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Copyright 2025 Manuals.Online. All Rights Reserved.

UDSVRWGVRON MaDWaL
for
TEE
Designed to meet
the
most ex-
acting demands of the more
advanced communication service
Price
10c
Whileintendedprimarily as an operating
instruction manual, it is hoped that this
booklet will also serve to better acquaint
the owner of a National HRO high-fre-
quency communication receiver with the
engineering details of its design. Only by
a proper appreciationof some ofthe many
unusual design features of this new re-
ceiver
is
it possible for the operator to
secure the unusually high degree of per-
formance that we have built into the HRO.
We express indebtednessto the American
Radio Relay League for permissionto re-
print, in part, articles published in past
issues of their official organ,
QST.
NATIONAL
COMPANY,
INC.
Malden, Mass.,
U.
S.
A.
Copyright
1939
The
HRO
Amateur Communications Receiver
T
HEHRO receiver is a high-frequency super-
heterodyne employing nine tubes,
as
fallows:
6eeondR.F
..............................
5s
or6D6
First
Deteotor.
...........................
.57
or
6C6
High
Frequency
OsciUator
.................
.57
or
6C6
First1.F
..................................
58
or6D6
Seoond1.F
................................
58
oieD6
Diode Detector,
AYC,
First Audio.
.........
.2B7
or
6B7
SeoondAudio
.............................2A5or42
Beat
Frequency
Osoilistor.
................
.57
or
6C6
Unless otherwise specified, all models are
equipped with 6.3-volt tubes, for either A.C. or
battery operation.The2%-volt tubes ean be used
if
desired,sincethetwotypesareinterchangeable,
but the6.3-volt tubes
are
to
be preferred.
For A.C. operation, the receiver
is
adjusted to
give best performance with
the
National type
697 AB power unit, which delivers 230 volts at
75 milliamperas, ~nd6.3 volts at3.1amperes.
The battery model, type HRO-B, is djusted
for maximumperformancewith a plate potential
of 180volts at a current drain of approximately
55 milliamperes. Normal operation from A.C.
lines with the
HRO-B
can be secured by the em-
ployment of a National type No. 5886 power
pack, a unit which, under load, delivers approx-
imately 170 volts D.C. at 50 milliamperes and
.
6.3 volts A.C. at3.1 amperes.
All
voltage dividers, bias requirements, etc.
are built into the receiver.
Other power units may be used provided they
will fulfil these specifications closely, but it is im-
portant that an adequate heater supply be fur-
nished to compensatefor the voltage drop in the
heater leads
of
the power supply crthle.
The HRO receiver
has
been designed around
and tested
with
RCA or Sylvania tubes; conse-
quently, we can vouch for its performance only
when these tubes are used.
Antenna
The input circuit of the HRO is arranged for
operation with either the doublet type or the
single-wire type of antenna. There are two input
binding posts, marked "ANT" and "GND."
When using a single-wire sntenna, the lead-in
shouldbe connected
to
the antenna post and the
short flexible lead, which is connected
to
the
chassis near the ground post, should be clamped
under the "GND" terminal. An externalground
connection mav
or
mav not be neoessarv. deoend-
,.
.
Lng
iupcm
rht ~r~if~ll~rt~~:~.
TL
ground
id
uiuaUy
rlcsi~.ablesvilett receiviug \r.avcle:.grlu ab~vz
100
n,cte<>,hut ior
STAY
,iragtl.r bcl>.v
80
lueter~,rhv
use of a ground may actually weaken signals.
Doublet antenna feeders should be connected
directly
to
the input terminals and the flexible
ground connection, mentioned above,
is
not used
atall.
TheInput impedanceof thereceivervaries over
the total frequencyrange but averagesabout 500
ohms.
Output
Circuit
T1.e plarc circuit
oi
the cutl,ut rubc is broughr
ro the cutl~ut
t~p
jack I>mted
~t
the
rehr
left-
I.:xl.rl -iJc. 'l'hcre is no
<,UlDUr
rr3nzformer
m
rhe
receiver.
Thespeaker requirementsarenot atallcritical,
5
but tone quality will, of course, depend almost
'
entirely upon speaker characteristics.
