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RADIO
DEPARTMENT
Th<e T
1f'
iUle
W
ii1f'
ce
li
ce
§§
By
NIH-OLA
TE§lL.A
IVrillt n
Enlusivtl:,. for TI.l' Elulriclll E.rptri",tnltr
E
VER
since the announcemmt of
application of these radiations for the pu
r.
pOse
was quite obvious. \Vhen Dr.
Hertz.
was asked whether such a system would
be of practical value, he did not think
so,
and he was co rrect in his forecast. The
best
that
might have been expected was a
methOd of communication similar to the
-_
.",
proved appliancu. Similar phenomena were
noted, greatly
ma~nified
in intensity, but
they were susceptible of a differem and
more plausible explanation.
I
considerM
this so important that in
1892
I
went to
Bonn. Germany, to ronfer with Dr. Hertz
in regard to my obsen'ations. H e seemed
disappointed to such a
de~ree
that J r e-
grettro
my tr ip and parted
from
him so
r-
rowfully. During the succeeding yea rs
I
made numerous exr,e rim en ls with the same
Obje<:tibnt the resu ts were uniformly nega-
t ive. n
1
900, however.
after I
had e\'olved
a
wireless Iransmitter which enabled me
t o obl.ain
eI«tro-magnetic
activities
of
many
millions
of
horse-power.
J
made a last des·
pe.rate atlempt to prove that the diSlUrb-
ances emanating from the oscillator were
ether vibrations akin to those of light. but
met again wit h utter failure. For more than
eifZhteen years
I
have been reading treat-
ises. reports of scientific transactions, and
articles on Herlz-wa\'e telegraph
y,
to keep
myself informed, but they have always im-
prest me like wo rk s of
fi
ction.
The history
of
science shows that theo-
ries are perishable. \Vith eve ry new truth
that is re \'ealed we ge l a better under-
standing
of
Nature and our conceptions
and views
arc
modified. Dr.
Hertz
did not
discove r a new principle. He merely gave
material support to a hypothesis which had
Maxwell's clet:tro-magnetic
theory
scientific investigators all the world
ov
er
had beeu bent on its experi-
mental verification. They were con-
\'inced that it would be done and livM in
an atmosphere of eager expectancy, un-
~,."'
E l
ec
t r Ic T
rantmlnlon
Thru
Two
WIre.
and
H
ydra
ull e
Analog.
F Ig. 3.
heliographic and subje<:t
to
the same or
evo:n
greater limitations.
usually favorable to the reception of any
evidence to this end. No wonder then that
the puhliGition
of
Dr. H einrich Hertz's re-
sults caused a thrill as had scarcely ever
~n
experienccd before. At that
III
the spring
of
1891
I
gave my demon-
strations with a high f requency
machine before
the
American
In
-
stit ute of Electrical Engineers al
Columbia College, which laid the
foundation to a new
and
far more
promising deparlure. Altho the
laws of electrical resonance were
well known at that time and my
lamented friend,
Dr
. J ohn H op-
kinson, had even indicated their
speeific application to an alterna-
lor in the ProceedinJ<S
of
the In-
stitute of Electrical Engineers.
London, Kov.
13,
1889,
nothing
had been done towards thc prac-
tical usc of this knowledge and
it is probable
that
th
Ose
experi-
ments of mine were the first pub-
lic exhibition with resonant cir-
cuits. more part,icularly of high
frequency.
\\'hlle
the spontane-
ous success of my lecture was
timc
I
was in the midst of press-
ing work in connection with the
commercial introduction of my
system of power transmission,
but, nevertheless, caught the fire
of
enthusiasm and fairly burned
with desire to behold the miracle
wi th my own eyes. According-
ly, a s soon as
I
had freed myself
o f these imperative duties and
r esumed research work in my
laboratory on Grand Street, New
York,
I
began, parane! with
high
frCCj.uen
cy alternators, the
constructIOn of several forms of
apparatus with tlu: object
of
ex-
ploring th e field opened
\IP
by
Dr. Hertz.
Re<:ogn
izing the lim-
itations
of
the devices
he
had
employed, I concentrated my at-
len
ti
on on the prodnction of a
I
N
thi
s r
em
arkable a
mI
co
lll p l.cle
s
lO
ry
01
his
di.!covery 01 tloe
:hicfl
mlt/s
mi
nio
ll
and
r ece
ption
,
el'en
in
the
pr
ese
nt
day
sys
le m
s, ar e
baud,
J
)r.
