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Tektronix 576 - Page 59

Tektronix 576
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Ci
r
cuit
Desc
r
i
p
tio
n
-Type
576
Dis
p
lay
Switc
h
ing
O
n
ce
t
he
d
esi
r
ed
voltages
an
d
cu
rrents
h
ave
b
een
sense
d
b
y
t
he
dis
p
lay
sensitivity
switc
h
ing
circuit,
an
d
once
t
h
e
d
esire
d
p
ositioni
ng cu
r
rents
h
ave
been
obtaine
d
from
t
he
d
is
p
lay
p
ositio
n
ing
circuit, t
he
resulti
ng
voltage
signals
and
p
ositio
n
ing
c
u
rre
n
ts
must
be a
pp
lie
d
to
t
h
e
dis
p
lay
am
p
lifiers
.
Before
being
applie
d
to
t
h
e
d
is
p
lay
am
p
lifiers,
h
owever,
t
h
ese
signals
p
ass
t
hroug
h
t
h
e
d
isplay
switc
h
ing
circ
u
it
(see
t
h
e
Dis
p
lay
Am
p
lifiers
and
Dis
p
lay
Positioning
sc
h
ematics)
.
U
nd
er
normal
op
erating
con
d
itions
wit
h
neit
h
er
t
h
e
DIS-
PL
AY
I
NVER
T,
t
h
e
Z
ER
O
nor
t
he
CA
L
bu
tto
n
s
p
resse
d
,
t
h
ese
sig
n
als
and
currents
p
ass
d
irectly
to
t
he
d
is
p
lay
am
p
li-
fers
.
If
t
h
e
DIS
PL
AY
I
NVE
RT
button
is
p
resse
d
,
however,
t
he
sig
n
al
a
n
d
cu
rrent
input
li
n
es
to
both
am
p
lifiers
a
r
e
reverse
d
.
T
h
is
causes
t
h
e
dis
p
lay
on
t
he
C
R
T
to
be
i
n
verte
d
,
both
vertically
an
d
h
orizontally
.
T
he
Z
ER
O
butto
n
,
w
h
en p
resse
d
,
d
isconnects
t
he
signal
in
p
ut
lines
from
both
p
ai
rs
of
h
ig
h im
p
ed
ance
in
p
uts
an
d
s
h
orts
t
he
in
p
ut
p
airs
toget
he
r
.
T
h
is
p
rovi
d
es
α
zero
r
efe
r
-
ence
fo
r
b
ot
h
d
is
p
lay
am
p
lifiers
.
If
t
he
DIS
PL
AY
O
FF
S
ET
controls
a r
e
bei
ng used
w
hen
t
he
Z
ER
O
bu
tton
is
p
resse
d
,
offset
p
ositioning
c
u rr
ent
is
cause
d
to
flow
as
if
t
h
e
C
EN
T
ERL
I
NE
VA
LUE
switc
h were
set
to
0
(see
Dis
p
lay
Positioni
n
g
sc
h
ematic
a
nd
d
isc
u
ssion
of
p
ositioni
n
g)
.
T
he
CAL
button,
w
hen
p
resse
d
,
disconnects
t
he
sig
n
al
i
np
ut
lines
from
both
pairs
of
h
ig
h im
p
edance
in
p
uts
and
a
p
plies
α
substitute
voltage
across
eac
h
inp
u
t
pair
w
h
ic
h
s
h
oul
d
cause
full
graticule
deflection
(10
divisions
by 10
d
ivisions)
.
T
h
is
p
rovi
d
es
α
means
of
ch
ec
k
i
ng
t
he
acc
ur
acy
of
calibration
of
t
h
e
d
is
p
lay
am
p
lifiers
.
T
he
substitute
volt-
age
is
d
etermine
d
by
R 501
t
hroug
h
R
513
and
by
D507
.
Since
eac
h
d
is
p
lay
am
p
lifier
h
as
t
h
ree
gains
to
c
h
ec
k
,
t
h
ree
s
ub
stit
u
te
voltages
m
u
st
be
available
.
