Energy propulsion by particle waves.

Designs that make simple harnessing of energy possible that can have many applications as wise labs proposes this question would it be possible to run a vehicle on a plasma plain or a solar wind and the answer could be "yes" technology cupped with solar given the right shape for example the sail shape or curved shape to counter resonance or force there are "few designs" but an effective one would power a wave back into craft like a "plasma plain propulsion system". This could lead designs with fibre optic channelling into the future working on the squaring of the atoms. This could be tested true the mingling of the structure of atom to give increased propulsion true a new Ion system or wave system this patent would exist with current ion technologies but powering a rotational surge. Also wise labs found in studies, plasma resonance for new proposed propulsion system in a surface wave that sustained plasma was investigated. Surface wave discharges have been successfully generated by a microwave planar vane-type slow wave structure generated enough power to justify them. Experimental results clearly demonstrated that the amplitude of the electric field of the microwave always became a local maximum in the position where the plasma density was equal to the same value. When the test of operating gas pressure and the input of microwave power were varied change of the plasma density profile occurred. The location of the maximum of the electric field was found to shift in compliance with the plasma density profile. Meanwhile, the peak of the resonance response was found to be proportional to the plasma density gradient while the spatial width of plasma resonance was inversely proportional to the plasma density gradient. These results were qualitatively in accordance with the theory.(Also known as the electron cavitation region in this reference picture) The study of the effect of striation plasma density disturbances on the generation intensity of longitudinal cold and plasma oscillations due to polarization of the magnetic field-aligned ionospheres plasma irregularities with "δNo grater than 0" by a powerful radio wave. It is assumed that the plasma density level inside the irregularity intersects the upper-hybrid resonance level, in the vicinity of which the cold oscillations excited directly by a powerful radio wave are transformed to shorter-wave plasma oscillations. We consider the short plasma wave limit to reduce the problem to a system of two coupled equations for the cold wave induction and plasma wave electric field. The first equation is supplemented by a local source equal to the integral of the plasma wave electric field in the resonance region.
The second equation involves the cold wave induction at the resonance point and describes the electric field of interacting waves in the resonance vicinity. We use simplifications connected with the small absorption of plasma waves propagating inside the irregularity and weak radiation of these waves outside the irregularity. These conditions correspond to the generation of egenmodes of plasma oscillations trapped in the irregularity. We have obtained a resonance-type nonlinear equation for the electric field intensity (or energy flux) of eigenmode plasma waves with allowance for striation disturbances of the plasma density profile in the resonance region. It is shown that the striation expulsion of plasma is responsible for the occurrence of coefficients describing the change in the intensity of excitation and radiation of plasma waves at the irregularity boundary. Such an expulsion leads to variations of the efficient generation band of plasma egenmodes with the total phase increment of the wave in the irregularity. It also leads to a change in the phase shift of the plasma wave reflected from the resonance. These coefficients and the nonlinear phase shift are expressed in terms of real wave functions of the nonlinear Airy equation which describes the electric field of the excited waves in the resonance vicinity when the dissipation is absent. This entropy graph shows longitudinal resonances many of these are just simple technologies that can work in conjunction to create a bow shock wave like in