Attenuators 775
When the impedances are unequal values, the resis-
tors are calculated with the following equations:
(22-36)
(22-37)
(22-38)
where,
R 1 and R 3 are shunt resistors in ohms,
R 2 is the series resistor in ohms,
Z 1 is the input impedance in ohms,
Z 2 is the output impedance in ohms,
.
The values of K, K^2 , and g are taken from Table 22-1.
An O-type attenuator is a balanced S attenuator. The
circuit element values may be obtained by first calcu-
lating for a S configuration and then dividing the series
resistor and placing half in each side of the line, Fig.
22-15. The shunt resistors remain the same value.
22.2.6 U Attenuators
U attenuators, Fig. 22-16, may be of a symmetrical or
balanced-type configuration and are useful for matching
a high impedance to a low impedance. The impedance
match is of first importance, the loss being secondary.
For a symmetrical configuration to work between
unequal impedances when the impedance match of Z 1 is
important, the resistors may be calculated as follows:
(22-39)
(22-40)
where,
R 1 is the series resistor in ohms,
R 2 is the shunt resistor in ohms,
Z 1 is the larger impedance in ohms,
Z 2 is the smaller impedance in ohms,
,
The value of K is taken from Table 22-1.
When the low impedance, Z 2 is to be matched the
equations are:
(22-41)
Figure 22-14. S and ' attenuators.
R 2
Z R 1 R 1 Z
Z 1 R 1 R 3 Z 2
R 2
p
p p
p
A. Between impedances of equal value.
B. Between impedances of unequal value.
R 1 Z 1 K
(^2) 1–
K^22 KS 1+–
©¹
̈ ̧
§·
R 2
Z 1 Z 2
2
=---------------- g
R 3 Z 2 K
(^2) 1–
K^22 K
S
–1--- -+
©¹
̈ ̧
̈ ̧
§·
S is
Z 1
Z 2
Figure 22-15. Balanced S or O attenuator.
Figure 22-16. A U pad configuration for operation
between impedances of unequal value.
Z 1 Z 2
Z (^1) R Z 2
1
R 1 R 1
R 3
R 2
2
p
p
p
p
p
p
p
p
B. Between impedances of unequal value.
A. Between impedances of equal value.
R 2
2
R 2
2
R 2
2
p
p p
p
Z 1 Z 2
R 1
R 2
R 1
R 1
Z 1
2 S
----- -KS 1–
K
©¹
= §·
R 2
Z 1
S
-----^1
KS–
= ©¹§·-------------
S is
Z 1
Z 2
R 1
Z 1
2 S
=----- - KS–