
The
analyzer
has
one
time-to-frequency
transform
mode:
F
orward
transform
mode
transforms
CW
signals
measured
over
time
into
the
frequency
domain,
to
measure
the
spectral
content
of
a
signal.
This
mode
is
known
as
the
CW
time
mode
.
In
addition
to
these
transform
modes
,
this
section
discusses
special
transform
concepts
such
as
masking,
windowing,
and
gating.
General
Theory
The
relationship
between
the
frequency
domain
response
and
the
time
domain
response
of
the
analyzer
is
dened
by
the
F
ourier
transform.
Because
of
this
transform,
it
is
possible
to
measure
,
in
the
frequency
domain,
the
response
of
a
linear
test
device
and
mathematically
calculate
the
inverse
F
ourier
transform
of
the
data
to
nd
the
time
domain
response
.
The
analyzer's
internal
computer
makes
this
calculation
using
the
chirp-Z
F
ourier
transform
technique
.
The
resulting
measurement
is
the
fully
error-corrected
time
domain
reection
or
transmission
response
of
the
test
device
,
displayed
in
near
real-time
.
Figure
6-61
illustrates
the
frequency
and
time
domain
reection
responses
of
a
test
device
.
The
frequency
domain
reection
measurement
is
the
composite
of
all
the
signals
reected
by
the
discontinuities
present
in
the
test
device
over
the
measured
frequency
range
.
Note
In
this
section,
all
points
of
reection
are
referred
to
as
discontinuities
.
Figure
6-61.
Device
Frequency
Domain
and
Time
Domain
Reection
Responses
The
time
domain
measurement
shows
the
eect
of
each
discontinuity
as
a
function
of
time
(or
distance),
and
shows
that
the
test
device
response
consists
of
three
separate
impedance
changes
.
The
second
discontinuity
has
a
reection
coecient
magnitude
of
0.035
(i.e
.
3.5%
of
the
incident
signal
is
reected).
Marker
1
on
the
time
domain
trace
shows
the
elapsed
time
from
the
reference
plane
(where
the
calibration
standards
are
connected)
to
the
discontinuity
and
back:
18.2
nanoseconds
.
The
distance
shown
(5.45
meters)
is
based
on
the
assumption
that
the
signal
travels
at
the
speed
of
light.
The
signal
travels
slower
than
the
speed
of
light
in
most
media
(e
.g.
coax
cables).
This
slower
velocity
(relative
to
light)
can
be
compensated
for
by
adjusting
the
analyzer
relative
velocity
factor
.
This
procedure
is
described
later
in
this
section
under
\Time
domain
bandpass
."
6-118
Application
and
Operation
Concepts
Содержание HP 8753D
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