Philips pm3232 Instruction Manual page 25

10 mhz dual-beam oscilloscope
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67
We
regard the
drift
voltages
from
pre-amplifier
and
control amplifier
as
being
due
to
d.c.
voltage sources
at
the
input
(Vdl and Vd2).
We
then
find:
<
CM
>
li
>
(1)
V2
=
-B
(VI
+ Vd2)
(2)
Vo
=
A(V2-Vi-Vd1)
(3)
It
follows
from
Vi
+
VI =
(1
)
and
(3)
that:
A(V2-
Vi-
Vdl)
A
2
V2-
Vdl
2
Substituting
this result
in (2)
gives:
V2
-
Vdl
V2
=
-B(
^
+Vd2)
V2
(1
+1
)
=
|vd
1
-
BVd2
V2
=
BVdl
BVd2
2.B
^^1
or
or
Substituting
this result
in (3)
gives:
A
2tB
B
2
^,Vi.^Vd.*-^Vd2
2
or
or
Vo
A
=
Vi
+
1
Vdl +
Vd2
The
last
two
terms
represent
drift
voltages
which
are
equivalent to
a
drift
voltage:
Vd
=
1
Vdl
+
Vd2
at
the input.
We
see that the
drift
of the pre-amplifier
is
reduced
by
a
factor
2
drift
due
to the control
amplifier,
which
is
given
by
Vd2
4
I
^
g
(1
+
^
0*^
^he other
hand,
we
have an
extra
The
drift
of the control
amplifier,
however,
is
so
low
(because
of strong
thermal coupling of the
amplifier
transistors,
and
optimum
design) that
the
term
2Vd2
can be
neglected.

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