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TECHNICAL NEXORANDUM #

Sone Psychoenergetic Davices

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pulse would not be efzective in producins the affeet. [owevar, work carried out in England using this approach has revealed very interesting photographs fromn xadiation in the citra-violet.] They mantionod that it was dangerous zo use D.C. rather than high frequency; with high fzeçuency inside the pulse envelope, one can work wich living systcms.

Although a static eleczric field of the same valuc as used in the A.C. systea ( l07 volts/cm) would also yieid cold clectron emission, the situation is not straightforward as strons polarization of the electrodes would occur (elcctroysis). They feel that it is necessary to have a discharge spacias be tweon the specimen and the film in order for proper channel formation to occur (as a result of positive ion clustering around the electron strean). /Thc elcctrons exit froa the surface with different velocities and this includes information about the object. If one uses a D.C. power source, equilihrazion few of electrons pccurs and the image is absent. With D.C., in the firstfwoments an image appcars but then disappears later as equilibration occurs. The H.F. signal is also used in the pulsc so that one can' decrease the size of the equi; ment. The use of different frequencies allows one to obtain quite difforent pictures, presumably associated with different resonances from different cells erc.; i.e., the electrons can come from different parts of tha skin.

Actually, one need use only one pulse to obtain a photograph. The slow pülse repetition rate is to provide low average power. It seoms that a pulse duration of about 2 x l0-3 sec is maxima ard if τ is much larger, the image is poor. On the other hand, if τ is too small, the channel discharge process docsn't have time to develop (for contact photography, one can use 7\~2 x 10 sse). The totol current drown fron the enrire surfece is less than l sep so

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that the sctual curront in a discharge chaanel is nach less. They sugsos: that this is the reason for the stability ož the coid clectror. enission.

larger, of course). Thus, quite smail generstors coing batteries, transforaer. transistors, etc., can ba built and taken out into the field. Hovever, such small generators gonerally do not have as much stability as one would like. -'

It vas stated that any dischárge includes photons but that only discharges in a strong field produce an inage. This seens to reiate to elcccron açcaleration which leads to photon enission. Of course, even the radiation damage effect of the electrons hitting the photographic grains can be expèatec to produce massive exposure of such grains.

(b) In the simplest Kirlian device, shaped like a sanáwich or parailel pate 2
condonscr, the objeet is placed botween the two plates to which voltage is
epplied. If the condenser plates are too close to the object, thera will be
no effect on the film. fn order to get good pictures, thare must be a die-7
lectric gap betwecn the object-and the filma. The exposure tine depends on
the film speed and on the power density of the electric field.

\_To improve the cffect and augment it, a fine scrcen (like a silk screen) may be placed between the object and capacitor plate (and fils). The film is between the condonser plate and the sareen. SThis scrcen enhances the effact, probably by its serving as a dielcctric /One type of effective screer material is film itself that. has been completely exposed and developed.

The device can be placed in a scissors arrangement as illustroted in Fig. 2, the scissors being used to apply a slight but evan pressure via tha paralon (o: sponge) pads. The elaetredee are developed x-ray fil: (Agte  Ap

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and the leads aze fastoned to them as indicated. The dull. catt finisà of. those cleetrodes provides poor reflectivity of iight and thus is an. aić to produciug a good inage. The spacing between object and fils is about 50 microns (caa ba 10. to 100).

To improve the resolution, a layer of saline water or other conduetive liquid is sometimes piaced between the object and the film, In this case, the filn is placed with the emulsion facing eway from the object so that tha emulsion won't be disturbad. The capacitor plate is then piaced outsice of the film. A further improvement can be zade by using the conduetive liquić as oae of the cspacitor plates, thereby permittiag better resolution. and faster work with the fila.

For taking pictures of a seccion of human skin or other part of the body. only onc cicctrode is needed. In this case, the body acts as grourá; i.e., only one half of the device, presented in Fig. 2, is needed. This same electrode procodure is used for the Kirlian microscope, illustrated in Fig. 3, when it is applied to the body. Photogrephs of the one-clectrode davice and the microscope are shown in Fig. 4.

