BRUEL & KJAER 2010 Instructions And Applications page 86

Heterodyne analyzer
Hide thumbs Also See for 2010:
Table of Contents

Advertisement

u
~
"E
E
"0
Q)
Q)
a.
en
Q:;
a.
10
3
I
~
i
~
I
I
~
:
~
'l
I'{
i
~
I
~
I
I
I
I
~
I
~
(~
I
I
t?
'X
I
~
I
'J
I
<"
~
~
~~~
6'-9
<"
I
~
:7~~
I
~
I
I
I
"'
a..
E
3.10-
1
I
~
~
N
~
:
t?~
I
'
~
~~~
'l
:::1
E
I
~
I
1\
(0~
:
~
~
-
~
10-
1
I
I
I
I
I
'-?;:\..
I
I
I
&~
I
I
~
I
I
~
3.10-
2
I
I
I
I
I
I
I
I
1
I
I
I
I
I
=
10%
I
I
:
i
I
3.10-
3
10-
3
l
I
l
I
3.10-
42
3.16
1
10
2o
100 200
6.3
'
~
'
1 k 2 k
I
I
'
I
I
~
~
I
~
I
~
I
I
'
I
1
'{
~
I
~
I
'
I
l
~
!
10 k 20 k
100 k 200 k
Analysis Frequency Limit (Hz)
171465
Fig.9.2.
Selection of maximum paper speed for less than 10% statistical
error
Therefore:
s
P·f
=21"T
(5)
Hence, for a maximum permissible error
€,
the requirement reduces to:
p
~
86.6f
€2 g2
(6)
where
B is the measurement bandwidth
f
is the highest measurement frequency
g2
It can be seen that the factor -f- plays an important role. In effect, if a
constant bandwidth is used, the bandwidth should be small in order to
obtain an acceptable resolution at low frequencies. Also, as the frequency f
in the denominator is the highest frequency considered by the analyzer, the
measuring time over a wide frequency range may be very long.
84

Advertisement

Table of Contents
loading

Table of Contents