A
good
*
'-
magnetic speaker will be satisfactory,provided it
is capable of carrying the plate current of the
output tube (about 30 ma.). Many magnetic
speakerswill requirea filtersystem,however, and
such a
filter
may consist of a l-to-1 transformer,
or a 30-henry choke and a l-mfd. condenser.
Dynamic speakers are, in general, superior to
the magnetic types, but if these are used some
DravisiOn must be made for field excitation. since
this
power
ramor be oornincd eitller ilo~uthe re-
ccivcr or t1.c pon.sr unir.
K,r
rhi. reat"", rLe per-
manent rnsgner r).p20i
dyunmi;
apesker
i>
rerorn-
mended, no field excitation being requ~red.The
output impedanceof the HRO is 7000 ohms, and
a dynamic speakermust, of course, have a snita-
ble built-in coupling transformer of 7000-ohm
input impedance.
Aheadphonejack is located on the front panel,
just below and to the right of the "S"-meter.
This jack
is
wired into the output of the pentode
section of the 6B7. When the phones are plugged
in,
thesignalinput to the la$t tube is completely
disconnected.Itis important, however, that the
plate circuit of the output tube be completed at
all times.
If
the speaker is to be disconnected,
a
jumper must be inserted in the tip jacks to con-
nectthemtogether.
If
thisprecautionisneglected,
theoutput tubemay be seriouslyinjured.
THE HRO RECEIVER
THE HRO RECEIVER
5
Controlr
The main tuning dial is located near the eent,er
of thefront panel and operates the Cgang tuning
condenser.
Full
details of the tuning arrangement
aill be found in the last section of this booklet,
which is reprinted from
an
article originally ap
pearing in
QST.
Starting atthe top right-hand sideof the front
panel, the uppermost knob is the Variable Selec-
tivity Control of the Single-Signal Crystal Filter.
With the crystal filter inuse, minimum selectivity
ill
be found with the pointer nearly vertical.
Rotating the knob in either direction
from
this
point
niU
increase thcselectivity. When the filter
is not in use, the knob should be set atthe point
giving maximum volume and sensitivity.
Immediately below the Selectivity Control is
the Phasing Control and the Crystal Filter
Su-itch. When this control
is
rotated to
0,
the
crystal filter is disconnected. When the control is
atanyothersettingbetwee11
1
and
10,
itacts
as
n
phasing condenser for balancing the crystal
bridge circuit, eliminating heterodyne?, etc. The
action of these two controls is explained in detail
in
Part
2
of the Alignment Section.
The switch below the phasing control is
eon-
nected in the
B+
lead of the receiver and its pur-
pose is
to
shut
off
the receiver
during
periods
of
transmission OR WHEN CHANGING COILS.
This lartfunction is important. Sel.ies connected
ulth the
B+
switch and mounted atthe rear of
the chassis is
a.
pair of oontaots, BSW, intended
forusewith relay control of thereceiver.
The
hottom controlon theright-hand sideis an
R.F. Gaul Control, connected to the second R.F.
tubeand to thetwo I.F.
tubes.
At the bottom left-handside of the front panel
is
located the C.W. Oscillator Switchand Vernier
Tuning Control. Thec.~.oscillator isused to ob-
tain an audible beat note when ~zceiving
O.W.
signals
or
to locate the carrier of
weak
phone and
broadcast stations. After the phone carrier has
been found, the
o.~.
oscillator is, of course,
turned off.
The switch just above the c.w. beat oscillator
dial is far turning the AVC on
or
off.
AVC
ie
dis-
connected with the toggle thrown to the right.
Above this switch is the Audio Gain Control,
which is wired into the output of the diode de-
tector and
swves,
therefore, to control audio
volume xrhen using either headphones
or
speaker.
The S-meter for indicating carrier intensity of
signal strength is in the upper left-hand comer.
Just below it, and to the left, is
a
push-switch
which connects the meter in the circuit.
Operating Instructions
Phone
or
Broadcart Reception
In receiving phone signals, the AVC may
or
may not be used,
as
desired. If it is not used, we
sueeest
onerxt,inr
t,he
audio gain control about
halfway
on
and controlling the sensitivity with
the
R.F.
gain control. If the operator prefers a
"quiet" receiver, the audio control may be op-
erated at
1
or
2.
