T.galen Hieronymus - Radionic Pioneer

7/23/2019 T.galen Hieronymus - Radionic Pioneer

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Journal of Borderland Research >> Vol. 44 >> No. 03

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T. GALEN HIERONYMUS - Radionic Pioneer November 21, 1895 to February 21, 1988

We mark the passing of r! "homas #a$en %ieronymus &ho &as a

true pioneer in the fie$' of ra'ioni(s! r! %ieronymus &as a 'is(overer of

uni)ue attributes of the $ife for(e &hi(h he terme' *e$opti( energy*! %is&ork stimu$ate' (ontinuing resear(h in ra'ioni(s, an' his patent No!

2,482,++ has be(ome a stan'ar' (on(ept &hi(h many ra'ioni(

instruments have been bui$t from, some using -ust the pattern 'ra&n on

paper! .eop$e &ith origina$ thoughts are fe& an' far bet&een! #a$en/s

presen(e on this earth has inf$uen(e' many to $ook beyon' the norm an'

0or'er$an' (ien(es esear(h Foun'ation honors a man &ho b$a3e' a

tria$ for others to fo$$o&! ather than eu$ogi3ing, &e present an important

eperiment from his patent for future resear(hers to &ork &ith!

Growing Plants in te !ar" by T. Galen Hieron#$%s

a'iations from ea(h of the kno&n e$ements of matter pro'u(e

some form of energy, probab$y e$e(trons &hi(h (an be ma'e to f$o&

a$ong e$e(tri(a$ (on'u(tors! "he f$o& from ea(h of the e$ements having

(hara(teristi(s 'ifferent from the others! onverse$y, the f$o& of

e$e(trons a$ong a (on'u(tor pro'u(es a ra'iation having (hara(teristi(s

of the ra'iation from ea(h respe(tive e$ement!

u(h of the kno&n e$ements as are re)uire' to fee' gro&ing p$antshave been transmitte' to the p$ants through meta$$i( (on'u(tors as the

p$ants &ere entire$y iso$ate' from the e$ements upon &hi(h they &ere

fe'! 6ore pre(ise$y, see's &ere p$ante' in boes in a 'arkene' basement

room!

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7ne of the boes of p$ants (ontaining some of the see's &as use'

as a (ontro$ an' no apparatus for transmitting e$ement ra'iations thereto

provi'e'! "he remaining boes of p$ants ha' e$e(tro'es or p$ates of

(on'u(ting materia$ mounte' or other&ise 'ispose' a'-a(ent thereto, an'

ea(h bo of p$ants &as separate$y atta(he' to a (on'u(tor eten'ing to a

point outsi'e the bui$'ing &here e$e(tro'es or p$ates &ere atta(he' to the(on'u(tors an' a$$o&e' to remain epose' to the $ight!

u(h of the kno&n e$ements as re)uire' to impart norma$

(hara(teristi(s to the p$ants &ere apparent$y fe' thereto by having the

ra'iations of the e$ements from the $ight (on'u(te' to the p$ants through

the &ires an' asso(iate' e$e(tro'es!

"he treate' p$ants &ere re$ative$y hea$thy but the (ontro$ p$ant

assume' the (hara(teristi(s of gro&ing vegetation &hi(h has been

'eprive' of the e$ements in natura$ $ight! .arti(u$ar$y &as the (ontro$ p$ant 'evoi' of (h$orophy$$ &hi$e the remaining p$ants &ere green!



US &'()&'**+ A

!ETE,TION O EMANATIONS ROM MATERIALS

AN! MEASUREMENT O THE OLUMES THEREOPatented Se/t. &*' 01(1.

To$as G. Hieron#$%s' 2ansas ,it#' Mo.

A//lication Octo3er &+' 01(4' Serial No. *56'5&)

0+ ,lai$s. 7,l. &65-)+8

"his invention re$ates to the art of 'ete(ting the presen(e of an'

measuring the intensity or )uantity of any of the kno&n e$e(tro(hemi(a$

series of e$ements of materia$ matter, or the (ombination of t&o or more

su(h e$ements, &hether in so$i', f$ui' or gaseous forms at or'inary room

temperatures an' &ithout spe(ia$ treatment or re)uiring any (hange in

the materia$ un'er observation!

"his app$i(ation is a (ontinuation in part of my (open'ing

app$i(ation for etters .atent eria$ Number 555,55, fi$e' eptember

2, 1944, an' no& aban'one' an' pertaining to improvements in

ete(tion of emanations from materia$s an' vo$umes thereof!

"he primary aim of this invention is the provision of a metho' an'

apparatus for 'ete(ting the presen(e of any e$ement or (ombination of

e$ements that may be in the substan(es un'er observation an' to

'etermine the intensity or )uantity thereof!

"his invention has for a sti$$ further ob-e(t to provi'e a metho'

an' means for 'ete(ting the presen(e of an' ana$y3ing an' measuring the

)uantity or intensity of e$ements or (ombination of e$ements in the

substan(e un'er observation through the (apture an' ana$ysis of

ra'iations emanating from the sai' e$ements, &hether the sai' ra'iations

be of e$e(tri(a$ or opti(a$ (hara(teristi(s, or both!

: yet further aim of this invention is to provi'e an instrument

having a rea(tion 'evi(e, the surfa(e &hereof is affe(te' by the

intro'u(tion of ra'iations thereto, in su(h a manner that the surfa(e of

the 'evi(e &i$$ have its abi$ity to resist movement of arti($es over its fa(e(hange' &hen energy f$o&s through the apparatus, of &hi(h the rea(tion

'evi(e is a part!

