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That, alone, would have been sufficient to earn Warshawski undying renown, but beneficial as it was, its significance paled beside her next leap forward, for in working out her detector, Dr. Warshawski had penetrated far more deeply into the nature of the grav wave phenomenon than any of her predecessors, and she suddenly realized that it would be possible to build an impeller drive which could be reconfigured at will to project its grav waves at right angles to the generating vessel. There was no converging effect to move a pocket of normal-space, but these perpendicular grav fields could be brought into phase with the grav wave, thus eliminating the interference effect between impellers and the wave. More, the new fields would stabilize a vessel relative to the grav wave, allowing a transition into it which eliminated the traditional dangers grav shear presented to the ship's physical structure. In effect, the alterations she made to Fleetwing to produce her "alpha nodes" provided the ship with gigantic, immaterial sails: circular, plate-like gravity bands over two hundred kilometers in diameter. Coupled with her grav wave detector to plot and "read" grav waves, they would permit a starship to literally "set her sails" and use the focused radiation hurtling along hyper-space's naturally occurring grav waves to derive incredible accelerations.
Not only that, but the interface between sail and natural grav wave produced an eddy of preposterously high energy levels which could be "siphoned off" to power the starship. Effectively, once a starship "set sail" it drew sufficient power to maintain and trim its sails and also for every other energy requirement and could thus shut down its onboard power plants until the time came to leave hyper-space. A Warshawski Sail hypership thus had no need for reaction mass, required very little fuel mass, and could sustain high rates of acceleration indefinitely, which meant that the velocity loss associated with "cracking the wall" between hyper bands could be regained and that use of the upper bands was no longer impractical.
This last point was a crucial factor in attaining higher interstellar transit times. The maximum safe velocity in any hyper band remained .6 c, but the higher bands, with their closer point-to-point congruencies, added a significant multiplier to the FTL equivalent of that velocity. Prior to the Warshawski Sail, not only had dimension shear made translating into the upper bands dangerous, but the successive velocity losses had made it highly uneconomical for any reaction drive ship. Now the lost velocity could be rapidly regained and the higher, "faster" bands could be used to sustain a much higher average velocity. As a result, the dreaded grav wave became the path to ever more efficient hyper travel, and captains who had previously avoided them in terror now used their new instrumentation to find them and cruised on standard impeller drive between them.
Of course, there wasn't always a grav wave going the direction a starship needed, but with the grav detector to keep a ship clear of naturally occurring grav waves impeller drive could, at last, be used in hyper-space. In addition, it was possible for a Warshawski Sail ship to "reach" across a wave (which might be thought of as sailing with a "quartering breeze") at angles of up to about 60° before the sails began losing drive and up to approximately 85° before all drive was lost. By the same token, a hypership could sail "close-hauled," or into a grav wave, at approach angles of 45°. At angles above 45°, it was necessary to "tack into the wave," which naturally meant that return passages would be slower than outgoing passages through the same region of prevailing grav waves. Thus the old "windjammer" technology of Earth's seas had reemerged in the interstellar age, transmuted into the intricacies of hyper-space and FTL travel. By 1750 pd, however, sail tuners had been upgraded to a point which permitted the "grab factor" of a sail to be manipulated with far more sophistication than Dr. Warshawski's original technology had permitted. Indeed, it became possible to create a negative grab factor which, in effect, permitted a starship to sail directly "into the wind," although with a marginally greater danger of sail failure.
The Warshawski Sail also made it possible to "crack the wall" between hyper bands with much greater impunity. Breaking into a higher hyper band was (and is) still no bed of roses, and ships occasionally come to grief in the transition even today, but a Warshawski Sail ship inserts itself into a grav wave going in the right direction and rides it through, rather like an aircraft riding an updraft. This access to the higher bands meant the first generation Warshawski Sail could move a starship at an apparent velocity of just over 800 c, but an upper limit on velocity remained, created by the range capability of the vessel's grav wave detectors. In the higher bands, the grav waves were both more powerful and tightly-spaced due to the increasingly stressed nature of hyper-space in those regions. This meant that the five-light-second detection range of the original Warshawski offered insufficient warning time to venture much above the gamma bands, thus imposing the absolute speed limitation. In addition, the problems of acceleration remained. The Warshawski Sail could be adjusted by decreasing the strength of the field, thus allowing a greater proportion of the grav wave's power to "leak" through it, to hold acceleration down to something a human body could tolerate, but the old bugaboo of "g forces" remained a problem for the next century or so.
Then, in 1384 pd, a physicist by the name of Shigematsu Radhakrishnan added another major breakthrough in the form of the inertial compensator. The compensator turned the grav wave (natural or artificial) associated with a vessel into a sort of "inertial sump," dumping the inertial forces of acceleration into the grav wave and thus exempting the vessel's crew from the g forces associated with acceleration. Within the limits of its efficiency, it completely eliminated g force, placing an accelerating vessel in a permanent state of internal zero-gee, but its capacity to damp inertia was directly proportional to the power of the grav wave around it and inversely proportional to both the volume of the field and the mass of the vessel about which it was generated. The first factor meant that it was far more effective for starships than for sublight ships, as the former drew upon the greater energy of the naturally occurring grav waves of hyper-space, and the second meant it was more effective for smaller ships than for larger ones. The natural grav waves of hyper-space, with their incomparably greater power, offered a much "deeper" sump than the artificial stress bands of the impeller drive, which meant that a Warshawski Sail ship could deflect vastly more g force from its passengers than one under impeller drive. In general terms, the compensator permitted humans to endure acceleration rates approaching 550 g under impeller drive and 4-5,000 g under sail, which allows hyperships to make up "bleed-off" velocity very quickly after translation. These numbers are for military compensators, which tend to be more massive, more energy and maintenance intensive, and much more expensive than those used in most merchant construction. Military compensators allow higher acceleration—and warships ca
In practical terms, the maximum acceleration a ship can pull is defined in Figure 2.
These accelerations are with inertial compensator safety margins cut to zero. Normally, warships operate with a 20% safety margin, while MS safety margins run as high as 35%. Note also that the cargo carried by a starship is less important than the table above might suggest. The numbers in Figure 2 use mass as the determining factor, but the size of the field is of very nearly equal importance. A 7.5 million-ton freighter with empty cargo holds would require the same size field as one with full holds, and so would have the same effective acceleration capability.