Patent Publication Number: US-2023137951-A1

Title: Offset Triggered Cantilever Actuated Generator

Description:
FIELD OF THE INVENTION 
     The present invention relates to energy harvesting electrical generators, in particular, single-motion or impulse actuated electrical generators with a damped sinusoidal output that are superior in instantaneous triggered resultant output compared to instantaneous triggered snap-action magnetic circuit types that have a short single electrical pulse output of a typical effective time duration of 2 milliseconds. 
     BACKGROUND 
     Energy harvesting devices cover a wide range of low to high power generation for many applications, especially generating electrical energy from mechanical motion produced by intentional operator or environmental incidental action and have size versus efficiency choices. For those low power applications many are significantly limited; and in general, offer inadequate wide range product utilization. Further efforts by some prior art related to continuous or short burst types have not shown significant improvements and do not show any greater problem or application understanding likely to provide any significant improvements thereof. 
     SUMMARY OF THE INVENTION 
     The present invention introduces and teaches a novel plurality magnet arrangement having distinct advantages and novelty over prior art whereby the present invention teaches a plurality magnet arrangement of a matrix of rows and columns has a novel method means of reducing the counter electromotive force (voltage) during electrically connecting a load to the coil winding terminals and this has novelty in extending the time duration of the damped sinusoidal output voltage waveform and this is accomplished by altering the magnet field alignment on the plurality of the magnet matrix comprise of rows and columns of plurality magnets in such a manner that there are at times a co-existing combination of changing attractive and repelling magnetic field region all throughout the coil winding volume. 
     The present invention also provides and teaches that a variable speed range of motion triggering, can be supplied by an external push force on a forked-cantilever that is movable and rotating on its offset inline axles that are on the opposite end of the fork arrangement, where the two fork end tabs come in momentary contact with a rotatable centre magnet disposed within a coil; and any trigger action causes an induced electromotive force (voltage) established at the coil terminals by a relativistic electrodynamic movement of electrical charge (electrons) within the coil winding in a continuous or pulsed periodic rotational energy harvesting generator. Whether the forked cantilever movement progression is slow action or fast action, once the forked cantilever moves the centre movable magnet (responsible for power generation) past the trigger release point of an dual set of angled plurality tooth arrangement situated on opposite sides of the centre movable magnet enclosure adjacent to its common inline axles, the individual response of the power generating centre movable magnet (in its enclosure) disposed within the centre of the coil in conjunction with the first and second set of a plurality of fixed position focusing magnets situated at opposite ends of the coil, creates “geometrically distorted” and “changing magnetic field tensors” surrounding and passing through the coil winding; a varying power envelope is produced. The overall “relativistic moving charge effect” of inducing a voltage at the generator coil terminals is further enhanced by utilizing the two plurality sets of fixed directive (counter emf reducing) magnets, fixed on opposite ends of the coil, to concentrate the magnetic field throughout the generator coil winding; and with every movement of the cantilever trigger, in momentary and periodic mechanical connexin to the centred situated rotatable magnet, a voltage is produced at the coil terminals due to the relativistic movement of charge by magnetic field changes With this arrangement a damped sinusoidal alternating voltage, with typical effective AC wave duration time under a “no-load” condition of several hundreds of milliseconds, is established at the coil terminals; and with the novelty of the present embodiment connecting a load to the coil will produce a substantially less decrease in the effective AC wave duration time. The novel structure utilizes modified effects of Ampere&#39;s Law, Lenz&#39;s Law, and the Lorentz Force in producing substantially less decrease in AC wave duration time. 
     The EMF (Electromotive Force, (defined below) generated by special relativistic charge movement and conforming to Faraday&#39;s law of induction (the flow of charge (current)) through a coil around an electrical complete circuit due to relative movement or change of a coil&#39;s magnetic field) is the phenomenon underlying electrical generators; however, most texts covering the Faraday Principle illustrates a moving coil through a stationary magnetic field source (a magnet), with the present invention the converse holds true where an independent magnet can be moved and rotated within the centre of an electric coil and whereby the coil has fixed on its opposite sides, two plurality sets non-movable fixed magnets. When a permanent magnet is moved relative to a conductor, or the converse condition, an electromotive force (voltage) is created at the coil end terminals. If the coil wire terminals are connected to an electrical load, current will flow in the completed circuit, and thus electrical energy is generated, converting the mechanical energy of motion to electrical energy, thus ‘harvesting’ mechanical energy as electrical energy for some application usage. 
     Special Relativity and Magnets 
     Now let us consider magnetism due to electrons. Apart from charge and mass, electrons also have an intrinsic magnetic moment that can be explained only through relativistic quantum mechanics. Thus, magnetism of a bar magnet is also a relativistic effect. Please note that magnetism in a bar magnet is because of the election&#39;s spin, orbital motion and magneto-crystalline anisotropy. 
     Materials with high magnetic anisotropy usually have high coercivity, that is, they are hard to demagnetize. These are called “hard” ferromagnetic materials and are used to make permanent magnets. For example, the high anisotropy of rare-earth metals is mainly responsible for the strength of rare-earth magnets. During manufacture of magnets, a powerful magnetic field aligns the microcrystalline grains of the metal such that their “easy” axes of magnetization all point in the same direction, freezing a strong magnetic field into the material. 
     The strongest permanent magnets available today rare earth magnets, such as but not limited to, Neodymium (Nd,Pr)FeB and Samarium-Colbalt SmCo varieties having magnetic properties due to the interaction of the electron&#39;s spin and orbital motion with the potential created by the material lattice. Permanent magnets are not simply produced from having excess, non-cancelled electronic spins or some such. The requirement needed crystalline or shape features. 
     In reality, electricity and magnetism are equally fundamental parts of physics. Special relativity unites electricity and magnetism into electromagnetism, in exactly the same way that it unites space and time into spacetime. Time does not cause space, space does not cause time, and SR (Special Relativity) causes neither space nor time. SR (Special Relativity) merely reveals the relatedness of space and time. Similarly, electricity does not cause magnetism, magnetism does not cause electricity, and SR (Special Relativity) causes neither electricity nor magnetism. SR (Special Relativity) merely reveals the relatedness of electricity and magnetism. 
     Electromotive Force (EMF) 
     All voltage sources create a potential difference and can supply current if connected to a resistance. On a small scale, the potential difference creates an electric field that exerts force on charges, causing current. We call this potential difference the electromotive force (abbreviated emf). Emf is not a force at all; it is a special type of potential difference of a source when no current is flowing. Units of emf are volts. 
     Electromotive force is directly related to the source of potential difference, e.g. such as the particular combination of the number of turns and the thickness of the wire in a coil winding in a generator. However, emf differs from the voltage output of the device when current flows. The voltage across the terminals of a coil winding, for example, is less than the emf when the coil winding supplies current, and it declines further as the coil winding is electrically loaded down. However, if the device&#39;s output voltage can be measured without drawing current, then output voltage will equal emf. 
     Terminal Voltage 
     The voltage output of a device is measured across its terminals and is called its terminal voltage V. Terminal voltage is given by the equation: 
         V =emf− Ir   (Eq. 1)
 
     where r is the internal resistance and I is the current flowing at the time of the measurement. 
     I is positive if current flows away from the positive terminal. The larger the current, the smaller the terminal voltage. Likewise, it is true that the larger the internal resistance, the smaller the terminal voltage. 
     The preferred embodiment of the present invention has a plurality of rows and columns of magnets up as a matrix, and for exemplary embodiments of this present invention, there are rare earth magnets disk magnets arranged in a three column by two row array (matrix), where each column member magnet is separated proximal from each other and each row of three member magnets is separated distal from each other; for this present invention, including the novel feature having in each row, the magnetic pole alignment of a member magnet opposite to an adjacent member magnet. Other embodiments may include a larger number of magnets in each row, and may have all adjacent row magnets pole alignment oppositely disposed. The arrangement is such that their respective “up &amp; down” magnetic pole circuitous alignment exists so that there is a first set of a 1st member S↓N with (poled S facing up), a 2 nd  member with (poled N N↑S facing up), and a 3 rd  member with S↓N (poled S facing up) and they are all separated on one side proximal of a coil bobbin with its wire winding and on a side opposite the coil bobbin with its wire winding is a disposed second set of a S↓N 1st member with (poled s facing up), a 2 nd  N↑S member with (poled N facing up), S↓N and a 3 rd  member with (poled S facing up); and disposed centred within the coil bobbin, is a rotatable about its axis, magnet. From this row and column arrangement is established a “complex-pole produced” three dimensional magnetic flux field encompassing the coil and its winding that is disposed in between the two rows of magnets and the rotatable centre magnet disposed within the coil bobbin (with symmetrically centred hollow core). Ergo, by analysis with the first row members there exists; [1] an attractive static magnetic field between proximal retained 1st row member and proximal retained 2 nd  row member, and [2] an attractive magnetic field between proximal retained 2 nd  row member and proximal retained 3rd row member; and with the second row members there exists; [3] an attractive static magnetic field between proximal retained 1st row member and proximal retained 2 nd  row member, and [4] an attractive magnetic field between proximal retained 2 nd  row member and proximal retained 3 rd  row member. [5] There exists a static attractive magnetic field between the 1st magnet of the first row and the 1st magnet of the second row distal. [6] There exists a static attractive magnetic field between the 3rd magnet of the first row and the 3 rd  magnet of the second row distal. [7] There is disposed a first changing differential function magnetic field region between the 2nd magnet member (centre position) of the first row and a first width side of the rotatable centre magnet disposed and free to rotate about its axis of rotation and [8] there is disposed a second changing differential function magnetic field region between the 2 nd  magnet member (centre position) of the second row and a second opposite width side of the rotatable centre magnet disposed and free to rotate about its axis of rotation. Their combined respective magnetic field polarity is arranged in a completed attractive magnetic force circuit, such that in a rest state with no triggering action, the bi-directionally axially rotatable magnet disposed within the centre of the coil winding are in a magnetic equilibrium position (minimum mechanical energy state). 