: further aim of the invention is to provi'e an atomi( ra'iation

ana$y3er, having as one of its important e$ements, a rea(tion 'evi(e, the

surfa(e &hereof is affe(te' to in(rease a'hesion or fri(tion as the



operator of the ana$y3er strokes the surfa(e of th 'evi(e an' manipu$ates

the instrument to 'ire(t ra'iation thereto!

;t has been 'is(overe' that there are ra'iations emanating from or

re$ease' from ea(h of the kno&n e$ements (onstituting materia$ matter!

"hese emanations o((ur at or'inary room temperatures, i! e! 4<=F! to9<=F! an' they have e$e(tri(a$ an' opti(a$ (hara(teristi(s an' fre)uen(ies

&hi(h are 'ispose' in the 3one from the vio$et ray portion of the visib$e

spe(trum up into the u$travio$et portion, &hi(h 3one has as yet not been

fu$$y ep$ore'! in(e it has been foun' that these ra'iations from the

e$ements or their effe(t may be (arrie' over e$e(tri(a$ (on'u(tors, it is

the ob-e(t of this invention to provi'e apparatus having suitab$e

(on'u(tors an' parts so that ana$y3ing of substan(es may be

a((omp$ishe'! "he ra'iations or the effe(t of su(h ra'iations from kno&n

e$ements or (ombinations oft&o or more e$ements of materia$ matter

may not on$y be (arrie' over e$e(tri(a$ (on'u(tors an' han'$e' in amanner simi$ar to an or'inary e$e(tri(a$ (urrent, but they may be affe(te'

by e$e(tri(a$ (apa(ity in'u(tan(e an' resistan(e! "he ra'iations may a$so

be refra(te', fo(usse', 'iffra(te' or other&ise manipu$ate' in the same

manner as the ra'iations of the visib$e spe(trum! :((or'ing$y, therefore,

this invention has for one of its aims to provi'e an instrument for

han'$ing the ra'iations, i'entifying their presen(e, ana$y3ing them an'

measuring their intensity > a$$ to the en' that the presen(e of one or

more of the kno&n e$ements maybe (on($u'e' from the (hara(ter of the

ra'iation as 'etermine' by the behavior of the ana$y3ing 'evi(e an' the

va$ues rea' from the appropriate s(a$es forming a part of the instrument!

7ther ob-e(ts of the invention &i$$ appear 'uring the (ourse of the

fo$$o&ing spe(ifi(ation, referring to the a((ompanying 'ra&ing, &herein?

Fig! 1 is a s(hemati(a$ an' 'iagrammati(a$ vie& i$$ustrating an

instrument for 'ete(tion of emanations from materia$s an' measuring the

vo$umes thereof, ma'e in a((or'an(e &ith the present invention!

Fig! 2 is an en$arge' 'etai$e' fragmentary s(hemati( vie&

i$$ustrating a portion of the instrument sho&n in Fig! 1!

Fig! is a fragmentary e$evationa$ vie& of a (hart, usab$e in

(onne(tion &ith the instrument, to trans$ate the s(a$e rea'ings into

i'entifi(ation of the substan(es@ an'



Fig! 4 is a 'iagrammati(a$ vie& i$$ustrating another type of

ra'iation refra(ting member, (apab$e of forming a part of the instrument

i$$ustrate' in Fig! 1!

.rior to referring spe(ifi(a$$y to the parts of the apparatus

'iagrammati(a$$y i$$ustrate' in the 'ra&ing, ($arifi(ation of the theoryupon &hi(h the invention is pre'i(ate' &i$$ be ma'e by ep$aining

eperiments heretofore (on'u(te' an' (apab$e of proving the

phenomena$ theories hereinafter 'is($ose' as having a bearing upon the

pra(ti(abi$ity an' uti$ity of both the e$e(tri(a$ an' opti(a$ apparatus!

a'iations from ea(h of the kno&n e$ements of matter pro'u(e

some form of energy, probab$y e$e(trons &hi(h (an be ma'e to f$o&

a$ong e$e(tri(a$ (on'u(tors! "he f$o& from ea(h of the e$ements having

(hara(teristi(s 'ifferent from the others! onverse$y, the f$o& of

e$e(trons a$ong a (on'u(tor pro'u(es a ra'iation having (hara(teristi(sof the ra'iation from ea(h respe(tive e$ement! u(h of the kno&n

e$ements as are re)uire' to fee' gro&ing p$ants have been transmitte' to

the p$ants through meta$$i( (on'u(tors as the p$ants &ere entire$y iso$ate'

from the e$ements upon &hi(h they &ere fe'! 6ore pre(ise$y, see's &ere

p$ante' in boes in 'arkene' basement room! 7ne of the boes of p$ants

(ontaining some of the see's &as use' as a (ontro$ an' no apparatus for

transmitting e$ement ra'iations thereto provi'e'! "he remaining boes of

p$ants ha' e$e(tro'es or p$ates of (on'u(ting materia$ mounte' or

other&ise 'ispose' a'-a(ent thereto, an' ea(h bo of p$ants &as

separate$y atta(he' to a (on'u(tor eten'ing to a point outsi'e the bui$'ing &here e$e(tro'es or p$ates &ere atta(he' to the (on'u(tors an'

a$$o&e' to remain epose' to the $ight! u(h of the kno&n e$ements as

re)uire' to impart norma$ (hara(teristi(s to the p$ants &ere apparent$y

fe' thereto by having the ra'iations of the e$ements from the $ight

(on'u(te' to the p$ants through the &ires an' asso(iate' e$e(tro'es! "he

treate' p$ants &ere re$ative$y hea$thy but the (ontro$ p$ant assume' the

(hara(teristi(s of gro&ing vegetation &hi(h has been 'eprive' of the

e$ements in natura$ $ight! .arti(u$ar$y &as the (ontro$ p$ant 'evoi' of

(h$orophy$$ &hi$e the remaining p$ants &ere green!