1\·i/.:ola T
e&Ia
,
/tOIl:!
US
II'at
li e is
indeed the MFather 01 the
Wire.
I
us."
To
Itim
lloe
He
r'::;
R '(
n:e
theory
ioJ
a (fef
ll
sion; it t
ook,
, ollnd
from
cerlui"
angtu,
bu
,
I
he
lacts telld
10
wove
tllat
il is
hollo
w
and
em
lJly.
11
1'.
co/willce!
I
II
Illat the
re(,1
lI
e
rl:
1(."(/tl
e6
are blul/ed
out
Il/fer II
IC
y
"atle
trav
eled but
a $
hort
diSlan
ce
from
tlo
e
",-" der.
It
lofloU't . lloer r.fo re, ,/out
th e
measured antenna c
urrent
is
110
indio
cation 01
the
effect. b ecau
,e
only
a
,mali
palt 01
it
is
effec
ti
ve
'"
a dislanee. Th
ll
limiled
a
ctivity
of
pure
li
e
n:
reace tr
an$mi.s.J
ion
and
r ecep l ion is
here
cfoorly expla
ined
, b l!l
id
u
sllmt"ing d efi
llild
y
that in
'p
ilf!
of
Ihem$e /, ;e6, Ihe radia
en g
ine
en
01
II I(
III
Y
lire
emplo)'i"g
IIII'.
origil/Ill T
e$
llf ,
uned
oscillutory
ly
&
lem
.
li
e
,
horCJ
by example,
with
diOerellt
lorm,
of
aer
illf$
tlou
' t
lo
e
&ig
ml/.$
Ilic
ked
up
by
,Ioe
instru m en!.f
IIU/..SI
actualfy
be
i"duced
by
earllo curr en
/.!
-
not
elh
e
ri
c ' I/(jCll
waves. T
ula
also d is proves
Ihe
M
ll
eaviside
layer"
theory
Irom
I,is
penonal
ob'en
'ations
and
1
e&U.
"
True
Wirel
us"
and
Ill e
principles
UPfJIl
1<
EDITOR
.
due to spectacular features, its
chief import was in showing that
all Kinds of devices could be operated
thm a single wire without return.
powerfnl in duction coi l but made
no notable progrcss until a happy
in spiration led me to the inven tion of the
oscillation transformer. In the latter part
o f
1891
1 was already so far advanced in
the development of this new principle that
I had
at
my disposal means vastly superior
been long ago formulated.
It
was a per-
feetly well-established fact that a circuit.
traversed by a periodic current. emitted
some kind
of
space waves, but we were in
ignorance as
10
their character. He ap-
parelllly ga\'e an experimental proof that
they wen'; t ransversal vibrations in th e
ether. Most
pwple
look upon this a s
hi
~
great accompli shment.
To
my lIlind it
Seems that his immortal merit was not so
much in this
as
in the focusing
of
the in-
vestigators' attention on the pr
OCessC5
tak-
ing place in
the
ambient medium.
Th
e
Hertz.-wave theory, by
il$
fascinating hold
on the imagination, has stifled creative
ef-
fo rt in the wireless art and retarded it for
twcntr-five :rears. But, on the other hand,
it is
ImpoSS
Ible to over-estimate the bene-
ficial e
ff
ects of the powerful stimulus it
has given in ma ny directions.
As regards signaling without wires, the
This
--
-;r
--{
'-'
Q:):':::
=-
-
---:J
~
-
I_*,
Jec_~
~~I;r=;
t h e
Cln:ult
Conn
ectio
n .
a n d
TunI
n g D
...
lcu
Employed by
T
es
la In
H Is
Ex
per
imental
D
emonltratlons
lJ efol"1l
the
Ame
r
1c;>
n In
ltlt
u h
of
E
lec
tr
ical En
g l
nee...
Wllh th
e H Igh F l"1Iquency Al
tern"or
Sho
.....
n
In
Fig. t.
F Ig. 2.
to those o f the Ge r man phys
ici
st. All my
r.
revious effort, with Rhumkorf (Oils had
D Ia g
ra
m
Itl
u.t
~.t
1
n
g
E lect r Ic
Tr
:tns
m
lulo
n T h
ru
II
S In g le
WI,..
H
ydraulic
A n
.log.
