I floated in the pho-torp vs. q-torp thread a theory regarding the actual operation of the q-torp, and wondered how I might go about verifying whether it could or could not physically work.
Essentially, my theory was that the q-torp is akin to a Ulam-Teller fission-primary fusion device, except instead of a fission trigger and fusion secondary, the trigger is matter/antimatter, and the secondary is a lump of several hundred or thousand kilograms of an extremely dense material. The casing would be a gamma ray mirror (dilithium?) capable of temporarily containing and reflecting the radiation back into the secondary--much as a Ulam-Teller design uses a depleted uranium shell to contain the fission primary's output.
The dense secondary is then compressed by the radiation pressure into a ("quantum," natch) singularity, which in Trek-speak is essentially synonymous with black hole.
The black hole of very small size (for a black hole) would evaporate nearly instantly in intense Hawking radiation, such as (probably) powers Romulan D'D-class warbirds.
The upshot is that you would be converting hundreds or thousands of kilograms into energy for the potential bargain price of a few kilograms of antimatter.
Now, what I don't know is how to calculate the energy requirements for compressing an arbitrarily large or small amount of mass into a black hole. I suspect it would be immense, and that the idea may not be feasible without an unrealistically large amount of antimatter, or perhaps infeasible altogether.
Essentially, my theory was that the q-torp is akin to a Ulam-Teller fission-primary fusion device, except instead of a fission trigger and fusion secondary, the trigger is matter/antimatter, and the secondary is a lump of several hundred or thousand kilograms of an extremely dense material. The casing would be a gamma ray mirror (dilithium?) capable of temporarily containing and reflecting the radiation back into the secondary--much as a Ulam-Teller design uses a depleted uranium shell to contain the fission primary's output.
The dense secondary is then compressed by the radiation pressure into a ("quantum," natch) singularity, which in Trek-speak is essentially synonymous with black hole.
The black hole of very small size (for a black hole) would evaporate nearly instantly in intense Hawking radiation, such as (probably) powers Romulan D'D-class warbirds.
The upshot is that you would be converting hundreds or thousands of kilograms into energy for the potential bargain price of a few kilograms of antimatter.
Now, what I don't know is how to calculate the energy requirements for compressing an arbitrarily large or small amount of mass into a black hole. I suspect it would be immense, and that the idea may not be feasible without an unrealistically large amount of antimatter, or perhaps infeasible altogether.