:pparatus for $aboratory or (ommer(ia$ use an' for 'ete(ting the

presen(e of any of the kno&n e$ements, preferab$y re$ies upon the

e$ement of tou(h, an' therefore, the ski$$ of the operator! "he instrument

'iagrammati(a$$y i$$ustrate' in Fig! 1 (omprises a unit 05 in($u'ing a

(oi$ 0& 'ispose' to pi(k up ra'iation from substan(e 0(, &herein the

kno&n e$ements are 'ispose' an' that are to be 'ete(te'! "he



temperature of substan(e 0( may be &ithin the range of from 4< to 9<= F!

but su(h temperature is not (riti(a$! "he range has been foun'

satisfa(tory in a(tua$ pra(ti(e!

oi$ 0& may be a spira$$y &oun' f$at bo'y approimate$y 2 in! in

'iameter an' forme' of magnet insu$ate' &ire of any (onventiona$ si3e!

:s an a$ternative, this (oi$ 0& may be a sing$e $ayer, (y$in'ri(a$ (oi$,&oun' on a (ore of insu$ating materia$ substantia$$y 1 in! in 'iameter!

"he eamp$es given for this (oi$ 0&are not (riti(a$ an' so $ong as the (oi$

is in the fie$' of ra'iation of substan(e 0(, the purpose of unit 05 &i$$ be

fu$fi$$e'!

;nstea' of emp$oying (oi$ 0&, &ire &5 may be 'ire(t$y (onne(te'

to substan(e 0( or &ire &5 may be terminate' in an e$e(tro'e an' the

$atter 'ispose' &ith re$ation to substan(e 0( as to pi(k up the ra'iations

therefrom, as 'oes (oi$ 0& in the i$$ustrate' embo'iment! ;n this (ase,

&ire 0) may be groun'e' or (onne(te' separate$y to substan(e 0( or

terminate' in another e$e(tro'e &hi(h may a$so be p$a(e' near

substan(e 0(! "he proimity of substan(e 0( to (oi$ 0& or the e$e(tro'es

as the (ase may be, is su(h as to be &ithin the fie$' of ra'iation of the

emanations from substan(e 0(!

:pparatus 04 is a manua$$y manipu$atab$e ana$y3er tuneab$e to the

spe(ifi( ra'iation 'esire'! ;t (onsists of t&o prin(ipa$ parts, the first

being the t&o stan'ar' type of variab$e (on'ensers, && an' &(, an' the

se(on' being the ray refra(ting 'evi(e ma'e up of e$e(tro'e +& >

passage&ay +4, prism &) an' e$e(tro'e +), a$$ as sho&n in Fig! 2!

:pparatus 04 is -oine' to unit 05 by (on'u(tors 0) an' &5 a(ross &hi(his 'ispose' a (onventiona$ variab$e (on'enser && an' &ith &hi(h is

emp$oye' a (on'ensor of simi$iar type &(, $o(ate' in (on'u(tor &4, as

i$$ustrate'! Aariab$e (on'ensers && an' &( may be of stan'ar' ra'io

broa'(ast type an' they are provi'e' &ith gra'uate' s(a$es in

(onventiona$ manner!

.rism &) is of any suitab$e ray refra(ting substan(e as g$ass,

)uart3, or ana$ogous materia$s! ;n pra(ti(e a prism &) having t&o

po$ishe' fa(es 'isposes at ang$es from < to B< 'egrees has prove'

satisfa(tory! :n e$e(tro'e +& is -oine' to (oi$ 0& by (on'u(tor &5 an'

(on'u(tor +(! tationary e$e(tro'e+& may be of any e$e(tri(a$ (on'u(tingmateria$ su(h as a$uminum, brass, (opper or substan(es having

ana$ogous e$e(tri(a$ properties! "he 'istan(e of e$e(tro'e +& from

prism &) is not (riti(a$ so $ong as the ra'iations or emanations rea(h

prism &) through a (onfine' path of trave$ in the nature of a thin ban' or

$ine! ;n pra(ti(e, this 'istan(e &as from oneha$f to t&o in(hes! :



passage&ay +4 forme' bet&een a pair of opti(a$$y opa)ue insu$ating

e$ements 'ire(ts the ra'iations to a 'esire' area on one fa(e of prism &)!

"he ang$e of in(i'en(e of this path of trave$ to the fa(e of the

prism &) &as of the or'er of 5!5= for best resu$ts an' for obtaining the

&i'est usefu$ segment a$ong s(a$e +0!

:n e$e(tro'e +) shiftab$e a$ong s(a$e +0 is -oine' to unit (5 by(on'u(tor (&! C$e(tro'e +) is of the same spe(ifi(ations as to materia$

an' 'istan(e from prism &) as e$e(tro'e +& but is suitab$y mounte' for

movement a'-a(ent to s(a$e +0 &here its position may rea'i$y be

in'i(ate' by a pointer *) movab$e there&ith an' eten'ing out&ar'$y

therefrom to&ar' s(a$e +0 in a$ignment &ith the path of trave$ of the thin

ray of energy in'i(ate' by the $ine *4! "he ais of rotation of

e$e(tro'e +) is substantia$$y on a me'ian $ine eten'ing $ongitu'ina$$y

a(ross the fa(e of prism &) proima$ to e$e(tro'e +)!

C$e(tro'es +& an' +)&ork best &hen they are re$ative$y thin an' of the

or'er of a fe& mi$s thi(kness!

:s i$$ustrate' in Fig! 2, s(a$e +0 is (a$ibrate' &ith in'i(ia ((, an'

these in'i(ia are on (hart (4 a$ong one e'ge thereof! "he in'i(ia on

(hart (4 have been given a (orrespon'ing referen(e numera$ to those on

s(a$e +0 for ($arifying the 'es(ription hereinafter set 'o&n! ;n'i(ia () on

(hart (4 'esignate the atomi( &eight of e$ements of matter an' (ontinue

up to in($u'e a$$ kno&n e$ements of the e$e(tro(hemi(a$ series &hen the

fu$$ si3e (hart is emp$oye'!

Dnit (5 is a variab$e resistan(e! ;t may be either a (ontinuous$y

variab$e type or it may (onsist of a series of nonin'u(tive resistan(eunits 65, 6&, 6(, an' 64 are ea(h a'iuste' by a s&it(h having movab$e

points 4&, 4(, 44 an' 4) respe(tive$y!

;n pra(ti(e, unit 65 &i$$ have ten times the resistan(e of unit 6&,

&hi(h in turn is ten times the si3e of unit 6(, et(! Ethe va$ues may range

from fra(tions of 1 ohm up to severa$ megohms! Dnit 65 e!g! might be 1

megohm in steps of 1<<,<<< ohms ea(h@ unit 6& then &ou$' be 1<<,<<<

ohms tota$ in steps of 1<,<<< ohms ea(h@ unit 6( then &ou$' be 1<,<<<

ohms tota$ in steps of 1,<<< ohms ea(h, an' so on unti$ the sma$$est unit

&ou$' have steps $o& enough to give the 'esire' ea(tness to the

measure' vo$ume or intensity of the ra'iations!Dnit (5 is -oine' to unit *5 by means of an untune' ra'io

fre)uen(y type transformer 6) through the me'ium of

(on'u(tors (& an' 45! Dnit (5 may be -oine' to unit *5 by resistan(e

(oup$ing or other (onventiona$ (oup$ing of the type fre)uent$y use' in

stan'ar' broa'(ast ra'io re(eivers an' &hi(h is ana$ogous to

transformer 6)!



Dnit *5 may be a (onventiona$ three stage tune' ra'io fre)uen(y

broa'(ast ban'type of amp$ifier &ith the usua$ variab$e (on'ensers

omitte' or it may be of the resistan(e (oup$e' or impe'an(e (oup$e' type

often use' in ra'io broa'(ast type amp$ifiers! ai' amp$ifier intensifies

the va$ue of the ra'iations rea(hing it so that the effe(t upon

'ete(tor *& is ($ear$y 'is(ernab$e! Dn'er some (on'itions, the rea(tionsfrom unit (5 may be put 'ire(t$y into 'ete(tor *& &ithout interposing

unit *5 but amp$ifi(ation of the ra'iations is 'esirab$e!

ete(tor *& is a 'evi(e that &i$$ in'i(ate a (hange from its norma$

state &hen the ra'iations from the ana$y3er 04 are (ause' to inf$uen(e it!

ete(tor *& may be (onne(te' to unit *5 by transformer *( or it

may be p$a(e' near enough to pi(k up the ra'iations from the output of

unit *5 &ithout 'ire(t (onta(t so $ong as it is p$a(e' &ithin the fie$' of

ra'iations!

ete(tor *& is preferab$y an e$e(tri(a$ (on'u(tor (oate' &ith a

materia$ having su(h (hara(teristi(s that un'er inf$uen(e of energy

f$o&ing through the (on'u(ting portion, the (oating &i$$ (hange its

surfa(e tension or vis(osity, or in some manner give evi'en(e of the

presen(e of the energy f$o&ing through the (on'u(ting portion by

pro'u(ing a greater 'rag or resistan(e to the movement of any part of the

bo'y of the operator thereover, su(h as the han' or fingers! ;t has been

foun' pra(ti(a$ to use a meta$ p$ate (overe' &ith a sheet of p$asti( or

(oate' &ith $a()uer, &hi(h p$ate is of an area (onvenient for stroking

&ith the tips of the fingers or pa$m of the han'! ;t may a$so be a sheet or

p$asti( &ith a (oi$ simi$ar to (oi$ 0& 'ispose' a'-a(ent thereto an'(onne(te' to the (oup$ing transformer *(!

Fig! 4 i$$ustrates another form of that part of unit 04, sho&ing Fig!

2, so far as the e$ement separator or fi$ter portion thereof is (on(erne'!

"his separation or fi$tering is a((omp$ishe' in the embo'iment i$$ustrate'

in Fig! 1 an' Fig! 2 by prism &)! ;n Fig! 4 a $ens 055 has the

e$e(tro'e +& 'ispose' a'-a(ent thereto an' movab$e e$e(tro'e +) is

shiftab$e to&ar' an' from $ens 055!

