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EG&G 113 - Operating Instructions; Introduction; Noise and Source Resistance

EG&G 113
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['3
SNOl.I.3H.I.SNl
9NI.l.V!:l3dO
III NOLLOHS
SECTION
III
OPERATING
INSTRUCTIONS
3.1 INTRODUCTION
To
obtain
optimum
performance
from
the
Model 113, care
must
be exercised in selecting
the
signal
source
impedance,
in
selecting
the
bandwidth,
and
in
ground
loop
considera-
tions,
all
of
which
are discussed
below.
Fundamentally,
the
instrument
is
powered
as
required
either
from
the
self-contained
batteries
or
from
the
ac line,
and
the
signal
to
be ampl ified
is
applied
to
the
input
connector(s);
the
amplified signal
is
available
at
the
output
jack
through
a resistance
of
600
ohms.
NOTE: Before
operating
from
ac line
power,
make
sure
the
rear-panel switch
is
in
the
position
indicating
the
line
voltage
to
be used,
and
be sure
the
proper
size line fuse
is
installed
(1/16
A for
115
V
operation
or
1/32
A
for
230
V
operation).
Operating
from
too
high a line voltage will
blow
the line fuse and possibly
damage
the
power
transformer
and
circuit
components.
3.2 NOISE
AND
SOURCE RESISTANCE
Best amplifier
performance
is
often
regarded
to
be
realized
under
those
conditions
where
it
least decreases
the
overall
signal-to-noise ratio. In
many
instances
the
thermal
noise
generated
by
the
signal source resistance
is
the
dominant
factor
in
determining
the
input
signal-to-noise ratio.
In
this
respect, amplifier noise
performance
can
be specified
by
the
amount
of
noise
the
amplifier
adds
to
the
amplified
source
thermal
noise; expressed in decibels, this
is
called
the
"Noise
Figure":
(1) Noise Figure =
20
I
total
rms noise voltage
at
the
ampl ifier
output
0910
gain x
source
thermal
noise voltage (rms) dB
where
the
Source
Thermal
Noise =
V4KTRl'lf
volts
rms
= E,
and
K =
Boltzmann's
constant,
1.38
x
10-
23
joules/K
T
=
absolute
temperature
in kelvins
M =
equivalent
noise
bandwidth
in
Hz
R =
source
resistance
in
ohms
(differential
source
resistance
for
Model
113;
if used single-ended,
set
the
coupling
selector
for
th.e
unused
input
to
ground,
and regard this
part
of
input
resistance
to
be
zero).
The
total
output
noise may be
converted
to
an
equivalent
input
noise
by
dividing
by
the
amplifier
gain.
The
noise
figure,
expressed
in
these
terms,
becomes:
(2) Noise Figure =
20
I
total
rms noise voltage referred
to
amp.
input
dB
0910
source
thermal
noise voltage (rms)
II
1-1
Each ampl ifier has its
own
characteristic
noise figure, wh ich
varies as a
function
of
frequency
and
source
resistance.
These figures are
obtained
experimentally,
and
plotted
graphically. Figure
111-1
is
a
typical
set
of
noise figure
contours
for
the
Model
113.
30dB
--'_---l,
10
-1
10-
1
00
IO~
~
IO~
FREQUfNr
i .N
Hz
Figure
111-1.
TYPICAL
NOISE
FIGURE
CONTOURS
FOR
THE
MODEL
113
In
using these
contours,
the
total
equivalent
rms
input
noise
is
usually
the
quantity
of
interest.
This can
be
obtained
from
the
graph
and
equation
(3):
(3)
Total
equivalent
rms
input
noise voltage =
source
thermal
noise x antilog
NF/20
volts rms
The
equivalent
noise
bandwidth
used in
determining
the
source
thermal
noise
is
a
function
of
the
external
circuitry
and/or
the
amplifier
bandwidth.
When
operating
dc
coupled
(LF
rolloff
to
DC),
the
equivalent
noise
bandwidth
of
the
M113
is
simply
the
HF
rolloff
frequency
multiplied
by
1T/2.
If
the
LF rolloff
frequency
setting
is
other
than
dc,
the
equivalent
noise
bandwidth
is
given
by
the
formula:

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