F Ig. 4.
e ft me unconvinced, and in order to set-
tle
my
doubts 1 wenl
over
the whole ground
once more, very carefully, with thcse im-
was the initial
!te~
in the evolution o f
illY
wirele
5s
system. The idea
pre
Sented itself
to me that it might be possible. under ob-
May, 19 19
ELECTRICAL EXPERIMENTER
29
number of
radial
improvements_ Suitable
high frequency generators and
dcctricaJ
os-
cillators had first to
be
prod~
The
energy of these had to be transformed in
effcct
i
n~
_
transmitters and collcct«l at a
distance in proper receivers.
Such
a sys-
tem would be manifestly cin:umscriJed
m
its
usefulnus if
all extraneous
inlttiu-
ence
were: nOt
prevented and
excJu
!;
"w
IUultratlng
T
ypica
l
Arrlngemenu
f
or
CoUectlng
E
nergy
In a
SYlum
Of
Trlnl
_
ml
..
lo n T
hru
a Slngl"
Wire. Fig.
5.
servance o f proper conditions of resonance,
to tran
smit electric energy
thru
the earth,
th
us
dispensing with all artificial conductors.
Anyone who might wish to examine ilnpar-
tially the me rit
of
that earlr suggestion
must not "iew it in the light
0
present day
scie nce.
I
only need to say that as late as
1893,
when
I
had prepared an elabdr.ue chap-
ter on my wireless system. dwelling on its
various instrumentali
ti
es and future pros-
pects, Mr. Joseph Wetzler
and other
friends
of mine emphatically proteSied against its
publication on the ground that such idle and
far-fetched speculations would
~n)ure
me in
the opinion of conservative busmcn men.
So it came that only a small part of what
I
had intended to say was embodied in my
address of that year before th e Franklin
Institute and National Electric Liltht As-
sociation under the chapter "On Electrical
~
secured. In time, however.
1
recognUed
that devices
of
this kind, to
be
most
~«1-
£Jnvkd",poci~
£
l
e
O'CfaJ~~
Ta
'a's
Sya-tem
of
W
lrelen
T
ranlmlnlo'"
Th",
th.
Earth
as
Actually Exposed
In
H I,
Lacturet
Be
for-e
th
e
Frankli
n In_
Itltute
Ind
Ele
ctric
Light
"'"oclatlon
In
I r
-,;,.,.
February
and Mlrch,
1893 , F
ig."
of
a condenser subdidded into small
sec·
tions. the fine r adju5tmrots being dlected
by a movable iron core: within
an
indllct·
ance coil. Loosely linked with the latter
was a high tension scocmdary which was
tuned to the primary.
The operation
of
devicC$
wire without return was
punl;,!"
because
of
its novelty,
explained
by
suitabJi!,:_
..
1~~,;
F.::;:
~
,
d
'
..
..
"""),!k"'~
..
lo n Of E lect
rical Energy
T
hru
th"
Eart
h
a.
IIlu lt
r~ted
In
Tnla'i
Lecture.
B".
f
ore the
Franl(lIn
Inltltute
and
E I"ct riC L
ight
A
ssocia
t ion In
F'bru~rl
and March.
1893.
an
d
Mech
anical Analog
0
.
1lih"
,
,
Tr~n.ml
,:",.",Iii;~
purpose refere
nc
e
';s
I n the former the
I
cond uctors are
¥ii¥
Tho
th
e
Same.
7.
ive and efficient. should
be
de:signed with
due
regard to
the physical
propertin
of
this planet and t he electrical conditions
obtaininc
on the:
same.
I
will briefly touch
upon the salient ad"ances as they
....
ere
made in the gradual deve:lopment of the
system.
The high frequency alterllator employed
in my first dellionstrations is illustrated in
Fig.
1.
It
comprised
a
field ring, with
384
pole projections and a d isc armature with
coils wound in one single layer which
were:
connected in va rious ways according to re-
quirements.
It
was an excellent machine
for experimcntal purposes, furnishing sinu-
soidal currents of from I
O,OClO
to 20,000
cycles per s.econd,
Th
e output was com-
paratively large, due to the
fact
that as
much
as 30
amperes
per
SQua
re millimeter
could be past
thru
the co
il
s without injury.
The
diag ram in Fig.
2
sh ows the circuit
a rrangeme:I\IS
as
used
ill
my lecture. Reso-
nant conditions were maintained by means
FI~.