R
elays
K537C,
K
541C,
K
637C
a
nd
K
641C
d
etermine
w
h
ic
h
voltages
are
app
lie
d
to
t
he
h
ig
h im
p
edance
in
p
ut
p
ai
rs
for
various
settings
of
t
h
e
VER
TICA
L
a
nd
H
O
R
IZO
N
TAL
switc
h
es
.
If
t
he
DIS
PL
AY
O
FF
SE
T
c
u
rre
n t
controls
are
being
use
d
w
hen
t
he
CA
L
b
u
tton
is
p
resse
d
,
offset
current
is
ca
u
se
d
to
flow
as
if
t
he
C
EN
T
ERL
I
NE
VA
LUE
switc
h
were
set
to
10
.
Dis
p
lay
Amplifiers
T
h
e
vertical
an
d
h
orizontal
d
isplay
am
p
lifiers
are
i
den
ti-
cal
wit
h α
few
mi
n
o
r
exce
p
tions
.
T
h
ey
a r
e both
differential
am
p
lifiers,
eac
h
wit
h
two
sets
of
differential
in
p
uts
an
d
one
set
of
d
ifferential
outp
uts
.
One
set
of
d
ifferential
in
p
uts
is
h
ig
h
impe
d
ance and
receives
its
in
p
uts
from
t
h
e
d
isplay
sensitivity
switc
h
ing
ci
r
cuit
.
T
he
ot
h
er
set
of
d
ifferential
in
p
uts
is
low
impe
dan
ce
and
t
h
eir
i
n
p
uts
are
t
he
d
iffere
n
tial
p
ositio
n
i
n
g
currents
from
t
he
d
isplay
p
ositioning
circuit
.
T
h
e
d
iffe
r
e
n
tial
out
p
uts are
connecte
d
to
t
he
deflection
p
lates
of
t
h
e
CRT
and con
trol
t
h
e p
otential
on
t
he
d
eflec-
tion
plates
.
T
h
e
simp
lified
sc
h
ematic
in
F
ig
.
3-12
will
h
el
p
in
und
er-
sta
nd
i
n
g
t
h
e
operatio
n
of
t
h
e
d
is
p
lay
am
p
lifie
r s
.
T
he
d
is-
3-
1
8
play
am
p
lifiers
control
t
he
voltage
between
t
he
deflection
p
lates
of the
C
R
T
b
y
controlling
t
he
c
ur
rents
t
h
roug
h
loa
d
resistors
R
L1
an
d
R
L2
.
T
h
e
curre
n
ts
1
L1
and
I
L2
con-
d
ucte
d by
t
he
loa
d
resistors
are
controlled
by
two
means
:
d
ifferential
cu
rre
n
t
1
s
an
d
p
ositioning
curre
n
ts
ΙΡ
1
an
d
Ιρ
2
.
T
h
e
d
ifferential
current
flows
t h
ro
ugh
source
coupling
resis-
tor
R
s
w
h
enever
t
h
ere
is
α
d
iffere
n
tial
voltage
sig
n
al
app
lie
d
to
t
h
e
h
ig
h
im
p
ed
ance
gate
in
p
uts
of
FETSQ1
A
and
Q1
Β
.
Positioning
curre
n
ts
ΙΡ
1
an
d
Ιρ
2
are
determined by
t
he
resistance
between t
h
e
emitter
of
Q2A
and
-75
volts
and
betwee
n
Q2
B
and
-75
volts,
res
p
ectively
.
T
he
relations
h
i
p
between
t
he
loa
d
resistor
cu
rrents
and
t
he
ot
h
er
cur
r
ents
i
n
t
he
am
p
lifier
is
as
follows
:
1L
=
Ιρ
-
(ID
+
1
s
)
(
Eq
uatio
n
3-1)
E
q
uation
3-1
p
ertains
to
t
h
e
currents
w
h
ic
h
flow
in
one
si
d
e
of
t
he
am
p
lifier
. 1
s
is
eit
h
er
p ositive
or
negative,
de-
pend
i
ng
on
w
h
et
h
er
it
a
dd
s
to or
s
u
btracts
from
ID
.