If
AVC is used (left-hand toggle
thrown to the left), the R.F. gain control may be
turned all the way on;i.e., to
10;
and the volume
controlled by the audio gain control only. The
setting of the turogain controls
is
largely a mat-
ter to be determined by the preference of the
operator and by receiving conditions. If, for in-
stance, local noise
01.
atmospheric static
is
high,
it aill be desirable to retard the R.F. gain con-
trol when using AVC
so
that the sensitivity of
the receiver will be held to
a
definite maximum.
1
If the
C.W.
oscillator is to be used for locating
carriers, as mentioned above, the AVC switch
must be intheoff position (to theright). Turning
on
the e.w. oscillator with the AVC an will block
the reccivei, making reception of anything but
.
extremely strongsignals impossible.
C.W.
Reception
When receiving c.w. signha, the c.w. oscillator
must be turned on and the AVC switch turned
off.Best signal-to-noise ratio will usually be ob-
tained by retarding the audio gain control
considerably and controlling sensitivity with the
R.F. gain control. Turning on the c.w. oscillator
switch will, of course, result in
a
considerable in-
crease in circuit noise. When the control is turned
back and forth, the characteristic pitch of this
noise will change. When the characteristic pitch
is fairly high, the semi-"single-signal" properties
of
the receiver are very pronounced, one side of
theaudio beat note beingseveral times
as
loud
tu;
the other.
Phone Reception Uring the Crystal Filter
The use of the crystal filter in phone reception
is recommended particularly when tho operator
must contend with heavy interference, static,
heterodynes, etc. Since such conditions prevail
at lnost times in the amateur phone bands, the
filter will be found particularly useful to amateur
phone operators. To receive
a
phone signal when
using the crystal filter,the fdter is switched in by
means of the phasing control and the phmhlg
dial set atapproximatsly mid-scalo. The selectiv-
ity control is then adjusted for minimum
selec-
tivity,
ar
indicated by maximum noise
as
the
control is rotated buck and forth. All phone sig-
nals will be greatly reduced in volume, making it
necessary to advance both audio and R.F. gain
rontrols. The signals may then be tuned in in
the usual manner, but it will
bc
found that the
selectivity is very high, with the result that all
audio frequency side bands above a few hundred
cycles are comparatively weak. Normally, thi?
nould result in low intelligibility of the received
signal, but since the background noise, static,
etc. hsve been oorrespondingly reduced, the net
result is usually animprovement.
The principal advantage of the crystal filter,
6
THE HRORECEIVER
however,
is
its ability to eliminate heterodynes.
Suppose,for instance,a signal hssbeen carefully
tuned in with reasonably good inteuigibility and
during the transmission an interfering station
comes on, causing a bad heterodyne, inverted
speech, etc., ordinarily the desired signal would
be "smeared," but careful adjustment of the
phasing condenser will eliminate the heterodyne
and the interfering station, in most oases, com-
pletely. Intelligibility will remain practically
ss
good
as
beforetheinterfering station came on.
From a practical standpoint, it is important
that the crystal filter be used most of the time
wheresuchinterferenceis aptto be encountered,
as
it
is almost impossibleto switch on thecrystal
filter and re-tune the desired signal through the
heterodyne. The phasing adjustment will remove
one signal only.
If
another interfering station
comes on, however, only one heterodyne will he
present, instead of the several resulting from
three station carriers beating together.
C.W.
Rece~ticnwith the Crystal Filtel
To use the crystal aterfor ow reception, the
flier
is
switched m by means of the phaslng
control and the
ha sing
condenser set about
mid-scale, The AVC switch must be off and the
c.w. oscillator turned on. Advancing the
R.F.
and audio gain controls mll result in a hollow,
ringing soundthepitch of which %dldependupon
the setting of the 0.w. oscillator dial. The actual
pitch is not important
as
long as
it
is
near the
middleof the audiorange, where thelondspefiker
or phones have good sensitivity.
When a signal
is
picked up, it
will
be found
that
as
the recaver
is
tuned slowly across the
carrier the beat note will be very sharply peaked
at the same pitch as that
of
the ringing noise,
previouslymentioned.
All
other parts of the beat
note will be extremely weak and, furthermore,
this peak will be foundto occur on only one side
of theaudio beat note. The sharpnessof thepeak
is
determined by the selectivity control (upper
righehand knob). At
maximum
selectivity, the
peak is so sharp that it may be hard to hd,
whereas at minimum selectivity thepeak will he
very broad. If a signal
is
being received, after
,
havlng been properly tuned in, and an inter-
feringstation comes on, theresulting heterodyne
and
interference
may be eliminated by adiust-
ment of the phasing condenser. Th~sphasing
adjustmentis effectivein elunmnatinginterference
regardlessof the setting of the selectivity control.