...
e"
Forerunne
r
of
Audlon
-
the
Se
n
sit
iv
e
Wlteletl
D
etector
Kn
ow
n.
ae
Oe
·
ICrlbed
by
T.
I II In
HI, L
ec
tu
re
B
efore
th.
I
nltltutlon
Of
E
lec
tri
cal
En
gl.
n.
a r
l.
London,
Februar
y,
1892.
Fi
g.
II.
ct
a
gr
lm
E lu
cida
t I
ng
Eff
"ct of
Ll
rge Capac_
Ity on
On
e
En
d.
Fig
. 5.
Resonance."
This
little salvage from the
wreck has earned me the title
of "Father
of
the Wire:Jess" from many well-disposed
fellow workers,
rather
than
the
invention
of Kores of appliances which bave brought
wireless trans-
mission within
the reach of
every young
amateur a n d
which.
>in
a
time not dis-
tant, will lead
to undertak-
ings overshad·
owing in mag-
nitude
and
importance all
past achieve-
menu of
the
engineer.
The
popular
impression is
that my wire·
less work was
begun in
1
893,
but as a mat-
ter of fact
I
spent the two
prec
e
ding
years in inves-
tigation
s.
em-
ploying fonns
of apparatus,
some of which
were
almost
like those of
today.
It
was
elear to me
from the very
start that the
successful
seclion , th e alternator by an oscillating
pi ston and the filament of an incandescent
lamp by a minute channel connecting the
pi
pes.
It
will
be
clear from a glance at
the diagram that "ery slight excursions
of the piston wo uld cause the fluid to rush
with high ve-
locity thru the
small channel
and that vir·
tually all the
ene
r
gy
of
movement
w
ou ld
be
t r a IIsfonned
into heat by
friction, si
mi_
larly to
that
of the electric
current
in the
lamp filament.
The
second
diagram
will
now be self-
ex])
lanalory,
Corresponding
to the termi-
nal capacity of
the
ele<:tric
syste:m
an
elastic re se r-
v o
ir
is em-
plo)'C-d
which
dispenses with
the
A,<lSb61.
_.,..1/InU
f~
01'1:'"
'
Ill
_b~"-~""
".a~"'i'w_
.
t
necessity
,,=,
b=:"'1.
"
"QUC'>(y
ar
€U"aPI
r
of a
return
pipe. As the
piston oscil-
lales
the
bag
expands
and
Cont
ra cts, and
the
fluid
is
_~
"""" ""'"'"
00'f:g"
18
"'Q_
..........
-
M>d
~
",bNr~
made
10
surge
thru the re-
stricted pas-
sagewithgre:at
speed,
thi.
",
con
summa-
'11. 10.
tion could only
be
brought
about
by
a
__
_
Tn
la
's Syllem of
Co
n
catenate.f
T
uned Clrcultl Shown
~nd
Described tn
U.
S.
P
atent
No. 568.178
S"ptember
22. 1896,
ard
':orrespondlng
.......
angementl
In
Wlrel
...
Trantml,,'an,
of
in the generation
of
he>t
u
in
the
incandesccnt lamp. Thooreticalh- consid-
ered, the efficicllcy
of conveulon of
energy
should
be
the samc in both
c",_es,
Gralllcd, then, that an economic system
of power
transmission
thr
u a single wire is
lions
of
the oscil lat
or
might be modified
tbm
the 'immense
extem of
the globe the
principles involved
arc
the same.
Consider now the effect
of
such a con-
ductor
of
vast dimellsiOlls on a circuit
ex-
ci ting it.
The
upper diagram
of
Fig.
6
il-
lu
stra
tes a familiar oscillating: liystem com-
prising a slr.light rod
of
sclf-mductancc
2L
with small
terminal capacities
((
and a node
in the center.
In
the lower diagram
of
the
figure a
large
capacity
C
is
auached to
the
rod
at one
end with the result
of
shifting
the node
to
the right.
thru
a distance cor-
res ponding
to
self-inductance
X.
As both
paru
of
the
s}stem
on either
side
of
the
node
vibrate
at
the sallie rate, v,c
have
c\·i-
suustance, is
the
system
of
toda~
;and
I
a!ll.
n
ot
aware
of
a single
authentical~
in-
stance
of
successful t
ransmi,sion
at eon-
5iderat~e
rc~uhing
distance hy different instrumen_
It might, vcrhaps, not be clear
to
\ql;
....
~
,
talities.
'i:
-,"',,,
...
