3.2.1 It is considered that the collision damage to the struck ships is large and heavy
because the damage penetration in the order of B/5 is to be investigated. This means
the side shell will be ruptured and decks or stringers or webs etc. could be
crushed.
3.2.3 The energy absorbed by destroying ship structural members in tension mode can be
determined from:
where
|
σ0 |
= |
is the flow stress of the materials and taken as the average of yield
stress and tensile strength, |
|
εc |
= |
is the critical rupture strain of the materials, and |
|
R1 |
= |
is the materials volume of the damaged structural members in tension
mode. |
3.2.4 The energy absorbed by destroying ship structural members in crushing mode can be
determined from:
where
|
σ0 |
= |
is the flow stress of the materials and taken as the average of yield stress
and tensile strength, |
|
R2 |
= |
is the materials volume of the damaged structural members in crushing
mode, |
|
t |
= |
is the structural member thickness, and |
|
b |
= |
is the width of the structural member. |
3.2.5 The total absorbed energy can be obtained from summation of the energy absorbed by
all damaged structural members: