Atek HP 8753D, Руководство пользователя, Страница: 397 / 677

T o increase the time domain measurement range , rst increase the number of points , but
remember that as the number of points increases , the sweep speed decreases . Decreasing the
frequency span also increases range , but reduces resolution.
Resolution
Two dierent resolution terms are used in the time domain:
response resolution
range resolution
Response resolution. Time domain response resolution is dened as the ability to resolve two
closely-spaced responses , or a measure of how close two responses can be to each other and
still be distinguished from each other . F or responses of equal amplitude , the response resolution
is equal to the 50% (06 dB) impulse width. It is inversely proportional to the measurement
frequency span, and is also a function of the window used in the transform. The approximate
formulas for calculating the 50% impulse width are given in T able 6-11 . F or example , using the
formula for the bandpass mode with a normal windowing function for a 50 MHz to 13.05 GHz
measurement (13.0 GHz span):
50% cal cul ated impul se w idth =
0: 98
13: 0 (GH z )
2 2
= 0: 151 nanoseconds
E l ectr ical l eng th (in air ) = (0: 151 2 10
09
s) 2 (30 2 10
9
cm=s)
= 4: 53 centimeter s
With this measurement, two equal responses can be distinguished when they are separated
by at least 4.53 centimeters . In a measurement with a 20 GHz span, two equal responses can
be distinguished when they are separated by at least 2.94 cm. Using the low pass mode (the
low pass frequencies are slightly dierent) with a minimum windowing function, you can
distinguish two equal responses that are about 1.38 centimeters or more apart.
F or reection measurements , which measure the two-way time to the response , divide the
response resolution by 2. Using the example above , you can distinguish two faults of equal
magnitude provided they are 0.69 centimeters (electrical length) or more apart.
Note
Remember , to determine the physical length, the relative velocity factor of
the transmission medium under test must be entered into the electrical length
equation.
F or example , a cable with a teon dielectric (0.7 relative velocity factor), measured under the
conditions stated above , has a fault location measurement response resolution of
0.45 centimeters . This is the maximum fault location response resolution. F actors such as
reduced frequency span, greater frequency domain data windowing, and a large discontinuity
shadowing the response of a smaller discontinuity , all act to degrade the eective response
resolution.
Figure 6-72 illustrates the eects of response resolution. The solid line shows the actual
reection measurement of two approximately equal discontinuities (the input and output of an
SMA barrel). The dashed line shows the approximate eect of each discontinuity , if they could
be measured separately .
Application and Operation Concepts 6-131