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THE SmartPAK POD

NEAR-UNITY DEVICE

B

μoH

 

 

 

L1

 

I

 

 

 

 

 

 

 

 

2.5mH

+

 

S

 

N

FERRITE

S

N

 

RODS

 

 

 

 

 

 

MAG1

 

-

 

MAG2

 

 

 

 

 

MAG3

 

 

+

MAG4

N

 

S

FERRITE

N

S

 

RODS

 

 

 

 

 

-L2

I 2.5mH

μoH

B

NOTE 1:

μoH: Produced by coil L1 and L2.

B: Produced by magnet MAG1 - MAG4.

L1 and L2 use 50ft of 16AWG magnet wire each. C-Core: METGLAS, AMCC-500.

MAG1 - 4 are NIB type magnets.

METGLAS

C-CORE

ELECTRICAL DIAGRAM

The SmartPAK POD is classified as a CATEGORY 2 Near-Unity Device. The coil L1 and L2 fields are mutually coupled to the ferrite rods' magnetic domains, which are magnetized in an opposing direction by permanent magnets.

(c) INTALEK, INC., 2002

11

THE NEAR-UNITY MODEL

OF THE SmartPAK POD

With switch S1 closed, the current (iBAT1 ) flows from the source battery (BAT1) and magnetizes coil L.

This action transfers or discharges energy from the source battery (BAT1) and stores it in L.

 

 

 

+

 

 

Source

iBAT1

vL

 

iBAT2 = 0

Load

Dipole

L

Dipole

(BAT1)

 

 

 

 

(BAT2)

 

 

 

-

 

 

 

S1

 

 

D1

 

t<0

MAGNETIZATION PHASE OF CYCLE

When switch S1 opens, the voltage (vL) across the coil L reverses (Lenz's Law) and the energy stored in

L flows out as a high-current impulse (iBAT2). Energy is transferred from L to the load battery (BAT2).

-

Source

iBAT1 = 0

vL

L

iBAT2

Load

Dipole

Dipole

(BAT1)

 

 

 

 

(BAT2)

 

 

 

+

 

 

 

S1

 

 

D1

 

t ³ 0

DEMAGNETIZATION PHASE OF CYCLE

(c) INTALEK, INC., 2002

12

THE ENERGETICS OF

FERROMAGNETISM

EXTERNAL

PERMANENT

COIL

MAGNET

IC

 

IM

+

N

+

V

LC LM

A

-

S

-

POLARIZED

FERROMAGNETIC

MATERIAL

CLASSIC TRANSFORMER ANALYSIS

The total field energy of the system is,

ESYS = EM + EC - EMUTUAL

1

where,

ESYS is total field energy.

EM is energy of permanent magnet (pm). EC is energy of coil.

EMUTUAL is mutual energy between coil and ferromagnetic core coupled to a pm.

(c) INTALEK, INC., 2002

13

2 LC. For classic

Differentiating ESYS with respect to time is the total instantaneous power, PSYS or,

ESYS = PSYS

2

Because EM is conserved and does NOT change over time,

EM = PM = LM IM IM = 0 Watts

3

Now, rewriting PSYS,

PSYS = PC - PMUTUAL

4

So,

P

SYS

= L I

C

I

C

+ I

C

2 L - M I

M

I

C

5

 

C

 

 

C

 

 

 

 

FLUX

 

PARAMETRIC

 

 

 

 

 

 

COUPLING COUPLING

 

 

 

 

 

 

TERM

 

 

TERM

 

 

 

 

 

 

 

 

 

 

PC

 

PMUTUAL

 

Now, of particular interest is LC of IC

CATEGORY 1 Under-Unity devices,

LC = 0 Ω

6

(c) INTALEK, INC., 2002

14

However, by "strategically" polarizing the ferromagnetic material, this increases the permeability μ, and increases the inductance LC. This reveals the "hidden" mechanism that makes these CATEGORY 3 Over-Unity devices,

LC ¹ 0 Ω

7

Since the coil dissipates power, the instantaneous power PSYS equates to,

P

SYS

= R I

2 + L I

C

I

C

+ I

2 L - M I

M

I

C

8

 

C

C

 

C

C

 

 

Since LC has the same units as resistance Ω, this resistance may be positive or negative depending upon the slope of LC. For example, if LC is "engineered" to be positive, then the power is positive, however, if LC is "engineered" to be negative, then the power is negative.

So, integrating PSYS with respect to time is the total energy, ESYS or,

ESYS = ò PSYS dt

9

In conclusion, given special operating conditions, the ferromagnetic domain can serve as a "hidden" source of energy simply by mutually coupling it to a coil. The energy is in the form of excess electrical energy, and the domains transforms this energy from the ambient thermal environment. This causes an observable cooling effect in the domains.