     Repulsive Effects and Levitation 
     Electrodynamic Suspension: 
     In a varying magnetic field the induced currents exhibit diamagnetic-like repulsion effects. A conductive object will experience a repulsion force. This can lift objects against gravity, though with continual power input to replace the energy dissipated by the eddy currents. An example application is separation of aluminum cans from other metals in an eddy current separator. Ferrous metals cling to the magnet, and aluminum (and other nonferrous conductors) are forced away from the magnet; this A cross section through a linear motor placed above a thick aluminium slab. As the linear induction motor&#39;s field pattern sweeps to the left, eddy currents are left behind in the metal and this causes the field lines to lean. can separate a waste stream into ferrous and non-ferrous scrap metal. With a very strong handheld magnet, such as those made from rare earth magnets, one can easily observe a very similar effect by rapidly sweeping the magnet over a coin with only a small separation. Depending on the strength of the magnet, identity of the coin, and separation between the magnet and coin, one may induce the coin to be pushed slightly ahead of the magnet even if the coin contains no magnetic elements, such as the US penny. Another example involves dropping a strong magnet down a tube of copper the magnet falls at a dramatically slow pace. In a perfect conductor with no resistance (e.g. a superconductor), surface eddy currents exactly cancel the field inside the conductor, so no magnetic field penetrates the conductor. Since no energy is lost in resistance, eddy currents created when a magnet is brought near the conductor persist even after the magnet is stationary, and can exactly balance the force of gravity, allowing magnetic levitation. Superconductors also exhibit a separate inherently quantum mechanical phenomenon called the Meissner effect in which any magnetic field lines present in the material when it becomes superconducting are expelled, thus the magnetic field in a superconductor is always zero. Using electromagnets with electronic switching comparable to electronic speed control it is possible to generate electromagnetic fields moving in an arbitrary direction. In some geometries the overall force of eddy currents can be attractive, for example, where the flux lines are past 90 degrees to a surface, the induced currents in a nearby conductor cause a force that pushes a rotatable magnet towards a coil. 
     Ergo, the “Magnet Array,” with its novel arrangement of a plurality of rows and columns of magnets, disposed and retained about a coil winding with a centred rotatable magnet, provides a method means for changing phase related angular and perpendicular magnetic fields that at rotational times act as resultant repulsive and at other times acting as resultant attractive and whereby the resultant fields are surrounding a coil winding with a disposed rotatable centre magnet leads to optimizing the overall performance and output power of the present invention. 
     The Effects of Wire Gauge 
     The effect of coil wire gauge in electromagnetic energy harvesting generators, and all other types as well, is determined by several mathematical factors. Consider Ohm&#39;s Law for power; 
         P=V   2   /R  (induced voltage squared divided by the load resistance) and now relating to Faraday&#39;s Law;  (eq. 2)
 
         P =( Nd ( B·A )/ dt )/ R   I   ∝N   2   /R   I   (eq. 3)
 
     Definitions are: 
     N=No. of R I  turns, =load resistance, B=vectoral strength of the magnetic field, 
     A=coil cross section. 
     Further consider that the maximum transfer of power is when the coil resistance equals the load resistance. The smaller the coil of wire radius (r), the more turns N can be wound over a length and depth I and p is the specific resistance of the wire gauge. 
       ∴ N∝ 1/ r  Then  R   c   =R   coil   =pI ∝(1/ r   2 )(π dN )∝(1/ r   3 )  (eq. 4)
 
     This means that the harvested power should increase proportionally with the radius of the wire. 
       Power∝ N   2   /R   c ∝(1/ r ) 2 (1/ r ) 3   ∝r   (eq. 5)
 
     “However,” the generated voltage decreases with the radius of the wire is; 
         V   coil   =Nd ( B·A )/ dt∝ 1/ r  This is a crucial mathematical balancing act.  (eq. 6)
 
     The novelty summarized of this invention is that it is an energy harvesting generator that has one coil with a rotating magnet in the coil centre and at opposite sides of the coil are situated, by a support mechanism, two plurality sets of magnets, a first set on the left side of the coil and a second set on the right side of the coil fixed within this support mechanism, and each of the fixed single magnet but can be a plurality magnets sets have magnetic poles that are poled axially, and each has one attractive pole that faces the centre rotating magnetic field directive magnet in an attractive magnetic pole situation. Further, when the centre rotating magnet is triggered by an external force on the forked cantilever trigger, the centre rotating magnet can bi-directionally rotate in either a clockwise or anti-clockwise direction along the axis of rotation. Upon a push downward of the forked cantilever mechanism the centre magnet rotates in a clockwise direction and when the cantilever springs upward the rotation is anti-clockwise; and this dual action from one push, causes two separate induced AC ring down (damped) voltage periods in the common coil until axial friction causes the bi-directionally rotatable magnet to stop bi-directionally rotating. 
     The present invention&#39;s exemplary embodiments include utilizing rare-earth or high field strength plurality magnet sets such as rare earth magnets. There also exists a novel category of rare earth magnets that are identified as ‘poly-magnets’. Poly-magnets start as regular rare earth magnets, such as but not limited to, Neodymium magnets. However, poly-magnets are entirely different from conventional magnets, which have one north and one south pole. Poly-magnets contain patterns of North and South poles, such as alternating north and south pole ‘lines’, on a single piece of magnetic material. The fields coming off of these patterns of north and south poles in turn define the feel and function of the poly-magnet. The field on the poly-magnet is tightly focused because the fields do not have to go as far to connect from north to south. The same amount of energy is present in both magnets, but the poly-magnet e.g. a flat flexible kitchen magnet, where one side is strongly magnetized, and the other side is weakly magnetized, has much more energy focused in front of the magnet where it can do work. Empirical research stemming from the development of the present invention indicate that the embodiments described herein have less counter emf to contend with when the generator of the present invention is connected to an electrical load. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG.  1    is a perspective view of one embodiment of the present invention showing the offset triggered cantilever actuated generator with its enclosure removed for generator display. 
         FIG.  2    is an exploded perspective view of the embodiment of the present invention of  FIG.  1   . 
         FIG.  2 A  is an exploded perspective rising top view of all components of the embodiment of the present invention of  FIG.  1   . 
         FIG.  2 B  is a exploded perspective rising bottom view of all components of the embodiment of the present invention of  FIG.  1   . 
         FIG.  2 C  is an exploded component view of components of the embodiment of the present invention of  FIG.  1   . 
         FIG.  2 D  is an exploded component view of components of the embodiment of the present invention of  FIG.  1   . 
         FIG.  3    is an illustration of a human finger in a pre-trigger position of depressing the movable push-button mechanism of the embodiment of the present invention of  FIG.  1    and showing all of the static state moveable components. 
         FIG.  4    is an illustration of a human finger depressing the push-button mechanism and the change of state in all of the movable components of the embodiment of the present invention of  FIG.  1   . 
         FIG.  5    is an illustration showing the equilibrium state of the comprised attractive interactive magnetic fields of the embodiment of the present invention of  FIG.  1   , with the central movable magnet that is diametrically poled and the two sets of inline lateral directive (counter emf reducing) magnets that are axially poled. 
         FIG.  5 A  is an illustration showing the equilibrium state of the comprised attractive interactive magnetic fields, including the surrounding field component above and below the coil volume, of the embodiment of the present invention of  FIG.  1   , with the central movable magnet that is diametrically poled and the two sets of inline lateral directive (counter emf reducing) magnets that are axially poled. 
         FIG.  6    is an illustration of the embodiment of  FIG.  1   , showing a first initial active state during a finger depression of the offset cantilever trigger mechanism and thus causing the central magnet to move; and further causing the interactive attractive magnet fields between the central magnet and the two sets of inline lateral directive (counter emf reducing) magnets to distort away from an equilibrium state. 
         FIG.  7    is an illustration of the embodiment of  FIG.  1    showing a second active state when a finger that depresses the cantilever trigger mechanism is released from the offset cantilever trigger mechanism and the central magnet is free to rotate and mechanically oscillate to move and thus further causing the interactive attractive magnet fields between the central magnet and the two sets of inline lateral directive (counter emf reducing) magnets to distort away from an equilibrium state; and during this period the damped sinusoidal voltage waveform, of substantial time duration, is produced at the coil terminals. 
         FIG.  8    is a typical damped sinewave voltage output waveform showing peak-to-peak voltage and the minimum acceptable operational voltage levels (e.g. 1.8 to 3.3 volts) for micro-transmitter chips currently in the marketplace. 
