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the “joined” points. The points on the boundary occupied by the medium

(Euler cells containing these points have at least one empty cell among their

adjacent cells) are excluded from this rule. If one Euler cell contains several

individual points, one of which is a boundary point, only the boundary

point is used for calculation and all the other points are excluded from the

calculation.

After redistribution of the individual points among the cells of the Euler

mesh the described computational procedure is repeated. An artificial

viscosity [1] is introduced into the described computational scheme

for continuous calculation of the shock waves. In case of the medium

compression this viscosity gives a summand added to the hydrodynamic

pressure acting at this point (a combination of linear and quadratic artificial

viscosity is used).

Integration time step

Δ

t

is selected under the Current stability condi-

tion [1] and it meets the following inequation:

Δ

t <

min

(

i,j

)

Δ

l

c

(

i,j

)

+

q

v

2

r

(

i,j

)

+ v

2

z

(

i,j

)

,

here

c

(

i,j

)

is speed of sound at Lagrangian points,

Δ

l

is least of the Euler

mesh steps along the radial (

Δ

r

) and axial (

Δ

z

) coordinates (generally, the

Euler mesh with square cells is used where

Δ

r

= Δ

z

).

The described above computational algorithm is implemented in the

numerical simulation software ERUDIT (Russian abbreviation for Heuristic

Calculation of Ordered Motion of Individual Points) developed at Bauman

Moscow State Technical University which was used in the presented

research. Computational method described here was tested while solving a

wide variety of explosive and impact continuous medium loading problems

(as well as penetration problems) and showed positive results [10–12]. One

of its advantages is the ability to calculate a motion of the continuous

medium with large deformations without using specialized procedures of

computational mesh regeneration.

In order to penetrate into the targets made of high-strength steel

of a large width (more than 500 mm) elongated metal projectiles are

used which have speed of approximately 1500 m/s. As it was mentioned

above such projectiles penetrate into the targets in a hydrodynamic mode

(when the projectile material spreads around the target contact area with

the corresponding reduction of the projectile length during penetration).

According to the hydrodynamic theory of penetration [2] the main factors

affecting the target cavity depth are the following: a projectile length and its

material density. Elongated projectiles made of the high density materials

must be used for increasing a penetration depth. Such materials include

70 ISSN 0236-3941. HERALD of the BMSTU Series “Mechanical Engineering”. 2015. No. 1