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Ericsson DIALOG - Page 23

Ericsson DIALOG
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22
Two
component's
resistor
r3
and
varistor
Vl
are
connected
in
parallel
with
the
2 - 5 - 3
branch
of
the
IC
winding.
The
varistor
Vl
is
a
non-linear
element
whose
impedance
is
high
with
low
voltages
across
it
but
decreases
(becomes
low-ohmic)
with
in-
creasing
voltage.
The
transmission
circuit
is
designed
to
provide
a
constant
trans-
mission
level
from
O
Ohm
up
to
about
1
000
Ohm
line
resistance.
In
order
to
achieve
this
the
shunting
circuit
(Vl-r3)
is
dimensioned
to
give
an
attenuation
of
about
4
dB
at
0
Ohm
line
resistance
with
a
continuous
fall
-
off
to
0
dB
at
approx.
1
000
Ohm
line
reisistance.
The
2 - 5 - 3
branch
is
in
the
primary
winding
and
4 - 5
in
the
secondary
of
a
transformer
circuit.
Considering
the
above,
when
the
primary
winding
is
almost
short-circuited
at
OOhm
line
resis-
tance
the
transformer
efficiency
is
reduced
by
about
4
dB
and
consequently
the
receiver
is
fed
with
a
lower
voltage.
The
instrument'
s
balancing
impedance
(c-r2)
is
designed
to
give
as
good
as
possible
sidetone
attenuation
over
lines
of
greatest
possible
length.
In
fig.
33
the
side
tone
reference
equivalent
is
shown
as
a
function
of
various
cable
lengths.
Fig.
33
Instrument
impedance
Cables:
0,4
mm,
r =
280n.
/km,
c%40
n
F/k
m « =
1,62
dB/km
0,Smm,r
1
BO
n
/km.c
•40
n{
/km~•
1,22
dB/km
0,6mm,r
•125si./km,c•40nf-'/km°'"'
Q9SdB/km
dB
Sidetone
Reference
Equivalent
rel.
to
NOSFER
0,5mm
20
O.L.mm
SIRE
5
km
The
instrument
impedance
must
be
variable
so
that.
seen
from
the
line,
it
coincides
with
the
line
impedance
and
causes
minimum
reflection
losses.
In
fig.
34
an
RX
diagram
shows
the
instrument
impedance
and
phase
angle's
variation
at
a
number
of
different
line
resistances.
Another
function
is
a
requirement
which
has
become
stronger
during
the
last
few
years,
namely
the
instrument
to
line
adaptation.
Attempts
have
always
been
made
to
achieve
the
best
results
in
this
respect,
but
it
is
only
with
the
coming
of
long-distance
interna-
tional
connections
that
a
real
need
has
arisen.
If
we
consider
the
case
of a
call
from
one
point
of
the
earth
to
another
point.
no
appreciable
transmission
losses
take
place
since
amplification
is
applied
over
the
entire
length
of
the
connection.
However,
noise.
added
and
amplified
at
every
point
of
amplification,
does
enter.
as
do
reflections
at
every
poor
matching
point.
One
point
where
reflections
can
arise
occurs
where
the
instrument
is
connected
to
the
line.
In
this
way
a
poor
connection
is
established
right
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