Ι
ρ
re
p
resents
t
h
e
FE
T
d
rain
current
.
It
originates
f r
om
α
co
n
-
stant
current
source
and
is
t
he
same
in
eac
h
si
de
of
t
he
am
p
lifier
.
T
h
is
e
q
u
atio
n
also
s
h
ows
t h
at
t
he
load
current
is
d
ependen
t
on
t
he
interaction
betwee
n
t
he
diffe
r
ential
cur
r
ent
(1
s
)
and
t
he
positio
n
i
ng
current
(
Ιρ
)
.
To
un
d
ersta
n
d
t
h
e
ope
r
ation
of
t
h
is
circuit,
first
assume
t
h
at
the
am
p
lifier
is
op
erating
i
n α
balance
d
con
d
ition
w
h
ere
the
two
p
ositioning
currents
are
eq
ual
(
ΙΡ
1
=
ΙΡ 2)
and
t
h
ere
is
no
voltage
difference
between
t
he
two
h
ig
h
impedan
ce
in
p
uts
(1
s
=
0)
.
In
t
h
is
case,
t
h
e
loa
d cu
rrents
on
each
side
of
t
he
am
p
lifie
r
are
e
q
ual
to
1
LO
.
E
q
uatio
n
3-1,
t
h
en,
becomes
:
ILO
=
I
L
1
=
I
L
2 =
ΙΡ
1
-
ID
=
ΙΡ
2
-
ID
(
Eq
uatio
n
3-2)
To
ill
u
strate
t
he
effect
t
h
e
hig
h im
p
e
d
ance
inp
u
ts
have
on
t h
e
loa
d
current,
assume
t
h
at
α
d
ifference
in
voltage
is
app
lied
across
t
he
gates
of
Q1A
and
01
Β
,
ma
k
i
ng
t
h
e
gate
of
Q1A
more
positive
.
T
h
is
voltage
differential
causes
d
if-
ferential
curre
n
t
1
s
to
flow
t
h
roug
h
so
u
rce
co
u
p
li
n
g
resist-
ance
R
s
.
W
it
h
t
h
is
a
dd
itional
current
(1
s
)
flowing
t
h
roug
h
QlA,
less
cu
rr e
n
t
is
nee
d
ed
from
Q2A
to
k
ee
p
d
rain
current
Ι
ρ
con
stant
.
T
h
e
current
con
d
ucte
d
by
Q2A
is
t
h
us
re
duced
to
ID
-
1S
.
Si
n
ce
t
h
e
p
ositio
n
ing
c
u
rrent
ΙΡ
1,
w
h
ic
h
su
pp
lies
t
he
current
cond
ucte
d
by
Q2A,
is
also
con-
stant,
t
h
ere
is
α
su
r
p
lus
of
p
ositio
n
i
ng
current
created
e
q
ual
to
IS
w
h
ic
h
must
be condu
cted
b
y
Q5,and
t
h
erefore
R
L1
.
T
he
loa
d
current
is
increased
to
1L1
=
1
LO
+
IS
.
On
t
he
ot
h
er
si
de of
t
he
am
p
lifie
r
,
t
h
e
curre
n
t t
h
ro
u
g
h
02
Β
is
i
n
crease
d
to
Ι
ρ
+
IS,
w
h
ic
h
d
ecreases
t
h
e
loa
d
current
t
h
roug
h
Q6
an
dR
L2
to
I
L2
=
ILO
-
1S
.
For
t
h
is
exam
p
le,
it
ca
n be
see
n
t
h
at
w
h
enever
α
d
ifferential
voltage
occurs
b
etween
t
he
two
h
ig
h
impe
d
a
n
ce
i
n
puts,
t
he
load
cur
r
ents
cha
n
ge,
t
h
us
ch
anging
t
he
voltage
p
otential
betwee
n
t
h
e
deflection
p
lates
of
t
he
CR
T
.
To
illust
r
ate
t
he
effect
t
he
p ositioni
ng
curre
n
ts
h
ave
on
t
h
e
loa
d
c
u
rrents,
ass
u
me
t
h
at
t
he
voltages
at
t
he
h
ig
h

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