S-Meter
The &meter serves
to
indicate the strength of
a received signal. It
1s
calibrated from
1
to
9
in
arbitrary nnlts which correspond,roughly, to the
defilutionof the mne points of the
"S"
scale of
the R-8-T system of amateur signalreports.
Probably no two operators
mll
agritgree
on just
how strong a signal must be to warrant an
8-9
report. After making measurements on a large
number of amateur signals, the present meter
scalewas chosen and we believe
it
will
provide
a
good practical
invans
oi giving svumate repow.
The
avcomp3nying rurvr rl.ow the
rplation
bcmeen averhpa mctcr rcadinci aud the actual
signal input toreceiver in mi&volts snd from
this curve it
wdl
he noted that each
"SS"
unit
is
equal to a change of app~oxunatelg
4
db. The
40
db. range above the
8-9
level is used for com-
parative checks on extremely strong
s1gnal.s.
Figure
3
shows the "S-meter" network eon-
nec$ed in the
B
supply circuit
to
the
RF.
and
I.F.
stages. Actually themeter
is
themdicator of
a
bridge clcuit, three legs of which
are
6xed
resistors, and the fourth (variable) leg the plate
circuitsof the a.v.c. controlledtubes. The br~dge
is hallanced by means of the manual R.F. gain
control, which, through
its
action of indirectly
changing the plate resistance of the tubes, auto-
matically adjusts the
R.F.
and
IF.
gain
to
a
predeterm~nedlevel at the same time that the
meter
a
brought to zero. The strength of the
incomngsignal
is,
therefore,accurately indicated
by the acQonof the A
V.C.
circuitsin controlling
high frequencygain.
Before making a measurement on a
signal,
certain adlnstmente must he made. Since the
meter is actuated by the amount
of
signal
reach-
ing thesecond detector, itis obviously necesary
that the receiver he adjusted to have a prede-
termined amount of ampli6cation betrreen the
antenna and second detector.
To
adjust the
amplificaizon to the proper value, the
.4VC
switch must be off, the C.W.oscillator
off,
the
crystal filter off, and the selectivity control set
for maximum sensitivity. Now
press
the meter
switch and advance the R.F gain control untll
the meter comes to
0.
The
R
F. gain dial
will
read about
9%.
The receiver
is
now adjustedand
THE
HRO
RECEIVER
7
the strength of any
signal
may he measured by
,
tbrouing the
AVC
switch on and tuning for
maximum meter deflection. The audio
gain
con-
trol does not have any effect onthe RF. adjust-
ments or upon the meter reading,
so
that itmay
be
retarded
as
much as necesary to prevent
audio overload when making the preliminary
.
adjustments.
If
the signal being measured
is
extremely
strong, honxever, or
if
loeal noise is exceptionally
high, it may
be
impossible to bring themeter to
0.
In
this
case.
it is necessary to detune the
&ve~
from the
signal
or to dimnnect the
antenna. The above procedure will hold true
when eheeking either phone or
C.W.
stations.
It
is, however, impossible to obtain
a
continuous
check on c.w.
signals,
as
the beat oscillatormust
be
off.
If
it should happen that the Smeter network
getsout of balance, thealignmentprocedure is
as
follows.Disconnectthe antenna and turn offthe
AVC,
set
the R.F.
gain
wntml at
9%,
then, by
means of a serew driver, adjust the wntml
No.
17
(as
shown in the top
view)
until the
meter
reads
0.
This wntml is located in the
chasis
in
back of the meter near the antenna
bindingpost.
Coil
Ranges
Four plug.in coil assemblies are supplied as
standard equipment for the
HRO
receiver, each
assembly consistine of three R.F. wils and one
oscillator coil,
all
individually shielded and
provided with built-in trimmer condensers.
Calibration curves
are
mounted on the fmnt of
eachassemblv.
The four Aemblies cover all frequencies be-
tween
1.7
and
30
megacycles, the division being
as
follows:
1.7
to
4.0
mc
3.5
to
7.3
mc.
