Wednesday, August 7, 2013

Note of Book for "Gandhiva" Experiment

Monday, August 5, 2013

The "Gandhiva" Experiment or CGSHL Experiment

The "Gandhiva" Experiment or Chandra (For Chandrasekhar)-Gauss-Saharov-Hunter-Lopez Experiment (CGSHL) is a continuation of GSHL Experiment or better say one evolution of the same, now using biggest energies, planning this time, to use the Tremendous Energy of Solar Electromagnetic Field like Ejection Trusth Force to stellar-ship more big

Is Ambitious but possible theoretically , because the sun is (using simple terms) one explosion self-containned for gravitational Forces. Now like in the GSHL-Experiment the Magnetic-Field-Compresion Principles (MFCG) is the same, even better, because now we economize on explosives this for always, and the loads (ships) can be more, more, and more big. The problem of couse, continue being the high temperature and strong radiations.

First that all, we begining our calculations of classic way with a balance equation like in GSHL Calculation, now of course, having account aspects like radiation, gravitation, and internal pressure forces.

To continue we proceed to calculate the inner currents using the Dynamo Theory and to finally obtain The Lopez'z Speed Equation.

Actually the lecture of instruments show modest magnetic fields (some kilogauss), but we believe, feeling fervent that inner core is different. Even if our physic intuition will failing us is even possible to use some class of thermoelectric effect to provide great currents for the teragaussian-coil.

The final concept is using this giants electromagnetic streams, produced for stars, like canals that would allow us voyage across the universe in similar form to antiquity peoples using the streams in sea or rivers to navigate.

Artistic visualization of Solar-Trusth

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Monday, June 10, 2013

Sketches and Notes

Wednesday, April 24, 2013

Projectil-Generator (Interior Detail)

Monday, April 15, 2013

Teragaussian Projectile-Ship (Details)

Wednesday, April 3, 2013

Lopez's Speed Calculation II (In Remodelling)

Lopez´s Ejeccion Speed Calculation

seg) take us 1hr 30 minutes arrive to mars

Speed by Experimental Thrust

Speed Ejection Constants:
Q(exp) : 4.2 x 10E15 [J]
T : 6.0 x 10E6   [K] or 0.5 [keV]
p : 3.14159264
µ : 4p x 10E-7 [TmA]
Insert Vehicle Weigh [Kg]:
Insert Coil Helix Number   :
Insert Coil Long [m] :
Insert Conductor Cross Section Area [m2]:

For reference the distance earth to Mars is 59 million of miles, is say to 10 [Lops] (10.000 kms/seg) take us 1hr 30 minutes arrive to mars

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Wednesday, March 20, 2013

Magnetic hysteresis (2)

Theoretical model of magnetization m against magnetic field h. Starting at the origin, the upward curve is the initial magnetization curve. The downward curve after saturation, along with the lower return curve, form the main loop. The intercepts hc and mrs are the coercivity and saturation remanence.
When an external magnetic field is applied to a ferromagnet such as iron, the atomic dipoles align themselves with it. Even when the field is removed, part of the alignment will be retained: the material has become magnetized. Once magnetized, the magnet will stay magnetized indefinitely. To demagnetize it requires heat or a magnetic field in the opposite direction. This is the effect that provides the element of memory in a hard disk drive.
The relationship between field strength H and magnetization M is not linear in such materials. If a magnet is demagnetized (H=M=0) and the relationship between H and M is plotted for increasing levels of field strength, M follows the initial magnetization curve. This curve increases rapidly at first and then approaches an asymptote called magnetic saturation. If the magnetic field is now reduced monotonically,M follows a different curve. At zero field strength, the magnetization is offset from the origin by an amount called the remanence. If the H-M relationship is plotted for all strengths of applied magnetic field the result is a hysteresis loop called the main loop. The width of the middle section is twice the coercivity of the material.[16]
A closer look at a magnetization curve generally reveals a series of small, random jumps in magnetization called Barkhausen jumps. This effect is due to crystallographic defects such as dislocations.[17]
Magnetic hysteresis loops are not exclusive to materials with ferromagnetic ordering. Other magnetic orderings, such as spin glass ordering, also exhibit this phenomena.[18]

Saturday, March 9, 2013

Reference Natural Events to GSHL (5)

New High-Intensity Cosmic Explosion (Reference for GSHL Experiment)

Nikola Tesla (Courtesy Of Hystory Channel)

Nikola Tesla (Courtesy of History)

Rotary magnetic fields

Electromagnetic Rail Gun Simulation

Simulations of Core Collapse Supernovae (Natural Events Reference for GSHL Experiment))

Supernova Simulation (Cosmic Magnetic Events for Reference to GSHL Experiment))

Type-II Supernova (Space Magnetic Events)

A simulation of magnetic field outflows from active galactic nuclei (Space Magnetic Events)

Go to Principal Page

Wednesday, March 6, 2013

Lopez's Teragaussian Ejection Speed Calculation

Lopez´s Ejeccion Speed Calculation

Monday, February 25, 2013

Ejection Speed Calculation

Friday, February 22, 2013

What is the GSHL?

The GSHL or Gauss - Saharov - Hunter - López Experiment is attempt by treating to make a super-impulse for stellar pre-jump, using Electromagnetic-Thermonuclear Propulsion . It would be utilized preview to a HTSL dimensional jump (View). Its Theoretical Foundations is on the MFCG study. In view of " experimental difficult obvious", it carry us to "squeeze" all the concerning with Teraflopian Simulations in High Energies to level never Think.

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