;
<,\7:,>:'>-
,
,.
~
-.::..-=:::.~~:,\
:,~?-::.-;t
"'\'
.-
/<~:;:;:?=
i'~~:::3-<~>"
""
..
v.',.
' " '
\\\
If",'1
I
/
'
1,/,,-......::.:...
Q
--,....
~
'.
I:
I
4q
n
I
I
I
,'"
I
,
\
I
\
!1-4~
Tcsm
four~JI''Cutf
tu"ui
_,-deu
SJU~
I
I
I
,
\
I
I
I
demly,
(L
+
X)
c
=
(L
_
X)
C
from
1.,-
'fCln
"
'
!
I
I
I
I
C-,
t
:
!
which X
=
L
c+,
pacily
C
becomes
commen~urate
to
that
of
the
earth,
X
approximates
L,
in
other
words, the noue is close to the ground con-
Ilcction.
The
I'X(l(/
detr'millPliulI
of
ils
po.dlioll
is
f.'Uy
imparl/lilt
{"
tilt
(01,
..
/(1-
tian
of
ct rloin 11"'(,.Ilrilll rlrctrical (llid
geodetic
dala
and I have devised spedaJ
means with this purpose in view.
~Iy
When
the ca-
Fig.
H.
D
iagram
E
xplainIng
th
e Re_
lati
on
Between
t
he
Effectille and the
Mea.u~d
Curren
t In
the
Antenna.
those who have perused my first descrip-
tion
of'thcse
improvemcnts that, besides
making known new and efficient types
of
apparatus.
r
gave to
the
world a wire
kss
system o f potentialities
far
beyond any-
thing
before conceived.
I made explicit
Q
6
Ifufz
(}Self/c/oI'
of
grwl
t!nO!I,Y
Ine
H«''''f
original
plan of tran
smitting energy
without wires is shown in the upjl('r dia-
gram
o f Fig.
7,
while the lower
one
Dlm-
t rates its mechanical
ana
lo
g,
first publisht
in my article in the
A/IJ{jazillt'
of
Jun
e,
1900.
An
alternator,
preferably of
high tension, has one
of
its terminals con-
neCled
to
the
ground
and the
othe
r to an
elevated capacrty
and
impresses its oscil-
lations upon the earth.
At
a distanl point
a receiving circuit, likewise connected
to
ground
and
to
an
elevated capacit)', collects
some
of the energy
and actuates a suitable
device. I suggested a multiplication
of
such
units
in o r
der
to intensify the effects,
an
idea which may yet prove \'aluable. In
the analog
two tuning forks
arc
provided,
one
at the
sending
and
the
other at
the re-
ceiving station, each having
attached
to
its
lower
prong
a piston fitting
in
a cy linder.
The two
cylinders communicate with a
large elastic
resen
·o
ir
filled with
an
incom-
Ct'''''Jr~
•
J
Fig.
15. IIIUltr
aUng One of the General
E
III
_
dence. Aga
ln . t
the Space Walle
Tranlmlulon.
and repeated statements
that
I
contem-
transmission, absolutely unlimited as
to terrestrial
distance
and amount of en·
ergy. Bm,
altho
1
have
oveTC{Jme all ob-
stacks
which st'emcd in the beginning
un·
surmountable and fowld elegant solutions
of
all the problems which
confronted
me.
yet, e,'en
at
this
very
day,
the majority
of
experts
are
stiJI blind to
the
possibilitiu
which
arc
within easv
attainment.
).Iy confi dence
that
a signal could
be
easily flashed a r
ound
the globe
waS
streng
thened
thru th
e discovery
of
the " ro-
tating
brush." a
wonderful
phenomenon
which I
have
fully dcscribed in my
addreu
before
the
I nstitution
of
Electrical Engi-
neers. London. in 1892,
and
which is illus-
trated
in Fig. 9. T his is undoubtedly the
most delica te wireless detector known, but
for a lo ng time it was
hard
to produce and
to maintain in
th
t' sensitive stat
e.
These
difficulties do
not exist
now
and
I am look-
ing to valua ble applicat'ions
of
this device,
particularly in connection with the high-
s~ed
photographic method, which I sug-
gested, in wireless,
a~
well
as
in wire,
trans-
mission.