(a$e in'i(ia (( are 'ispose' in a $ine para$$e$ to the path of trave$

of e$e(tro'e +) an' the e$ement or e$ements invo$ve' &i$$ be 'etermine'

by the $o(ation or the s(a$e of pointer *) at the instant a rea(tion isobtaine' at 'ete(tor *&!

hart (4 is of (ourse pro'u(e' as a part of the (omp$ete apparatus

&hen su(h apparatus is manufa(ture' an' after the prism &) Eor $ens 055,

as the (ase may be is insta$$e' as a unit of the materia$ 'ete(tor! : sma$$

)uantity of ea(h of the kno&n (hemi(a$ e$ements is p$a(e' a'-a(ent to

(oi$ 0& an' &ith fu$$ kno&$e'ge of the e$ement, the ang$e of ra'iation



forme' by $ine *4 an', the fa(e of the prism &), is 'etermine' an' the

'egree numera$ on s(a$e +0, &hi(h i'entifies the ang$e of the ra'iation, is

p$a(e' on (hart (4 as one of the in'i(ia ((! :fter this (hart (4 is so

(onstru(te' an' the interse(ting $ines are eten'e' from

in'i(a (( E'egree rea'ings from s(a$e +0 an' in'i(ia () Ethe atomi(

&eight of the kno&n e$ements then &hen the apparatus is in pra(ti(a$use, any materia$ or substan(e may be $o(ate' a'-a(ent to (oi$ 0& an' its

(omponents 'efinite$y 'etermine' by positioning of e$e(tro'e +) on a

$ine of ra'iation *4&here the 'egree number on the fa(e of s(a$e +0 is

)ui(k$y rea' an' use' by referring to (hart (4! When the 'egree

in'i(ia (( is so $o(ate', the $ine on (hart (4 eten'ing therefrom is

fo$$o&e' unti$ it rea(hes the 'iagona$ $ine (6 on (hart (4 &hereupon the

operator then fo$$o&s the interse(ting $ine to the $o&er e'ge of the (hart

&here the va$ue of the atomi( &eight () is rea'! "hese atomi( &eights

are &e$$ kno&n an' are use' in (onventiona$ tets an' s(ientifi( &orks!

;n pra(ti(e, for eamp$e, $et it be assume' that

substan(e 0( (ontains (a$(ium but it is not kno&n that su(h is the (ase!

"he ang$e at &hi(h the unkno&n ray or ra'iation $eaves prism &) &i$$

tea(h its name for, as the operator moves the fingers over the surfa(e of

'ete(tor *&, e$e(tro'e +) is shifte' s$o&$y an' pointer *) moves a$ong

s(a$e +0 unti$ a greater 'egree of a'hesion or resistan(e to motion at the

surfa(e of 'ete(tor *& is set up! "his o((urs &hen the energy or ra'iation

f$o&s from unit 04 through units (5 an' *5into 'ete(tor *&! When

e$e(tro'e +) is at a position &here it is inter(epting a ra'iation from

prism &), or $ense 055, the resistan(e to stroke at 'ete(tor *& &i$$ be of highest or'er!

:s soon as e$e(tro'e +) has been positione' as 'es(ribe', variab$e

(on'enser && is a'-uste' &hi$e the operator (ontinues to stroke

'ete(tor *& to a position &here the greatest 'rag at 'ete(tor *& is again

manifeste'! Net, variab$e (on'enser &( is simi$ar$y manipu$ate' to

obtain a setting &here the 'rag at 'ete(tor *& again rea(hes a maimum!

C$e(tro'e +) is then rea'-uste' for a fina$ position! "he emp$oyment of

(on'ensers && an' &( insure a more a((urate setting of pointer *) by

virtue of their a''itiona$ fi$tering a(tion!

;n the i$$ustration, e$e(tro'e +) has inter(epte' the path of ra'iation &ith pointer *) at the numera$+5 on s(a$e +0 an' referen(e to

(hart (4 &i$$ tea(h the operator that the e$ement having atomi( &eight

+9!2 is that from &hi(h the ra'iation a$ong 'otte' $ine *4 is trave$$ing! ;f

atomi( &eight +9!2 is (a$(ium then that e$ement in substan(e 0( has been

$o(ate'!



"he manner of using $ens 055 is substantia$$y the same as

'es(ribe' in (onne(tion &ith the use of prism &)! "he fo(a$ point of

paths of ra'iation of the e$ements &i$$ (ause 'ete(tor *& to rea(t an'

estab$ish a 'rag to the operators tou(h, &hereupon the s(a$e +0 may be

rea' an' its rea'ing trans$ate' by referen(e to (hart (4!

What a(tua$$y happens at 'ete(tor *& to in(rease an' 'e(rease its'rag to the tou(h of the operator, is not kno&n but the apparatus

fun(tions as above set forth &hen (onstru(te' as spe(ifie', an' therefore,

a positive$y a(ting ana$y3er for atomi( ra'iations is pro'u(e' even

though the prin(ip$e upon &hi(h it is base' is not fu$$y kno&n!

a'iation from hy'rogen passes through prism &) at the sharpest

ang$e or at the $o&est 'egree measure' from the fa(e of prism &)!

a'iations from other e$ements an' their isotopes pass through

prism&) at greater ang$es but in the same or'er as their atomi( &eight >

the heavier the e$ement or its isotope, the &i'er the ang$e!

: substan(e (ompose' of t&o or more of the kno&n e$ements may

be ana$y3e' as herein set 'o&n to 'etermine its (omponent (onstituents!

"he substan(e itse$f &hi(h (onsist of t&o or more kno&n e$ements may

be i'entifie' be(ause the emanations therefrom &i$$ pro'u(e a (omposite

fre)uen(y pe(u$iar to that (ombination of e$ements! :$$ (ombinations

may be (harte' in pre(ise$y the same manner as herein 'es(ribe' for a$$

the in'ivi'ua$ kno&n e$ements in the e$e(tro(hemi(a$ series!

