EasyManua.ls Logo

Technics SL-P202A - Page 43

Technics SL-P202A
46 pages
Print Icon
To Next Page IconTo Next Page
To Next Page IconTo Next Page
To Previous Page IconTo Previous Page
To Previous Page IconTo Previous Page
Loading...
SL-P202A
The
processing
formula
produced
by
the
radial
error
processor
is
RE
=
k d
(411412413414)
-
k(il+i2).
The
factors
k
and
d
are
detected
from
the
loop
itself
by
processing
a
low
frequency
wobble
fault
signal,
which
is
injected
into
the
loop.
Injection
of
this
causes
a
displacement
of
+/-
0.05
um
of
the
arn.
The
k
is
again
factor
and
has
to
compensate:
eThe
tracking
angle
fault
(varies
between
90
degrees,
smallest
radius,
and
45
degrees,
largest
radius).
eThe
pit
geometry
of
disc
(causing
the
amplitude
of
radial
error
signals
to
vary
up
to
100%
from
disc
to
disc).
@Deterioration
of
the
laserdiode.
3-2-2
Automatic
(k-factor)
gain
eontrol
Detection
of
the
desired
value
is
done
by
detecting
the
phase
angle
of
an
injected
wobble
signal
in
the
radial
loop.
The
closed
loop
transfer
function
has
a
phase
shift
of
135
degrees
at
650
Hz
(the
wobble
frequency).
To
maintain
the
loop
gain,
the
phase
of
the
closed
loop
signal
of
RE
is
compared
with
a
-45
degrees
shifted
signal
derived
from
the
650
Hz
wobble
injection
oscillator.
If
the
gain
is
nominal
the
output
of
this
phase
comparator
is
zero.
In
other
cases
a
positive
or
negative
phase
error
signal
is
detected.
The
detected
signal
is
integrated
by
C2538.
The
value
of
this
integrated
signal
sets
the
gain.
This
completes
the
set
up
for
the
k
factor
in
TDA8809.
Note:
The
phase
comparator
is
a
linear
multiplier
which
ensures
that
the
a.g.c.
loop
is
unaffected
by
spurious
signals
near
the
odd
harmonics
of
the
wobble
frequency.
The
open-loop
gain
control
is
clamped
to
an
internal
reference
level
during
sstarting-up
and
searching.
t<+—
3-2-3
Automatic
asymmetry
control
(d-factor)
The
radial
error
signal
in
a
single-beam
pick-up
is
derived
froma
comparison
of
the
light
intensity
in
each
pupil
half.
Errors
in
this
signal
can
be
caused
by:
eAsymmetry
in
the
far-field
pattern
of
the
laser.
eLight
path
to
the
disc.
eImperfections
in
the
beam
splitter.
Errors
can
be
corrected
by
bringing
the
d-factor
in
the
total
transfer
function.
The
wobble
used
to
measure’
the
k-factor
is
also
used
to
measure
the
asymmetry.
The
signal
causes
the
beam
to
wobble
with
an
amplitude
of
0.05
um.
When
the
reading
spot
is
to
the
right
of
the
track
the
total
amount
of
L.F.light
(iTOT
=
i14+12+i3+i4
=
RE1
+
RE2)
is
in
phase
with
the
wobble
in
the
radial
error
signal.
When
the
reading
spot
is
to
the
left
the
I.f.
sum
signal
(RE1
+
RE2)
is
180
degrees
out
of
phase
with
the
wobble.
The
sum
signal
is in
practice
multiplied
by
a
90
degrees
shifted
version
of
the
wobble
signal.
The
multiplier
is
again
linear
giving
the
above-mentioned
benefits.
The
loop
has
a
filter
which
is
set
by
the
value
of
C2537.
The
imperfections
mentioned
above
make
the
beam
follow
the
track
at
one
of
its
edges.
The
wobble
component
in
the
RE
signal
for
such
a
_
situation
is
visualised
below.
Note:
C2537
is
the
capacitor
which
integrates
the
d-factor.
—sum
signal
track
(
in
phase
opposition
as
deviation

Related product manuals