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Table 2 Comparison between theoretical solution and numerical LCP solution.

From: An Improved Linear Complementarity Solver for the Dynamic Analysis of Blast Loaded Structures

 

Theoretical solution

Numerical

Lumped mass

Error

Lumped mass

(%)

Numerical

Continuous mass

Error

Continuous mass

(%)

\({P}_{0}=2.5{P}_{c}\)

 Hinge position \(\overline{t }=0\) (Fig. 12)

\({\xi }_{1}^{*}/L\)

0.54265

0.54000

0.49

0.54500

− 0.4331

 Hinge position \(\overline{t }=0\) (Fig. 12)

\({\xi }_{2}^{*}/L\)

0.61629

0.62000

− 0.60

0.61500

0.2093

 Hinge position at the end of Phase 1

\({\xi }_{*}/L\)

0.58579

0.59000

− 0.72

0.59000

− 0.7187

 Displacement at the end of Phase 1

\({\bar{W}}_{1}=({W}_{1}/L).(mL){M}_{p}/{I}^{2}\)

0.05224

0.05205

0.35

0.05292

− 1.3017

 Time when hinges coalesce

\({\bar{t}}_{1}={M}_{p}{T}_{1}/IL\)

0.05300

0.05308

− 0.14

0.05339

− 0.7358

 Displacement at the end of motion

\({\bar{W}}_{3}=({W}_{3}/L).(mL){M}_{p}/{I}^{2}\)

0.63318

0.62575

1.17

0.63128

0.3001

 Cessation time

\(\overline{t }={M}_{p}T/IL\)

0.34272

0.34005

0.78

0.34394

− 0.3560

\({P}_{0}=12.5{P}_{c}\)

Hinge position \(\overline{t }=0\) (Fig. 12)

\({\xi }_{1}^{*}/L\)

0.28706

0.28500

0.72

0.28500

0.7176

 Hinge position \(\overline{t }=0\) (Fig. 12)

\({\xi }_{2}^{*}/L\)

0.79702

0.79500

0.25

0.79500

0.2534

 Hinge position at the end of Phase 1

\({\xi }_{*}/L\)

0.58579

0.59000

− 0.72

0.59000

− 0.7187

 Displacement when the pulse terminates

\({\bar{W}}_{1}=({W}_{1}/L).(mL){M}_{p}/{I}^{2}\)

0.14686

0.14689

− 0.02

0.14666

0.1362

 Displacement at the end of Phase 1

\({\bar{W}}_{2}=({W}_{2}/L).(mL){M}_{p}/{I}^{2}\)

0.38234

0.38247

− 0.03

0.38145

0.2328

 Time when hinges coalesce

\({\bar{t}}_{1}={M}_{p}{T}_{1}/IL\)

0.11372

0.11214

1.39

0.11339

0.2902

 Displacement at the end of motion

\({\bar{W}}_{3}=({W}_{3}/L).(mL){M}_{p}/{I}^{2}\)

0.83904

0.84450

− 0.65

0.83042

1.0274

 Cessation time

\(\overline{t }={M}_{p}T/IL\)

0.34248

0.34439

− 0.56

0.34323

− 0.2190