______________________________________________________________________________ | File Name : TOMIMOTR.ASC | Online Date : 04/30/95 | | Contributed by : Stefan Hartman | Dir Category : ENERGY | | From : KeelyNet BBS | DataLine : (214) 324-3501 | | KeelyNet * PO BOX 870716 * Mesquite, Texas * USA * 75187 | | A FREE Alternative Sciences BBS sponsored by Vanguard Sciences | |----------------------------------------------------------------------------| The following file was sent to me on the InterNet by Stefan. ------------------------------------------------------------------------------ Return-Path: Received: from uropax.contrib.de by ix.ix.netcom.com (8.6.12/SMI-4.1/Netcom) id OAA23352; Fri, 28 Apr 1995 14:40:35 -0700 Received: from shb.contrib.de by uropax.contrib.de with uucp (Smail3.1.28.1 #3) id m0s4xLx-0007bbC; Fri, 28 Apr 95 23:13 MET DST Received: by uropax.contrib.de from shb (policy router $Revision: 1.22 $) id <799103612.1522>; Fri, 28 Apr 95 21:13 UTC Received: by shb.contrib.de (CrossPoint v3.02 R/A2148); 28 Apr 1995 23:12:21 +0100 Date: 28 Apr 1995 22:58:00 +0100 From: harti@shb.contrib.de (Stefan Hartmann) To: keelynet@ix.netcom.com Message-ID: <5kjBHpHPldB@shb.contrib.de> In-Reply-To: <199504281534.IAA17307@ix4.ix.netcom.com> Subject: Re: Howdy! X-Mailer: XP v3.02 R/A2148 MIME-Version: 1.0 Content-Type: text/plain; charset=us-ascii Content-Transfer-Encoding: 7bit PM_Square enhanced : The new free energy generation device ! ============================================================ Latest news: ------------ 1. MPEG movie now available at: 194.77.35.1 in pub/harti/energy/PM_Square/pm_sqlin.mpg about 485 KBytes. Shows, how the Linear Mode works with multiple stator tracks ! Could be used to propel a train along a railway ! 2. A new Enhanced Linear version shown down there ! ===================================================================== Hi, do you remember the TOMI (also called TMI) device ? Well, I have worked together with the inventor and another "magnet freak" during the last weekend on the design and we found the solution how to power a motor just via using Permanent Magnets ! I will call this design from now on: PM_Square = (PM)^2 Permanent Magnet Powered Motor ! = = = = Well, here it is how it is working: I will first describe a Linear Motor design and later post a few MPEG movies of the enhanced rotor version experiments... I will publish all my results and findings, so you are ready to duplicate it yourself and prove me right or wrong. This way the basic design goes to the Public Domain and can't be bought out or will be suppressed... I just claim the inventor rights on the Angle Steel add-on design ! Please copy this file to all people, which care about environment pollution and want to have a so called "free energy" machine. For the full understanding of this PM_Square design you should have read the TOMI description ! Here the PM_Square design goes: The most important enhancements over the TOMI design are introduced via 2 angle steel plates at the endings on each track-magnet (in the TOMI description called: Runner-magnet) I will call these "Runner-Magnets" from now on Stator Track-magnets, because they don't "run" , but are just the Stator-Magnets, which build the track ! Okay, so how are these 2 Angle Steel plates fitted to the Track-Magnets ? Here is a simple ASCII drawing: Top View ======== ____ ____ | track magnets (stator) | <-----Angle Steel |_____ _____ ___________ _____ ______ ______| at each ending ! | | | | | | | | |N S|N S|N S|N S|N S|N S|N S| |_____|_____|_____|_____|_____|______|______| ------->| Roller Magnet dropped into the track from above at 90 degrees at this place ! ----- | N | | S | ----- | N | | S | Roller Magnet, ----- rolls this way --------> | N | along out of the track ! | S | ----- | N | | S | ----- ------->| Roller Magnet dropped into the track from above at 90 degrees at this place ! _____ _____ _____ _____ _____ ______ ______ | | | | | | | | |S N|S N|S N|S N|S N|S N|S N| |_____|_____|_____|_____|_____|______|______| | | <------Angle Steel |____ track magnets (stator) _____| at each ending ! This is the Top View of the Linear Motor design ! All magnets used are circular magnets. So the Roller Magnet can roll through the track ! The number of stator track magnets can vary, but should not be too many , cause it weakens the flux inside the track. Go for around 7 to 10 magnets first. (7 are shown over here !) By using Angle Steel plates of ST37 or ST100 (thickness of about 1 to 2.5 mm), one can force the