I’ve made a 3D model of the HVAP carrier for the 76mm M93.
Spoiler
As I was looking at it, a thought came to my mind. Let me show you something first:
Here is the tungsten core for the 76mm HVAP:
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It’s exactly 5in. long. The body from the base to the bourellet is about 4in long. Which means for vertical armour plates thinner than 4in. the core will perforate them before the base impacts the armour, assuming they stay together during penetration process, like this:
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if its true, then for plates around 4in. and thinner, the ballistic limit for this shell would be as for an equivalent projectile with the total mass equal to that of the core AND the steel base, but diameter of only the core.
Now let’s calculate the two and compare them to historical data:
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What do we see? The historical ballistic limits for 4 and 5in. plates at 0° are much closer to those that we get by assuming that the core penetrates without any additional help from the steel base.
Which implies that this is the case IRL. We don’t know for sure, but its a safe bet to assume that on impact with the armour the cylindrical base of the tungsten core applies so much force to the steel base of the HVAP projectile, that it shears a steel disk out of the base and it no longer contributes any kinetic energy towards the penetration of the armor.
Now, the historical ballistic limits are still a bit lower than my estimates for a naked core, which suggest that the carrier still contributes a little bit of kinetic energy to penetration, but a much smaller amount than previously thought.
I apologise to all people who came to this forum to talk about a videogame and not to read a lecture on physics. :)
Edit:
@KillaKiwi I believe that the higher than expected ballistic limit in that trial with .40in tungsten core is due to excessive projectile yaw. It is much more detrimental to penetration of subcaliber projectiles than full caliber ones. My estimates still match very closely to every other 0° APCR testing data I have. It gives the expected BL of 2762fps against 1.5in./0° RHA of 300 Brinell.