Crown Studio Reference I Service Manual Page 20

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Figure
4.3
is
a
simplified
exampfe
of
the
grounded
bridgs output topology.
It
consists of
four
quadrants
of
three deep DarDington (composite) emitter-follsw~r
stages per channel: one
NPN
and
one
PNP
an
the
High Side of
the
bridge (driving the
Isad),
and
apse
NPN
and
one
PMP
an
the
Low
Side
of the bridge (con-
trolling
the ground reference for %Re rails).
The
output
stages
are biased
ta operate
class
AB+B
far ultra
low
distortion
in
the signal zero-crossing region and
high
efficiency.
4,5.%
High
Side
[NS)
Thhe
High
Side (HS)
af the bridge operates much like
a
conventional
bipolar push-pull output configuration,
As
the input drive vsitage becomes more po%itive, the
HS
NPN
conducts
and
delivers positive voltage
to
the
10ad,
Eventually
the
NPN
devices reach
full
conduc-
tion
and
+Vcc
is
acrsss the
load,
At
this time the
HS
PNP
is
biased
off.
When
the
drive
signal is negative
going,
"Be
HS
PNP
canducts to deliver -Vcc to the load
and
the
HS
NPN
stage
is
off.
The
output
of
the
+LVA
drjvm the base
of
$8.~
pradriver
device.
Sgsgethar, the predriver
and
driver farm
the
first
two parts
sf
the three-deep Darlington and are
biased
class
AB,
They
provide output drive
through
the
bias
resistorx
bypassing
the
output devicas,
at
Bevels
be-
Isw
about
180mW,
An
RLC
network between
the
predriver and driver
provide
phase
shift
csmpensa-
tion
and
limit driver
base
current
$a
safs Bevels. Output
devices
are biased class
B,
Just
below
s%sculotf.
At about
1QOmW
blr~tpat
they
switch on
to
eonduct
high
current
to
the
load. Together with predriver
and
driver? the out-
put
device provides
an
averall cFass
AB+B
output,
The
negative half
sf
the
HS
is
almsst
identical
to
the
positive half, except that
the
devices are
PNP
One
difference
is
that the
PNP
bias
resistor is
slightly
greater
in
value
sa
that
PNP
output
devices
run
closer
to
the
cutoM
level
under static
(no
signal)
conditions,
This
is
because
PNP
devices require greater drive current.
WS
bias
is
rsgulated
by
Q18,
the
Bias
Seavs,
QlS
is
a
Vbe
multipiier which maintair-rs approximately
3,2V
Vee
under static conditions,
The
positive
and
negative
halves
of
the
WS
output
are
in
parallel
with
this
3.2V
With
a
full base-emitter on voltage
drop
across
predrivers
and
drivers, tha balance of
voltage
rasuits
in approximately
.3V
drop across
the
bias
resistors in
the positive half,
and
about
.5V
acrsss
The
bias resis-
tor in the negative
half,
Q
J
bn$
~~nd~clior~
{and
thus bias)
A
diode suing pr~vents
excessive
charge
build
up
within the
high
conduction output devices
whew
off,
Flyback
diodes
shunt
bask-EMF
pulses
from
reactive
loads
to
the
power supply to protect output devices
from
dangerous reverse voltage levels. An output
ter-
minating circuit blocks
WF
on
output
lines
from
enter-
ing
the
amplifier
through its output connectors,
4,5,2
L@w
Side
(L8)
The
tow Side
(LS)
operates
quite
differently.
The
power
supply
bridge
rectifier
is not ground referenced, nor
is
the
secondary
of
the main transformer,
in
othsr
wards,
tha
high
vsltage power supply
floats
with respect
ta
ground,
but
~Vcc remain canstant with respect
to
each
other,
This
allows
the pswer
supply
to deliver
+Vcc
and
-Vcc
from
the
same
bridge
rectifier
and
fiitsr
as
a
total difference
io
potential, regardless
of
their voltages
with
respect
ts
ground.
The LS
uses
inverted feed-
back
from
the HS
output
$0
control
the
ground refer*
ence
for
the
rails
(AVCC),
Both
LS
quadrants are ar-
ranged
in
a
three-deep Darlington
and
are
biased
AB+B
in
the
same
manner as
thc
WS,
When
the
amplifisr output swings positive,
the
audio
is
fed to an
sp-amp
stage
where
it
is
inverted,
This
inverted signal is delivered direeIIy to
the
bases
of
the
positive
(NPN)
and
negative
(PNP)
LS
predrrivers.
The
negative drive forces the
LS
PMP
devices on
(NPN
off),
As
the
PNP
devices
coaduct, VCB
af
the
PNP
Darlington drops.
With
LS
dsviics emitters tied
to
ground, -Vcc
is
pulled toward ground reference.
Since
the pswer supply
is
not ground referenced (and the
tatai
vsltage from
aVcc
to
-Vcc
is
constant)
+VGC
is
forced
higher
above
ground potential.
This
continues
until,
at
the
positive
amplifier output peak,
-Vcc
-.
OV
and
+VGC
eq~aIs the total
power
supply potential with
a
positive pslarily'
In
the
Reference
1,
for
example,
%he
power
supply
produces
a
totat
af14488
from rail ts
rail
(k72VDC
me?asur@d
from
ground
with
ns
signal),
therefore,
the
amplifier output can reach
a
positiva
peak
sf
+"I
44v*
Cosrversely, during a negative swing
af
the
HS
output
where
HS
PNP
devices conduct,
the
op-amp
would
output
a
positive
voltage forcing
hS
NPN
devices
to
canduct.
This
would
result
in
+Vcc
swinging
tsward
ground
potential
and
-Vcc
swinging
further from
groidnd
patentraf.
At
tl-$6
negative
amplifier sutpvt
peak,
SVCC
=z
OV
and
-Vcc
equals
the tstal power supply
potential with
a
negative pofariWy. Using
the
same
ex-
Circuit
Theory
4-4
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