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Overunity Machines Forum



STEORN DEMO LIVE & STREAM in Dublin, December 15th, 10 AM

Started by PaulLowrance, December 04, 2009, 09:13:07 AM

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Omnibus

Stefan,

It would be interesting and pretty straightforward to see the input VI product integrated over a certain period and compare it with the output VI product integrated for the same period. This they can do as we speak with this kind of oscilloscope. As for calorimetry, they can use a Seebeck calorimeter which at their level of funding they can acquire or rent without a problem. These are mostly games they are playing and that's because of investors involved, a company that has to be run and many other factors in the corporate world. In a way I can understand them seeing all this negativity, envy and sheer animosity directed at Steorn, aside from what the corporate world requires.

PaulLowrance

If the energy comes from ambient, then the calorimetry method might not work.

Omnibus

Quote from: PaulLowrance on December 23, 2009, 11:50:14 AM
If the energy comes from ambient, then the calorimetry method might not work.

Calorimeter will help to determine the energy balance. It will be equally as curious if there's a disbalance as deficiency (anti-OU) -- energy will be destroyed. Don't think that's the case, though.

gravityblock

This is a long post and I hope it is a good read.  Permeability is the magnetic conductivity of a material.  A higher permeable core will have a greater attraction for the rotor magnets than a low permeable core (I hope I got this right).

Now let's take a look at the "Expanding Field Model".  Let's assume a new flux-line begins as an infinitesimal small loop around the primary-wire. Since loops can not overlap or cross, this new loop must physically displace pre-existing loops outward when it is created.  Therefore magnetic fields must expand from, or contract to, the source wire.  This expanding field method is the only way that a magnetic field can expand (or contract) without violating Ampere’s Circuital Law.

In classical electromagnetic theory, it is common to talk about expanding and collapsing magnetic fields; however, this phenomenon is only addressed in the following simplistic terms: When the current is large, the magnetic field is large; when the current is small, the field is small. Classical electromagnetism does not discuss the manner in which a field expands, or contracts. The mechanism of field expansion and collapse is the concept for the Expanding Field Model. This model shows that flux expands and contracts through free-space with an actual real velocity which depends upon a number of factors.

To illustrate the expanding flux method, consider Figure 1 below showing the toroidal system at steady state. In this diagram, only one turn of the primary is shown for simplicity. The primary winding is shown relatively far away from the core for the purpose of examining the behavior of the flux near the primary. Since Ampere’s Circuital Law must not be violated, there must be flux between the primary-wire and the core as represented by the violet/thick flux-loop.  Each flux-loop is shown as a different color to aid in the discussion.  “Thicker” loops indicate higher magnetic field intensity (flux-lines/area).

We begin by considering the system prior to the increase in primary current as shown in Figure 1.  At this moment, there is a constant current in the primary which is responsible for the steady state magnetic field represented by flux-loops engaged by the core (blue/thin) and flux-loops near the primary which have not touched the core (violet/thick).  "G" is the secondary.

When the primary current increases in Figure 2, new flux-loops (red/thick) are created near the primary-wire which then displace the violet flux-loops out. As the violet flux-lines displace, they expand in perimeter which causes their intensity to decrease (represented by the diminished line thickness of the violet loop). When the flux-line expands to the point where it touches the core, the “engagement” process begins. The “engagement” process continues as the remainder of the flux-loop is drawn into the core.  The black arrows in the diagram represent the flux velocity.
                                                                       
In the engagement process, the right violet loop (inside the core) simply expands across the center as shown in Figure 2. Since, the left violet loop can not pass through other loops, it must therefore swing around the primary to the left or right (like a door slamming shut). When steady state is achieved, the violet flux-loops are completely engaged by the core (we are assuming an ideal core).

This method preserves the integrity of the classical flux model and Ampere’s Circuital Law; however, it shows that the flux-lines “cut” the secondary on their journey to engage the core.

The permeability of the core affects the number of flux lines that will pass into the space contained by the secondary when the primary current increases.  It is not hard to see that with increased core permeability, more flux-lines pass into the interior of the secondary for any given increase in primary current.

I hope this is helpful in replicating a Lenz free motor or even a motionless OU Generator.


GB
Insanity is doing the same thing over and over again, and expecting a different result.

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