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HP 435B - Page 80

HP 435B
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S
ERV
IC
E
S
HEE
T
2
(Cont'
d
)
An
in
c
r
ease
d
n
o
i
se
l
e
v
e
l
m
ay
b
e
ca
u
se
d
by
C1,
C6
o
r
C30
l i
n
e
n
o
i
se
filters
.
R
an
ge-to-
r
a
n
ge
i
nacc
ur ac
y
b
et
w
ee
n
t
h
e
100
m
W
r
an
ge
a
nd
a
n
ot
h
e
r
r
an
ge
m
a
yb
e
du
e
to
α
s
ha
pin
g
c
ir
c
ui
t
d
ef
ect
.
R
ange
Switc
h
R
a
n
ge-to-
r
a
n
ge
in
acc
ur ac
y
w
hi
c
h
i
s
ca
u
se
d
by
t
h
e
RAN
G
E
s
wi
tc
h
atte
nu
ato
r
sca
n
easily
be
i
so
l
ate
d
by
p
e
rf
o
rmin
g
o
n
eof
t
h
e
In
st
rum
e
n
tat
i
o
n
A
ccur ac
yP
e
rf
o
rm
an
ce
T
ests
(r
ef
er
to
Sect
i
o
n
IV)
.
T
h
ir
d
Amplifier
Ad
j
u
st
t
h
e
C
AL
ADJ
co
n
tr
o
l
fro
m
i
ts
pr
ese
n
t
sett
in
g
to
t
h
e
εεω
sto
p
.
Th
e
n
ad
j
u
st
t
h
e
co
n
tr
o
l
to
t
h
e
εω
sto
p
.
Th
e
m
ete
r r
ea
din
g
will
n
o
rm
a
lly
c
han
ge by
±2
dB
(>4
dB
fr
o
m
sto
p
to
sto
p
) .
Th
e
ac
v
o
l
tage
at
ΤΡ
4
will
c
h
an
ge
fro
m
t
h
e
n
o
min
a
l
sett in
g
to
a
ppr
o
xi-
m
ate
ly
-35%
ο
(cc
w
sto
p
)
a
nd
+70%
(
εω
sto
p
) .
Sync
h
ronous
Detector
Th
e
ph
ase
c
h
a
n
geof
t
h
e
220
Hz
s
i
gna
l
b
et
w
ee
n
t
h
epo
w
e
r
sensor's
sa
mplin
g
gate
a
nd
t
h
e
S
yn
c
hr
o
n
o
u
s
D
etecto
r
ca
nn
ot
b
e
m
ea-
s
ur
ed
dir ect
ly
b
eca
u
se
t
h
e
d
etecto
r ou
t
pu
t
i
s
do
r
at
h
er
t
han
ac
.
H
o
w
e
v
e
r
,
t
h
e
ph
ase
diff
e
re
n
ce at
ΤΡ
4
(t
h
e
inpu
t
to
t
h
e d
etecto
r
c
ir
c
ui
t)
can
b
e
m
eas
ur
e
d
.
B
ecau
se
t
h
e
ph
ase
c
han
ge
b
etwee
n
ΤΡ
4
a
nd
t
h
e
d
etecto
r
i
s
kn
o
wn,
t
h
e
ph
ase
re
l
at
i
o
n
ship
betwee
n
t
h
e
driv
e
s
i
g
n
a
l
(
ΤΡ
7)'
a
nd
t
h
e
ΤΡ
4
s
i
gn
a
l
indi
cates
t
h
e
tota
l
ph
ase
s
hif
t
t
hrou
gh
t
h
e
ac
a
mplifi
e
r
s
.
Thi
s
is
t
h
e
ste
p
-
by
-ste
ppr
oce
dur
e
f
o
r
c
h
ec
kin
g
ph
ase
s
hif
t
.
α
.
Set
t
h
e
P
owe
r
M
ete
r
a
nd
(if
u
se
d
)
t
h
er
an
ge
ca
libr
ato
r
con-
trols
as
s
h
o
wn
in
t
h
ege
n
er
a
l
t
ro
ubl
es
h
oot
in
g
inf
o
rm
at
i
o
n
abo
v
e
.
b
.
Co
nn
ect
t
h
e
osc
ill
osco
p
e's
v
e
r
t
i
ca
l
inpu
ts to
t
h
e
220
Hz
d
r
iv
e
(
ΤΡ
7)
t
hr
o
u
g
h
α
divid
e-
by
-te
n
pr
obe
(C
h
a
nn
e
l
Β
)
a
nd
to
ΤΡ
4
t
hr
ou
ghα
o
n
e-to-o
n
e
pr
o
b
e
(C
h
a
nn
e
l
Α
) .
ε
.
Set
t
h
e
osc
ill
osco
p
e
co
n
t
r
o
l
s
as
f
o
ll
o
w
s
:
C
ha
nn
e
l
Α
se
n
s
i
t
iv
-
i
t
y
to
0
.05
V
/
divi
s
i
on
w
i
t
h
ac
co
uplin
g,
C
ha
nn
e
l
Β
se
n
s
i
t
ivi
t
y
to
0
.2
V
/
divi
s
i
o
n,
h
or
iz
o
n
ta
l
s
w
ee
p
to
0
.5
m
s/
divi
sio
na
nd
t
h
e
dis-
play
m
o
d
e
to
Ch
a
nn
e
l
Α
a
nd
Β
,
c
h
o
pp
ed wi
t
h
t
ri
gge
rin
g
fro
m
Β
.
d
.
Ad
j
u
st
t
h
e
v
ert
i
ca
l
p
os
i
t
i
o
n
co
n
t
r
o
l
s
un
t
il
b
ot
h
t
r
aces
a
r
e
s
ym
etr
i
ca
l
wi
t
h
r
es
p
ect to
t
h
e
h
o
riz
o
n
ta
l
ce
n
te
r
lin
e
(r
efe
r
to
t
h
e
t
ypi
ca
l
w
a
v
e
fo
rm
b
e
l
ow)
.
e
.
Set
t
h
e
t
im
e
b
ase
m
ag
ni
fie
r
co
n
t
ro
l
to
Χ
10
.
Th
e
h
ori
zo
n
ta
l
sca
l
e
i
s
now
50
As/division
(r
efe r
to
t
h
e
e
xp
a
nd
e
d
wa
vefo
rm
b
e
l
ow)
.
Troubles
h
ooting
B
loc
k
Diagram
,
S
ERV
IC
E
S
HEE
T

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