Model 333A/334A 
Section IV 
SECTION 
IV 
THEORY 
OF 
OPERATION 
4-1. 
OVERALL  DESCRIPTION. 
4-2.  Models 333A and 334A Distortion Analyzers in- 
clude 
an 
impedance converter, 
a 
rejection amplifier, 
a 
metering circuit,  and 
a 
power  supply.  The Model 
334A  also 
contains 
an 
AM 
detector.  The impedance 
converter  provides a 
low 
noise  input  circuit with 
a 
high input impedance independent 
of 
source impedance 
placed 
at 
the INPUT terminals.  The rejection ampli- 
fier 
rejects the fundamental frequency of  the 
input 
signal 
and 
passes 
the remaining frequency components 
on to the metering circuit for measuring distortion. 
The metering circuit provides visual indications  of 
distortion 
and 
voltage 
levels 
on the front panel meter, 
M1.  The 
AM 
detector (Model 334A only) detects the 
modulating 
signal 
from the 
RF 
carrier 
and 
filters 
all 
RF 
components from the modulating 
signal 
before 
it 
is 
applied 
to 
the impedance converter circuit, 
(Refer to Figure 4-1) 
4-3. 
BLOCK  DIAGRAM  DESCRIPTION. 
level 
applied to 
the 
metering circuit to 
1 
mV  for  full 
scale deflection.  Sensitivity 
of 
the metering circuit 
is 
increased to 300 
pV 
for full scale deflection onthe 
.0003 
Vrange. 
The metering circuit provides a visual 
indication  of  the  distortion level 
of 
the input  signal. 
In 
addition to the indication provided 
by 
the 
meter,  the 
OUTPUT  terminals  provide 
a 
means 
of 
monitoring 
the distortion components. 
4-8.  DISTORTION MEASUREMENT 
IN 
AM 
CARRIERS. 
4-9.  The 
Model 
334A Distortion Analyzer contains an 
AM 
detector circuit for measuring envelope distortion 
in 
AM  carriers.  The input 
signal 
is applied to the in- 
pt 
of 
the  AM  detector circuit where the modulating 
signal 
is 
recovered from 
the 
RF carrier.  The sipal 
is 
then  applied  to the  impedance  converter circuit 
through 
the one megohm  attenuator and then  through 
the  same circuits previously described in the distor- 
tion measuring mode operation. 
4-4.  DISTORTION MEASURING OPERATION.  4-10.  VOLTMETER OPERATION. 
4-5.  For distortion measurement,  the input signalis 
applied to 
the 
impedance converter  (Assembly 
A2) 
through the  FUNCTION  selector,  S1,  and the  one 
megohm attenuator.  The one megohm attenuator 
is 
a 
voltage 
divider 
network which provides 50 dB atten- 
uation 
in 
10 
dB 
steps.  The desired level of  attenuation 
is 
selected 
by 
the  SENSITIVITY selector, 
S2. 
The 
impedance 
converter provides impedance matching and 
unity 
gain between the INPUT terminals and the input 
of  the rejection amplifier. 
4-6.  The rejection amplifier consists of 
a 
preamplifier, 
a 
Wien 
bridge, andabridge amplifier.  The SENSITIVITY 
VERNER control, 
at 
the input 
of 
the preamplifier, 
provides 
a 
set 
level 
signal 
to 
obtain 
a 
full scale read- 
ing on the meter for any voltage level at the input 
of 
the 
instrument. 
With the FUNCTION switch inthe SET 
LEVEL position, 
a 
ground 
is 
applied to the Wienbridge 
circuit to allow 
a 
signal 
reference level to be set up 
on the meter. 
With 
the FUNCTION switch 
in 
theDIS- 
TORTION position,  the Wien bridge 
is 
used as an in- 
terstage coupling network between the preamplifier 
and bridge amplifier.  The Wien bridge 
is 
then tuned 
and balanced to reject the fundamental frequency 
of 
the 
applied input 
signal. 
Two automatic control loops con- 
sisting of 
two 
phase detectors,  lamp drivers,  lamps, 
and photocells provide fine 
tuning 
and balance  in  the 
AUTOMATIC MODE.  The remaining frequency com- 
ponents are applied to the bridge amplifier and 
are 
measured 
as 
distortion by  the metering circuit. 
Nega- 
tive feedback from the bridge amplifier to the preamp- 
lifier narrows the rejectionresponse of  the Wien bridge. 
4-7.  The output of  the rejection amplifier 
is 
applied 
to the  metering circuit through the post-attenuator. 
The post-attenuator 
is 
used  to limit the input  signal 
4-11.  In the voltmeter  mode  of  operation, the input 
signal 
is 
applied to the impedance converter  circuit 
through the 
1:l 
and 
1OOO:l 
attenuator.  The 
1:l 
atten- 
uation ratio isusedonthe0.0003 too. 
3 
VOLTSrangcs, 
and 
the 
1OOO:l 
attenuationratiois used in the 
1 
to 300 
VOLTS  ranges. 
With 
the  FUNCTION switch 
in 
the 
VOLTMETER  position,  the  output of 
the 
impedance 
converter bypasses the  rejection  amplifier  and 
is 
applied  to the  metering  circuit  through  the 
post- 
attenuator (METER RANGE  switch).  Metering circuit 
sensitivity 
is 
increased  from 
1 
mV  for  full  scale 
deflection to 
300 
pV on the ,0003V range, 
as 
it was in 
the distortion measuring operation.  The function 
of 
the post-attenuator and metering circuit 
is 
the same 
for 
voltmeter operation as for the distortion measuring 
operation. 
4-12. 
DETAILED  CIRCUIT  DESCRIPTION. 
4-13.  IMPEDANCE  CONVERTER CIRCUIT. 
; 
4-14.  The input 
signal 
is 
applied  to the  impedance 
converter circuit through the 
1: 1 
and 1000: 
1 
attenuator 
S3R12 
in  voltmeter  operation,  and  through  the  one 
megohm  attenuator  S2R1 through 
S2R6 
in distortion 
operation. 
Capacitive dividers SC1 through SC10 
in 
the  attenuator  keep 
the 
frequency response flat. 
The  impedance  converter 
is 
a 
low  distortion,  high 
input impedance amplifier circuit with gain indepen- 
dent  of  the  source impedance  placed  at the  INPUT 
t erm inals. 
4-15.  Instrument  induced  distortion of  the  signal 
being  measured 
is 
minimized 
hy 
keeping  the  input 
impedance  and the  gain  of 
the 
impedance converter 
4-1