7
0
to
14.4
mc.
14.0
to
30
0
mc
Inspectionof the milterminalpanels
win
show
several small rectangular metal pieces. There
are
two of thesepiemsorterminal blocksoneach
of the coil pad.
A
small flat-head machine
screw
will
be found in the left-hand termmal
block of
each
mil, looking at the assembly from
the front. With the screws in the lefeband posi-
A
tion, the coil range will he that shown in theleft-
hand, orgeneralwverage, cbart.
If
itisdesiredto
change the calibration to smateur band-spread,
as
shown on the righehand chart,
it
isonlyneces-
sary
to move the four serews to the righehand
terminal block of esch mil.
A
complete description of the wils, tuning
condensers, and the rwechanging system, is
given in the lastsection of this booklet.
In addition to the coils furnished
as
standard
equipment, other assemblies are available, wv-
ering frequencies fmm
2.05
mcs. to
50
kc. and
rsre listed on the back cover of this manual.
Alignment and Service Data
T
HE four high-frequency coil &lies are
slirmed in the laborato~to the individual
receiver
with
which the" agto
be
used.
No wil
~~~
~-
~
"
~ ~ ~
~~
~~~~~~
~
~~
~
sdjusrments
of
any kind shouldbe ny
after
the receiver is put inu, operation, but
d
cokare
purebased separ~telythe &went should be
checked in aocordsncc with the following pro-
cedure.
The mil panel screws must be in the left-hand
terminal
blocks togive thefullcoverage range,
as
described in the preceding section. The tuning
dial is turned
to
aonrohtelv
490
and
a
fre-
.
.
quency meter, or
accurate
test
oscillator,
is set to
the frequency in&caied b.v the general wverage
calibrauon chart.
This
nffl,
moldentally, always
be near the high-frequency edgeof someamateur
band. The dtorcoil trimmer, shown on
the top view of the receiver
as
No.
8,
is then
adjusted so that the
dial
reading checks the cali-
bration curve. TrimmersNos.
Z,4
and
6
arethen
adjusted for
maximum
sensitivity. In adjusting
these three trimmers, no
signal
is nee-ry,
as
the correct adjustment is that wbich
mill
give
dumbackground cr tube noise. This back-
pund noise should be fairly loud when the
R.F. and audio
gain
wntmls arefully advanced,
the crystsl filter being switched off. The tuning
dial
should then he rotated to the low-frequency
end of the range. The hackground noise should
not vary greatly as the dial is being turned.
If
it
does, however, poor ganging
is
indicated.
Thegangingis checked by pressing the outside
rotor plate of the osoiUator condenser sideways
toward the stator, but not
far
enough to short the
condenser.
If
sensitivity
is
increased, more in-
ductance is needed in the oscillator coil. On the
two low-freauencv mil assemblies oscillator in-
ductance is &creased by loosening the nut which
holh the inductance trimmer disc, inside the
crscillstor coil, so that the
disc
may move toward
the back of the coil shield.
If,
however, sensitiv-
ity decreases when the osdator rotor plate is
bent toward the stator, the other condensers,
particularly the first detector tuning condenser,
should he tested the same way.
If
sensitivity
decreaseswhen the mtor plate is moved in, gang-
ing
is perfect and the general wverage range
is
wmpletely adjusted. However,
if
sensitivity
increases, the oscillator mil inductive trimmer
must be adjusted to decrease inductance. In the
caseof the
14
to
30
and
7
to
14.4
megacyclemils,
inductivetrimming is accomplished by moving a
8
THE
HRO
RECEIVER
-
TOP
VEW
HRO
loop of wire around the end of the oscillator coil.
Bending this loop from right to left across the
end of the coil form \rzill increase inductance.
After any change in the oscillator coil inductance
has been made, it will be necessary
to
tune back
to
the high-frequency end of therange in order to
readjust the No.
8
trimmer condenser. The pro-
cedure
rts
outlined above is then repeated until
the gauging is correct.
It
will he found that the setting of the various
trimmers, particularly the No.
8,
is quite critical,
but that the setting of the inductive trimmer is
not at
a11 sharp and, whenmaking theinductance
adjustment, the nut may be rotated a full turn
for eachtrial.
In the case of the 14 to 30 megacycle coils,
special care must be exeroised
to
see that the
oscillator
is
operating on the high-frequencyside
of the signal. Two points dlbe found when ad-
justing the No.
