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Spiral Magnetic Gradient Motor: Axial & Radial Magnets Thomas Valone, PhD, PE Integrity Research Institute Vigier Symposium, Morgan State Univ., November 19, 2014 http://www.NoeticAdvancedStudies.us/index9.html Credit: Tom Schum for this 4” spiral stator construction

Spiral magnet grad radial mags 2014

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Page 1: Spiral magnet grad   radial mags 2014

Spiral Magnetic Gradient

Motor: Axial & Radial Magnets

Thomas Valone, PhD, PE

Integrity Research Institute

Vigier Symposium, Morgan State Univ., November 19, 2014

http://www.NoeticAdvancedStudies.us/index9.html

Credit: Tom

Schum for

this 4” spiral

stator

construction

Page 2: Spiral magnet grad   radial mags 2014

II met Vigier in 2002

at Swiss Weinfelden

conference

sponsored by the Inst.

of New Energy

Technology (INET)

Here Prof. Vigier

shows Lithium-7

and a proton will

yield “more than

400% excess

energy” producing

hydrogen and a

gamma ray

Weinfelden Conference

summary is online

Page 3: Spiral magnet grad   radial mags 2014

Key to Future Energy Sources:

Gradients are the Requisite Means

• Thermal gradient is used for heat pump

• Voltage gradient is used for electrical power

• Gravity gradient is used for hydroelectric power

• Pressure gradient used for natural gas and water

pumping

• Magnetic gradient from inhomogeneous

permanent magnets is used for nothing so far

except in physics labs for experiments

Page 4: Spiral magnet grad   radial mags 2014

Net Force in the

direction of gradient

= the magnetic field

gradient multiplied

by the induced

magnetic moment,

as with the Stern-

Gerlach Experiment

Hartman Patent #4,215,330

Side View

10 degree incline

drop-off

--Modern Physics, Schaumm’s Outline Series, Gautreau et al., McGraw Hill, 1978

Their experimental setup: The magnetic field B is more

intense near the pointed surface at the top than near the flat

surface below, creating a slope in a graph of B vs. z ,

which is the gradient dB/dz.

Steel ball

bearing #4

Top View

Fz

z

Inhomogeneous Magnetic Fields =

Magnetic Gradient

Two experimental examples that utilize the magnetic field gradient

Page 5: Spiral magnet grad   radial mags 2014

Spiral Magnetic Motor (SMM)

Uses the Magnetic Gradient

Popular Science, June 1979

Hartman Patent 4,215,330

d

dBMF cos

dz

dBFZ cos z

In both cases cos Φ is angle between

magnetic moment and B

Page 6: Spiral magnet grad   radial mags 2014

Spiral Magnetic Motor (SMM) Archimedean spiral is used

for SMM stator magnets

where r = 6 + θ/2 and B(r) is

linearly dependent on θ

6”

Creates a constant torque for

more than 75% of each cycle

F = U where U = M ∙ B and

        r rU M B M B

        r rU M B M B

Resultant force is the vector sum of the tangential (θ) and the centripetal (r)

Spring

Latch

overshoot

Page 7: Spiral magnet grad   radial mags 2014

Multi-Stage SMM

Page 8: Spiral magnet grad   radial mags 2014

Three-Six Magnet SMM

Page 9: Spiral magnet grad   radial mags 2014

Mirror Image Impacting SMM

Page 10: Spiral magnet grad   radial mags 2014

SMM Governing Equations

r

BM

B

r

MF rr

Fr

BMT r x

2

21 EU oE

o

B

BU

2

21

For a maximum B field in air of 20 kG

(2 Tesla), UB = 2 MJ/m3 (megajoules)

For a maximum E field in air of

3 MV/m, UE = 40 J/m3

(2,000,000 = 40 X 50,000)

Maximize radial B field (Br) for maximum torque*

0

ENERGY DENSITY CONSIDERATIONS: B-FIELD = 50K x E-FIELD

dTW

*So this paper will include the Radial Magnetic Field models

Page 11: Spiral magnet grad   radial mags 2014

Experimental Results

Six SMM

designs were

tested: 1, 3, 4,

6, 10” rotors

kG

▲ = rotor, ♦ = stator magnetic flux density

Page 12: Spiral magnet grad   radial mags 2014

Spiral Magnetic Motor Angular Velocity

0

2

4

6

8

10

12

14

16

18

0.4 0.8 1.6 2.4 3 3.8 4.6

Angular Displacement (radians)