magnetic flux at the endings of the permanent magnet Stator Track to be going the right way! In this case it prevents to pull the Roller Magnet back into the track, when it leaves the track at the right side ! You can also try to use a "V"-shaped placement of the Stator Track magnets (not putting them in parallel as shown, but at an opening angle of maybe 5 to 10 degrees), which I can't draw over here with this simple ASCII-"art"! This enables the Roller magnet to get out of the Stator Track at the ending even better and the killing force at the end of the track is far more weaker ! One has to drop the Roller Permanent Magnet for the best performance (acceleration) into the track at around 90 degrees (also 45 degrees would still work!) at around 1/5 to 1/4 length of the track. This way, the Roller Magnet is just pulled into the track and don't have to go via the slight repulsion gate at the entrance of the track at the very left side ! With using the steel plates fitted to the end of the track magnets you can also try to push the Roller Magnet into the track at the left side, but it will almost kill the received acceleration force from the previous track ! But with using the Angle Steel plates, this killing effect is much less, than without using the Angle Steel plates... So the secret to a Real Working Linear PM_Square motor are just these Angle Steel Magnetic Flux guidance plates ! The best design to get the Roller going through an unlimited number of Magnet Stator tracks would be the following design: Side View: ========== Roller Magnet climbing the hills -----> going this direction --> | | wooden cardboard downhill track | | (without any stator magnets !) | | | __ | __ | / \ | / \ \ | /--. \ \|/ /--. \ \ | / ; \ / ; \ \ \|/ / / \ / / \ \ / \ / \ \ o / ^ ^ \ / \ \ / | | \ / \ / / | | / / / | | / / / | | / / <___ | | <___ <__ | | ^ | | | | Angle Steel Angle Steel | Stator magnet track ______________________________________________________________________ This Linear Motion Permanent Magnet Motor design should really work. It uses the gravitational force to go downhill into the next magnetic Stator Track. In this Side View only the front Stator magnet is shown with the Angle Steel at each end with the "wrong" angle drawn, due to the bad perspectivic drawing view !(I am not able to draw it better with using this ASCII- "art" ! Normally in the Side View the Angle Steel Plates would point into direction of your face and not downwards ! But I have drawn it downwards to make it clear, where the placement of the Angle Steel is located !) Have a look again above to the Top View and it will getting clear to you, how the Angle Steel has to be placed ! Enhanced Linear Motion version: =============================== Side View: ---------- Roller Magnet climbing the hills -----> going this direction --> | | wooden cardboard downhill track | | (without any stator magnets !) | | | | | # # | # # | / / | / / | /\ /\ | /\ /\ \|/ / \ / \ | / \ / \ o/ \ / \ \|/ / \ / \ \ / \ / \ / \ / \ / \/ \/ \/ \/ \/ / / / / / # # # # # /|\ |_______ Angle Steel plates at each ending of the Stator Magnets ! In this enhanced Linear version you use only the "phase" inside the stator track, that really accelerates the roller magnet. The fields at the beginning and ending of the Stator magnet track are not used ! The roller magnet can thus come into and out of the accelerating Stator Track without any killing force. The roller will just be accelerated each time it goes into the next hill ! Okay, so far for now. Please try to duplicate this Linear Motion design of PM_Square and let me know, if it will work for you. If you have any question, please drop a note to my email account at: harti@contrib.de or harti@b-2.de.contrib.net You can also have a look at my FTP site at: ftp://ftp.b-2.de.contrib.net in pub/harti/energy/pm_square (194.77.35.1) or into pub/incoming There will be soon a few MPEG movies of my experiments with this PM_Square device ! Theoretical explanation: ======================== I received this from an "anonymous" friend. Please read it and let me know what you think about this theory for the explanation of the TOMI and PM_Square effect ! I believe, that with using Permanent Magnets the Zero Point Energy can be tapped ! (See Dr. Harraold Putthof's explanation of Zero Point Energy) Irreversible Processes in Fields ================================ It is well known theory that the thermodynamic potentials go to an extremum. This is regarded as equivalent to Planck's 2nd law although the complete