lektor January & February 2021 77
other filters, but the point where the curve drops below the defined
amount of ripple. If you would like to normalise the curves to the
-3dB point, in order to compare them better, you will have to adjust
the corner frequency accordingly.
the stop band. How much ripple we can allow depends on the
application.
In Figure 8 we have enlarged the pass-band from Figure 7. Here
we can see that the corner frequency is not the -3dB point, as with
L4
R 1 C 1
L5 R 2
C 2
C 4 C 5
- Order
BS Shunt First BS Series First
L1 L2
L6
C 3
C 6
L3
R 1 C 4
L2 R 2
C 5
C 2
L4 L5
L3
C 6
C 3
L6
L1
C 1
- Order
L4
R 1 C 1
R 2
C 4
L1 L2 C 2 L3 C 3
L1
R 1
C 1 R 2
C 4
L4
C 5
L5
C 2 L2
C 6
L6
C 3 L3
- Order
- Order
BP Shunt First BP Series First
C 7
L7
L5
C 5
L6
C 6
L7
C 7
200522-004a
L3
R 1 C 1
R 2
C 3
L1 L2 C 2
L1
R 1
C 1 R 2
C 3
L3
C 4
L4
C 2 L2
L4
C 4
C 7
L7
L7
C 7
200522-004b
L3
R 1 C 1
L4 R 2
C 2
C 3 C 4
L1 L2
R 1 C 3
L2 R 2
C 4
C 2
L3 L4
L1
C 1
Figure 4: Basic schematics for band-pass and band-stop filters of fifth and seventh order with Cauer or inverse Chebyshev characteristics in PI and T
configurations.
L1
1287
L2
1287
C 1
1n97
C 2
6n36
C 3
1n97
R 2
50
R 1
50
200522-005
Figure 5: Butterworth fifth-order low-pass filter with PI structure and with a
corner frequency of 1 MHz.
Figure 6: Frequency response of a fifth-order Butterworth
low-pass filter in the pass-band. The green curve is the correct
response and the red line shows what happens when a 100-Ω
filter is connected to a source and load of 50 Ω.