         FIG.  9    is a magnetic field concentration of a prior art embodiment using a uniform horizontal inline column arrangement of a plurality of magnets, all poled in the same direction in a horizontal plane and a plurality of those column arrangements in a plurality of rows; and in a special case of a three by two column-row instance there is a centred single rotatable magnet along its horizontal axis; where the rotatable magnet is poled in a moment of time in one direction through a complete possible rotation. 
         FIG.  10    is a magnetic field concentration of a novel magnet arrangement according to an embodiment of the present invention, that in contrast to  FIG.  9    of prior art is a uniform horizontal inline column arrangement of a plurality of magnets, where the centre magnet is pole in an opposite direction to the remaining other member magnets, in a horizontal plane and a plurality of those column arrangements in a plurality of rows; and in a special case of a three by two column-row instance there is a centred single rotatable magnet along its horizontal axis; where the rotatable magnet is poled in a moment of time in one direction through a complete possible rotation. 
         FIG.  11    is a magnetic field concentration of prior art (e.g.  FIG.  9   ) using a uniform horizontal inline column arrangement of a plurality of magnets, all poled in the same direction in a horizontal plane and a plurality of those column arrangements in a plurality of rows; and in a special case of a three by two column-row instance there is a centred single rotatable magnet along its horizontal axis; where the rotatable magnet is poled in a moment of time in a direction opposite to that of  FIG.  9    through a complete possible rotation. 
         FIG.  12    is a magnetic field concentration of a novel counter emf reducing magnet arrangement embodiment according to the present invention, that in contrast to  FIG.  11    of prior art is a uniform horizontal inline column arrangement of a plurality of magnets, where the centre magnet is pole in an opposite direction to the remaining other member magnets, in a horizontal plane and a plurality of those column arrangements in a plurality of rows; and in a special case of a three by two column-row instance there is a centred single rotatable magnet along its horizontal axis; where the rotatable magnet is poled in a moment of time in a direction opposite to that of  FIG.  10    direction through a complete possible rotation. 
         FIG.  13    shows the composite resultant magnetic fields surrounding the coil winding caused by an embodiment of the present invention of  FIG.  12    affect during a maximum induced voltage segment of time. 
         FIG.  14    shows the composite resultant magnetic fields surrounding the coil winding caused by an embodiment of the present invention of  FIGS.  10 ,  12  and/or  13   . 
         FIG.  15    is a block diagram drawing of the resultant associated magnetic flux of the embodiment of  FIG.  14   , during a centre group of the rotatable centre magnet and the top and bottom centred fixed disk magnets are in an attractive magnetic opposite-pole alignment. 
         FIG.  16    is a block diagram drawing of the resultant associated magnetic flux of the embodiment of  FIG.  14   , during a centre group of the rotatable centre magnet and the top and bottom centred fixed disk magnets are in an repulsive magnetic like-pole alignment. 
     
    
    
     DETAILED DESCRIPTION OF THE DRAWINGS 
       FIG.  1    shows the preferred embodiment 100 of the present invention that has an enclosure comprised of the enclosure body  101  and a movable push-button disposed element  101   p  that is removed from enclosing to expose some of the major components of this embodiment. This exposure includes a base substrate  103 , which supports a wound coil bobbin  105 , a forked cantilever  107  comprised of bifurcated ends  117   f  &amp;  117   r  (shown in  FIG.  2   ), and a set of snap-on supports  119   f  &amp;  119   r  (shown in  FIG.  2   ) including a first snap-on front side support  119   f  and a second snap-on rear side support  119   r , where they both snap-on for easy connection to the base substrate&#39;s  103  first rear support cylinder protrusion  129   r  and the second front support cylinder protrusion  129   f . The push-button  101   p  disposed section of the device enclosure  101 , when it covers the remaining components of this embodiment, come in mechanical contact with the bifurcated plunger  107  and the push-button  101   p  has the action of angular movement (downward and upward) to cause by mechanical induction, the bifurcated plunger  107  to trigger the operational action of clockwise rotating about the bifurcated plunger&#39;s  107  axis  163  downward, the centre magnet enclosure  108  and its enclosed centre magnet  112  (shown in  FIG.  2   ) and thereafter freely releasing the centre magnet enclosure  108  and its magnet  112  to rotate about its axis  161  backwards in anti-clockwise rotation. The base substrate  103  has two sets of blind rectangular inline holes  113   a,b,c  and  113   d,e,f  (shown in this figure and in  FIG.  2    complete) disposed within the structures  111 L &amp;  111 R on opposite sides of the coil bobbin  105  with winding  104  (shown in  FIG.  2 A ) that in addition act as a support for the coil bobbin  105 . The base substrate also has an enclosure  109  where the centre rotational magnet  112  and its enclosure  108  (shown in  FIG.  2    and  FIG.  2 A ) are seated and free to rotate and is held in place by magnet support base  110  and its two protrusions  130   f  &amp;  130   r  (note: front protrusion  130   f  is shown in  FIG.  2 A ); the front protrusion  130   f  and the rear protrusion  130   r  support the axles of the magnet  112  and its enclosure  108  that allows for rotation with minimum friction since the entire substrate  103  would be made of Nylon with 30% glass and the enclosure segment  109  would be made of Delrin or some equivalent low coefficient of friction material. 
       FIG.  2    is an exploded view  200  showing the present invention&#39;s preferred embodiment identifying all of the components that make up the generator without showing the cover that is shown in  FIG.  1   . With this embodiment, the coil bobbin  105  is designed with a built-in (moulded-in) attachment  105   a  with a disposed centre through hole  106 ; and two opposite break-off tabs  106   a  &amp;  106   b ; where there is a first break-off tab  106   a , and a second break-off tab  106   b  on the opposite end of the attachment  106 , whose purpose (in the production coil winding phase) is to allow the coil bobbin  105  to be mounted on a coil winding machine and then post-winding, the attachment  105   a  is easily snapped off in production. With this embodiment there are two sets of a plurality of blind slots  113   a, b, c  &amp;  113   d, e, f ; for the insertion of a plurality of magnets  141   a, b, c  &amp;  141   d, e, f  (shown in  FIG.  2 C ) and they are disposed and permanently secured in a fixed position within the slots, with their respective “up &amp; down” magnetic pole circuitous alignment so that there is a first set of a 1 st  member 2 nd  S↓N a 2 nd  member with N↑S, and a 3 rd  member S↓N and they are all separated on one side proximal of the coil bobbin  105  with its wire winding  104  and on a side opposite the coil bobbin  105  with its wire winding  104  is a disposed second set of a 1 st  member with S↓N, a 2 nd  member with N↑S, and a 3 rd  member with S↓N and disposed centred within the coil bobbin  105 , is the rotatable magnet  112 . These plurality of small disk type magnet sets are axially poled and act as counter emf reducing magnets directing the combined magnet fields (shown in  FIGS.  7 ,  8   , &amp;  9 ) through the coil winding  104  wound around the coil bobbin  105 ; and the first intermediate magnetic field  701  (shown in  FIG.  5    is in its equilibrium non-trigger state) between plurality magnets  113   a,b , c and the centre rotating magnet  112  passes through the first half of coil  105  and its winding  104 ; and the second intermediate magnetic field  703  (shown in  FIG.  5    is in its equilibrium non-trigger state) plurality magnets  113   d, e, f  and the centre rotating magnet  112  passes through the second half of the coil  105  and its winding  104 . The centre drive magnet  112  is disposed (fixed) within its axially rotatable enclosure  108  and is free to rotate about its dual inline axles  115 F &amp;  115   r  (about the axles  115 F &amp;  115   r  axis  161 ) as the complete drive magnet assembly  112  &amp;  108 ; and this assembly  112  &amp;  108  is disposed within the magnet drive housing  109  that is a section of the base substrate  103 . The magnet drive assembly  112  &amp;  108  is supported by its axles  115   f  &amp;  115   r ; and respectively free to rotate about its axis  161  between the two protrusions  130   f  &amp;  130   r  (that are tangent along the plane of the support cover  108 ) and the open slots  133   f  &amp;  133   r ; and when the support cover  108  is inserted and fixed in place by insertion of the two protrusions  130   f  &amp;  130   r  into the open slots  133   f  &amp;  133   r  the free space created by this action acts as a complete rotatable magnet axle drive assembly  112  &amp;  108  that upon triggering has bi-directional damped rotating action resulting in the damped oscillatory voltage waveform. 
       FIG.  2 A  is a “top looking down” exploded perspective drawing of the preferred embodiment of this invention showing all components for a clear understanding of the novelty of few parts required for comprising this invention. 
     Basically, there is the base substrate  103  that has as part of its monolithic design, a centre magnet section  109  for holding in place the centre drive magnet  112  disposed within the rotatable magnet enclosure  108  (about its axis  161 ). In addition, there is inserted and fixed within two separate monolithic counter emf reducing magnet support subsections, a first left side focus magnet support monolithic subsection  111 L and a second right side focus magnet support monolithic subsection  111 R, where both left and right focus magnet support subsections are separated in distance to allow for the insertion of the coil bobbin  105  with its winding  104  and its wire terminals  102   t   1  &amp;  102   t   2 ; and the sides of the coil bobbin are butt up against the inner areas of the left and right focus magnet support monolithic subsections  111 L &amp;  111 R, and this arrangement brings both plurality magnets  113   a, b, c  &amp;  113   c, e, f  disposed within the two focus magnet supports  111 L &amp;  111 R as close as possible to optimise the amount of induced voltage produced during triggering. 