A simple roliing device, which has the advantagc of operating at less than l watt average power, was also deseribed. It is illustrated in Fiz. 5. In this device, ro discharge occurs at points A or C but does occur at poiat B where the spacing is about l0 microns. The cylinder is rolled at about 10 em/min and gives a roving line.discharge to expose the film in sequence. A devicc for taking moving pictures is illustrated in Fig. 6. It utilizes the arrangement of Fig. 2. Controlled veights are applied to the device and sid. fils, is pulled through at some partieuln. speod while the dischizge

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procass is going on. The film is rolled in the usual way end ali is corcained within a casctte.

In Fig. 7, an extremely useful device idca is iliustrated. The previcus mathods utilized rigid capacitor plates which do not ailow oae to teke pictures of ohjoctshaving izregular profiles. In the new method (cescribed in Russian patent \$209958 filed in l965 by Adamenko and Kirlian), the device takes the shape of the body. The trassparent elcctrode is a silicon organic fiim; howcver, many other possibilities exist, With this device, aay portion of ths body can be photographed directly. In facs, one could make a snus-fittins vost or garment of the matezial which could then be monitored photographicaily fron a distance or displayed continuously via closed-circuit T.V.

This new method grew out of an earlicr idca of Kirlian's (pateat #lC-s0s in l963) which utilizcd a conductive trensparent matorial as part of the capacitor, to which a hinged mirror was attached,, and a flexible conductive material which is laid upon the cbject to be photographed. The nirror .is concave and acts as a lens, enlarging the object to be studied. The.mirror is apparcntly used for visual cxamination when not taking photographs. Eetwsen the object and the flexible, transparent condenser plate is placed a dielectric not. A photographic plate is placed over the front or top of the conuuctor so that the prints were merely contact prints wichout' focusing. 4

The foregoing devices all operate in air at l atuosphere pressure. If the pressure is ruduced to l0-s πn ož mercury, the image is still retainec even with the clectrode scparation. inereased to 20-30 cm. At a pressurc o 10- ma of mercury, the image disappcars. A visuai display systen usins raaching like a television tobe Ls illestratd ir. Pig. 8. In this OT ¿evi:

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cleetrons from the objest iapinge on a 200u-thick dialectrie fila cnd thelr 1：
charge pattera induces charge poiarization on the other sice os the Eilm vkist
in turn, affeets the prezerencial geometry of elcctron emission from the
Thus, the eventusi image on. the soresn is indead that of che objact. Thís is
a very important phenomenon which allows many interesting Fodifications of
device design. :

The wethods have been developed for image explification (magnificatioz). In the first case, they use cold emission obtained in the small spazing.davice (50) of Fig. 2 with a high electric field at the edges, $z _ { e } \sim i \pi V _ { 1 } = \cdots$ However E is causod to dacrease in the middle to Ey\~ losV/ca (see Fis. 9a). Tous, the megnification, μ, is given by

$$
\begin{array} { r c l } { \dot { \mathbf { z } } } & { = } & { \displaystyle \frac { \mathbf { \vec { z } } _ { \mathrm { e } } } { \mathbf { \vec { z } _ { \mathrm { i } } } } } \end{array}\tag{1}
$$

They have obtained values of μ\~ 340. The second method is carried out in ε CRT type device as illustrated in Fig. 9b. The short electrode (cathode) hes a field $\Xi _ { \Im }$ and the larger electrode (anode) has a field $z _ { 2 } ( z _ { 3 } \sim 2 0 ) \sqrt { 2 }$ $E _ { z }$ is saaller). In this case, the magaification, μ, is given by

$$
u = \frac { z _ { 2 } } { z _ { 2 } } = \frac { s _ { 2 } } { s _ { 2 } }\tag{2}
$$

where $\mathfrak { s } _ { \mathtt { r } }$ and ${ \mathfrak { s } } _ { \mathfrak { z } }$ are the tensions of the two electrodes $( S _ { i } E _ { 1 } = S _ { z } E _ { z }$ froa Gaess' 3.
law and charge conservation).