equivalence between both formulations of the second law never have been proved generally, especially if we apply the extremum principle of the thermodynamic potentials to electromagnetic fields. In this article we investigate this question. I. Irreversible Processes in Vapour-Liquid Mixtures We begin here with a well known and quite trivial example. We regard two cylinder volumes connected by a tap in the middle. Both the volumes can be set by moving a piston up and down into or out of the volume. With this experimental setup we proceed the following isothermic irreversible cycle, comp fig.1a):We take a fluid (for example water) being at the dew line of the phase diagram. We expand both the pistons isothermically from point 1 to point 2. So liquid condenses and is collected in the lower cylinder. Now the tap is closed and both the volumes are recompressed at equal pressures until the starting volume is reached again. Now we regard the question whether Planck's law is fulfilled. This question can be answered by writing the 2nd law for free energy which states that the free energy F tends to be a minimum. Therefore, if we leave the minimum in doing the cycle Fstart-Fend = - circle integral P dV > 0 must hold because the cycle is isothermal (dT=0) with no matter exchange (dn=0). The orientation of the integral shows that Planck's second law holds, comp. fig.1b). II. Irreversible Processes in Fields a) General According Landau and Lifshitz (1) the free energy of a system including electric fields and linear dielectrics is defined by F'(V,T,D) = F(V,T) + 1/(8*Pi*eps) Int D^2 dV The Legendre transform of this potential is F''(V,T,E) = F(V,T) - eps/(8*Pi) Int E^2 dV Both these definitions are not useful for thermodynamics because they are non-homologous functions regarding the molar ratios. Therefore, the following definitions are used and specified for constant dielectrics f'(V,T,P) = f (V,T) + 1/(8*Pi) Int E dP = f + 1/(8*Pi*Xi) P^2 f''(V,T,E) = f(V,T) - 1/(8*Pi) Int P dE = f - Xi/(8*Pi) E^2 Regarding the 2nd derivative of the electric variable of both these potentials we see that for a constant homogene dielectrics f'(V,T,P) approaches a minimum and f''(V,T,E) approaches a maximum in the equilibrium state, if Xi > 0. Similar considerations hold for magnetic fields as well. b) Mixing Processes Now, similar like in section I, we investigate an isothermic and isochoric cycle if an intense field is applied to a non ideal - non linear binary dielectric liquid (2). We start at the phase separation line at low field and apply a stronger field. Then demixing of the solution occurs. We close the tap and discharge the field. In the endpoint of the cycle at lower field we reopen the tap and return to equilibrium. Because we leave the equilibrium in performing the cycle the unequality df'' = - circle integral P dE < 0 holds according the last lines of section II a). Regarding the orientation of this integral we realize that it is a negative hysteresis relative to the usual ferroelectric hysteresis. Therefore, our consideration predicts a violation of Planck's second law for electrically induced irreversibilities. The irreversibility goes the other way round according to the Gibbs formalism contrary to Planck's 2nd law. c) Permanent Magnet Motors In Landau/Lifshitz (1) there exists a proof which shows that if we introduce a para- or ferromagnetic body into a fixed magnetic field (j=constant) the following relation holds: df' = - M dH Because df' approaches a maximum we interprete this equation that a self accelerating perpetual motion is possible in a magnetic field as an irreversibility. Therefore, in order to find an example we first rule out the conditions under which a perpetuum mobile is impossible. This is always the case if the magnetic field can be described as a potential field. According Jackson(3) a magnetic field of a closed loop or the field of a hard permanent ferromagnet can formally be decribed by a potential. This means that rot B vanishes. This has as a consequence that a perpetuum mobile acceleration of a magnetic charge is impossible.Therefore, the question arises whether there exists the possibility to break this zero rot B - field. The question can be answered positively. Using by Mu metal shieldings a non zero rot B field can be generated from a potential field by shielding off the unwanted parts of the field . We illustrate this idea by the following axial motor construction proposal which is derived by us from the linear Harris TMI set up (4), comp. fig.3)+b), which works and which has been confirmed and discussed by different persons(4,5). We do not claim that our proposal is a perpetuum mobile. We use a cylindrical tube of Mu metal as housing for the motor. In the housing tube we have a tube of lower diameter made from conducting material having the same axis as the housing tube. A current flows in the inner tube along the length equally distributed across the thicknell of the wall.The common axis of both these cylinders consist of a wire carrying a current flowing in the opposite direction relative to the current tube. If we look at the configuration of the field we have a circular non vanishing rot B field in one direction near the wall and a circular B field in the opposite direction near the central wire. Now we use the wire as an axis of a rotor which carries at least two symmetrically balanced permanent magnets rods whose north poles point radially and the south poles axially. The north poles are standing under the influence of the B field near the wall, the south pole feels the opposite field near by the wire. So a permanent torque is exerted on the rotor which begins to spin around the central wire as the axis. We see that our motor works only with permanent fields and needs no brushes. Therefore, the question arises: Is it not possible to use permanent magnets + Mu metal shields to replace the current wires by permanent magnets generating circular non vanishing rot B fields of opposite orientation to get the rotor spinning, comp. fig.5a). Similar constructions are already patented and can be found in the literature (6), comp. fig. 5b). Furthermore, we emphasize that until today there exist no generally accepted magnetic force law between differential current loops. Only for closed current loop the situation is clear, because all the different differential form coincide in one. Different forms have been proposed by Biot Savart (7), Ampere (7) (includes actio and reactio and conservation of angular momentum), Whittaker (8) (includes only action=reaction), Aspden (7) (includes only conservation of angular momentum) , and Marinov (9). Marinov claims that he would have proved experimentally his form as the correct one. Therefore, there seems to be an interesting field where important questions can be solved. Bibliography: 1) Landau L.D., Lifshitz E.M. Electrodynamics of Continous Media Pergamon, Oxford, 1984 2) Wirtz D., Fuller G.G. Phys.Rev.Lett.71, 2236, (1993) Debye P., Kleboth K. J.Chem.Phys.42, 3155, (1965) 3) Jackson,J.D. Classical Electrodynamics 2nd edition John Wiley, New York, 1975 4) Decker, J. BBS Keelynet PO-Box Mesquite Texas USA 75187 Modem ..214 324 3501 Filename: TOMIBILD.ASC harti@shb.contrib.de TMI device, free energy device ? 24.2.95 in ALT.SCI.PHYSICS.NEW-THEORIES 5) anff@qvwp.demon.co.uk TMI device, free energy device? 26.2.95 in ALT.SCI.PHYSICS.NEW-THEORIES harti@shb.contrib.de TMI + MRA updates, free energy 25.2.95 in ALT.SCI.PHYSICS.NEW-THEORIES harti@shb.contrib.de TOMI enhanced ! Free emergy device ! 31.3.95 in CL.ENERGY.ALTERNATIVEN prebys@puhep1.princeton.edu TMI device, free energy device ? 25.2.95 in SCI.ENERGY 6) Johnson, H.R. Permanent magnet motor U.S.Patent No. 4.151.431 Apr.24,1979 7) Aspden, Harold Physics without Einstein Southampton 1969 Aspden, Harold Modern Aether Physics Southampton 1975 8) Whittaker, Edmund Sir A history of the theories of Aether and Electricity Vol I The classical theories Humanities Press New York 1975 9) International Glasnost Journal of Fundamental Physics Vol.3, No.11, Marinov, Stefan; p.18 _________________________________________________________________ Figures: || || || | || | |======| | || | |======| | | |======| | | | | | | --- --- --- --- --- --- | | | | | | | |---| |--|-| |--|-| | | | | | | --- --- --- --- --- --- | | | | |//////| |======| |//////| |======| | || | |======| | || | || || || 1 2 3 fig. 1a): Isothermal cycle of a simple fluid with irreversibility 1 starting a the dew line 1-2 expansion, condensation of liquid 2 separating volumes by closing the tap 2-3 recompression 3 opening the tap, work has to be added to proceed the cycle P ^ 3 ._ r | | |_ e | | |_ s | | |_ 3 s | 1 ._ |_ u | |_ |< r | |__ |_ e | |_>_ |__ | |___.| | 2 | | | | | -----------------------------------------> Volume fig. 1b): Isothermal cycle of a simple fluid with irreversibility Pressure-volume diagram: 1 starting a the dew line 1-2 expansion, condensation of liquid 2 separating volumes by closing the tap 2-3 recompression 3 opening the tap, work has to be added to proceed the cycle ^ P | o | l | a | r | 2 i | -------. s | __| ____| a | 1 _>_| _<_| t | .