       FIG.  2 A  also shows the bifurcated trigger plunger  107  with its features of bifurcated protrusions, a first rear protrusion  117   f  and a second front protrusion  117   r , and when the bifurcated trigger plunger  107  is snapped onto the dual axle protrusions  129   r  &amp;  129   f  the bifurcated trigger plunger  107  is free to rotate about the dual axles  129   r  &amp;  129   f  (about their common axis  163 ). During a triggering event, the bifurcated protrusions  117   r  &amp;  117   f  mechanically strike (hit) the two separate inline tri-finger (tri-fingered for strength) axle tabs  132   f  &amp;  132   r  causing clockwise rotation on the down-stroke that causes a first polarity induced voltage produced and when the bifurcated trigger plunger springs back this causes an anti-clockwise rotation that causes a second polarity (opposite to the first down-stroke polarity) going induced voltage; and in both instances an induced AC (alternating current) voltage is produced (See  FIG.  8   ). 
       FIG.  2 B  is a “bottom looking up” exploded perspective drawing of the preferred embodiment of this invention showing all components for a clear understanding of the novelty of few parts required for comprising this invention and it further illustrates several feature shown from the under sections therein, where the bottom support cover  108  is inserted flush with the monolithic base substrate&#39;s  103  centre magnet monolithic base section enclosure  109  and fits into the two opposite slots  133   f  &amp;  133   r  of the centre magnet monolithic section enclosure  109  that acts as the axle support assembly for the centre magnet axially rotatable enclosure  108  that contains the centre magnet  112 . Another feature of this embodiment that is a substantial aid during production is to have the coil bobbin designed with a keyed insert slotted arrangement, where there are four uniform spaced in a rectangular paradigm position arrangement that contains four protrusions of a first protrusion that is a key  121   p  and three identical cylinder protrusions  123   p ,  125   p ,  127   p  that fit into identical through holes of a first key hole  121  and three identical through holes  123 ,  125 ,  127 . for insertion and lock-in. A method of coil production with automatic coil winding machines is to allow easy quick mounting of the coil bobbin  105  on a coil winding machine and to do a fast winding procedure for a finished winding  104 . This method can be accomplished easily if the coil bobbin  105  has a break-off rectangular attachment  105   a  at the centre of the coil bobbin  105  and at the centre of the break-off attachment  105   a  is a centred through hole  106  for insertion on a bobbin rod of a coil winding machine. 
       FIG.  2 C  is an exploded component view comprising the two separate plurality sets of focus directive magnets  141   a, b, c  and  141   d, e, f  that are inserted and fixed into the open blind hole slots  113   a, b, c  and  113   d, e, f  respectively and fixed within. Also in  FIG.  2 C  is the centre magnet rotatable enclosure with its blind rectangular hole  108   s  that holds fixed within the centre magnet  112  (shown in  FIG.  2 D ) and the comprised centre magnet enclosure and its magnet  112  is positioned above the enclosure support  108  and its two support protrusions  131   f  &amp;  131   r  that are in contact at support contact points  116   f  &amp;  116   r  with the rotatable enclosure  108  and the rotatable enclosure  108  is free to rotate about its axis  161 . Where in  FIG.  2 D , the centre magnet  112  is disposed and fixed within the centre magnet slotted blind rectangular hole  108   s  and the comprised magnet  112  and its enclosure  108  are pivotal about its axis  161 . The two axles  115   f  &amp;  115   r  are contiguous with the enclosure  108  support member&#39;s  108  two separate tangent (to the plane surface of the support member  108 ) protrusions. The trigger receiver tabs  132   f  &amp;  132   r  become contiguous with the bifurcated cantilever&#39;s (see  FIG.  3    and  FIG.  4    and  FIG.  5   ,  FIG.  6   , &amp;  FIG.  7   ) finger tabs  117   f  &amp;  117   r  respectively. 
       FIG.  3    illustration  300  shows the present invention&#39;s preferred embodiment as a side cutaway view, in its static equilibrium state before a trigger is caused by the urging of the spring  513  by the push-lever  101   p  that experienced the urging of a finger  501  or other mechanical force source. All “action-sequential” triggering, caused by the following members, which are utilised to produce electrical power, comprised of the; [1] push-button  101   p  as part of the device enclosure  101 , [2] the tangent extension  505  of the push-button  101   p  that is contiguous with the dual fork fingers  117   f  &amp;  117   r  that are a sub-member of the bifurcated cantilever trigger member  107 , [3] the spring  513  for urging forward force downward and potential-to-kinetic energy release upward (after instant release) of the bifurcated cantilever trigger member  107 , whose action and reaction causes the dual fork fingers  117   f  &amp;  117   r  to create a contiguous connection between the dual fork tab fingers  117   f  &amp;  117   r,  [4] and the upper tabs  132   f  &amp;  132   r  as a sub-member of the inline axles  115   f  &amp;  115   r  remain in a static equilibrium state until a finger  501  or some other external mechanical energy source initiates a “turn ON trigger-action” state described in  FIG.  4   . 
       FIG.  4    illustration  400  shows the present invention&#39;s preferred embodiment as a side cutaway view, during the “turn ON action procedure” of a human finger  501  or an external trigger caused by the urging of the spring  513  by the push-lever  101   p  that experiences the urging of a finger  501  or other mechanical force source. The “turn ON action procedure” produces a “Rube Goldberg type action-sequential” triggering by its members that are utilized to produce electrical power by action of pressing-in, the push-button  101   p  that is part of the device enclosure  101 , and the push-button tangent extension  505  of the push-button  101   p  then comes in instant contact with the dual fork cantilever  107  and whose dual fork fingers  117   f  &amp;  117   r  that are a sub-member of the bifurcated cantilever trigger member  107 . 
     The bifurcated cantilever trigger member  107  urges the spring  513  to produce a forward force downward and the resultant compression of the spring  513  stores potential energy that is created during this process. Then by the instant finger  501  release upward of the bifurcated cantilever trigger member  107 , action and reaction that is created causes the dual fork fingers  117   f  &amp;  117   r  to instantly create a contiguous connection between the dual fork tab fingers  117   f  &amp;  117   r , and the upper tabs  132   f  &amp;  132   r  as respective sub-members of the inline axles  115   f  &amp;  115   r  that are part of the centre magnet  112  contained in its rotatable enclosure  108  and remain in a damped oscillatory alternating electrical energy producing state ( FIG.  8   ) until the frictional forces diminish to a rotational stoppage of the centre magnet  112  in its rotatable enclosure  108 . 
       FIG.  5    is an illustration  500  of a partial cutaway view of the preferred embodiment  500  that illustrates the rest “non-trigger” state of the invention&#39;s encompassing attractive magnetic field  701  and  703  and purposely not showing (for simplicity) the complete magnetic circuitous path that travels all through the invention&#39;s embodiment but is shown for understanding in  FIG.  5 A . 