Using the T.V. tube type of device, one might cxpect that the cse of clectron lenses would allow one to build an clectron microscope with very bish magnification. lowever, because of the high vacuum needed in such a device, a oevere limttetion exists, As jor7 - loe qa o5 cercuzy prersure, ine cer

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no image bocause of the loss of channeling ions but at io-\* . l0-s um Ns, cne docsn't even need a lens. [The use of the dielactric imprinting tochniquc may be a heipful aić hore.]

In concluding this saction, it was noted that, if e person's fingerprints wore sanded oii, the Kirlian photographs still zevealed the criginal L fingerprints, Likewise, if 2 to l0% of a leaf has been cut away from one edge, the entire radiation pattorn of the unaltered lcaf was still revecled in the Kirlian photograph. [It would be useful to perform the exporimant by cutting successive strips fron the leaf and photogzaphing in order to ses what percontage of the leaf can be removed without an alteration in the total radiation pattern. Dr. Adanenko suggested that the number of radiation sources in the leaf or finger may be so numerous as to produce sufficient rodundancy of iniormation that, if a portion of the leaf or skin is removed, the lost sources do not significantly disrupt the multiple array pattern.

2. Acupuncture and the Tobiscope

Although it was not possible to obtain a circuit desiga for the Tobiscope described in Ref. 1, it is possible to piece together çonversational information and propose critical circuit desiga features from which a persoa, skilled in.electronics, could make an instrunent. Nost simply, the device is a D.C. aaplifier with a high input impedance and is battery powered. Very likcly, the extoraal skin impedance is arzanged to be placed in parallel. with the input impedanee of the Tobiscope.. Thus, if the skin impedance is reasonably large, the total operating input impedance is unaltered by increasing the shts puth lcogth. Hosever, if a mnber of locatiors ere found wiieh

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produce shuating or shozt cireuit paths of low iipedanco, thoa the efzuctiva iuput impedance of the devics is significantiy lowercd. For contact vich such points, the enrrant Soving througà the device will be grcatly inercased and the curzozt change (or voltage change) zay' ba multiplied by the D.C. amplifier to a sufficient degree to light a bulb in tha hoad of the device. The illunination of this light signals the location of a shunting path or an 1 acupuncture point.

The device operates on less thaa 1 aiero amp at 4 volts with the 3 transistor D.C. amplifier baing very stable over the voltage range of l.3 to.3.5 volts. The input resistance is about 4-5 x 10ª ohms and the devicc neads dry skin to be effective ia locating the scupuncture network points (vet, saity skin leads to surface shunt paths). It is found thzt a resistance of about 50 x 103 ohas exists between these nezwork points and that the valuu iaercases greatly during sleep. The equivalent resistance over the same length of skin botwecn two non-network points is in the range \~l0 ohas. At present, they are investigating an alternating current device and find that vory interesting effects occur in the region of 1 K per second (since one now sees the imaginary part of the impedance).

The D.C. resistance between one acupuncture point and another is about 5Q. KO for two adjacent network points and varies slowly, as the distauce betweca points increases, to about l00 K. The saae range of variation occurs due to cmotional change, light stimulus, ete. The'procedure here is to use a suall current and a bridge balance method, As pointed out by Adamenko(2) in tho cose of emotional excitation the points vary in diameter (as revealed by conductivicy czaa) and there is the posrisility of tha arens ovarlappins

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Again, it must be omphcsiuad one asocher to form higà conduczivity chat measuxesenrs aro moaniogãul only on dry akin,

