On the accuracy of barrel-scaling
Posted: Fri Jan 08, 2016 8:03 pm
There have been attempts to gauge the relative firepower of certain guns by comparing their barrel lengths, operating under the assumption that a gun that is ten times as long will have 1000 times the volume and thus also have 1000 times the firepower. Of course, some have responded by questioning the relationship between a gun's volume and its firepower. This subject came up during my stint on SDN, and shortly before I left, I went through the trouble of doing a case study (which, IIRC, I never actually posted. Oops.) based on the Iowa class battleship.
The Iowa had 9 16-inch Mark 7 guns, 20 5-inch Mark 12 guns, 80 40mm Bofors guns, and 49 20mm Oerlikon guns. Some research turned up the following information:
The Mark 7 gun had a length of 20.3 m and could fire a 1225 kg armor-piercing projectile at 762 m/s, or it could fire a 862 kg high-explosive shell at some 820 m/s.
The Mark 12 gun had a length of 5.83 m and could fire a 25 kg shell at 760 m/s.
The Bofors 40 mm had a length of 2.25 m and could fire an 0.9 kg projectile at 900 m/s.
The Oerlikon 20 mm had a length of 1.4 m and could fire an 0.13 kg projectile at 820 m/s.
It's fairly easy to use Microsoft Excel to graph the relation between the length of each gun's barrel to the kinetic energy of its projectiles, and from there it's even easier to get a regression line that fits the data fairly well.
If L is barrel length in meters and E is kinetic energy of the projectile in Joules, then for the set of guns aboard an Iowa class battleship, the following equation approximately holds:
E = 20002 * L^3.2402
For whatever it's worth, R^2 = 0.9963, which means that the above equation fits the data pretty damn well.
So what does this mean?
Well, it means that, for projectile weapons at any rate, the relationship between volume and firepower is actually pretty close!
Mike Wong says that the "light turbolasers" aboard an ISD can produce about 1500 TJ of energy. We'll take this as a theoretical upper limit. MW also says that the heavy turbolasers aboard an ISD are some 5x longer. If the above relation works for energy weapons as well as projectile weapons, the heavy turbolasers aboard an ISD would be some 184x as powerful as the light turbolasers. That gives us an upper limit of about 276,000 TJ for heavy turbolasers. For those who prefer their data in terms of TNT equivalence, light turbolasers peak out at around 375 kilotons, and heavy turbolasers peak out at 69 megatons.
These are probably generous upper-end figures, given the explosive nature of the Hoth asteroids, the fact that they were less than half the size MW said they were, etc. etc.
Anyways, just food for thought.
The Iowa had 9 16-inch Mark 7 guns, 20 5-inch Mark 12 guns, 80 40mm Bofors guns, and 49 20mm Oerlikon guns. Some research turned up the following information:
The Mark 7 gun had a length of 20.3 m and could fire a 1225 kg armor-piercing projectile at 762 m/s, or it could fire a 862 kg high-explosive shell at some 820 m/s.
The Mark 12 gun had a length of 5.83 m and could fire a 25 kg shell at 760 m/s.
The Bofors 40 mm had a length of 2.25 m and could fire an 0.9 kg projectile at 900 m/s.
The Oerlikon 20 mm had a length of 1.4 m and could fire an 0.13 kg projectile at 820 m/s.
It's fairly easy to use Microsoft Excel to graph the relation between the length of each gun's barrel to the kinetic energy of its projectiles, and from there it's even easier to get a regression line that fits the data fairly well.
If L is barrel length in meters and E is kinetic energy of the projectile in Joules, then for the set of guns aboard an Iowa class battleship, the following equation approximately holds:
E = 20002 * L^3.2402
For whatever it's worth, R^2 = 0.9963, which means that the above equation fits the data pretty damn well.
So what does this mean?
Well, it means that, for projectile weapons at any rate, the relationship between volume and firepower is actually pretty close!
Mike Wong says that the "light turbolasers" aboard an ISD can produce about 1500 TJ of energy. We'll take this as a theoretical upper limit. MW also says that the heavy turbolasers aboard an ISD are some 5x longer. If the above relation works for energy weapons as well as projectile weapons, the heavy turbolasers aboard an ISD would be some 184x as powerful as the light turbolasers. That gives us an upper limit of about 276,000 TJ for heavy turbolasers. For those who prefer their data in terms of TNT equivalence, light turbolasers peak out at around 375 kilotons, and heavy turbolasers peak out at 69 megatons.
These are probably generous upper-end figures, given the explosive nature of the Hoth asteroids, the fact that they were less than half the size MW said they were, etc. etc.
Anyways, just food for thought.