Dnit (5 is use' to measure the intensity of the ra'iations from a

given e$ement or substan(e by a'-usting the severa$ s&it(hes (omprisingunit (5 unti$ the maimum amount of resistan(e has been intro'u(e' into

the (ir(uit &ithout interrupting the rea(tions manifeste' at 'ete(tor *&!

"he s&it(hes are (a$ibrate' in (onventiona$ resistan(e va$ues an' a (hart

must be prepare' that &i$$ re$ate the va$ue in'i(ating by s&it(h settings

of unit (5 the )uantative units of measurement!

;t is rea$i3e' that apparatus for 'ete(ting materia$s an' measuring

the vo$umes thereof, having physi(a$ (hara(teristi(s 'ifferent from those

i$$ustrate' an' 'es(ribe', might be ma'e &ithout 'epartment from the

spirit of the invention or s(ope of the appen'e' ($aims!

%aving thus 'es(ribe' the invention, &hat is ($aime' as ne& an'

'esire' to be se(ure' by etters .atent is?

1! "he metho' of ana$y3ing substan(e to 'ete(t the presen(e of

any of the kno&n e$ements (ontaine' therein, &hi(h (omprises (apturing



on$y the ra'iations emanating from one of the e$ements, having both

e$e(tri(a$ an' opti(a$ (hara(teristi(s@ an' i'entifying the sai' ra'iations

to a((omp$ish the 'esire' purpose!

2! "he metho' of ana$y3ing substan(e to 'ete(t the presen(e of

any of the kno&n e$ements (ontaine' therein, &hi(h (omprises (apturingon$y the ra'iations emanating from one of the e$ements having both

e$e(tri(a$ an' opti(a$ (hara(teristi(s@ an' measuring the )uantity of sai'

ra'iations!

! "he metho' of ana$y3ing a substan(e (ontaining a p$ura$ity of

(hemi(a$ e$ements to 'etermine the (omponent e$ements of sai'

substan(e &hi(h (omprises (apturing the ra'iations emanating from the

substan(e having both e$e(tri(a$ an' opti(a$ (hara(teristi(s@ an'

i'entifying the ra'iations to a((omp$ish the 'esire' purpose!

4! "he metho' of 'ete(ting the presen(e of (hemi(a$ e$ements in a

spe(imen un'er test by (apturing an' ana$y3ing the e$e(tri(a$ an' opti(a$

ra'iations (hara(teristi( of su(h e$ements emanating from sai' spe(imen

&hi(h (omprises, impressing sai' ra'iations on an e$e(tri(a$ (on'u(tor@

(on'u(ting the ra'iations through a tunab$e (ir(uit in($u'ing sai'

e$e(tri(a$ (on'u(tor to an e$e(tro'e in sai' (ir(uit from &hi(h e$e(tro'e

sai' ra'iations emanate@ 'ire(ting the ra'iations emanating from sai'

e$e(tro'e through a refra(ting bo'y@ a'-usting a se(on' e$e(tro'e unti$ it

inter(epts sai' refra(te' ra'iations@ (on'u(ting sai' ra'iations from sai'

se(on' name' e$e(tro'e to a 'ete(tor (omprising a (on'u(tive so$i'having a smooth p$anar surfa(e to vary the surfa(e fri(tiona$

(hara(teristi(s of sai' so$i'@ tuning sai' tunab$e (ir(uit unti$ a maimum

of the ra'iations from sai' spe(imen are emitte' from sai' first name'

e$e(tro'e@ an' rea'-usting sai' se(on' name' e$e(tro'e unti$ the

variation of the surfa(e (hara(teristi( of sai' 'ete(tor in'i(ates that a

maimum of refra(te' ra'iations are impresse' on sai' se(on' name'

e$e(tro'e!

5! "he metho' of 'ete(ting the presen(e of (hemi(a$ e$ements in a

spe(imen un'er test by (apturing an' ana$y3ing the e$e(tri(a$ an' opti(a$ra'iations (hara(teristi( of su(h e$ements emanating from sai' spe(imen

&hi(h (omprises, impressing ra'iations on an e$e(tri(a$ (on'u(tor@

(on'u(ting the ra'iations through a tunab$e (ir(uit in($u'ing sai'

e$e(tri(a$ (on'u(tor to an e$e(tro'e in sai' (ir(uit from &hi(h e$e(tro'e

sai' ra'iations emanate@ 'ire(ting the ra'iations emanating from sai'

e$e(tro'e through a refra(ting bo'y@ a'-usting a se(on' e$e(tro'e unti$ it



inter(epts sai' refra(te' ra'iations@ amp$ifying the ra'iations inter(epte'

by sai' se(on' name' e$e(tro'e@ (on'u(ting sai' amp$ifie' ra'iations to

a 'ete(tor (oup$e' &ith sai' amp$ifier &hi(h 'ete(tor (omprises a

(on'u(tive so$i' having a smooth p$anar surfa(e to vary the surfa(e

fri(tiona$ (hara(teristi( of sai' so$i'@ tuning sai' tunab$e (ir(uit unti$ a

maimum of the ra'iations from sai' spe(imen are emitte' from sai'first name' e$e(tro'e@ an' rea'-usting sai' se(on' name' e$e(tro'e unti$

the variations of the surfa(e fri(tiona$ (hara(teristi(s of sai' 'ete(tor

in'i(ates that a maimum of refra(te' ra'iations are impresse' on sai'

se(on' name' e$e(tro'e to obtain an in'i(ation of the presen(e of a

(hemi(a$ e$ement in sai' spe(imen!