Tay aave invoetagated the variation of condeetivity detveen the rataor? poinns according to the pationt's condipion ia bypdonis (see Fig. l1). The conditions or states of hypnosis are listed alons the abseissa as: () criinary state, (2) slcep with closed eyes, (3) sicep with open eyes, (4) sugzestion of hellucinations, (5) "artificial reincarnation", (6) vork in "reincarnation" state, The four graphs show variations in four groups of sybjects ranging from control group A (those not hypnotizable) through B, C and D in increcsing order of hypnotizability. As seen from the graphs, there exists a certsin relationship Setween the patient's hypnobility and the chazacter of conductivity variations. In the control sroup, no conductivity variazion has been recorded vwhich indicates the absonce of emotional raactions to the hypnotist's words. However, in the case of ordinary enotional states, thcse patients exhibit conductivity variations.

It has also been discovered that & voltage signai can be detccted between two network poines provided two different types of metals are used as electrodes. On dry skin, using plated circular electrodes of 5 to 7 mm dia 六 eter, a Ni-Ag combination yieided s potential difference of about 50 mv. skin jocations vhere such points are absont, the potential differonce is clo to zero, Likewise, betwoen two network points, using the sana electrode me. torial (Ni-Ni or Ag-Ag, say), the potential diffcrence is again close to zero It is sufficiant to place.cu eloctrodes with Ni or Ag (they use chrome-Ni e: chroac-Ag). Adamenko finds that, the greater the work function difference, Ap. berms tae eteesrele aitartaia, tre crerter the voltage, AV. devaleped

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They thiak that this is a galvanic call. effect with the channoi. of ueridian botveen the two network points ceting as an cieetrolyte (like a Zh-Za bastery). The curxent drava frou this battery is about 10 uiero-aups; hovever, this Tae cuc

current level polarizes the electzoses so they use an impedance to reduce tha current level to about 2u axps and then axplify the signai for display purposes In cases of cnotionai-volitive excitation, the potential difference AV may in-1
Using parallel connections between several netcrease up to 100 millivolts.
work points, the voltage obtained may be as high as 0.5-l voit and the current accordingly increased up to soze saturation limit (L l0pA fox 1 pair, L" 18pA for 2 pairs, ete.). They feel thar this high curront drain could be dangarous to the body. This netvork potential difference has been used to power'a simple transistor radio and a small toy vehicie.

They find that, as the clectrode area, A, increases, the developed voltage, V, increases. They also find that an A.C. pulse is diminished as the arec of the clectrode incrcases. This is illustrated in Fig. 12 as a piot of V vs. tine; it probabiy represents an sveraging phenomenon, .wherein the A.C. signal arises only et the acupuacture point (loss than l ma in diameter) in the central region of the electroda and potential averaging occurs.

In Fig. l3, the dependence of seniconductor properties of asupuacture points on the physiological state of the internal organs conmnected with these points is given. The vertical scale shows.the difference in resistance (dR) betwcen syumetricai poiats in the direct and reverse directions. Each verticai line represents a particular acupuncture connection. Curves 1 and 4: "healer" before and after trdataant. Curves 2 and 3: "petient" before and efter treatwat.

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To festen electrodes to à plast, gius can be vsed. To iastan eleceroto. to huaasns, around the head for axampla, en open heluot is used vhieh coniains serew contset eloctrodes that caa be moved about and broughe into lighe but constont prassure contact.

/ An inzerestins testing or training Cevice, using a cylindzical cspacitor of the type illustrated in Fis. l4, was mentioned. One hand was placed on tho A casins grasping the cylinder in a natural way (sone acupuncture points toue! the alusinua can). The thuab and forefinger of the other hand hold the ceatra? contact post (acupunctnre points in finger touch the siiver-plated coutact). The capacitor is held in this way for one minute of charging and it is then discharged through a nicrosmacter yielding a Eaxirua. signal I, say. Noxe, charging again occurs for one sinute,but this time the iavestigator also men-5 tally concentrates on charging the capacitor. The maximum discharge current is Ia, say, yielding à ratio K = I./I, - the greater is K, the greater is the ability to use one's uind ia controlling the energy body. The imagination. of stress (or actual muscle tension) or excitement doring this one-minute period can bc used to alter Ig. Using a 30 nicrofrared capacitor,the author found I ≈ l0gd; a larger cepacitor (up to 10,co0uf) vould probably be better. This simple devicc can be used to study one's ability to concentrate and focus the mind and by practice, oneshould be able to increase K significantly. It was statod that Alla V, the PX performar, is able to produce K = 9 without tqo muc difficulty.

