Dear All,
Last posts I discussed a refined take on what has aptly been termed the “sledgehammer approach”. I outlined using high intensity pulsed lasers to achieve higher E field densities, and how this potentially directly relates to local negative energy densities in the QV. I cannot prove it empirically due to lack of resources but I have a strong suspicion that the resonant frustum, among other effects, produces a spacetime distortion with a mass/energy gradient in the longitudinal axis. The related mechanisms are outlined in these papers.
http://www.earthtech.org/publications/davis_STAIF_conference_1.pdf https://arxiv.org/pdf/1005.5682 I have refined and revised my design suggestion regarding a metallic photon ‘lattice’ with feedback loop. I have dropped the idea of using entangled photons due to the practical impossibility of sufficiently regulating internal temperature.
Design idea(s):
1)
Thin resonating cones (hollow needles) – Single high power solitonized pulse laser split at the top of the device aimed towards each of the needles via diffractive/beam splitting material or antennas. Top of the device has a tapered conical chamber shape where noise can accumulate and dissipate. Each thin cone resonates and has own propulsive effect. Net propulsion is Cones*laser input assuming relatively equal power distribution but slower loading. Concerns: resonance in open cone is impossible, how to implement one way mirrors on the tops of the cones?
Key point here is that E field density is several orders of magnitude higher than with magnetron designs. If linear scaling applies to thrust as experimentally suggested by Eagleworks then we have some serious potential thrusts.
2)
Carbon nanotube lattice – Carbon nanotubes are absolutely fantastic tunable complex mini frustums. Q is low but imagine many tens of thousands being excited by a high intensity emitter. Regarding structure I suggest two options: many straight tubes. Second is honeycomb with multiple clusters stacked in multiple layers. Each layer will catch a certain % of total radiation from the emitter with sum adjustable by shifting layer position. Added bonus with honeycomb design is improved modularity, cooling and repairs to damaged or inefficient layers. Required reading
https://arxiv.org/pdf/1506.07352 Key point is the economy of scale which comes from many thousands of frustums. Additionally, carbon nanotubes can be tuned to facilitate phase lock and they can accept much smaller wavelengths. Areas to explore are nanotube architecture such as conical nanotubes (currently confined to um scale
http://pyramid.spd.louisville.edu/~eri/papers_pres/Sunkara_Small_Materials_2008.pdf) and connected/feedback loops within nanotube mesh.
EDIT: I forgot to clarify, honeycomb design would apply on both macro and micro levels. Imagine on the macro level something analogous to racks in a grill.
I am currently investigating the implications of this paper on EM absorption. It, and much other literature, posits that carbon nanotubes dissipate EM energy via vibration, in fact it is an established use.
http://cdn.intechopen.com/pdfs/17295/InTech-High_frequency_properties_of_carbon_nanotubes_and_their_electromagnetic_wave_absorption_properties.pdfHowever, I am optimistic as http://cdn.intechopen.com/pdfs-wm/17303.pdf clearly demonstrates on pp 475-476 that wavelength decreases along the tube creating quasimomentum in the microfrustum(!!!), sounds familiar doesn't it? If sufficiently cooled (to prevent kinetic energy loss) there is clear theoretical support for this concept working in a similar way to existing designs.
Another related paper for the interested: http://www.jpier.org/PIER/pier94/25.09062001.pdfFinal edit: The more I look into carbon nanotube properties the more alluring the idea seems. Would be interesting if somebody creates a honeycomb-like mesh of interconnected tubes (similar to graphene but perfectly aligned). Quite honestly, the potential interactions between high energy lasers and carbon-surface plasmonics in the context of such a design is beyond my current understanding and even my imagination.
http://www.ece.rice.edu/ece/xugroup/Papers/Excitation%20of%20Plasmonic%20Waves%20in%20Graphene%20by%20Guided-Mode%20Resonances.pdf All this being said, we are still at a frontier in terms of maximizing intra-cavity power, as 5.6kW is the last empirical limit I could find before severe kinetic degradation of the walls occur. Potential solutions include the layered graphene pseudo-tubes I mentioned, cooling techniques, and taking advantage of the sheer number of microfrustums. Here's a 2007 paper dealing with mode-locked high energy pulse lasers in carbon nanotubes and the practical limitations.
http://www.photon.t.u-tokyo.ac.jp/~maruyama/papers/07/SongAPL.pdf Best Regards,
LA