       FIG.  5 A  is a simplified illustration  500 -A showing a complete and circuitous effective magnetic field of the invention&#39;s preferred embodiment  500 -A where the surrounding magnetic field  700  extends from the outside pole of the left focus magnet inline array  113   abc  to the right focus magnet inline array  113   def , thus making a closed circuitous path for the magnetic lines of force. The entire inner  701  &amp;  703  and outer overhead  702  magnetic circuit path changes (see  FIG.  6    &amp;  FIG.  7   ) its field flux intensity through the coil  105  during the damped cyclic oscillatory bi-rotation of the centre inline axles centre magnet  112  rotatable enclosure  108  (shown in  FIG.  2   ) The angular sequential induced voltage producing operation of the preferred embodiment and influence of the changing magnetic field  705  &amp;  707  is shown in the illustration  600  in  FIG.  6    during an instant of downward depression, by the urging of a finger or some other external intentional mechanical energy source (shown in  FIG.  3   ), on the bifurcated cantilever  107  that simultaneously rotates downward  107   d  on its axis of rotation  163 . During the instant downward depression phase, the two fork tab fingers  117   f  &amp;  117   r  of the bifurcated cantilever  107  (note: with the cutaway views, only the front fork finger tab  117   f  is shown and the rear fork finger tab  117   r  is not shown but works instantly in parallel inline sequence) comes in instant contiguous contact with the axle tabs  132   f  &amp;  132   r  (note: with the cutaway views, only the front inline axle tab  132   f  is shown and the rear inline axle tab  132   r  is not shown but works instantly in parallel inline sequence) causing the centre magnet  112  fitted within its rotatable enclosure  108  to rotate from 0 degrees up to 90 degrees clockwise on its axis  161  (this effectively and simultaneously causes the centre magnet  112  to rotate to a new angular position  112   cw ) and as the forked finger tabs  117   f  &amp;  117   r  disconnect from a contiguous state with the rotatable magnet enclosure&#39;s  108  finger tabs  132   f  &amp;  132   r . The centre magnet  112  in its rotatable enclosure is free to oscillate; and this action creates the surrounding encompassing magnetic fields  701  &amp;  703  to change periodically in a sinusoidal movement  705 ,  707 ,  709 ,  711 . This periodic clockwise rotation of the centre magnet  112  simultaneously in union within its enclosure  108  causes a changing left magnetic field  701 / 705  that firstly passes up through the left side of the coil  105  and simultaneously the changing right magnetic field  703 / 707  secondly passes down through the right side of the coil  105 ; thus producing an instant first half sinusoidal duty cycle of induced EMF (voltage) that is felt at the coil terminals ( 102   ti  &amp;  102   t   2  shown in  FIG.  1   ). Once the bifurcated tab fingers  117   f  &amp;  117   r  moves past the maximum point of contiguous connection with the inline axle finger tabs  132   f  &amp;  132   r , both members are noncontiguous and the centre magnet  112  in its rotatable enclosure  108  and its contained centre magnet  112  is free to oscillate between a diminishing repeating travel angle range of 0° to +900 ( 112   cw ), to 0° to −90° ( 112   acw ), back to 0° with decreased terminal EMF (voltage) following a mathematical path conforming to the damping values of X e  ( 173 , as shown in  FIG.  8   ). This first cyclic duration of the downward depression phase; gives way to the second cyclic duration when the “contiguous-to-noncontiguous” finger  501  to bifurcated cantilever plunger  107  connection is forced back upward by the stored potential energy in the spring  513 , being converted to upward (spring expanding) kinetic energy (explained in  FIG.  7   ) 
       FIG.  7    illustration  700  represents the duration when the bifurcated cantilever springs back  107   u  to its non-triggered rest position  107 . This spring  513  produced forced action causes the bifurcated tabs  117   f  &amp;  117   r  to endure a contiguous connection between the enclosure  108  finger tabs  175   f  &amp;  175   r  that causes magnet  112  in its rotatable enclosure  108  to rotate anti-clockwise  112   acw  to +900 and when the dual fingered cantilever  107  travels to its non-triggered rest position, the centre magnet enclosure with its enclosed centre magnet  112  are free to oscillate between a diminishing repeating travel angle range of 0° to −90° ( 112   acw ), to 0° to +900 ( 112   cw ), back to 0° with decreased terminal EMF (voltage) that following a mathematical path conforming to the damping values of X ( 173 , as shown in  FIG.  8   ). 
       FIG.  8    is a graph  800  of a S N typical generated AC (alternating current) peak-to-peak Vp-p  165  voltage waveform  161  by the present invention over a time Δt duration of  169 , firstly under a no electrical load appliance connected at the coil terminals; and second the generated AC (alternating current) peak-to-peak Vp-p  165  voltage waveform  161  affected by an electrical load appliance connected to the coil terminals. Following the same damping effect X e    163  for each case by friction on the invention&#39;s embodiment producing the voltage, providing and indicium of the reduction in power output increase as the electrical load increases by nature. 
       FIG.  9    is a top comparison illustration  900  of the prior art  01   pa  that depicts a first plurality arrangement of magnets and in this referred to exemplary embodiment there are two separated sets of three inline disk magnets with all of their magnetic poles aligned in the same and parallel direction. The first set consists of a first inline magnet  011  with South pole up (along a line in the plane of the drawing, i.e. 7n paper”) and North pole down (in paper), a closely separated centre inline second magnet  012  with South pole up (in paper) and North pole down (in paper), and a third closely separated inline magnet  014 ; and a second set of a first inline magnet  016  with South pole up (in paper) and North pole down (in paper), a closely separated centre inline second magnet  018  with South pole up (in paper) and North pole down (in paper), and a third closely separated inline magnet  010 . Then there is a rotatable centred and separated equidistance between the two described magnet sets, and this centred rotatable magnet is disposed in a centre region of a coil winding  01 C.  FIG.  9    represents the centre magnet  020  in a moment during cyclic rotation about its axis A 1  when its South pole is up (in paper) and its North pole is down (in papeq The resultant lines of force contours that encompass the coil winding  01 C during that moment in time when the rotating magnet  020  is parallel to the horizontal plane of the coil winding  01 C. This stopped moment in time is when the induced AC voltage sinusoidal waveform is going through its instantaneous zero value. The magnetic lines of force for these comparisons was done by using a two dimensional visual software programme for calculating and displaying magnetic lines of force. The magnetic intensity contour plot shows a uniform distribution without any strong lines of force density with the area of the coil winding, and that would conclude an non-optimized design feature that would “not” offer any optimized maximum power generation from the generator. 
     Also in the illustration of  FIG.  9    are the prior art&#39;s magnetic contour plotted regional zones where all of the magnetic flux regions are attractive showing relative magnetic flux densities; there are four marginal attractive magnetic flux density zonal regions r 1 ′, r 3 ′, r 4 ′, &amp; r 6 ′ that pass through the coil winding  01 C due to the top row magnets  011 ,  012 ,  014  all being of the same attractive magnetic pole alignment; and there are two marginal magnetic flux density attractive zonal regions r 2 ′ &amp; r 5 ′ all being of the same attractive magnetic pole alignment. 
       FIG.  10    shows an illustration  1000  for novel and advantageous N features of the present invention&#39;s magnetic array over that of the referenced prior art  01   pa  in  FIG.  9   . Now with the array according to one embodiment of the present invention, there exists a first set consisting of a first inline magnet  141   a  with its South pole up (in paper) and North pole down (in paper), a closely separated all important centre inline second magnet  141   b  with its North pole up (in paper) and with its South pole down (in paper), and a third closely separated inline magnet  141   c  with its South pole up (in paper) and its North pole down (in paper); and a second set of a first inline magnet  141   d  with South pole up (in paper) and North pole down (in paper), a closely separated all important centre inline second magnet  141   e  with North pole up (in paper) and South pole down (in paper), and a third closely separated inline magnet  141   f  with its South pole up (in paper) and with its North pole down (in paper). Then there is a rotatable centred and separated equidistance between the two described magnet sets, and this centred rotatable magnet is disposed in a centre region of a coil winding  104 .  FIG.  10    represents the centre magnet  112  in a moment during cyclic rotation about its axis A 2  when its South pole is up (in paper) and its North pole is down (in paper). The resultant lines of force contours that encompass the coil winding  104  during that moment in time when the rotating magnet  112  is parallel to the horizontal plane of the coil winding  104 . This stopped moment in time is when the induced AC voltage sinusoidal waveform is going through its instantaneous zero time derivative value. The magnetic intensity contour plot shows a densely concentrated magnetically attractive zonal distribution with strong magnetic flux lines of force density r 1 , r 3 , r 4 , &amp; r 6  passing through the area of the coil winding  104  and moderate repulsive magnetic flux lines of force density r 2  &amp;r 5  passing through the coil winding  104 , and that would conclude the “Magnet Array” does offer and teach, by empirical evidence, a novel optimized design feature for maximum power generation from the present invention generator over that of the cited prior art  01   pa.    
     Also in the illustration of  FIG.  10    are the prior art&#39;s magnetic contour plotted regional zones at magnetic equilibrium (pre-S↓N triggering) where there are attractive and repulsive magnetic flux regions showing N S relative magnetic flux densities: there are S↓N; four separate proximal-distal substantially attractive angular magnetic flux density zonal regions r 1 , r 3 , r 4 , &amp; r 6 , attractive in respect to the centre rotatable magnet  112  in this moment in time of N magnetic equilibrium and the flux line contours, at a cosine angle vector N↑S value, pass substantially strong through the coil winding  104  due to the two separate top row end magnets  141   a , &amp;  141   c  being of the same attractive magnetic pole alignment, but the centre top row magnet  141   b  is like-poled; and is repulsive to the centre magnet  112 ; and there are two separate inline marginal magnetic flux density repulsive zonal regions r 2  &amp; r 5  all being of the same repulsive magnetic pole alignment as the centre rotational magnet  112 . Also aiding and magnetically encouraging the four separate attractive zonal regions r 1 , r 3 , r 4 , &amp; r 6  are the common inter proximal attractive coupling between the top row&#39;s first  141   a  and third  141   c  members&#39; and the top row centre magnet  141   b  plus the bottom row&#39;s common inter-proximal attractive coupling between first  141   d  and third  141   f  members&#39; and the bottom row centre magnet  141   e ; this inter-proximal coupling effect allows for increased bidirectional rotation performance. In conclusion, this inter coupling reduces significantly the number of repelling flux in the region of the centre zone region r 2 ; and provides less repelling flux, which allows for more attractive zones r 1  &amp; r 3  and r 4  &amp; r 6 , which in turn when triggered, the generator bi-directional rotational operation will rotate with increased velocity and will generate a longer time duration damped sinusoidal voltage waveform compared to prior art. All of these dynamically changing coupling factors allow for an improved method of generator operational output. 