B! "he metho' of 'ete(ting the presen(e an' )uantity of (hemi(a$

e$ements in a spe(imen un'er test by (apturing an' ana$y3ing the

e$e(tri(a$ an' opti(a$ ra'iations (hara(teristi( of su(h e$ements

emanating from sai' spe(imen &hi(h (omprises, impressing sai'ra'iations on an e$e(tri(a$ (on'u(tor@ (on'u(ting the ra'iations through a

tunab$e (ir(uit in($u'ing sai' e$e(tri(a$ (on'u(tor to an e$e(tro'e in sai'

(ir(uit from &hi(h e$e(tro'e sai' ra'iations emanate@ 'ire(ting the

ra'iations emanating from sai' e$e(tro'e through a refra(ting bo'y@

a'-usting a se(on' e$e(tro'e unti$ it inter(epts sai' refra(te' ra'iations@

(on'u(ting sai' ra'iations from sai' se(on' name' e$e(tro'e through a

variab$e resistan(e@ amp$ifying the ra'iations passing through sai'

variab$e resistan(e@ (on'u(ting sai' amp$ifie' ra'iations to a 'ete(tor

(oup$e' &ith sai' amp$ifier &hi(h 'ete(tor (omprises a (on'u(tive so$i'

having a smooth p$anar surfa(e to vary the surfa(e fri(tiona$

(hara(teristi(s of sai' so$i'@ tuning sai' tunab$e (ir(uit unti$ a maimum

of the ra'iations from sai' spe(imen are emitte' from sai' first name'

e$e(tro'e@ rea'-usting sai' se(on' name' e$e(tro'e unti$ the variations of

the surfa(e fri(tiona$ (hara(teristi(s of sai' 'ete(tor in'i(ates that a

maimum of refra(te' ra'iations are impresse' on sai' se(on' name'

e$e(tro'e to obtain an in'i(ation of the presen(e of a (hemi(a$ e$ement

an' varying the resistan(e in sai' variab$e resistan(e unit unti$ the

surfa(e fri(tiona$ (hara(teristi(s of sai' 'ete(tor are unaffe(te' to obtain

an in'i(ation of the )uantity of sai' e$ement in sai' spe(imen!

+! "he metho' of 'ete(ting the presen(e in any bo'y of a spe(ifi(

e$ement as &e$$ as the )uantity thereof &hi(h (omprises, impressing on

an e$e(tri(a$ (on'u(tor ra'iant &aves having opti(a$ an' e$e(tri(a$

properties &hi(h are generate' by an' &hi(h are (hara(teristi( of a

spe(ifi( e$ement@ tuning sai' &aves@ impressing the tune' &aves on an

e$e(tro'e@ amp$ifying sai' &aves by an amp$ifying (ir(uit &hi(h in($u'es



a (oup$ing e$ement, a gap a'-a(ent sai' $ast name' e$e(tro'e, an' an

a'-ustab$e e$e(tro'e, sai' $ast t&o e$e(tro'es being at opposite en's of

sai' gap@ (ausing sai' &aves to pass through a refra(ting bo'y in passage

through sai' gap@ impressing sai' amp$ifie' &aves on an in'i(ator

(omprising a (on'u(tive so$i' having a smooth p$anar surfa(e (oup$e' to

sai' (oup$ing e$ement@ a'-usting sai' a'-ustab$e e$e(tro'e an' operatingsai' in'i(ator an' sai' a'-ustab$e e$e(tro'e unti$ a maimum intensity of

refra(te' rays is in'i(ate'!

8! :pparatus for ana$y3ing substan(e to 'ete(t the presen(e an'

)uantity of any of the kno&n e$ements therein (omprising, in

(ombination, a pi(kup unit having e$e(tri(a$ (on'u(tive properties for

absorbing (hara(teristi( ra'iations of an opti(a$ an' e$e(tri(a$ nature

from the substan(e being ana$y3e'@ an e$e(tro'e in (onne(tion &ith sai'

unit from &hi(h the ra'iations move out&ar'$y a$ong a parti(u$ar path of

trave$@ a refra(ting member of transparent materia$ in sai' path tointerse(t sai' ra'iations@ a s(a$e having in'i(ia thereon &hereby any one

of the e$ements may be i'entifie'@ a se(on' e$e(tro'e bet&een the sai'

member an' the s(a$e to (o$$e(t ra'iations passing through the member

after their path of trave$ has been a$tere' thereby@ an' apparatus

measuring the )uantity of the ra'iations (o$$e(te' by the se(on'

e$e(tro'e!


)uantity of any of the kno&n e$ements therein (omprising, in

(ombination, a pi(kup unit having e$e(tri(a$ (on'u(tive properties for absorbing (hara(teristi( ra'iations of an opti(a$ an' e$e(tri(a$ nature

from the substan(e being ana$y3e'@ an e$e(tro'e in (onne(tion &ith sai'

unit from &hi(h the ra'iations move out&ar'$y a$ong a parti(u$ar path of

trave$@ a refra(ting member of transparent materia$ in sai' path to

interse(t sai' ra'iations@ a s(a$e having in'i(ia thereon &hereby any one

of the e$ements may be i'entifie'@ a se(on' e$e(tro'e bet&een the sai'

member an' the s(a$e to (o$$e(t ra'iations passing through the member

after their path of trave$ has been a$tere' thereby@ apparatus measuring

the )uantity of the ra'iations (o$$e(te' by the se(on' e$e(tro'e@ an' a

'ete(tor member (on'u(tive$y -oine' to the $astmentione' apparatus(hara(teri3e' by the property of having its effe(t upon the tou(h a$tere'

in a((or'an(e &ith the f$o& of ra'iations thereto!