Possibly Ih e most important advances
dur-
ing
the follow';ng
three or
four
years
were
my system
of
concatenated tuned ci r
cuia
,
plat~
F o
ur
Ctn;ult Tu
ned
Syltem
Con_
W i
th th
e
Contemporanlo
u ,
Hertz
_
Walll
Syltem,
F
ig.
11.
practicable, the question arises how to col-
lett
the energy in the receilers. \Vith this
object attention is called
to
Fig. 5, in which
a co nductor is sho\\ n excited by an
osdl-
la
tor
jo!ne~
t? it
alone
end. Evidently,
as
the
penodlc
Impulses pa n
Ihru
the
win
~
,
uifferellces
of
potential will be created along
the same
as
we
ll
as at
right
angles to il
in the
surrounding
medium and either
of
these may
be
usefully applied.
Thus at
a,
a circuit compr ising
an
inductance and
(3-
padty
is resonantly excited in the t rans-
verse, and
at
b,
in the longitudinal sense.
At
c,
ener~,'y
is collected in a circuit parallel
to Ihe conductor but not in contact wilh it,
and again
at
d,
in a ci rcui t which is pa rtly
sunk into
the
conductor
and
may be, or
not, electrically connected
to
the same.
It
is
important
to keep these typ ical disposi-
tions in mind.
for
howel'er the distant ac-
JiI~S21i~
,.
','''/
.'
/
---'-"-
-',,-::"
"
'
.
k::W;::----
··
~~:>::~:\
f!li/I:!
--
\\\\'.\\
'
..
\\\
..
··'\;'1
'\'
\'
"'1"
11111',1,1
"::i):!
•
.
4_
~
.
au
;
1 111.1'
-_."",
,
~
-",.~
...:...--
. -'--
_.
.,.:;....,
-
D
iagram
E
xpol
l
ng
the Fail
icy
0'
th
e G liding
Walle
Th
eory
Wlrel
..
1
.1
P
ropounded
In
T
ext
B
ookl. Fig.
11.
pressible fluid.
The
vibr ations transmitted
to
either of
the tuning forks excite them
by resonance and, thru electrical contacts
or
otherwise. bring about the desired re-
sult. This, I may say, was not a
mere
mechanical illustratiOll, but a simple rep-
resentation
of
my
apparatus for
submarine
si/{naling. perfected
bf
me in 1892, but not
appreci
ated at that
time,
altho more
effi-
cit'nt than the
instruments
now in us
e.
The
electric diagram in Fig. 7, which
was reproduced from
my
lecture. was
meant only
for the
exposition
of
the prin-
ciple.
The
i'rrangement. as I described it
in detail, is sh
own
in Fig. 8. In this case
an
alternator
energizes
the
primary
of
a
transfonner,
the high tension secondary
of
which is connected
to
the ground and an
dented
capacity
and
tuned to the imprest
oscillations.
The
receiving circuit consists
of an
inductance connected to the f,:round
and
to
an elevatcd terminal without brea k
and
is resonantly responsive to the trans-
mitted oscillations. A specific form
of
re·
cciving de"ice was not mentioned, but I
had in mind
to transform
the recei" ed
cur·
rents and thus make
their
\'ohlme
and
ten-
sion suitable for any
purp
ose,
Fig.
16.
Showlnll
Un
lmporUnce of
Rel.;n·lle
Po.ltlon
o f
Tr
an.mlUln
g
and
Re
cellling
An_
tennae
D
llprollal
of
the
Hertz·w.lve
In
Th
eo
r
y.
and methods
of
r egulation, now univer_al_
adopted.
The
in timate bearing
of
th
e"C
:n-
l'C'ntions on the development
of
the wirele·
art
will
appear
from Fig.
10,
which illu--
(COnl;'JUCd
0/1
page
(1)
Arrangementl
Qf
D
l
re
~(I"e
Clrc
u 1ts
D
ncrlbed
In
Tnla',
U. S.
Patent
No.
613,8011 01 NOllember 8.
189l1,
on
"Method
of
and
Apparatul
for
Con_
lroiling Mech.nl
l m
Moving
Vu-
o f
..
II
or
Vehlcl
et."
Fig.
12.
This, in
May, 19 19
Th
e T
rue
Wireless
By
Niko{fJ TU/fJ
(ColllilllUd from
page
30)
trates an a rrangement des<:ribed in my U.
S.