__| __| i | | __| o | .__| n | 3 | | | -----------------------------------------> electric field fig.2: isothermal cycle with electrically induced irreversibility 1 starting at the phase separation line with low field 1-2 applying a field 2 closing the tap 2-3 dicharging of the high field 3 opening of the tap and returning to starting point 1A negative hysteresis is predicted according the Gibbs formalism. _ _ _ _ _ Top view S |_|_|_|_|_| N <--------moveable ROLLER magnet direction S |<--track-->| N of ROLLER ____________|____________ | | ___| | |___ | | | |___| (start) |___| | | | |___| |___| | RUNNERS | | |___| incline |___| <--------roll of magnets,positioned at | | |___| |___| | the same angle as the slope of | | |___| |___| | the incline \|/ | |___| |___| | | |___|____________|___| | | N | | S | | | decline | |<-------no magnets here, but not as much | S | | N | space between the rolls as shown | ___|____________|___ | | |___| |___| | | |___| |___| | | |___| incline |___| | | |___| |___| | | |___| |___| | | |___| |___| | | |___|____________|___| | | | | | | N | decline | S | | | | | | |____________| | | (finish) |<-------ROLLER winds up here |________________________| fig.3a) the TMI device, top view the two magnets along the incline are stationary, the magnet in the middle begins to roll standing under the influence of the stationary magnets. It is drawn over the fulcrum. There it rolls down under the influence of gravitation until it reaches the bottom of the second hill. Side view ! (enhanced version !) =========== ROLLER starts here \|/ | ----------------> direction of moveable magnetic ROLLER | /\ /\ | / \ / \ | / \ / \ / \ / \ /-------------- / -------------- <--------Magnetic ROLLER ends up / / here fig.3b) the TMI device, side view comp. textthe two magnets along the incline are stationary, the magnet in the middle begins to roll standing under the influence of the stationary magnets. It is drawn over the fulcrum. There it rolls down under the influence of gravitation until it reaches the bottom of the second hill. ___________________________ / \ / \ Mu metal / \ housing / \ / \ / \ / _______________ \ / / -------> \ \ | current / B-fields \ | | tube / | \ | | / | \ | | | /---------|----------\ | | | | / _______ <-- ________ \ | | | | ||S N| /-\ |N S|| | | | | ||_______| \-/ |________|| | | | | \ axis wire / | | | | \--------------------/ | | | \ rotor / | | \ \ / | | \ \----> / | \ \ ___________________/ / \ / \ / \ / \ / \ / \ / \_____________________________/ fig.4 magnetic motor with no brushes; top view the magnet charges on the rotor are spinning around the axis wire in the stationary double circular and opposite rot B fields of the wire and the current tube. fig.5a) our magnetic motor proposal using only permanent magnetsthe central wire is replaced by an inner ring consisting of permanent magnets and Mu metal shields generating an non vanishing B-field; the current tube is replaced by an outer ring of permanent magnets and Mu metal shields. the rotor is the same as in fig. 4. The field configuration seen by the rotor is in effect the same as in fig.4., only both the opposite non vanishing rot B fields of the stator are generated by permanent magnets. Unwanted parts of the field are shielded by Mu metal. It is clear that the configuration can be multiplied to enforce the power by taking more circles. Magnets similar as used by Johnson are recommended for the stator fields, comp fig.5b). Using electromagnets instead of permanent magnets would enhance power. fig.5b) the Johnson motor, US Patent Nr. 4,151,431 permanent magnets as stator, rotor with non vanishing rot B -field , see original patent disclaimer regarding employer Anti-Copyright - can be copied by everybody for nothing Berlin, Germany, on the 4th of April 1995. Best regards, Stefan Hartmann. -- Hartmann Multimedia Service Dipl. Ing. Stefan Hartmann Keplerstr. 11 B, 10589 Berlin, Germany Tel: ++ 49 30 344 23 66 FAX: ++ 49 30 344 92 79 email: harti@contrib.de harti@b-2.de.contrib.net Web access: http://www.b-2.de.contrib.net/harti/harti.html -- Hartmann Multimedia Service Dipl. Ing. Stefan Hartmann Keplerstr. 11 B, 10589 Berlin, Germany Tel: ++ 49 30 344 23 66 FAX: ++ 49 30 344 92 79 email: harti@contrib.de harti@b-2.de.contrib.net Web access: http://www.b-2.de.contrib.net/harti/harti.html ## CrossPoint v3.02 ## ------------------------------------------------------------------------------