       FIG.  11    is a top comparison illustration  1100  of the prior art  01   pa  that depicts a first plurality arrangement of magnets and in this referred to exemplary embodiment there are two separated sets of three inline disk magnets with all of their magnetic poles aligned in the same and parallel direction. The first set consists of a first inline magnet  011  with South pole up (in paper) and North pole down (in paper), a closely separated centre inline second magnet  012  with South pole up (in paper) and North pole down (in paper), and a third closely separated inline magnet  014 ; and a second set of a first inline magnet  016  with South pole up (in paper) and North pole down (in paper), a closely separated centre inline second magnet  018  with South pole up (in paper) and North pole down (in paper), and a third closely separated inline magnet  010 . Then there is a rotatable centred and separated equidistance between the two described magnet sets, and this centred rotatable magnet is disposed in a centre region of a coil winding  01 C.  FIG.  11    represents the centre magnet  020  in a moment during cyclic rotation about its axis A 1  when its North pole is up (in paper) and its South pole is down (in paper). The resultant lines of force contours that encompass the coil winding  01 C during that moment in time when the rotating magnet  020  is parallel to the horizontal plane of the coil winding  01 C. This stopped moment in time is when the induced AC voltage sinusoidal waveform is going through its instantaneous maximum value. The magnetic lines of force for these comparisons was done by using a two dimensional visual software programme for calculating and displaying magnetic lines of force. The magnetic intensity contour plot shows a uniform distribution without any strong lines of force density with the area of the coil winding, and that would conclude an non-optimized design feature that would “not” offer any optimized maximum power generation from the generator. 
     Also in the illustration of  FIG.  11    are the prior art&#39;s magnetic contour plotted regional zones where magnetic regions are all repulsive showing relative magnetic flux densities; there are four concentrated repulsive magnetic flux density zonal regions r 1 ′, r 3 ′, r 4 ′, &amp; r 6 ′ that pass away from the coil winding  01 C due to the top row magnets  011 ,  012 ,  014  all being of the same magnetic pole alignment S↓N repulsive to the rotatable centre magnet  020  in a repulsive Ns moment in time; and there are two marginal magnetic flux density repulsive zonal regions r 2 ′ &amp; r 5 ′ all being of the same magnetic repulsive pole S↓N alignment. This moment in time during a triggered rotation is the most unstable and therefore the effective rotational zone limit is between zero degrees (pole vector horizontal  ) and ninety degrees (pole vector vertical  ); practically though, with the prior art the degree of freedom for rotation with the prior art is approximately 80 to 85 degrees depending on design tolerances for the trigger mechanism. 
       FIG.  12    shows an illustration  1200  for novel and advantageous features of one embodiment of the present invention&#39;s magnetic array over that of the referenced prior art Olpa in  FIG.  9   . Now with the embodiment of the present invention shown, there exists a first set consisting of a first inline magnet  141   a  with its South pole up (in paper) and North pole down (in paper), a closely separated all important centre inline second magnet  141   b  with its North pole up (in paper) and with its South pole down (in paper), and a third closely separated inline magnet  141   c  with its South pole up (in paper) and its North pole down (in paper); and a second set of a first inline magnet  141   d  with South pole up (in paper) and North pole down (in paper), a closely separated all important centre inline second magnet  141   e  with North pole up (in paper) and South pole down (in paper), and a third closely separated inline magnet  141   f  with its South pole up (in paper) and with its North pole down (in paper). Then there is a rotatable centred and separated equidistance between the two described magnet sets; and this centred rotatable magnet is disposed in a centre region of a coil winding  104 .  FIG.  10    represents the centre magnet  112  in a moment during cyclic rotation about its axis A 2  when its South pole is up (in paper) and its North pole is down (in paper). The resultant lines of force contours that encompass the coil winding  104  during that moment in time when the rotating magnet  112  is parallel to the horizontal plane of the coil winding  104 . This stopped moment in time is when the induced AC voltage sinusoidal waveform is going through its instantaneous maximum time derivative value. The magnetic intensity contour plot shows a densely concentrated distribution with strong lines of force density within the area of the coil winding, and that would conclude the embodiment(s) of the present invention does offer and teach, by empirical evidence, an novel optimized design feature for maximum power generation from the present invention generator over that of the cited prior art  01   pa.    
     Also in the illustration of  FIG.  12    are the prior art&#39;s magnetic contour plotted regional zones at magnetic equilibrium (pre-triggering) where there are attractive and repulsive magnetic flux regions showing relative magnetic flux densities; there are four separate proximal-distal substantially moderate repulsive angular magnetic flux density zonal regions r 1 , r 3 , r 4 , &amp; r 6 , N s repulsive in respect to the centre rotatable magnet  112  in N↑S this moment in time of magnetic equilibrium (pre-triggering), and the flux lines at a cosine angle vector value, repel substantially moderate away from the coil winding  104  due to the two separate top row end magnets  141   a , &amp;  141   c  being of the same repulsive magnetic pole alignment N↑S, but the centre top row magnet  141   b  and the centre bottom row magnet  141   e  are both opposite-poled S↓N and they are proximal attractive to the centre rotational magnet  112 ; and there are two separate inline marginal magnetic flux density attractive zonal regions r 2  &amp; r 5  all being of the same attractive magnetic pole alignment S↓N as the centre rotational magnet  112 . Also affecting and magnetically limiting the four separate repulsive zonal regions r 1 , r 3 , r 4 , &amp; r 6  are the common angular inter proximal attractive coupling between the top row&#39;s first  141   a  and third  141   c  members&#39; and the top row centre magnet  141   b  plus the bottom row&#39;s common angular inter proximal attractive coupling between first  141   d  and third  141   f  members&#39; and the bottom row centre magnet  141   e ; this effect allows for increased bidirectional rotation performance. In conclusion, this inter coupling reduces significantly the number of changing repelling flux in the region of the top row first zone region r 1 , and third zone region r 3  plus bottom fourth zone region r 4  and sixth zone region r 6 ; and provides less repelling flux, which allows for more attractive magnetic flux zones&#39; r 2  &amp; r 5  desired rotational torque, when triggered, the generator bi-directional rotational operation will rotate with increased velocity and will generate a longer time duration damped sinusoidal voltage waveform compared to prior art. All of these dynamically changing coupling factors allow for an improved method of generator operational output. 
     The Array of Magnets 
       FIG.  13    and  FIG.  14    are illustrations of an embodiment of the present invention having a plurality of rows and columns of magnets including a plurality of inline magnets set up as a matrix, and for this present invention, there are rare earth disk magnets arranged in a three column by two row array (matrix), where each column member magnet is separated proximal from each other and each row of three member magnets is separated distal from each other; for this present invention&#39;s embodiment, and what distinguishes and renders novel is in each row is the magnetic pole alignment of each member magnet to each other. The arrangement is such that their respective “up &amp; down” magnetic pole circuitous alignment exists so that there is a first set of a 1 st  member  141   a  S↓N with (poled S facing up), a 2 nd  member  141   b  with N S (poled N facing up in paper), and a 3 rd  member  141   c  S↓N with (poled S facing up in paper) and they are all separated on one side proximal of a coil bobbin  105  with its wire winding  104  and on a side opposite the coil bobbin with its wire winding is a disposed second set of a 1st member  141   d  with S↓N (poled s facing up in paper), a 2 nd  member  141   e  N□S with (poled N facing up in paper), and a 3 rd  member  141   f  with S↓N (poled S facing up in paper); and disposed centred within the coil bobbin  105 , is a rotatable about its axis, magnet. From this row and column arrangement is established a “complex-pole produced” three dimensional magnetic flux field encompassing the coil and its winding that is disposed in between the two rows of magnets and the rotatable centre magnet disposed within the coil bobbin (with symmetrically centred hollow core). Ergo, by analysis with the first row members there exists; an attractive static magnetic field between proximal retained 1st row member  141   a  and proximal retained 2 nd  row member  141   b , and an attractive magnetic field between proximal retained 2 nd  row member  141   b  and proximal retained 3 rd  row member  141   c ; and with the second row members there exists; an attractive static magnetic field between proximal retained 1st row member  141   d  and proximal retained 2 nd  row member  141   e , and an attractive magnetic field between proximal retained 2 nd  row member  141   e  and proximal retained 3 rd  row member  141   f . There exists a static attractive magnetic field between the 1st magnet  141   a  of the first row and the 1 st  magnet member  141   d  of the second row distal. There exists a static attractive magnetic field between the 3 rd  magnet member  141   c  of the first row and the 3rd magnet member  141   f  of the second row distal. There is disposed a first changing differential function magnetic field region between the 2 nd  magnet member  141   b  (centre position) of the first row and a first width side of the rotatable centre magnet  112  disposed and free to rotate about its axis of rotation and there is disposed a second changing differential function magnetic field region between the 2nd magnet member  141   e  (centre position) of the second row and a second opposite width side of the rotatable centre magnet  112  disposed and free to rotate about its axis of rotation. Their combined respective magnetic field polarity is arranged in a completed attractive magnetic force circuit, such that in a rest state with no triggering action, the bi-directionally axially rotatable magnet disposed within the centre of the coil winding are in a magnetic equilibrium position (minimum mechanical energy state of the rotatable magnet). 
       FIG.  13    shows the “complex-pole produced” magnetic flux field distribution during a time when the instantaneous rotating of the centre rotatable magnet  112  is rotating about its axis A 2  and the rotatable magnet  112  is in a proximal and perpendicular to the axis of rotation A 2  “attractive-opposite-pole magnetic alignment” with the first row centre magnet member  141   b , and the rotatable magnet  112  is in a proximal and perpendicular to the axis of rotation A 2  “attractive opposite pole magnetic alignment” with the second row centre magnet member  141   e ; and in this instantaneous time the induced output voltage of the generator is going through the maximum induced generator output voltage duration. In addition during this time there is a proximal-distal angular, against the rotation axis A 2 , repelling like pole pole magnetic alignment between the the first row&#39;s 1st magnet member  141   a  and the rotating centre magnet  112 ; and there is a proximal-distal angular, against the rotation axis A 2 , repelling like pole magnetic alignment between the first row&#39;s 3rd magnet member  141   c  and the rotating centre magnet  112 . 