8
trimmer and of these, the cor-
rect oneis on the counter-clockwise side. Further-
more, in adjusting the No.
6
trimmer of this coil
assembly, there will be someinteraction or inter-
locking between the &st detector and oscillator
circuits.
In
adjusting the No.
2
trimmer,
it
will
he necessary to have the antenna connectedwith
some signal
or
noise input.
The band-spread range may now be adjusted.
It should be pointed out here that adjustments
forthegeneral coveragerangewilldeetthehand-
spread range, but the separate band-spread ad-
justments may be made without changing the
general coveragealignment.
The four screws must be shifted to the right-
band terminal blocks, as outlined under "Coil
Ranges" in theprecedingsection.Thetuning dial
is set at 450 and a test oscillator adjusted tothe
exact high-frequency edge of the proper amateur
hand. Trimmer No.
7
of (the top view) is
adjusted until thesignal is picked up. Trimmers
Nos.
1,
3
and
5
are then adjusted for maximum
sensitivity. The dial is then rotated to the low-
frequency end of the band; thatis, to 50; and the
right-hand calibration curve should be checked.
If found incorrect. it will be neeesssrv to adiust
from the rear by means
of
a screw driver. If the
low-frequency end of the hand
is
tuned in atany
dial reading above 50, the capacity of this series
padding condenser must be decreased.
If
the
.
low-frequencyedge of the band is found between
0 and 50, the capacity must be increased. The
setting is critical. After making a trial adjust-
ment, the dial is returned to 450 and trimmer
No. 7 readjusted. The above procedure
is
re-
peated until thedialchecksthe calibration curve.
Tracking of the two
R.F.
and first detector
circuits may then'be checked by tuning to the
low-frequency end of the band and checking the
adjustment of the Nos. 1,
3
and 5 trimmers. If
more capacity is needed for best sensitivity (as
indicated by improved signal strength when the
trimmer is rotated clockwise), the series padding
condenser of the coil beine adiusted must have
more capacity. If any of tge
Gas.
1,
3
or 5 trim-
mers require less capacity, a col~espondingde-
crease must be made in the capacity of the series
padding condenser. After the series padding
condenser has been adjusted for trial, the dial is
returned to 450 and the procedure repeated.
Theabove instructions may seem complicated,
but they cover complete alignment under the
worst possible conditions, where everything is
out of adjustment. Thechances are that the only
adjustments that !%.ill need to be made
are
the
conventional trimmer adjustments of the trim-
mers Nos.
1
to
8.
Simple antenna compensation for the general
coverage range is made by adjusting trimmer
No. 2, and for the bandspread range by adjust-
ing trimmer No. 1.
The inst~uctions!+,ill probably be simplified
after reading the general description of the tun-
ingaystemgiven inthelastsectionof this booklet.
With regard to the coil groups covering the
frequencies between 2.05 megacyales and 50
kilocycles, there are only five tl.immer adjust-
ments. These are Nos. 2,4,6,7 and
8.
The No.
8
adjustment is used here
as
in the other coils for
adjusting the oscillator circuits
to
correspond
with the calibration. The No. 7 trimmer is the
conventional seues paddmg adjustment. Nos.
2,
4 and 6 are the usual trunmers.
I.F. and Crystal Alignment Instructions
Before attempting to check the alignment or
adjust a single signal receiver it is essential that
the operator be familiar with the principles in-
volved and the type of performance to be ex-
pected.
A
receiver of this type is simply a superhetero-
dyne which may be adjusted to have extremely
high selectivity on all signals. The effective
rr~idthof theselectivity curve is only a few cycles,
usually between 20 and 100. This means that
when tuning in
a
given c.~.signal, tuningis going
to be very sharp and the dial must be turned
slowly in order to avoid missing the signal en-
tirely. As compared to the straight superhetero-
dyne, the single signal receiver is about 100times
as selective. The straight super will pick up a
signal and \\-illreproduce both sides of the audio
beat note atabout the same strength;thatis, the
carrier whistle may be varied from either side of
zero beat up to about 3000 cycles when the re-
ceiver is tuned and the rhistle
will
remain about
the samestrengthat any pitch. The
s.8.
receiver,
however, being 1W times
as
sharp, will not per-
formin this manner, but as the receiver is tuned
across the carrier the audio response will be very
sharply peaked at
one certain pitch of the carrier
whistle. Detuning the receiver a small fractionof
a degree, while it changes the pitch only slightly,
vill make the signal much weaker, since it has
been detuned from the sharp selectivity peak.
