Stormer said:
I thought the point of artillery is to affect a area, so a equal dispersion of frag going in every direction.
Sure, but that doesn't include up and to the sides. If you have a long, rod-shaped projectile, it would be difficult to shape a charge that does anything other than send shrapnel out horizontally when detonated at ground level, when what you really want is an air burst that sends a cone of shrapnel down over a wide area.
Stormer said:
And aerodynamic stability is the reason a long slender sabot dart can be shot accurately without spin stabilization. A normal artillery shell on the other hand would tumble without spin stabilization.
You still have to carefully balance that projectile to make sure it is stable, which is not a given if you also have to pack a warhead in there.
Stormer said:
If you are using a brass case anyway the total length does not have to be so much longer because you can put the sabot projectile all the way down to the bottom of the case with the propellant around it just like in a saboted tank shell.
View attachment 313857
Stormer said:
I also think a slim sabot artillery shell with the same weight as a normal artillery shell would get a better ballistic coefficient and that alone would give it a longer range, plus the higher speed because of no losses going to spinn up the projectile. And all of that with a cheaper barrel to make because of no rifling, and probably a longer barrel life too because of the lack of rifling.
Let's test this theory:
- The penetrator for an M829 APFSDS weighs 4.6 kg and is 68.4 cm long and 2.7 cm in diameter, so the aspect ratio is 25.3. It also has 11.9 kg of propellant and casing.
- The M795 howitzer shell weighs 47 kg, 10.8 kg of which is high explosive.
Let's assume we want the same aspect ratio as the M829 penetrator in the form of a howitzer projectile. TNT has a density of 1.654 g/cm
3, so the M795 has 6529.6 cm
3 of TNT inside. To mold that into a projectile the same shape as the M829 penetrator (i.e., with the same aspect ratio), it should obey the rule
<br />
L = \left(\frac{4V(AR)^2}{\pi}\right)^{1/3},<br />
which results in a shell that is 174.7 cm long. That's already 1/3 the length of the barrel of the M777. Here's the kicker: you can't just shape the explosive like the penetrator because it's the
casing that produces the blast frag effect for an artillery round. I don't have number for how much the casing on an M795 weighs, but it's the majority of the remaining weight of the shell since the propellant charges are separate. Let's assume it's 80% of the remaining 36.2 kg, so about 29 kg of high-frag steel casing. That has to surround the high explosive. It has a density of about 7.85 g/cm
3, so the volume is 3694.3 cm
3. That makes the total volume of the projectile 10,022 cm
3, leading to a length of 203.0 cm. with a diameter of 8.0 cm. That's about 40% the length of the M777 barrel.
Now let's assume the ratio of projectile mass to the total mass of the round (including propellant, casing, and sabot) is the same as for the M829. The M829 weighs 20.9 kg, so is about 43% projectile by mass. This means the above shell with a mass of 39.8 kg would be part of a round whose total mass is 92.6 kg.
So your idea is to launch rods that are taller than an average adult male from a round with a mass that is greater than the average adult male. This is a bad idea for several reasons:
- The round would require de-elevating the howitzer in order to load it, slowing down firing operations.
- The round would not work with existing howitzers, whose barrels are far too short for this.
- The round would require considerably more complicated logistical chains to transport it and deliver it to the battlefield (they are twice the mass and almost 3 times the length but with the same diameter as the M795 in this example).
- The round would require multiple soldiers to lift it and load it into the howitzer, meaning you need more men to man an artillery battery.
- There still isn't likely to be enough room to ideally shape the charge to produce optimal blast frag without further increasing the size and mass.