     Simultaneously as shown in  FIG.  13    the “complex-pole produced” magnetic flux field distribution during a time when the instantaneous rotating of the centre rotatable magnet  112  is rotating about its axis A 2  and the rotatable magnet  112  is in a proximal and perpendicular to the axis of rotation A 2  “attractive opposite pole magnetic alignment” with the first row centre magnet member  141   b , and the rotatable magnet  112  is in a proximal and perpendicular to the axis of rotation A 2  “attractive opposite pole magnetic alignment” with the second row centre magnet member  141   e ; and in this instantaneous time the induced output voltage of the generator is going through the maximum induced generator output voltage duration. In addition during this time there is a proximal-distal angular, against the rotation axis A 2 , repelling like pole pole magnetic alignment between the second row&#39;s 1st magnet member  141   d  and the rotating centre magnet  112 ; and there is a proximal-distal angular, against the rotation axis A 2 , repelling like pole pole magnetic alignment between the the second row&#39;s 3rd magnet member  141   f  and the rotating centre magnet  112 . 
     The resultant perpendicular summation of the proximal attractive magnetic forces acting between the first row centre magnet  141   b  and the second row centre magnet  141   e  on the rotating centre magnet and the accompanying magnetic field proximal density induces an AC current within the coil winding  104  and this combined with the angular summation of the proximal-distal repelling magnetic forces between the rotating magnet  112  and the second row&#39;s 1st magnet  141   d  and the proximal-distal repelling magnetic forces between the rotating magnet  112  and the second row&#39;s 3rd magnet  141   f . causes a reduction in the overall rotational torque acting on the rotatable magnet  112  and the advantage of this overall action of angular force vectors that are affected by Ampere&#39;s Law describing the effects of eddy currents within the coil and also the rotating magnet and creating a opposing field vector [∇×H=J (H=magnetizing field, J=current density)] that is the counter emf of Lenz&#39;s Law shown by the negative sign in Faraday&#39;s law of induction, and the Lorentz [F=qvB·sin Θ] Forces on moving charges results in a longer time duration for the damped sine wave when an electrical load is applied to the coil producing voltage. 
       FIG.  14    shows the “complex-pole produced” magnetic flux field distribution during a time when the instantaneous rotating of the centre rotatable magnet  112  is rotating about its axis A 2  and the rotatable magnet  112  is in a “repelling-like-pole magnetic alignment” with the first row centre magnet member  141   b , and the rotatable magnet  112  is in a proximal and perpendicular to the axis of rotation A 2  “repulsive opposite pole magnetic alignment” with the second row centre magnet member  141   e ; and in this instantaneous time the induced output voltage of the generator is going through the minimum induced generator output voltage duration. In addition during this time there is a proximal-distal angular, against the rotation axis A 2 , attractive-opposite-pole magnetic alignment between the the first row&#39;s 1st magnet member  141   a  and the rotating centre magnet  112 ; and there is a proximal-distal angular, against the rotation axis A 2 , attractive-opposite-pole magnetic alignment between the the first row&#39;s 3rd magnet member  141   c  and the rotating centre magnet  112 . 
     Simultaneously as shown in  FIG.  14    the “complex-pole produced” magnetic flux field distribution during a time when the instantaneous rotating of the centre rotatable magnet  112  is rotating about its axis A 2  and the rotatable magnet  112  is in a proximal and perpendicular to the axis of rotation A 2  “repelling-like-pole magnetic alignment” with the first row centre magnet member  141   b , and the rotatable magnet  112  is in a proximal and perpendicular to the axis of rotation A 2  “repelling-like-pole magnetic alignment” with the second row centre magnet member  141   e ; and in this instantaneous time the induced output voltage of the generator is going through the minimum induced generator output voltage duration. In addition during this time there is a proximal-distal angular, against the rotation axis A 2 , attractive-opposite-pole magnetic alignment between the second row&#39;s 1 st  magnet member  141   d  and the rotating centre magnet  112 ; and there is a proximal-distal angular, against the rotation axis A 2 , attractive-opposite-pole magnetic alignment between the second row&#39;s 3rd magnet member  141   f  and the rotating centre magnet  112 . 
     The resultant perpendicular vector summation of the proximal attractive magnetic forces acting between the first row centre magnet  141   b  and the second row centre [∇×H=magnet  141   e  on the rotating centre magnet and the accompanying magnetic field proximal density induces an AC current within the coil winding  104  and this [F=qvB·sin Θ] combined with the angular vector summation of the proximal-distal attractive magnetic forces between the rotating magnet  112  and the second row&#39;s 1st magnet  141   d  and the proximal-distal attractive magnetic forces between the rotating magnet  112  and the second row&#39;s 3 rd  magnet  141   f . causes a reduction in the overall rotational torque acting on the rotatable magnet  112  and the advantage of this overall action of angular force vectors that are affected by Ampere&#39;s Law describing the effects of eddy currents within the coil and also the rotating magnet and creating a opposing field vector that is [∇×H=J (H=magnetizing field, J=current density)] the counter emf of Lenz&#39;s law shown by the negative sign in Faraday&#39;s law of induction, and the Lorentz Forces on moving [F=qvB·sin Θ]charges results in a longer time duration for the damped sine wave when an electrical load is applied to the coil producing voltage. 
       FIG.  15    is a block diagram DA 15  of the “Magnet Array,” which is a novel matrix of magnets in a two row three column, with a centred rotatable magnet and showing the resultant vectors F 1 , F 2 , F 3 , F 4 , F 5 , &amp; F 6  for the magnetic flux lines of force in the present invention with the centre rotatable magnet  112  magnetically interacting with the resultant magnetic flux. 
     The following are the key differences between the magnetic field and magnetic flux. 
     [1] The area around the magnetic field where the poles and the moving charge experience the force of attraction and repulsion is called a magnetic field. Whereas, the magnetic flux shows the quantities of the magnetic lines of force passes through it. 
     [2] The magnetic field is expressed as the product of the magnetic strength and the direction of the moving F=qvB charges, 
     Whereas, the magnetic flux is the product of the field strength and the area around the Φ=BA poles. 
     [3] The SI unit of the magnetic field is the Tesla whereas the SI unit of magnetic flux is the Weber. 
     [4] The magnetic field only depends on the magnet which generates it whereas the magnetic flux depends on the magnetic strength and area. 
     In  FIG.  15    during an opposite-pole transitional period DA 15  where the centre rotating magnet  112  that is poled through its width and has its rectangular width area in a plane substantially parallel to the horizontal plane, and where the first row&#39;s 2 member magnet&#39;s  141   b  axially poled characteristic is attractive to the centre rotating magnet  112 ; and the sectional resultant dynamic force vector F 2  between them are magnetically attractive; and also during this opposite pole transitional period DA 15  where the centre rotating magnet  112  that is poled through its width and has its rectangular width area in a plane substantially parallel to the horizontal plane; and where the second row&#39;s 2nd member magnet&#39;s  141   e  axially poled characteristic is attractive to the centre rotating magnet  112 , the existing sectional resultant dynamic force vector F 5  between them are magnetically attractive. 
     In this same transitional period DA 15  where the centre rotating magnet  112  that is poled through its width and has its rectangular width area in a plane substantially parallel to the horizontal plane; and where the first row&#39;s 1st member magnet&#39;s  141   a  axially poled characteristic is transitionally repulsive to the centre rotating magnet  112 ; and the sectional resultant dynamic force vector F 1  between them are magnetically repulsive; also during this sectional repelling like-pole transitional period where the centre rotating magnet  112  that is poled through its width and has its rectangular width area in a plane substantially parallel to the horizontal plane; and where the second row&#39;s 1st member magnet&#39;s  141   d  axially poled characteristic is repulsive to the centre rotating magnet  112 , the existing resultant substantially sectional dynamic force vector F 5  between them are magnetically repulsive. 
       FIG.  15    also shows the magnetic flux field intensity between 1st row centre magnet  141   b  and the magnetic flux field intensity of centre rotatable magnet  112  separated by proximal distance d 1  and where the attractive force F 2  varies to the inverse cube of the distance d 1 . Likewise the magnetic flux field intensity between 2nd row centre magnet  141   e  and the magnetic flux field intensity of centre rotatable magnet  112  separated by proximal distance d 1  and where the attractive flux force F 5  varies to the inverse cube of the distance d 1 . 
     There is a repulsive magnetic flux resultant F 1  between 1st row 1st magnet member  141   a  and the centre rotatable magnet  112  and separated by distance of F 1  that varies to the inverse cube of the cosine of d 1 ; also there is a repulsive magnetic flux resultant F 3  between 1st row 3rd magnet member  141   c  and the centre rotatable magnet  112  and separated by distance of F 3  that varies to the inverse cube of the cosine of d 1 ; and also there is a repulsive magnetic flux resultant between 2 rd  row magnet  141   d  and the centre rotatable magnet  112  and separated by distance of F 4  that varies to the inverse cube of the cosine of d 2 ; plus there is a repulsive magnetic flux resultant between 2nd row magnet  141   f  and the centre rotatable magnet  112  and separated by a a distance of F 6  that varies to the inverse cube of the cosine of d 2 . 
