PRACTICAL PROBLEMS

PRACTICAL PROBLEMS<= /o:p>

An eter= pump (EP) has one or two rails to drive eter-io= ns. They are high voltage electrodes. Working in air they must be covered by a thick insulator material. Such material must be slightly conductive. If not, equipotential surface move and the dielectric can burn down. In air, that surface of highest voltage is the electrode’s surface. The insulator&= #8217;s external surface is in direct contact with the air. So it is the null volta= ge equipotential surface. Inside the insulator material there is a voltage-gradient. As the high voltage is a little more than the ionizing voltage, the eter-ionizing surface is inside the insulator. Then eterons disappear at that surface. So the eter flow must cross the insulator from its external surface. In other words, it= is unavoidable an eter current through the insulat= or.

In the case of a linear EP u= sed as NID propulsion unit, the prow is an eter-absorb= ing end. First it absorbs inside the insulator. The eter-hole moves an eter current around so from the electr= ode as from the frontal part. At the stern it is the eter-emitting end. It also generates an eter flow but emittin= g as a source, also through the insulator. Every eter = flow with matter inside, that matter generates introns of a speed oriented again= st the flow. Once the introns are in balance with the flow, at the prow the frontal part of the EP (the insulator’s frontal surface) have atoms t= hat absorb eter with theirs introns. But those intr= ons do not push the atoms ahead because at the back eter is swallowed by the EP. Introns have no loaning surface to push atoms because instead of being supported at the back they lose eter<= /span> in the EP. By this way the insulator is a corridor for eter; there are no forces between such insulator and the electrode. Now, if the E= P is switched off, introns suddenly have support at the back; then if the insula= tor is not strongly stuck to the electrode it flies ahead like a projectile. EP must be inactivated slowly to diminish the intron’s force, letting th= em to accelerate ahead and slowly the whole EP.

When the EP is working as NI= D, at both ends the insulator is in balance with introns. At the back it emits eter, also through the insulator whose introns “pump” eter outwards. Eter do not f= low towards the electrode; just emitted eter pushes= the whole EP ahead. The only way of emitted eter is= moving the EP inside the frontal hole. If the EP is switched off introns will seek= to insert insulator’s atoms inside the electrode. Again, EP’s inactivating must be slow.

At its time, the frontal abs= orber (the prow) do not absorb from the frontal part of the electrodes because introns of the insulator saturate it. In other words, it is easier to absor= b eter from outside than from the electrode.

The conclusion is the next: = one, the EP must be inactivated slowly. Two, the insulator must be strongly stuc= k to the electrode and made up of resistant mechanically material.

The phenomenon described abo= ve limits the craft’s speed to a low value (not more than a few hundreds= of km/h). High space-speeds like 100000 km/h are impossible because it wou= ld imply to accelerate the insulator covers to such inertial speeds. Moreover,= the craft never could reach the speed of light.

What happens in vacuum? As v= acuum does not conduct electricity the electrode can face directly to vacuum. Removing the insulator each time the craft reaches vacuum is definitively n= ot practical. If not removed, equipotential surface of ionizing voltage will migrate to the external surface of the insulator. Remember that such insula= tor is slightly conductive. Then it works as a naked electrode. Electric resist= ance of the insulator does not disturb; there is NO ELECTRIC current inside the = high voltage electrodes while NID works. It conducts only e= ter-ions that ignore electric resistances.

Problems wi= th lifting wheels (LW).

Observe the diagram “L= IFTING WHEEL”. As the wheel spins its material enters and exits fast inside = the eter flow. Being inside, it acquires introns and the = EP generates a dense-eter-zone between the emittin= g end and the wheel’s ring, above. So that part of the wheel is inside an <= span class=3DSpellE>eter-density-gradient. As a consequence, the Absolute= Speed Vector (ASV) undergoes a deviation (remember the intron-turbine). This time= it can be disturbing. Deviation-angle (between the axis and the ASV) depends on the orientation of the wheel’s axis. When the angle is 90° (horizontal ASV), there is no deviation and even it doubles the lifting for= ce (never diminishing). If the angle is null (vertical ASV) it does not distur= b at all. An angle of 45° degrees is the worst one. Then the lifting force is deviated 22.5° degrees regarding vertical. Maybe for a craft soaring in= a wide land means no problem, but in the case of a crane or in the slow and n= ice landing of a craft it is unbearable.

It is solved building the wh= eel in such a way that its axis can be tilted to counteract lateral deviation. We = jump over the calculation; less than 22° degrees of tilting for the axis is enough to achieve a vertical force. It is better to only the EP-supports keeping the wheel’s axis always vertical with regard to the craftR= 17;s ground. It avoids an intense gyroscope effect of a heavy spinning wheel.

Health prot= ection.=

When the first H-bomb has be= en proved at Bikini islands an interesting phenomenon happened. At 40 km far from the explosion an Iowa-type battleship had serious disturbing of its electronic equipment due to what they knew at that time as “electromagnetic pulse”. It was a strong pulse of subelectricity, an eter-i= on current. Steel-shield of 40 cm did not stop it. At the meantime a submarine was observing the explosion through the periscope. It was only 10 km far from the explosion. It underwen= t not any electric disturbing effect. What was the difference? It is trivial: the water shield, one of 1= 0 km thick. Calculating the energy of that explosion of 1 megaton, if we use EP = of double rail whose subelectricity-dispersion is = much lower than that of an EP of one rail, a water shield of 50 cm is enough for a generating set of many thousands of KW. Although we don’t know the protecting mechanism of water, at Bikini islands it worked.

What changes will the water undergo after working as shield, let us say, during one year? Will it become radioactive or poisonous? What will happen if a human being will drink a gl= ass of that water? What will happen if we water a plant with it? Is it enough to throw it into the sea? Or we must treat it before? Or we must send it to the sun?

We’ll see…<= /o:p>