00 Lpdbrief

A Tale of Two Materials ! ! ! At first glance it appears impossible to utilize the vast energy of the Zero-Point Energy Field. Why? A more descriptive name for the Quantum Flux is light-pressure. The photons of the Quantum Flux exert many tons of light-pressure on us all the time; however, since this pressure is equal in all directions, all of these forces seem to add up to zero net force; fortunately, things are not always as they seem! ! ! In principle, the quantum-pressure of the photons of the Zero-Point Energy Field (ZPE) can impart up to twice as much momentum to one side of a solitary macroscopic object as to its opposite side---despite the fact that the quantum pressure is the same on both sides! This is possible because the material on one side of the isolated object can be engineered so that it primarily reflects the photons of the Quantum Flux while the material on its other side primarily absorbs them. In other words, one side experiences elastic collisions with these photons while its opposite side experiences inelastic collisions with these photons. This results in a net Quantum Light-Pressure Force that acts on a single isolated macroscopic object! Nichols Radiometer is a well-known example of a light-pressure device. It demonstrates light-pressure using visible light. (Not to be confused with Crookes Radiometer which actually works on a weird kind of convection that only takes place in a partial vacuum!) Light pressure phenomenon has been independently repeated and published in peer-reviewed journals and in textbooks. Astronomers have found that it changes the course of Asteroids and NASA has found that it even wreaks havoc with geostationary satellites that refuse to remain so!!! A Quantum Light Pressure Device is far easier to construct than other Quantum Flux Devices such as Z-PEC, since we are not dealing with nano-scale structures. We merely have to identify or create two materials, one which does an especially good job of absorbing EUV wavelengths and a second material that does an especially good job of reflecting these wavelengths. Preferably in the 50 nm wavelength or smaller. Smaller is much better!!! It is overwhelmingly likely that somebody out there already has the materials I am looking for, or knows where to find them, or how to make them ! ! ! At this point, I don't even need high-performance materials; I just need two materials that perform well-enough to produce a conclusive experiment, an experiment that can be easily replicated by others. Then I can easily raise the money to pay people to quickly improve the materials. Potentially, we can generate enormous macroscopic scale forces that vary from grams to tons, depending on the effective relative bandwidth of the two materials.

Down Where the Sun Always Shines ! ! ! Historically, Quantum Physics revealed the quantized nature of energy but failed to explain such mysteries as why the orbit of the electron that is circling the hydrogen atom does not decay and fall into the nucleus—even though it is constantly accelerating, and is consequently radiating Cherenkov Radiation energy into Space due to its circuitous motion. The notion of a Quantum Flux was created to provide an energy field for the electron to exchange energy with. In other words, the electron had to have a source of energy to replenish what it was constantly losing due to Cherenkov Radiation. The sub-field of quantum physics that grew out of this model is called QED for Quantum Electrodynamics. It tries to model all particle and energy interactions in terms of the quantum flux. Naturally the question arose as to how its wavelengths are distributed? Stochastic Theory solves this problem by invoking Lorentzian Invariance, which is a cornerstone of Special Relativity. In other words, the vacuum flux distribution must appear constant to all observers in non-accelerating reference frames despite red-shift/blue shift phenomenon. In other words no matter how fast you travel in Space you must always witness the same quantum flux distribution even though your velocity causes some wavelengths to red-shift. The only wavelength distribution that yields Lorentzian Invariance must adhere to the formula: k / d^4

Incidentally, abundant the experimental evidence matches this formula perfectly within the limits of our ability to make accurate measurements!!! It turns out that k = 1.30 X 10^(-27) So, back to our formula, if we want to know how much Quantum Flux light pressure is exerted on a perfectly reflecting surface by all ZPE wavelengths from 9 nm on up, we simply have to plug in these values! 1.30 X 10^(-27) / (9 X10^(-9))^4 = 198,141 Pa. nm

PSI

1 191,676 2 11,980 3 2366.37 4 748.73 5 306.68 6 147.9 7 79.83 8 46.80 9 29.21 10 19.17 11 13.09 12 9.24 13 6.71

nm

PSI

nm

PSI

nm

PSI

14 15 16 17 18 19 20 21 22 23 24 25 26

4.989 3.786 2.925 4.989 3.786 2.925 2.295 1.826 1.471 1.198 0.9856 0.8182 0.6849

27 28 29 30 31 32 33 34 35 36 37 38 39

0.5777 0.4907 0.4194 0.3607 0.3118 0.2710 0.2366 0.2075 0.1828 0.1616 0.1434 0.1277 0.1141

40 41 42 43 44 45 46 47 48 49 50 51 52

0.1023 0.09192 0.08285 0.07487 0.06783 0.06160 0.05607 0.03928 0.03611 0.03325 0.03067 0.02833 0.02622

The table on the left, shows these pressures in pounds per square inch. For example, at 6 nm we see a value of 148 psi. This is the total quantum pressure that is attributable to all wavelengths that are greater than or equal to 6 nm To determine the light pressure that is attributable to just those wavelengths that include 9 nm and ten nm and every wavelength inbetween: We simply subtract the pressure value for 10 nm and above, from the (larger) pressure value for 9 nm and above: 29 – 19 = 10 psi

This chart gives the amount of pressure caused by each one-nanometer bandwidth.

Wm. Scott Smith Spokane, WA 99205 USA +509 315-9602 US Pacific Coast Time [email protected]