3. Telekinesia (P)

They find that the placing of a filn on Nelya K's head during. the PK esperiaast leels to the prancnae of a larga esposed epot on the fue, They

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slso find that fils expostze oseurs if the fila is placud under tho objeet used in a Pk éxperiuene. In addition, the fiim may also be exposed airor exporiment due to a residuci chargo ož some sort on the ooject. Ve hoard Nelye K actuallycaused a frog's hoart to stop(and that it then could not started sgaia electricaliy). We also learsed that she can influence the h rhytha of otherpeople and can alter their skin condition so as to produce 1 burning fecling on contact. They have found that hypnosis can be used to hanee PK abilities and that autogenic trainins was used to holp inerease / PK abilities. It was also statcd that Nelya K cannot zove objects if the in a vacuum and that after the levicatior of ε snall ball in air, an elec static charge of 5 x 105 coulombs was fouad on the ball.

It was not possible to odtain any specific information concerning th Sergeyev detector of pulsating magnatic fields in the vicinity of the pX However, it is likely to be the dotcction of a magnetic ficld using a sen It vas lcarned that plants make elcnent of the barium tiranate variety. better detectors of the-PX fields, when electrodes are applied to two aci ture points of the plant/ Using 5 mm diameter elcectrodes of Ni and Ag, obtain about 50 mv betwcen two points which is aaplified. During a PK e ment, current pulses occur vhich change frou 5 mA ambient to over l00 a4 pulse peak (see Fig. 15).

They bave not fully studied the distzibution of field strength betw the operator and object during 2K and find i\* to be a difžicult questior field intensity does increase as one 'reaches the object but probably no the radiatioa type code illustrated in Fig, 16. They. don't know what ty Zeld pattorn esires on the otter side oi the objaet crd soen to thint

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the fozee fs somahow just manifest in tae viciaiey ol the cbject wi gible intervenias field linkages beztcon the oporator and object. of the rollina eylindor ssed ia che 2 expzvimants by Alla V, Aéame that a charge dipole ioras, as Miustrated in Fig. 17, which givas such thes one coulá cove the objeet in eicher directioa depending o held his hand. [This is not clear to me either.]

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7 T= 17-21

to jenerstir paraton (er qpeage) electredes Serssers clomp objet 50 ipcs phetngrphe filn Cemmolrion sode t dpe ) enend phtapple fh

oljiit ↓. Elccirrdes film

polh  weigtts f onrill Capasfr cevice

Trans perent Elrí dete Eleetinde 2oyn Spece patiint

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Fis. 3. "Discharge - optical housing

3. Upper hat2 os hoeskog

4. Pn for focesing

5. Eread

6. Lower half of housing

7. No orifices (φ 4sa) disposed one in of the ocher

3. Rubber washer

9. Csncact to power source

10.Xazallic viro (for protecticn cgaiast circuit disruption becausa of water evaporation)

1i. Thickeniag in fora of a ring

12. Pressirg cut, freely revolving

13. Collers

14. Thread

.15. Treverse

16. Orifice  5ma

17. Bottom of the traverse

18. Glass wich thickness 0.6-1.Giza

19. Glass with thickaess 0.13-C.l4mz

20. Chanber (cell), flooded by water throve ozifice 7

21. 8-12 times odjective

22. Bushing vhich carries objective

23: Thread (in accordance with aicxosccpe tube thread)

Fiz. 4

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で 111 Ee EM. Ec

Fi9

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cdedrde

Tot casing

Fi

二 三 ray二 三 energyopereter Objed. 一

1