LEVITATION USING STATIC MAGNETIC FIELDS
LEVITATION USING STATIC MAGNETIC FIELDS
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SPACE PROPULSION USING EARTH'S MAGNETIC FIELD
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---- Other Methods of Levitation and Propulsion ----
GRAVITY CONTROL AND
WARP DRIVE FOR SPACE TRAVEL
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AERODYNAMIC
LIFT ANALYSIS OF AN ENCLOSED-FLOW
HALF-DUCT
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Copyright © 1999-2010 John Cipolla/AeroRocket. All rights
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LEVITATION USING STATIC MAGNETIC FIELDS
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A
levitation device based on the use of several
ceramic magnets has been developed to demonstrate that
levitation can be achieved using a single thread
to vertically secure a levitated magnetic device from below while the
levitated magnetic device is also being supported from below using the mutual
repulsion of opposing magnetic fields.
It is simple to achieve levitation using a
single thread to secure a levitated magnetic
device from
below while it
is also being supported from above using another
magnet of opposite polarity. However, using a
single thread to vertically secure a levitated magnetic
device from
below while the levitated magnetic device is also being
supported from below requires the levitated device
to
be located in a uniform magnetic field of
opposing polarity. In the design presented below the
bottom-mounted thread is used to "pull" the
levitated upper magnet into the potential well of
the support magnetic field located below. If the
levitated magnetic device drifts into the negative curvature
portion of the support magnetic field the levitated
magnetic device will tip over and become unstable. The split
design of the support
magnetic field device provides a larger potential
well for the levitated magnetic device resulting in greater
overall stability.
To assure the levitated magnetic device is located in the
potential well of the support magnetic field a mechanism to position
the thread support-point relative to the center of
the split support magnets is illustrated below. The upper
Plexiglas plate is positioned and secured
using two cap screws until the levitated magnetic
device
is centered and stable. In this configuration the
levitated magnetic device is stable and will not crash even while carrying the system from
place to place.
Levitation without the physical constraint of a
bottom-mounted thread is possible if the levitated
magnetic device is allowed to rotate like a top and if the proper amount
of ballast or weight is added. The precession or
gyroscopic action of the spinning magnetic device provides sufficient flipping resistance (torque) to prevent
the top from overturning and aligning north to south
with the base magnet. Also, the ballast acts to push
the top into the potential well of the support
magnet where the magnetic lines of force are
optimum. As an example of this technology the Levitron
Anti-Gravity Top
achieves levitation without external constraint by using gyroscopic
precession to counter the torque engendered by
opposing magnetic fields and weight adjustments for optimum vertical top
placement within the support magnetic field. However, gyroscopic levitation is a
challenge to achieve and difficult to maintain
because of temperature related effects on
magnetic field strength. A totally new product
called the Levitron
Anti-Gravity
Globe overcomes the Earnshaw theorem constraint
problem by using an
electronically controlled electromagnet to properly
position the levitated object within the support
magnetic field but time varying magnetic fields not
static magnetic fields are used to achieve
levitation. The electronic kit provided by this link
shows how levitation is achieved using a linear
Hall effect sensor combined with an electromagnet to
levitate a very small device containing one or more rare
earth magnets. However, this article admits the
technology is not scalable to larger sizes.
The object of this work is to remove as
many constraints (degrees of freedom) as possible
from the levitating magnetic device without violating Earnshaw's theorem.
Earnshaw's theorem states
that no static arrangements of magnetic or electric
charges can be stable, alone or under gravity. More
information on the use of static magnetic fields to
achieve levitation using a minimum number of
constraints will be posted here as work
continues... |

Figure-1: Side view of the levitated
device

Figure-2: Slightly elevated view of the levitated device

Figure-3: Oblique angle view of the levitated device

Figure-4: Bottom view of the levitated device without "flying
saucer"

Figure-5: Oblique angle view of the levitated device without
"flying saucer"

Figure-6: Levitation device illuminated in the dark
Illumination uses a MagLight and inside-mounted 3/8" diagonal
mirror
REFERENCES
Levitron Anti-Gravity Top
Levitron AG Anti-Gravity Globe
Electronic Magnetic Levitation Kit
Diamagnetic Levitation
Magnetic Levitation Cradle
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SPACE
PROPULSION USING EARTH'S MAGNETIC FIELD
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A magnetic field as quantified by the
magnetic field part of the Lorentz equation
exerts a sideways force on electrons moving in a wire.
The magnitude of the magnetic field deflecting force
F, is given by F = i L X B. The relationship
between vectors in this equation is illustrated in Figure-7
and Figure-8 using the rules for vector products. The
deflection force F, being at right angles to the
plane formed by i and B, will always be at
right angles to i and to B. In the
Lorentz equation i is the direction of positive
charges moving in the wire which means electrons drift
in the opposite direction. In addition, B is the
magnetic field vector surrounding the wire and L
is the vector defining the length and direction of the
current carrying wire. Units for B, the magnetic
field vector, is given the special name tesla or
more commonly, weber/meter^2.
Where, 1 Tesla = 10,000 Gauss.
As a means for space propulsion the magnetic field
vector B is replaced by the Earth's magnetic
field which normally ranges from 0.3 to 0.6 Gauss
and averages 0.57 Gauss.
Applying the Lorentz equation the force F
exerted on the spacecraft depends on the length, number
and current carrying capacity of a bundle of
cryogenically cooled conductors. |

Figure-7: Magnetic field part of the Lorentz equation


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Figure-8:
Lorentz equation used for space propulsion in
vicinity of Earth's magnetic field. This image
illustrates the relationship between the Earth's
magnetic field B, force generated F,
conductor current i and conductor
length/direction, L |
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LORENTZ FORCE
DEMONSTRATION
For this
experiment the Earth's magnetic field was replaced
by the uniform magnetic field between two ceramic magnets.
The effective length of current carrying wire between
the ceramic magnets is approximately 1.25 inches. The remaining
length of conductor on the 18 inch long Plexiglas
support goes unused because it is not immersed in a
magnetic field. Power is supplied by four C cells for a
total voltage of 6V. When power is switched "ON" a
mass reduction of 0.8 grams was repeatedly measured
using an Ohaus scale meaning a force of 784.5 dynes was
applied to the conductor. |

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Figure-9:
Experiment where current carrying wire (positive charges
travel from right to left) is placed in a magnetic field
generated by two ceramic magnets |

Figure-10: Current not flowing. Lorentz force on wire is 0.0
dynes

Figure-11: Current flowing. Lorentz force on wire is 784.5 dynes
(0.8 grams)

Figure-12: Animation of upward wire deflection by Lorentz force, F = i L X B
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COMING: DEFLECTION FORCE
MEASUREMENT OF CRYOGENICALLY COOLED CONDUCTORS USING THE
EARTH'S MAGNETIC FIELD FOR SPACE PROPULSION
DEMONSTRATION |
REFERENCES
Magnets (WIKIPEDIA)
Magnetic Fields (GSU)
Earth's Magnetic Field (WIKIPEDIA)
Magnetic Field of the Earth (GSU)
Earth's Inconsistent Magnetic Field (NASA)
The world's First Flying Saucer Made Right Here on Earth: A
University of Florida researcher has plans on the drawing board
for a flying saucer-shaped aircraft that turns the surrounding
air into fuel
Fundamentals of Physics, Halliday and Resnick, 7th Edition
(Text Book)
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