
Page 31
by
Rob
Schenck,
W2CU,
on
an
online
AM
forum.
From
Rob’s
description:
“This
circuit
is
a
variation
of
the
classic
"Precision
Half
Wave
Rectifier"
as
described
in
many
op
‐
amp
application
notes
as
shown
below
[in
Figure
1]:
Figure
1.
Half
wave
AM
detector
“Its
operation
is
based
upon
ba
‐
sic
principles
of
operational
am
‐
plifier
circuits.
An
ideal
op
‐
amp
has
extremely
high
input
imped
‐
ance,
extremely
low
output
imped
‐
ance,
and
extremely
high
gain.
Note
the
operative
word
‘extremely’.
The
non
inverting
input
(+)
of
the
op
‐
amp
is
con
‐
nected
to
ground.
Feedback
is
provided
by
the
two
paths
R2+D1
and
D2.
The
op
‐
amp
will
drive
its
output
pin
to
a
voltage
such
that
the
inverting
input
(
‐
)
is
at
ground
voltage.
There
will
be
a
slight
variation
(a
few
mil
‐
livolts)
from
0
volts
as
a
result
of
what
is
known
as
input
offset
voltage,
a
property
of
real
op
‐
amps.
The
inverting
input
is
of
‐
ten
called
the
summing
junction,
as
the
sum
of
the
currents
in
that
node
will
be
zero.
Since
virtually
no
current
flows
into
the
inverting
input
(
‐
)
of
the
op
‐
amp
itself,
any
current
coming
in
through
the
input
resistor
R1
will
be
met
by
an
equal
and
oppo
‐
site
current
coming
through
ei
‐
ther
of
the
two
paths
of
R2+D1
or
D2.
“The
I.F.
input
signal
will
pro
‐
duce
an
input
current
of:
Iin
=
Vin/R1
“During
the
negative
half
of
the
input
AC
waveform,
the
op
‐
amp
output
will
drive
positive
such
that
the
current
through
R2+D1
will
be
equal
and
opposite
the
input
current,
or:
Iin
=
Vin/R1
=
‐
ID1
=
‐
IR2
“The
voltage
developed
across
R2,
and
hence
the
output
voltage
as
the
left
side
of
R2
is
at
ground
potential,
will
be:
V
=
Vout
=
‐
IR2
*
R2
=
‐
Vin/R1
*
R2
“By
setting
R1
=
R2,
the
output
voltage
will
be:
Vout
=
Vin
“Similarly,
the
positive
going
input
cycle
produces
a
feedback
current
through
D2.
Any
non
lin
‐
ear
voltages
developed
across
the
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