
[1.284/1800] = -1.23

Range = 0.018

Range = 0.64

Range = 2.30

Range = 0.49

Range = 0.088

vbulletafter

vlurch

Q

vlurch

mfrag1

vlurch

mfrags23

vlurch

vfrag1

vlurch

 

 

12

-1.255

0.022

-1.258

0.005

-1.278

 

 

0

-1.155

13

-1.260

0.023

-1.263

0.006

-1.279

100

-1.203

50

-1.190

14

-1.265

0.024

-1.268

0.007

-1.280

150

-1.228

100

-1.223

15

-1.271

0.025

-1.273

0.008

-1.281

200

-1.250

150

-1.255

16

-1.277

0.026

-1.278

0.009

-1.282

250

-1.268

200

-1.284

17

-1.284

0.027

-1.284

0.010

-1.284

300

-1.284

250

-1.310

18

-1.291

0.028

-1.289

0.011

-1.285

350

-1.295

300

-1.335

19

-1.298

0.029

-1.294

0.012

-1.286

400

-1.304

350

-1.357

20

-1.306

0.03

-1.299

0.013

-1.287

450

-1.309

400

-1.377

21

-1.314

0.031

-1.304

0.014

-1.288

500

-1.310

 

 

22

-1.322

0.032

-1.310

0.015

-1.289

 

 

Sensitivity = 
[(-1.310 + 1.255)/100]/
[1.284/200] = -0.086

Sensitivity = 
[(-1.298 + 1.271)/4]/
[1.284/17] = -0.089

Sensitivity = 
[(-1.294 + 1.273)/0.004]/
[1.284/0.027] = -0.11

Sensitivity = 
[(-1.286 + 1.281)/0.004]/
[1.284/0.01] = -0.0097

Sensitivity = 
[(-1.295 + 1.268)/100]/
[1.284/300] = -0.063

Range = 0.22

Range = 0.067

Range = 0.052

Range = 0.011

Range = 0.107

 

vfrags23

vlurch

Qfrag1

vlurch

Qfrags23

vlurch

Qcl

vlurch

100

-1.281

20

-1.328

50

-1.312

25

-1.984

150

-1.283

25

-1.320

55

-1.306

30

-1.795

200

-1.285

30

-1.309

60

-1.299

35

-1.616

250

-1.285

35

-1.297

65

-1.291

40

-1.446

300

-1.284

40

-1.284

70

-1.284

45

-1.284

350

-1.281

45

-1.268

75

-1.276

50

-1.128

400

-1.278

50

-1.252

80

-1.268

55

-0.979

450

-1.273

55

-1.234

85

-1.259

60

-0.835

500

-1.267

60

-1.215

90

-1.251

65

-0.697

Sensitivity = 
[(-1.267 + 1.284)/200]/
[1.284/300] = 0.020

Sensitivity = 
[(-1.268 + 1.297)/10]/
[1.284/40] = 0.090

Sensitivity = 
[(-1.276 + 1.291)/10]/
[1.284/70] = 0.082

Sensitivity = 
[(-1.128 + 1.446)/10]/
[1.284/45] = 1.11

Range = 0.014

Range = 0.113

Range = 0.061

Range = 1.29

 

fkefrag1

vlurch

fkefrags23

vlurch

fI

vlurch

 

 

 

 

1.06

-1.344

 

 

 

 

1.07

-1.332

 

 

 

 

1.08

-1.319

1

-1.295

1

-1.288

1.09

-1.307

1.1

-1.291

1.1

-1.286

1.10

-1.295

1.25

-1.284

1.25

-1.284

1.11

-1.284

1.4

-1.277

1.4

-1.281

1.12

-1.272

1.5

-1.272

1.5

-1.279

1.13

-1.261

 

 

 

 

1.14

-1.250

 

 

 

 

1.15

-1.239

 

 

 

 

1.16

-1.228

Sensitivity = 
[(-1.277 + 1.291)/0.3]/
[1.284/1.25] = 0.045

Sensitivity = 
[(-1.279 + 1.288)/0.5]/
[1.284/1.25] = 0.018

Sensitivity = 
[(-1.228 + 1.344)/0.1]/
[1.284/1.11] = 1.003

Range = 0.023

Range = 0.009

Range = 0.116

Ordered summary of sensitivities

Variable Sensitivity of vlurch Range of vlurch, ft s-1 Magnitude
Positive effect on lurch (reduces rearward velocity)
fkefrags23 0.018 0.01 Small
vfrags23 0.020 0.01 Small
fkefrag1 0.045 0.023 Small
Qfrags23 0.082 0.06 Small
Qfrag1  0.090 0.11 Small
fI 0.99 0.12 Small
PE 0.19 0.49 Small
mbody 1.01 0.64 Small
Qcl  1.11 1.29 Large
Negative effect on lurch (increases rearward velocity)
mfrags23 -0.010 0.01 Small
mbullet -0.22 0.02 Small
mfrag1 -0.11 0.05 Small
Q  -0.089 0.07 Small
vbullet -1.23 0.09 Small
vfrag1 -0.063 0.11 Small
vbulletafter -0.086 0.22 Small
mcloud -0.86 2.30 Large

    As expected from the fact that the addition of three-dimensionality to the large fragments didn't change the lurch perceptibly, the sensitivities and their orders also remained nearly unchanged. The two new parameters, fkefrag1 and fkefrags23, also had extremely small sensitivities.

Summary
    The addition of three-dimensionality to the motion of the large fragments changed the solution by only negligible amounts, and didn't change the sensitivities either.

Ahead to Lurch 5 Angular
Back to Lurch 3 Angular
Back to Physics