Patent
No. 5681
78
of September 22, 1
896,
and corresponding dispositions of wireless
apparatus. The captions of the individual
diagrams
are thought
sufficiently explicit to
dispense with
further
comment. I will
merely remark that in this early record. in
addition to indicating how any number of
resonant circuits may be linked and regu-
lated, I ha"e shown the advantage of the
pro~r
timing
of primary
impnlses
and
use
of ha r monics. In a farClcai wi reless suit in
London, some engineers. reckless of their
reputation, have claimed
that
my circuits
were
not
at all
attuned;
in fact they as-
serted that I had looked upon resonallce as
a
sort
of wild alld ull tamable beast!
It
will be
of
interest
to
I;ompare my sys-
tem as
fin!
deSl;
ribed in a Belgian palent
of 1
897
with the H ertz-wave system
of
that
period.
The
signifil; all t di
ffe
rences between
them will be observed at a glance. The
firs t enables
liS
to transmit economically
energy
to
ally distance and is o f inestimable
value; the latter is capable o f a radius of
ouly a few miles and is worthless. t n the
first there are no spark-gaps and the al;tion s
are C'normously magnifiC'd by resonance. In
both transmitter and recei"er the currents
are transformed and rendered morc effec-
ti,'e and suitable fo r the operation of any
desired de"ice. Properly constructed, my
system is safe against static and other in-
terference and the amount of energy which
may
be
trans mitt cd is
billiolu
of
Ii/lit:
greater
than with the H ertzian which has
1I0ne of these \'irtues, has ne\'er been used
successfully and of which no t race can
be
found
at
prese nt.
A well -adve rtised expert ga"e
out
a sta te-
ment in 1899 that
my
apparatus d id not
work and that it would take 200 yea rs be-
fo re a ml;ssage would be flashed across the
Atianl'iI; and he eve n accepted stolidly my
congratulations on a supposed great feat.
But subsequent exami na tion of the records
showed that my devices were secrt'lly used
all the t ime and ever since I learned o f this
I ha
ve
trea ted these Borgia-Medici methods
.....
ith the con tempt in
.....
hich th ey arc held
by all
fa ir-min ded men.
T he who les al e
o f my inve nti ons was, how-
ever,
no
t al ways without a dive rting side.
A s an example 10 the point I may ment ion
my osciilalion tr
ansfonner
operating wi th
an ai r ga
p.
T his was in tu rn re placed by
a carbon are, quenched gap. an atmosphere
o f hydrogen. ar gon o r helium. by a me-
chanical break
.....
ith oppositely rotating
members, a mer cury interrupter or some
kind of a vacuum bulb and by such
t
Ollrs
de
fo~(t
as many new "systems" ha"e been
-produced. I refer to th
lS
of
course. with-
out the slightest ill-feeling, let us ad,'ance
by all tn('ans. But I cannot help thinking
how much be
tt
e r it would ha\'e been
if
the
ingenious men,
.....
ho have originated these
"systems," had 4n\'emfii something of their
own instead of
de~nding
on me altogether.
Before
19(X)
two mos t "aluable improve-
ments were made. One of tbese was my
individualized system wilh tr.l nsmitters emit-
ting a wave-.::omplex and recei\'ers compris-
ing s('parate tuned elements eoOperatn'el,y
associate
d.
The unde
rl
ying principle can
be
explained in a few words. Suppose that
there are
II
simple vibrations swtable for
use in wireless
tra
nsmission, the probabil-
ity that
anyone
tnne
'l\'
ilI
be str
uc
k
by
an
1
app
r
opr
ia~
i
OIl
extraneous disturbance is -
.
There will
"
then r emain
11-1
vibrations and the chance
1
that one
of
tlleSe
will
be
excited is _ _ ,
II
- I
hence the probability that two tune$ would
[
E
..
•
be
str
llck
at
the
sam
e time is
. Sim-
/I
'
1I~1)
Harly, for a combina tion of three the chance
1
and so on.
It
will
be
will be
n (
n-I
)
(11
-2)
rea
d ily seen
th
at
in
this
ma nner a ny
desired
degre
e
of
safety against the sta tics o r
other
kind
of
disturbance
can
be
a ttained pro-
vided the
Te1:eiving
apparatus is so designed
that
its
oper
.ttioll is possible only I
hru
the
joint
aCiion
of
all the
tutled e lcmcnL.
This
was a difficult problem which I have suc-
cessfully solved
so that
now
auy desired
mUllb
..
r
of
simultalli'ous
messages
is
prac-
!icable
in
the
Inmsmi.uioll
IIrru
the eorlh as
wi'll
as
thrrl
artifi
cial
rOllductol's.
