Theemile wrote:Compensators actually work on a volume of space, not an actual mass. It's just a ship of x mass fills said volume. Empty or full, everything inside the volume is compensated.
This is described in ACD, where we see the Sub-optimal havenite designs with spin sections, and slower speeds are accepted for a wider compensated volume.
The reason for the mass statements is the Great Resizing, where mass was the only dimension kept from the early books to the latter books.
Ok, so when we hear that 9 or 10 million tons is the current upper practical limit for a ship's size, it's not due to the mass of the ship actually being that size, it's because a ship of the maximum practical size typically has that mass. That is, ships tend to keep to an average density across all volumes.
I'm not sure this makes sense. I'd expect the biggest portion of the mass of a ship to be its hull, especially the armour for a warship. Given the square-cube law, you'd expect that the fraction of mass dedicated to the armour to decrease as the volume of the ship increases. Internal spaces start to take a bigger proportion and those have much smaller density. Even missile and other ammunition shouldn't mass as much as armour. The only thing I can think of that could even come close to that density is highly-compressed hydrogen -- if you can use gravity to compress it to fusion, you can compress it to less than fusion and just pack a lot of it.
It's more likely it's like Jonathan_S said and the mass assumes a constant density for historical reasons which may not apply anymore. Let's take these figures:
Jonathan_S wrote:I don't think you're right about the freighters being listed as their loaded weight. I'm using the numbers of the Starhauler class listed in the SITS books. A small modular freighter for Silesian trade is a 1.9 mton design, 767 m long, 128 m across, and 119 m tall.
Assuming an elliptical cross-section and modelling the entire ship as a cylinder, that would give an a volume of 767*128*119*π = 36.7 million m³ and an average density of ~47 kg/m³ (less than half as dense as wool, slightly more than polyurethane foam). Those numbers only make sense if the volume is mostly air (1.225 kg/m³ at STP) or even vacuum. In turn, if the 1.9 MT is mostly hull and the hull material clocks at 10,000 kg/m³ (more dense than iron), volume occupied by the hull is 190,000 m³. That's 0.5% of the total volume. Or, again assuming our perfect cylinder, it would mean the hull is between 8.5 and 9 m thick.
That makes sense to me.
Now, of course, a warship's armour is likely to be thicker and denser than a freighter's hull.