It
is
evident. therefore, that the ereat selec-
riviry &vallaule
chows
up a5
:t
peak in the audio
response
and
\rlrcn
tl,,:
receiver is in operation all
;ig!~ul-.after theilly c.rrectly tuned, n.111 pe~kut
the same audio frequency,
General
Superheterodyne Theory
and
the
Explanation of Single Signal Operation
(It
is
extraelg important
lhol
these
par*
graphs
be
vow
carefullv studied.
if
a full
Tothose who are not entirely familiar with the
operating principles of a superheterodyne, the
,
followingexplanation may he of interest:
Itis the function of the first detector and high
frequency oscillator of a super to convert a high
frequency signal to the tlequency of the inter-
mediate amplifier. If, for instance, a 7000-k.c.
signal is being received, the high frequencyoscil-
lator, in the case of the
HRO
receivers, will be
tuned to 7456 k.c. producing
u
heat with the
signal equal to the difference between these two
frequencies;that
is,
456 k.c., thefrequency of the
I.F. amplifier. The456-k.c. beatisamplifiedin the
I.F. amplifier and is detected or de-modulated in
the case
of
phone signals at the second detector.
When receiving
C.W.
signals a beat note is ob-
tained by theuse of
a.
separatebeat osoillator oou-
pled to the second detector and operating at,
or close to, the intermediate frequency. If the
beat oscillator is tuned exactly to 456 k.c. and
if
the signal mentioned above is tuned to give
an
I.F.
beat of exactly
456
k.c., itisevident that
the receiver
as
a whole will be tuned to Zen
beat.
An audibleheatnote maybeobtained by doin(
either one of two differentthings. The first is
ta
change thetuning of the highfrequency oscillato:
(by means of the tuning dial) slightly, so that ix
wrll produce
a
different I.F. heat with the signal.
For example, suppose the dial is changed so that
the high frequency oscillator oscillates at 7457
k.c.; the I.F. beat will now be 457 k.c., which will
he amplified
as
before by the intermediate am-
plifier, hut when reachingthe second detectorwill
produce a
1
k.c.
(thousand cycle) audio beat with
the beat oscillator, which is operating at456 k.c.
as beiore. Similarly, the tuning dial could he
moved in the other direction, so that the high
frequency oscillator is tuned to 7455 k.c., in
which event the I.F. beat wouid be 455 k.o. and
the audio beat note would
be
a
thousand cycles
but on the other side of the carrier.
Theselectivitv of theI.P. amolifier
is
suchthat
a
signal
derultrd from ir by obly one klh,cycle
(.2
oi
1%)
sill
-rill
be
,.mpliticd almost
as
much
ash
l.-~ti->r.
.igual, altht~ugl.tl.ere \\'.II,
oi
vourre,
be some lossingain.
The other method of getting an audible beat
THE HRO RECEIVER
note
is
toleave the signaltuned exactly,as in the Preliminary Adjustments -The
I.F.
originalcase, with the 456-k.c. I.F. signal hut to
detune the heat oscillator so that it operates at From theaboveexplanation,thereader
wi!l
see
ay
457 l~.~.~h~ I.F. amplifieris
now
exactlyin that it is absolutely essential that the I.F. trans-
tune with the I.F. sigdal and will amplify it & formers be aligned to the crystal, since the two
fullefficiency.Theheat note
will
he 1000cycles,as m& work together. This alignment myhe
before. This method, wherein the signalis tuned accomplished in a number of ways.
If
the
I.F.
exactlyand the beat obtained by detuningof the tramformers are far out of adjustment,
it
is
beat oscillator,is fundamentallythat used in any necessary
$0
Connect an externalcrystaloscillator
single signal or semi-single signal receiver.
It
is
which uses the crystal from the receiver. This'
evident that cbngingthetuningdialslightlywill oscillatoris putin operationand is coupled tothe
detune the I.F. signal from the I.F. amplifierso &st detector of the receiver. In most cases no
that it will not be amplified
its
much, actual connection will he required since the field
corresponding decrease in the strength
of
the fromthe oscillatorwill be sufficientlystrongto be
audio beat note: thw,
if
tuning is changedin such picked up, even with the I.F. far out of adjust-
s.
way as to raise the pitch of the heat note, the ment.