(c) INTALEK, INC., 2002

15

THE FREE ENERGY "Alek Effect"

(B)

 

DENSITY

B-H CURVE

 

PERMEABILITY and FLUX

PERMEABILITY (μ)

 

 

MAGNETIZING FORCE (H)

NORMAL VARIATION OF μ ALONG MAGNETIZATION CURVE

DENSITY (B)

 

FLUX

MODIFIED PERMEABILITY (μm)

and

(CAUSED BY ELECTROSTRICTION /

MAGNETOSTRICTION OF IRON

 

PERMEABILITY

ALLOY CORE)

COMPONENT DUE TO

 

B-H CURVE IS SHIFTED LEFT

 

EXCESS FREE ENERGY

 

INITIAL MAGNETIZATION

MAGNETIZING FORCE (H)

MODIFIED VARIATION OF μ ALONG MAGNETIZATION CURVE

(c) INTALEK, INC., 2002

16

DYNAMIC B-H LOOP TEST FIXTURE

POWER

10K

"POD" HEAD

OSCILLATOR

 

ASSEMBLY

(SQUARE WAVE)

0.7uf

UNDER TEST

 

 

CURRENT

PROBE

P6042

HORIZ

VERT

SCOPE GND

Engineering LC will shift the BH curve either left or right.

(c) INTALEK, INC., 2002

17

The SmartPAK ZPOD

OVER-UNITY DEVICE

D1

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

n x LSEC

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

+

 

LSEC1

 

 

LSEC2

 

 

LSEC3

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

H

T1

H

T2

H

T3

o

1:1

o

1:1

o

1:1

μ

μ

μ

 

 

 

+

LPRI2

LPRI3

LPRI1

 

 

LPRI

 

 

n

LSECn

-

H

Tn

o

1:1

μ

 

 

-

 

LPRIn

SECONDARIES WIRED IN SERIES

PRIMARIES WIRED IN PARALLEL

ELECTRICAL DIAGRAM

T h e S m a r t P A K Z P O D i s c o n s i d e r e d t o b e a Thompson-Plank PERPETUAL MOTION MACHINE, and is classified as a CATEGORY 3A Over-Unity Device.

(c) INTALEK, INC., 2002

18

THE OVER-UNITY MODEL

OF THE SmartPAK ZPOD

With switch S1 closed, the current (iBAT1 ) flows from the source battery (BAT1) and magnetizes coil L0.

This action transfers or discharges energy from the source battery (BAT1) and stores it in L0.

 

 

 

+

 

 

Source

iBAT1

vL0

 

iBAT2 = 0

Load

Battery

L0

Battery

(BAT1)

 

 

 

 

(BAT2)

 

 

 

-

 

 

 

S1

 

 

D1

 

t<0

MAGNETIZATION PHASE OF CYCLE

When switch S1 opens, the voltage (vL) across the coil L reverses (Lenz's Law) and the energy stored in L (increased permeability μ, of L0) flows out as a high-current impulse (iB A T 2 ). Excess energy is transferred from L to the load battery (BAT2).

-

Source

iBAT1 = 0

vL

 

iBAT2

Load

Battery

L

Battery

(BAT1)

 

 

 

 

(BAT2)

 

 

 

+

 

 

 

S1

 

 

D1

 

t ³ 0

DEMAGNETIZATION PHASE OF CYCLE

(c) INTALEK, INC., 2002

19

THE MAGNETIZATION / DEMAGNETIZATION CYCLE

+

μoH

+

T1

LPRI1

LSEC1

 

1:1

 

μoH

 

LPRI2

T2

LSEC2

 

1:1

LPRI

μoH

HIGH

n

T3

VOLTAGE

LPRI3

LSEC3

 

1:1

 

μoH

 

LPRIn

Tn

LSECn

-

1:1

 

-

iMAG

 

 

 

MAGNETIZATION PHASE OF CYCLE

-

μoH

-

D1

 

T1

 

LPRI1

LSEC1

 

 

1:1

 

 

μoH

 

LPRI2

T2

LSEC2

 

1:1

L

PRI

'

μoH

n x LSEC'

 

n

 

 

 

LPRI3

T3

 

 

 

LSEC3

 

 

 

1:1

HIGH

CURRENT

 

μoH

 

LPRIn

Tn

LSECn

+

1:1

 

+

iDEMAG

 

 

 

DEMAGNETIZATION PHASE OF CYCLE

Excess electrical energy is released from the device d u r i n g t h e d e m a g n e t i z a t i o n p h a s e o f a magnetization/demagnetization cycle . A s a consequence of releasing this excess electrical energy, the device transforms it from the ambient thermal environment, thereby cooling itself.

(c) INTALEK, INC., 2002

20

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