– Clip 1 Radiant Energy, Part 1 – Clip 2 Magnetic Shielding diagram – Clip 3 Magnetic Shielding – Clip 4 Test Parameters – Clip 5 Test Equipment Part 1 – Clip 6 Components and Equipment – Clip 7 Front Motor with Sensor – Clip 8 Back Motor and electronics – Clip 9 Demonstrate Magnetic Shielding – Clip 10 Measure Battery Voltage – Clip 11 Calculations 1, base measurements – Clip 12 First Run of the Motor – Clip 13 Calculations 2 – Clip 14 FreeWheel diode integration diagram – Clip 15 Demonstrate FreeWheel diode – Clip 16 Calculation FreeWheel diode – Clip 17 Demonstrate Runtime Capacitor – Clip 18 Calculations Runtime Capacitor – Clip 19 Reference – Clip 20 End of Part 1

Clip 1

Clip 1

This video is the kickoff of the Radiant Energy projects. Magnetic shielding versus magnetic repulsion. Here in the first part I give an introduction to Magnetic shielding.

Clip 2

Clip2

Magnetic Shielding diagram

A current is induced into a coil around a torroid.
Any magnetic fields, including from a permanent
magnet is deflected without feedback. The coil
appears to be invisible. The energy required to
deflect is less than the attraction force of energy
of the magnet. There is a net force gain which
can be harnessed as kinetic energy.

Clip 3

Clip 3

Magnetic Shielding

– Outline the functions and parameters of the magnetic motor.
– Investigate the functions of the Back EMF
– Apply industrial standards to suppress back EMF

Clip 4

Clip 4

Test Parameters:

1. Voltage source is a battery with 12 Volt and 8 AH
2. A Snubber diode 1N4007
4. Run time capacitor 6.3 uF, 450 Volt
6. Magnetic motor with 2kg or 4 pound rotor
7. Four Nanocrystalline cores for toroids as stators

Clip 5

Clip 5

Test Equipment Part1

Tools

– Keithley 2110 Bench 5.5 Digital Multimeter
– Agilent InfiniiVision 7000 Series oscilloscope MSO7014B
– Optical Digital handheld Tachometer
– UNI-T UT203 Current Digital Clamp Meter

Clip 6

Clip 6

Here I explain each equipment and component. The equipment is listed in the previous clip above. The components in Clip 4.

Clip 7

Clip 7

This is the view of the front of the motor. I have 8 sets of permanent magnets with north and south polarisation. The stator contains the toroid to deflect the magnetic field. On the bottom is the optical sensor. I contains the led as well to be reflected and received by the transistor. On the current setup I use 4 stators.

Clip 8

Clip 8

Here hyou sett the back of the motor with the wiring exposed and connected in series. On the bottom is the control circuitry.

Clip 9

Clip 9

I demonstrate the function of the magnetic shielding. I use a ring magnet which has each side polarised to north and south pole. The toroid is surrounded by magnet wire.  Once energized a circular field is created which deflects and magnetic field in a way that it is not reflected back to the magnet. That is important and is the difference to magnetic repulsion or attraction.

Clip 10

Clip 10

My first test is to measure the battery charge level. I take this value and add it to the formula for my calculation.

Clip 11

Clip 11

V = 13.023 Volt
R = 3.784 Ohm

I = V/R = 13.023 Volt / 3.784 Ohm =  3.443 A. This value is for direct loading from the battery. (Initial maximum value at power up)

Power,  P= V * I = 13.023 Volt * 3.443 A = 44.82 Watt

Clip 12

Clip 12

Now I start the motor and take base measurements for my calculations. I take 12.7 Volt and register the frequency between 75-80 Hz. I measure the current with 0.684 A and the RPM with 574. The back EMF is good to see. Focus on the orange Y1 in the bottom right corner when I use the cursor to mark the base voltage. It does show the 12.7 volt level. Up to 60-70 Volt amplitude is the back EMF.

Clip 13

Clip 13

V = 12.7 Volt
R = 3.784 Ohm

I = V/R = 12.7/3.784 =  3.36 A (initial load)

Measured Current = 0.684 A

P = V * I = 12.7 Volt * 0.684 A = 8.2 Watt

Measured RPM = 574

Calculated RPM based on Frequency 70 – 80 Hz

77 Hz / 8 Magnets * 60 Seconds = 578 RPM

Clip 14

Clip 14

As industrial standard is displayed the function of the FreeWheel diode. The orientation is opposite the polarisation that only the positive back EMF is shunted to the coil but not the polarity of the battery.

Clip 15

Clip 15

I demonstrate now the action of the FreeWheel diode in the circuit. Observer the wave form on the oscilloscope. It will change it into a square wave which is within the voltage level of the source power. The downside is that it has a performance impact which I consider unacceptable. there are better ways to deal with it which I will show in later videos.

Clip 16

Clip 16

E = 12.330 Volt
I = 0.768 A

P = I*E = 0.768 A * 12.330 Volt  =  9.45 Watt

Measured RPM =  561

Including the Snubber Diode

E = 12.288 Volt
I = 0.789 A

P = I*E = 0.789 A * 12.288 Volt  =  9.70 Watt

Measured RPM =  507

Efficiency

Increase of 0.25 Watt and reduction of efficiency by 9.6%

Clip 17

Clip 17

We replace now the FreeWheel diode with a Runtime capacitor. Observer the waveform. It decreases the voltage of the back EMF and stretches the peak voltage longer. We end up with only one wave per cycle which is a combination of the base voltage and the back emf. This does lead to an increased RPM but also to a higher current draw. We also notice a second short spike between the square waves.

Clip 18

Clip 18

V = 12.37 Volt
R = 3.784 Ohm

I = V/R = 12.37/3.784 =  3.27 A (initial load)

Measured Current = 0.684 A

P = V * I = 12.37 Volt * 0.770 A = 9.52 Watt

Measured RPM = 560

Values under Run Time Capacitor with 6.3 uF and 450 Volt

Measured RPM = 575 RPM
Current = 0.849 A
P = V * I = 12.37 Volt * 0.849 A = 10.5 Watt
Increase of power consumption of 9.4 %
Increase of RPM by 2.7%

Clip 19

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Clip 19

Reference

Steorn Orbo design and the delayed magentic field propagation
http://www.steorn.com/orbo/

Professor Dr. Claus W. Turtur the Zero Point Energy
http://wiki.vorticesdynamics.com/researchers/#S

Clip 20

Clip 20

This is the END of Part 1

Introduction to Magnetic Shielding

Upcoming:

  • Harnessing the excess energy
  • Increasing the EMF spikes by reducing the input power
  • Magnetic resonance as in QEG
  • Improved performance and configuration  compared to the Bedini circuit

clip 21