Successful Brushless A.C. Power Extraction From The Faraday Acyclic Generator

Transcription

1 Successful Brushless A.C. Power Extraction Fro The Faraday Acyclic Generator July 11, 21 Volt = volt 1) If we now consider that the voltage is capable of producing current if the ri of the disk is connected to the axis through a suitable load resistance, then current is also a direct function of the rate of rotation, ω. by Jerry E. Bayles The A vector circulates around the B vector in the anner of the flux circulation around a current carrying wire in the standard definition for the right hand rule. I. E., If the right hand thub points in the direction of agnetic flux, then the A vector rotates or circulates in the direction of the curled fingers of the right hand. The right hand rule for the direction of agnetic flux is established as being in the direction of the curled fingers of the right hand when the current flow is in the direction of the thub. This is for the conventional current flow theory where positive charges flow fro a positive terinal to a negative potential terinal. This is the prerequisite for the following two force generations. The next order of action is to establish the right hand three vector generator rule where the thub is force of rotation action F, the index finger is the direction of agnetic flux B and finally the current I is the iddle finger where all three vectors or fingers are 9 degrees to each other. The last order of action is the right hand rule for the generation of axial force that utilizes the thub in the direction of the A vector, the index finger in the direction of force, and finally, the iddle finger in the direction of the sae current as for the agnetic rotational force above. The Faraday equation for the acyclic generator is presented below as equation 1. Let: B := 515 gauss B =.515 tesla R1 :=.125 in R2 := 1. in r:= R2 R1 RPM := 12 f := RPM 6 1 sec 1 f = 2Hz ω := 2 π f Total resistance of the current path is easured to be : R t := oh Then: R2 Volt := ω R1 Br dr Volt I := I = ap R t Note: Another way of looking at the generated current is to consider that the current flows whether a load is connected or not. This by reason that the near space to the surface of the conductive agnetic disk has a current flow fro energy space. In: R2 volt sec A := B dr A = ( ) Note that A is not dependent on the rotation rate. 2) R1 X Y Z X and Y are in the plane of agnetic disk rotation. B field is along the axis of rotation, Z. Note: B volt sec r 2 A sec dr volt r Zero frequency results in zero current as current depends on the circuit path having a source voltage which will be zero at zero Hz. Superconducting agnet surfaces ay yield very large current capability which could allow for significant force to be developed without overheating the agnet surfaces. 3)

2 ABUnits_1.MCD 2 In figure 1 below, the standard generator force vector notation for the right-hand rule (thub, index finger and iddle finger respectively) of F, B, and I for force F, agnetic flux density B, and current I respectively is used. This is for a two disk syste. Case 1: F B1 := B I ( r) F B1 = A) Case 2: F B2 := B I ( r) F B2 = B) The force of action is along the Y direction as referenced to figure 1 below. Fig. 1 Case 1 Case 2 For the A vector, the thub points in the direction of the agnetic flux and the fingers curl in the direction of the circulation of the A vector. The direction of the B flux is fixed regardless of the rotation of the disks since the disks are peranent agnets. A force ay exist as shown iediately below where the cross product of the radial current I and the A vectors produce an axial force F. The generator ode is shown with a short circuit load. Case 1: F A1 := I A F A1 = A) Case 2: F A2 := I A F A2 = B)

3 3 Fig. #2 Case 1 Case 2 +A eans clockwise as viewed fro the left to the right along the Z axis of rotation. The net vector force along the Z axis adds. Force in the AFI pictorial is action force. This is 9 degrees to the action force involving the generator ters FBI shown in Fig. 1 above. The AFI ters are derived fro the FBI action vectors which ust occur first. It is obvious that having both agnetic disks aiding in their B fields will cause a net force to the right. The A vector follows the rotation direction for this case. Equation 5, case 1 and 2 is shown in fig. 2 above pictorially. Using the right-hand generator rule, a new sequence is generated by using A, F, and I as thub, index and iddle finger respectively. The force (F) nexus occurs at the intersection of the (A) vector and the current (I) vector and is 9 degrees to to both since all of the vectors are 9 degrees to each other. The voltage appears evenly around the ri of the disk and is easured fro R2 to R1. It is obvious that the voltage increases in direct proportion to the rate of rotation ω. B and A agnitudes are independent of the rate or direction of rotation of the agnetic disk. R2 vel1 := ω dr R1 W B1 := W B1 S B1 := λ1 2 P B := F B1 ( ω r ) W B1 λ1 2 vel1 vel1 = sec -1 W B1 = S B1 = P B = watt watt Also: ω r = sec -1 vel1 λ1 := f λ1 = Wavelength reains constant with a change of rotation frequency. The Poynting vector power S B1 as well as the regular power P B are radiated radially fro the axis of rotation of the agnets as will be explained below. This is related to the B field force above. 6) 7) 8) 9) E := vel1 B E = volt E increases in direct proportion to the disk frequency. 1)