     Electric Effects 
     All of these flux fields are dynamic and changing with their effective intensity and polarity during a complete rotational cycle of operation caused by a triggering of the generator; and with that complete cycle action there are induced Foucault (eddy) currents that create counter electromotive forces (cemf; opposing voltages) that appear and change within the coil and also in the rotating magnet as well such that these repulsive flux force F 1 , F 3 , F 4  &amp; F 6  producing currents create counter electromotive forces that cancels a portion of the Foucault currents induced in the coil and the rotatable magnet  112  that were initially created by the action of the rotatable magnet  112  rotating within the coil winding  104 . The net effect is the reduce the counter torque on the rotating magnet  112  during operation and this results in the rotating magnet to experience more rotations with less torque drag and lengthens the duration time of the damped sinusoidal waveform and thus generating an increase in power over time. 
     Magnetic Effects 
     Now also in  FIG.  15   , consider only the resultant effects of the relative magnetic pole polarities changing during a complete operational cycle caused by triggering of the generator; as the rotatable magnet is forced into rotation by triggering, and during this transitional phase of rotation there are existing strong major inline pulling forces acting on the centre rotating magnet  112  from the magnetic attraction between the 1st row centre magnet  141   b  and the rotating magnet  112 , plus the existing strong major inline pulling force between the 2nd row centre magnet  141   e  and the rotating centre magnet  112  that, isolated by itself in thought, will see a dragging mechanical impedance on the rotational torque of the rotating magnet  112 ; however, always simultaneously, there are the resultant moderate angular repulsive secondary pushing forces from the 1st row&#39;s 1st magnet member  141   a  and 3 rd  magnet member  141   c  plus the 2 nd  row&#39;s 1 st  magnet member  141   d  and the 3rd magnet member  141   f  all acting on the centre rotating magnet  112  that gives a resultant pushing force to lessen the amount of dragging mechanical impedance on the rotational torque of the rotating magnet  112 , which in causes and increase in the number of rotating cycles before all frictional forces stop rotation. 
     Note 1: the resultant pulling forces are considered major (in strength) because of the proximal (shorter) distances d 1  and d 2  (d 1 =d 2 ), and the resultant pushing forces are considered moderate (in strength) because of the proximal-distal distances (longer) F 1 , F 3 , F 4  &amp; F 6  that all vary as the cosine of the distance d 1 =d 2 .; and this results in the rotating magnet to experience more rotations with less torque drag and lengthens the duration time of the damped sinusoidal waveform and thus generating an increase in power over time. 
       FIG.  16    is a block diagram DA 16  of an embodiment of present invention having a novel matrix of magnets in a two row three column, with a centred rotatable magnet and showing the resultant vectors F 1 , F 2 , F 3 , F 4 , F 5 , &amp; F 6  for the magnetic flux lines of force in the present invention with the centre rotatable magnet  112  magnetically interacting with the resultant magnetic flux. 
     In  FIG.  16    during a like-pole transitional period DA 16  where the centre rotating magnet  112  that is poled through its width and has its rectangular width area in a plane substantially parallel to the horizontal plane, and where the first row&#39;s 2nd member magnet&#39;s  141   b  axially poled characteristic is repulsive to the centre rotating magnet  112 ; and the sectional resultant dynamic force vector F 2  between them are magnetically repelling; and also during this like-pole transitional period DA 16  where the centre rotating magnet  112  that is poled through its width and has its rectangular width area in a plane substantially parallel to the horizontal plane; and where the second row&#39;s 2 nd  member magnet&#39;s  141   e  axially poled characteristic is repulsive to the centre rotating magnet  112 , the existing sectional resultant dynamic force vector F 5  between them are magnetically repelling. 
     In this same transitional period DA 160  where the centre rotating magnet  112  that is poled through its width and has its rectangular width area in a plane substantially parallel to the horizontal plane; and where the first row&#39;s 1st member magnet&#39;s  141   a  axially poled characteristic is transitionally attractive to the centre rotating magnet  112 ; and the sectional resultant dynamic force vector F 1  between them are magnetically attractive; also during this sectional repelling like-pole transitional period where the centre rotating magnet  112  that is poled through its width and has its rectangular width area in a plane substantially parallel to the horizontal plane; and where the second row&#39;s 1st member magnet&#39;s  141   d  axially poled characteristic is attractive to the centre rotating magnet  112 , the existing resultant substantially sectional dynamic force vector F 5  between them are magnetically repulsive. 
       FIG.  16    also shows the magnetic flux field intensity between 1st row centre magnet  141   b  and the magnetic flux field intensity of centre rotatable magnet  112  separated by proximal distance d 1  and where the repulsive force F 2  varies to the inverse cube of the distance d 1 . Likewise the magnetic flux field intensity between 2nd row centre magnet  141   e  and the magnetic flux field intensity of centre rotatable magnet  112  separated by proximal distance d 1  and where the repulsive flux force F 5  varies to the inverse cube of the distance d 1 . 
     There is an attractive magnetic flux resultant F 1  between 1st row 1st magnet member  141   a  and the centre rotatable magnet  112  and separated by distance of F 1  that varies to the inverse cube of the cosine of d 1 , also there is an attractive magnetic flux resultant F 3  between 1 51  row 3rd magnet member  141   c  and the centre rotatable magnet  112  and separated by distance of F 3  that varies to the inverse cube of the cosine of d 1 : and also there is an attractive magnetic flux resultant between 2″ row magnet  141   d  and the centre rotatable magnet  112  and separated by distance of F 4  that varies to the inverse cube of the cosine of d 2 ; plus there is an attractive magnetic flux resultant between 2″  6  row magnet  141   f  and the centre rotatable magnet  112  and separated by a a distance of F 6  that varies to the inverse cube of the cosine of d 2 . 
     Electric Effects 
     All of these flux fields are dynamic and changing with their effective intensity and polarity during a complete rotational cycle of operation caused by a triggering of the generator; and with that complete cycle action there are induced Foucault (eddy) currents that create counter electromotive forces (cemf: opposing voltages) that appear and change within the coil and also in the rotating magnet as well such that these repulsive flux force F 1 , F 3 , F 4  &amp; F 6  producing currents create counter electromotive forces that cancels a portion of the Foucalt currents induced in the coil and the rotatable magnet  112  that were initially created by the action of the rotatable magnet  112  rotating within the coil winding  104 . The net effect is the reduce the counter torque on the rotating magnet  112  during operation and this results in the rotating magnet to experience more rotations with less torque drag and lengthens the duration time of the damped sinusoidal waveform and thus generating an increase in power over time. 
     Magnetic Effects 
     Now also in  FIG.  16   , consider only the resultant effects of the relative magnetic pole polarities changing during a complete operational cycle caused by triggering of the generator; as the rotatable magnet is forced into rotation by triggering, and during this transitional phase of rotation there are existing moderate inline pushing forces acting on the centre rotating magnet  112  from the magnetic repulsion between the 1st row centre magnet  141   b  and the rotating magnet  112 , plus the existing substantially strong inline pushing force between the 2 nd  row centre magnet  141   e  and the rotating centre magnet  112  that, isolated by itself in thought, will see a minimization of the mechanical impedance on the rotational torque of the rotating magnet  112 ; however, always simultaneously, there are the resultant major angular attractive secondary pulling forces from the 1 st  row&#39;s 1 st  magnet member  141   a  and 3 rd  magnet member  141   c  plus the 2 nd  row&#39;s 1 st  magnet member  141   d  and the 3rd magnet member  141   f  all acting on the centre rotating magnet  112  that gives a resultant pulling force to increase the amount of dragging mechanical impedance on the rotational torque of the rotating magnet  112 , however, the resultant effect of the inline pushing forces of the 1 st  row&#39;s centre magnet  141   b  and also 2 nd  row&#39;s centre magnet  141   e  on centre rotating magnet  112  and both the 1 st  row&#39;s 1 st    141   a  and 3 rd    141   c  member magnets along with the 2 nd  row&#39;s 1 st    141   d  and 3 rd    141   f  member magnets, which in causes and increase in the number of rotating cycles before all frictional forces stop rotation. 
     Note 2: the resultant pulling forces are considered here moderate (in strength) because of the proximal-distal (longer) distances F 1 , F 3 , F 4  &amp; F 6  that all vary as the cosine of the distance d 1 =d 2 , and the resultant pushing forces are considered strong (in strength) because of the proximal distances (shorter) F 2  &amp; F 5  that all vary as of the distance d 1 =d 2 ; and this results in the rotating magnet to experience more rotations with less torque drag and lengthens the duration time of the damped sinusoidal waveform and thus generating an increase in power over time. 
     The present invention includes additional magnets in each row disposed according to the teaching of the present invention, and lesser or greater number of trigger receiver tabs and corresponding finger tabs with corresponding modifications to related or surrounding structures to accommodate such additional magnets or tabs. Further modifications and/or substitutions by one of ordinary skill in the art according to the present invention is considered to be part of the present invention.