The
other invention.
of
still g
reater
1m-
partance,
is a peculiar o scill
ator
enabling
the
t
ransmis
s ion
of
energy
witho
ut
wires
in any
quantity
that
may
ever
be
require!1
for illuustrial use,
to
any
distance,
and
with
very hiGh ec
ono
my.
l
t was the
ou
tcome
of
years
of
systematic
stu
dy and
investiga-
ti
on and wonders
will
be
achieved
by
its
means.
Th
e
prevailing
misconception
of
the
mech-
anism involved
in
the wireless transmis-
sion
has
been resp-onsible for
various
unwarranted
;lIlnO\lncements which have
misled
the
public a
nd
worked
hann.
Bv
keerJing s teadily ill
mind that the
tran
smi
i-
~iun
thru
the
earth
is in every respect
identical
to
that
t
hm
a s
traight
wire, o ne
will gain
a
cle
ar understanding
o f
the
phe-
no me lla and wi!! be ab
le to
jud~e
correctly
lhe
merits
of
a
new
scheme.
\Vlthout
v.";
sh-
ing to det r
act from
the value
of
any
plan
that
has been put forwa
rd
1
may say
t hat
they a re devoid
of
llOvelty.
So for
i ns t
an
,e
in Fig.
12
arrangem
e
nts
of
tr
a nsmittin¥"
and
re<:
e
i"ing
circuits
arc
illustrated.
whICh
I
have
describe d
in
my
U. S. Patent
No.
613809
of
November
8,
1898
011
a
1lethod
of
and
Apparatus
for ControUi.ng Mechan-
ism
of
Mol'ing
Vessels
or
Vehicles,
and
which
ha\
'e been r ecently di s hed up
as orig
-
inal disc
over
ies. I n
other
pat
en
ts a nd tet:h-
nical publi
cations
I
have suggested
conduc
-
tors
in the
groun
d as one
of the:
obvio\1~
modifications
in
dicat
ed in
Fig.
S.
F
or
the sa
me
re
a son
the
statics
are
slil1
die ba ne o f lhe wireless.
There
is aoout
as milch vi r
tue
in the remedies
recenth
'
p roposed as in
hair·restorers
.
A
.mwll
aud
compact apparatu.r has b.-nt prodl/crd which
does ·au'IlY eulir.-l"
witlt
tltis
trouble
at
least in plants
smiably
remodelJcd. '
Xo
thi ng is more impor
tant
in the
pr
e sent
!)hase
of
development
of
the wireless
art
than
to
dispose
of
the
d o
minating
erroneous
ideas.
With
this objcct I shal1
advanc
e a
few
a
r~uments
ha sed
on
my
own
observa-
tions
which
prm/{'
Illal Hert:;
~MVI'S
hov
l!
little
10
do
witlt
the r ('sulls obtailied
1!t.'CII
at
S11l0/l
disto.,,/!.!.
In
Fig.
13 a
transmitter
is shown
radi
a t-
ing
space
wav
e s
of
cO'l si derable frequency.
It
is general1), believed
that
these
wave~
fI~sS
along
the
ear
th's
surface
and thus
affect
tile receiv
ers.
I
can
hardly
think
of any-
thing
mo
re
improba
ble
than
this
"g
li ding
wave"
theor}'
and
t
he
c oncepti
on of
the
"guided wi.reless" which
are contrary to
all
laws
of
actio n and reaction.
\Vhy
should
these disturban
ces
cling
to
a
conduclor
whe
re
t
hev
are
counteracted by
induced
cur-
r
ents
, when they can
pr
op
agate
in all
other
directions unimped
ed? The fa
ct is
that
the
radiations
of
the
transmitter
passing
along
the
earth's surface
are
soon
extin
g uished.
Ihe height.
of.
the
inactive zone
indicated
in
the
diagram.
bein g some function
of the
wave
length.
the
bulk
of
the waves
trave
r
s-
ing
freely
the
a tmosphere.
Terres
t rial phe-
n
ome
na
which I
have
noted
conclusively
show that
there
is
no
Hta
v isidr layer.,
or
if
it exists,
it
is
of no
effect.
It
certain!)'
would be
unfortunate
if
the
human
race
were thus <imprisoned and
for
ever without
!lOwe r to
reach
011t
into the def)ths
of
space.
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