4 4 The above syste is based on a variable pereability space-tie if it is copared to free space. The above syste is not in our ordinary space-tie as a result. An increase of rotation frequency induces greater energy and thus power fro energy space. The result is propulsion which can be used in deep space and therefore releases us fro the gravitational chains of our Earth. Electroagnetic Poynting vector equations for free space radiation power per eter squared is shown below and yields results that are uch greater than the above calculation S B1. c := sec µ o 4 π henry := S rad := EB 2 µ o P c := S rad c 1 S rad = watt 2 P c = Note: E is in the X and Y plane and points radially fro the Z axis. B points along the Z axis. Any vector chosen arbitrarily in the X-Y, (E vector plane), taken as a cross- product of the B vector will produce a pressure vector outwards 9 degrees fro the Z axis and 9 degrees to the E and B vectors. 11) 12) The above suggests that a relative pereability ay be solved for to reconcile the velocity of free space c to the vel paraeter of the two disk agnetic syste of figures 1 and 2 above. Let: S B1 = EB 2 µ r µ o Then: EB µ r := S B1 2 µ o µ r = ) S := EB 2 µ r µ o S = watt Ck: (o.k.) Relative pereability decreases with an increase of rotation frequency. It can even be less than unity. 14) S above is now equal to the result in eq. 8 above for the two disk agnetic rotating syste. S B1 = watt 16) For the radial pressure discussed above: P rad := E B 1 2µ r µ o vel P rad = 17) Note that the outwards pressure is 9 degrees to the axis of rotation. It is in the XY plane of the agnetic disk rotation

5 5 The following interesting relationships exists: ( ) µ o µ r I 2 F fund := F fund = finally, 2 π 2 F fund = 1 F B1 18) The pereability of space ties current equals the A vector and the A vector ties current again is force. ( µ r ) µ o I 2 π 2 = volt sec ( µ r ) µ o I 2 2 π 2 = ) The inductance and capacitance for resonance of the above syste related to the disk circuference is: ( ) µ o L := µ r 2 π r L = H (Millihenry) 2) C := 1 C = µf (Microfarad) 21) 4 π 2 f 2 L Check: 1 f r := f r = 2 Hz (o.k.) 2 π LC 22) The current derived fro rotation ties the pereability of free space yields an A vector uch less than in equation 2 above. Let: µ o 4 π henry := Then: A µo := µ o I A µo volt sec = 23) This inor A vector is inline with the current I in deference to the ajor A vector generated around the B vector. Further, both are 9 degrees to each other. Then there is not a cross product force associated with the inor A vector. Relative pereability is: A µ Ar := µ Ar = Relative pereability increase due to I. 24) A µo Finally: µ r µ Ar 2 π 2 = 1 25)

6 6 Tests show a resonance of an aeter needle as well as a uch ore assive pair of peranent agnets ounted on a swivel arrangeent as in the below pictures in figures 3 and 4. Both ove vigorously at near the Schuan frequency and a definite force can be felt by the finger tips when attepting to stop the vibration of the swivel agnet arrangeent. Since the ain disk agnets are nearly unifor in the diaeter and thus agnetic field, there would not be expected such a powerful oscillation under noral circustances. Perhaps a field is being radiated that is free energy at near the Schuann frequency. With that in ind, the following atheatical analysis is presented. Fig. 3 Fig. 4 North Side Magnetic Balance South Side Magnetic Balance In the above figures, the brush contacts are dropped below the disk agnets and are thus out of the easureent. f Schu := 8Hz Known epirically established Schuann frequency. λ2 := 2 π R2 λ2 = (All λ's are constant.) 26) λ := λ2 λ1 λ = f Schu ( λ) = sec -1 Note: 1 λ = in 1 and 4 π = ) ( = square root of the Golden Ratio.) f Schu ( λ) λ2 = 1Hz One (1) hertz is one 1/1second and therefore the expression at the left at 8 Hz is hidden in all frequencies. Any frequency other than 8 Hz will not yield the exact one hertz or second. A resonance at 2π Hz and 8. Hz occurs during testing. At the 2π Hz resonance, the entire test bed vibrates and at 8. Hz, the balance agnets in figures 3 and 4 swing back and forth violently. The eter also vibrates and sees to follow the action of the balance agnets. Further, the static alignent of the balance agnets reain relatively still as shown if the disks are rotated slowly by hand. Due to the alignents being 9 degrees out fro one side of the disks to the other, it is postulated that there is soe sort of active standing quarter wave across the disks even when they are not being rotated. Further, it is locked into an geographical North-South alignent for this setup. The North-South alignent ay not be ore than coincidence but the standing wave is locked into the above alignent. When the disks are spun, the standing wave is force to degenerate and radiate. This radiated field power has been easured and the results are encouraging. This eans that no contacts are needed on the Faraday disk to extract power under the above setup conditions.