1<! :pparatus for ana$y3ing substan(e to 'ete(t the presen(e an'

)uantity of any of the kno&n e$ements therein (omprising a pi(kup unit

having e$e(tri(a$ (on'u(tive properties for (o$$e(ting (hara(teristi(



ra'iations of an opti(a$ an' e$e(tri(a$ nature from the substan(e being

ana$y3e'@ an e$e(tro'e in (onne(tion &ith sai' pi(kup unit from &hi(h

the ra'iations move out&ar'$y a$ong a path of trave$@ a $ens in sai' path

of trave$ to refra(t ra'iations emanating from the sai' e$e(tro'e an'

trave$ing in sai' path, sai' $ens having a fo(a$ point for ea(h kno&n

e$ement@ a se(on' e$e(tro'e to (o$$e(t ra'iations passing through the$ens@ an' a s(a$e having in'i(ia thereon, provi'e' &ith referen(e

(hara(ters ea(h in'i(ative of one of the kno&n e$ements an' ea(h being

at a fo(a$ point of sai' $ens!


)uantity of any of the kno&n e$ements therein (omprising a pi(kup unit

having e$e(tri(a$ (on'u(tive properties for (o$$e(ting (hara(teristi(



the ra'iations move out&ar'$y a$ong a path of trave$@ a $ens in sai' pathof trave$ to refra(t ra'iations emanating from! the sai' e$e(tro'e an'


e$ement@ a se(on' e$e(tro'e to (o$$e(t ra'iations passing through the

$ens@ a s(a$e having in'i(ia thereon, provi'e' &ith referen(e (hara(ters

ea(h in'i(ative of one of the kno&n e$ements an' ea(h being at a fo(a$

point of sai' $ens@ an' apparatus for measuring the )uantity of the

ra'iations (o$$e(te' by the sai' se(on' e$e(tro'e!


)uantity of any of the kno&n e$ements therein (omprising a pi(kup unithaving e$e(tri(a$ (on'u(tive properties for (o$$e(ting (hara(teristi(



the ra'iations move out&ar'$y a$ong a path of trave$@ a $ens in sai' path

of trave$ to refra(t ra'iations emanating from the sai' e$e(tro'e an'


e$ement@ a se(on' e$e(tro'e to (o$$e(t ra'iations passing through the

$ens@ a s(a$e having in'i(ia thereon, provi'e' &ith referen(e (hara(ters

ea(h in'i(ative of one of the kno&n e$ements an' ea(h being at a fo(a$

point of sai' $ens@ apparatus for measuring the )uantity of the ra'iations(o$$e(te' by the sai' se(on' e$e(tro'e@ an' a 'ete(tor member

(on'u(tive$y -oine' to the $astmentione' apparatus (hara(terti3e' by the

property of having its effe(t upon the tou(h a$tere' in a((or'an(e &ith

the f$o& of ra'iations thereto!



1! :n apparatus for ana$y3ing a substan(e to 'ete(t the presen(e

of any of the kno&n (hemi(a$ e$ements in sai' substan(e (omprising, an

e$e(tri(a$ (on'u(tor for absorbing the (hara(teristi( ra'iations of an

opti(a$ an' e$e(tri(a$ nature from a (hemi(a$ e$ement in the substan(e

being ana$y3e'@ a tuning (ir(uit (onne(te' to sai' e$e(tri(a$ (on'u(tor@

an e$e(tro'e in sai' tuning (ir(uit from &hi(h sai' ra'iations emanate ina 'efine' path of trave$@ a refra(ting bo'y a'-a(ent sai' e$e(tro'e an'

positione' in the path of trave$ of sai' ra'iations for refra(ting sai'

ra'iations@ an a'-ustab$e e$e(tro'e positione' a'-a(ent a portion of sai'

retra(ting bo'y from &hi(h the refra(te' ra'iations emanate@ a s(a$e

provi'e' &ith in'i(ia for i'entifying any one of the (hemi(a$ e$ements

asso(iate' &ith sai' a'-ustab$e e$e(tro'e@ an' a 'ete(tor (omprising a

(on'u(tive so$i' having a smooth p$anar surfa(e (on'u(tive$y (oup$e'

&ith sai' a'-ustab$e e$e(tro'e, sai' 'ete(tor being (hara(teri3e' by the

property of varying its surfa(e fri(tiona$ (hara(teristi(s &hen a

maimum of refra(te' ra'iations are (on'u(te' thereto!

"%76: #! %;C7NG6D!

REEREN,ES ,ITE!

"he fo$$o&ing patent referen(es are of re(or' in the fi$e of this

patent?

UNITE! STATES PATENTS

N%$3er Na$e2,115,5+8 %a$$

*.$us $its 6inus $its* [HH]

[;n'e]

[II] *ress ee'$ings espon' to ight, Fee'ing*

https://borderlandsciences.org/journal/vol/44/n03/US2115578.pdf


https://borderlandsciences.org/journal/vol/44/n03/How_Seedlings_Respond_to_Light_and_Feeding.html

https://borderlandsciences.org/journal/vol/44/n03/US2115578.pdf


https://borderlandsciences.org/journal/vol/44/n03/How_Seedlings_Respond_to_Light_and_Feeding.html



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K1 E+<+ 49+B911 J bor'er$an's(ien(es!org

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T.galen Hieronymus - Radionic Pioneer

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