Ivar


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Cc

L(1

Vx (t)

z (t)

↵)

C

Iy (t)

1 H = 4EC n ˆ 2 + EL ˆ2 2

EJ (

z (t))

= 2EJ | cos(

EJ (

EJ2

L↵

z (t)) cos(

z (t)e/h)|

EJ1

ˆ

ext )

Cc 2eˆ nVx (t) Cc + C

symmetric case

asymmetric case



~ ˆ Iy (t) 2e