7 7 The hidden frequency constant above is coparable to the hidden force in y electrogravitational equation that is also a constant and since it is a constant it does not show up in the output force that is a variable. The electrogravitational equation is shown below and a full explanation is presented on y web site at Fig. 5 A cylindrical outwards slow oving field of agnetic radiation at the Schuan frequency ay be fored by the cross product of the agnetic Z axis B field and the velocity vel1 in the X and Y axis. vel S Schu := vel1 S Schu B Tesla ties velocity indicates a agnetic field in linear otion. = sec -1 tesla This resonates and induces free 28) Schuann frequency energy at 8 Hz. The units also can be expressed in volts/eter. I suggest that the two fors can alternate with distance in a longitudinal anner. In that case, the field can act not only on other agnetic fields but also electrically charged objects. Even neutral field ass ay be acted on since another unit for is per coulob which involves ass ties acceleration over charge. The two disks are aligned with fields aiding and nearly perfectly unifor in the radius of rotation. That being so, the fields can be expected to show little non-unifority around the axis of rotation for a given radius to the circuference. It is found by epirical tests however that when the disks are rotated, an electroagnetic field is radiated in proportion to speed. Thus equations 1 through 17 above are substantiated by actual easureent. The increase in current and voltage in the pickup coil(s) are close to equal regardless of whether the core is iron or air. Equation 1 above shows that the E field will increase as the disk rotation velocity increases and this is easured to be the case. This suggests that there is a current and potential in the radiated field and as a result the field changes in aplitude with distance and tie but in a longitudinal fashion? Whence the variation in the field around the disks? Perhaps a standing wave between the disks exists and also around the disks when they are standing still. Two identical sall agnets ounted on a rotor free to ove on a low friction point of balance is brought to the sides of the agnet disks and if placed on the near side, the balanced agnet indicator lines up parallel to the axis of the disks. If however the balanced indicator agnets are placed on the far opposite side, the balance agnets line up towards the axis and between the disks! Since the disks are uniforly agnetized and unifor radially fro the axis, this is ost unexpected. If the disks are slowly oved in rotation, the sae results are obtained. Is there a standing wave fixed around the agnets? Further tests reveal that free fro any contacts, the near side balance test oscillates the test agnet balance the ost at 8.3 Hz and the far side position oscillates at 6.28 Hz. Also, at 6.28 Hz, the entire support for the agnet disk rotors and drill otor is observed to shake vigorously with a sharp resonance point at 6.28 Hz. If we divide 8 Hz by 4/ π we will arrive at 2π exactly. (See eq. 28 above for relevance.)

8 Below is the pickup coil that was used to extract the field energy fro the spinning quarter wave resonant Faraday disk generator as described above. Fig. 5 8 It is interesting that 2π ultiplied by the sexagesial nuber 6 yields a nuber that in agnitude is extreely close to the free space resistance of ohs. Divide this by 2 and then divide again by the fine structure constant α and we arrive at the quantu oh. Then it is possible that the disks are acting as a quantu energy space to free space energy transforer using resonant standing waves? Results are for botto coil 12 RPM. D.C. coil resistance: Max. current: Open circuit voltage: 6.7 oh 68 A v pp.68 v rs, 2. v pp With both lower and upper coils in series, the resistance was: 19.7 oh. The current was 38 A a.c. and the voltage was.812 v rs, 2.5 v pp. It is obvious that a lower resistance aids in the current generation by alost doubling the current while the voltage drops to only 2/3 that of the double coil pickup arrangeent. A superconducting pickup coil ay deliver large quantities of current, especially if the agnet surfaces are also superconductors. Below is a preliinary setup for deterining the brush current utilizing copper braid. This is no longer needed! Fig. 6 Disk agnets are shown with brushes attached. This is an early test where the disks are ounted with opposing fields to build the output voltage in series fashion. This was prior to discovery of the standing wave phenoena around the disks as described above. The output axiu was about 3 aps d.c. at 12 RPM. The connecting shaft is coon to both disks electrically and echanically.

9 Conclusion: It ay be serendipitous that the diensions of the agnets used develop a standing wave that yield the properties of being related to the golden ratio as shown in equations 26 and 27 on page 6 above. 9 The reader ay be interested in duplicating the above siple test arrangeent. If so, the agnets can be purchased fro: These are very strong agnets and therefore great care should be exercised in the handling of the. Use wood and brass claps, etc. Help on the construction details of the above apparatus will be provided as needed or requested. Researched and tested by: Jerry E. Bayles jebayles21@yahoo.co ElectrogravityWorks July 11, 21