An

gu

lar

Velo

cit

y (

rad

/sec)

1" rotor

3" rotor

4" rotor

6" rotor

10" rotor

Poly. (4" rotor)

Polynomial Fit

0 90⁰ 180⁰ 270⁰ - - degrees

- - -Data acquisition limit- - -

315° is latch

point

315/360 = 88%

3” rotor

SMM ANGULAR VELOCITY

Page 13: Spiral magnet grad   radial mags 2014

Measuring Back Torque

Ohaus linear force scale +/- 1 N

Page 14: Spiral magnet grad   radial mags 2014

Peak KE, Back Torque, Mass, B-Field

5 Rotors Tested: 1.25”, 3”, 4”, 6”, 10”

10” rotor:

0.80 Joules

Highest KE

Phototransistor detail

Peak Values:

Page 15: Spiral magnet grad   radial mags 2014

-0.5

0

0.5

1

1.5

Angular Displacement (degrees)

10"

Roto

r T

orq

ue (

N-m

)

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

10" R

oto

r P

ote

nti

al E

nerg

y (

J)

0 90 180 270 360

Rotor Torque and Potential Energy for One Cycle

Torque Measurement T=rxF

dTW

Positive

Work

Region

Negative Work Region

315°

Positive work required to

move latched rotor at 315° to

end (starting point) at 360° :

W = 0.52 Joules

which is less than 0.80 J KE

10” rotor tests

88%

Page 16: Spiral magnet grad   radial mags 2014

Prof. Eric Laithwaite’s Suggestion

for Increased Torque

Place metal plate of particular permeability underneath rotor in order to produce:

Favorable Hysteresis Currents

Laithwaite Eric, Propulsion Without Wheels, English Univ. Press, 1970

Page 17: Spiral magnet grad   radial mags 2014

Hysteresis is Lag Response –

Depends on Permeability and

Resistivity*

teH

B

2

81

Designing the Growth of Eddy Currents to Match Rotation Speed

teH

B

2

81 )4/( 2

*Bozorth, Ferromagnetism, J. Wiley & Sons, 2003

ρ = resistivity, µ = permeability, δ = thickness of plate, H field is suddenly applied

Choosing aluminum or copper for example, the permeability will be the same as free

space (µo = 4π × 10-7), which is very low and the resistivity is also low. Choosing an

aluminum plate that is about a centimeter (1 cm) thick would also be a good choice

since the thickness of the sheet "delta" is squared and also in the numerator. Altogether,

the calculation shows a relatively slow build-up over a tenth of a second and only

about 30% at a millisecond after the stator field magnet is applied to the rotating disk,

which is in keeping with a delayed eddy current that would push instead of retard the

changing flux as is normally expected from Lenz’ Law.

Page 18: Spiral magnet grad   radial mags 2014

Wiegand wires are FeCoV bistable

Vicalloy metal with 2 regions

US 1973 patent # 3,757,754

Used for years for auto ignitions

Provides repeatable magnetic pulse

Pop. Science Wiegand causes Barkhausen avalanche of magnetic domain alignment

Page 19: Spiral magnet grad   radial mags 2014

Inverse

magnetostrictive (MS)

effect combined with a

piezoelectric material

(PZT) and voltage

MS-PZT

coil

IEEE Trans on Magnetics, V. 43, N. 8, 2007

Page 20: Spiral magnet grad   radial mags 2014

Switching Actuation for SMM

Piezo actuator can

move ½ lb object

repeatedly with only

voltage from

Smart-Materials.com

0.12 mH ultra-minature

coil inductor is a simple

pulse generator

Page 21: Spiral magnet grad   radial mags 2014

New Radial Magnet Rotor

Dual V-Track Design

Note: former STATOR magnets are now on the ROTOR and a

single pair of magnets are on the movable stator above.

Page 22: Spiral magnet grad   radial mags 2014

Radial V-Track Stator Magnet

Page 23: Spiral magnet grad   radial mags 2014

Conclusion

• SMM designs now provide almost 90%

permanent magnet powered cycle

• Actuation needed for switching magnetic

fields during last 10%

• Many energy harvesting means for

powering actuation now have emerged to

make this long-sought-after goal

achievable

• Details provided in paper