If
Coupling is required, a lead twisted
signal will he weaker. Similarly,
if
the tuning
is
aroundthe grid cap of the detector tube and
run
changed tolower thepitch down toward the sen,
near
the oscillatortank coil,
will
be suitable.The
heat region, the signal
will
he weaker.
If
the
tun.
beat oscillatoris turned onand adjusted untilthe
ingisstillfurtherchanged, so
that
theaudionote orystal signalis picked up. Thepitch of the heat
passes through the zero beat, region,and
nup
the note is not. important as long
as
it is well inside
other side of the carrier," the signal will beoome the audiblerange.
weaker still. Thefalling
off
in signalstrength, as All the I.F. transformers
are
now adjusted
for
the receiver tuning is Changed, is due entirely
to
maximum signal. This adjustment need not he
the selectivityof the I.F. amplifier. Supposenow madewith anygreat degree of precision, sincethe
that the I.F. amplifier has very high selectivity, cr~8talwill not oscillate at exactly the same fre-
as is the case when filter employedin quency to which it will he resonant in the re-
singlesignalreoeption;the crystalwill pass only a ceiver. Thephasing controlshould he set at"0".
very narrow hand of frequencies, say from455.9 The five I.F. adjustments are indieatedon the
k.c. to 456.1 k.c. It will he necessary, therefore, top view, NOS.10to 14 (inclusive).
to tune the signalso that the I.F. beat
is
isxactly The crystal filter output ooupling condenser,
456 k.c., and in order to obtain sn audible beat adjustment No.
9,
servesas a fixedI.F. gain con-
note, the heat oscillator MUST be detuned.
If
trol and, in general, sliould notbe touched.
-.
the heat osciUatoris set
as
beforeat457 k.c., the The crystal may now be removed from the
beat note will be 1000cycles.Detunjng, asin the oscillatorand installedinthereceiver. Throwthe
shove ease, will make the signal in- switch to connect the crystal for single signal
mdihle, except atthis one pitch, and "the other reception.Settheseleotivity controlformaximum
iideof thecarrier," or audioimage,will be almost selectivity; that
is,
with the pointer rotated
all
?ntirelysuppressed. the way totheright. Now, tune in a steady signal
With the receiver tuned exactly so that the from a looal oscillator or monitor. Tuning very
;rystal will pass the 1.F. beat, the beat waillator 810~1~across the carrier, there should be one
nay be adjusted to giveany desired
audible
beat point atwhich the signal
will
peak very sharply.
lote. Inthe above case, the heat oscillator being The audio pitch of
this
peak
will
he nearly the
;et at 457 k.c. produced a 1000-~~clebeat same as the pitch of the beat used when the
ghich all signals would be ~eaked.
If
the beat crystal oscillator was being picked up.
)scillator were set at 458 k.c., all signals would
)e peaked at 2000 cycles. The
Beat
Oscillator
If
the receiver tuning is left alone, then, the
beat oscillator may be adjusted to give any de- Once the peak h& been found,itwould he well
4
siredpitoh without changing the signal strength. for the operator to familiarize himself with the
Any change in tuning which changes the pitch action of the heat oscillator control by changing
of the audio signal will greatly weaken the its tuning
in
orderto obtain an audio note which
signal. ismost pleasing to, copy,
or
which coincides with
any peak in the loudspeaker or headphones.
It
makes little differenceto which side of the audio
.
The
main
point
to
Iemember
when
'On-
heat the beat nosoillator
&
tuned. After a
sstb
sidering anglesignal receivers is that they factory pitoh has been found, tune the signal by
aresimplyultra selectivesuperheterodynes, means of the tuning dial so that the signal
goes
which must be tuned exactly tothe signal down through zero heat and UP to approldmately
the samepitch on theother side. Thisresponse
is,
and
that
the
beat
oscil'ator
bedetuned
of course,much weaker thenthat of the peak and
fromthecr~stalfrequenc~inordertoobtain it
may
he to
turn
up
the volume
eon-
anaudible beat note. trol inordertoobtainfairvolume. Thephasing,or