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LTC1064CS Folha de dados(PDF) 10 Page - Linear Technology

Nome de Peças LTC1064CS
Descrição Electrónicos  Low Noise, Fast, Quad Universal Filter Building Block
PDF  16 Pages
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Fabricante Electrônico  LINER [Linear Technology]
Página de início  http://www.linear.com
Logo LINER - Linear Technology

LTC1064CS Folha de dados(HTML) 10 Page - Linear Technology

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10
LTC1064
ODES OF OPERATIO
–
+
∫
∫
LP
1064 F08
+ Σ
AGND
NS
1/4 LTC1064
–
R1
R2
VIN
R3
R4
BP
Figure 8. Mode 2: 2nd Order Filter Providing Notch, Bandpass and Lowpass
Mode 3a
This is an extension of Mode 3 where the highpass and
lowpass outputs are summed through two external resis-
tors RH and RL to create a notch. This is shown in Figure
9. Mode 3a is more versatile than Mode 2 because the
notch frequency can be higher or lower than the center
frequency of the 2nd order section. The external op amp of
Figure 9 is not always required. When cascading the
sections of the LTC1064, the highpass and lowpass out-
puts can be summed directly into the inverting input of the
next section. The topology of Mode 3a is useful for elliptic
highpass and notch filters with clock-to-cutoff frequency
ratios higher than 100:1. This is often required to extend
the allowed input signal frequency range and to avoid
premature aliasing.
When the internal clock-to-center frequency ratio is set at
50:1, the design equations for Q and bandpass gain are
different from the 100:1 case.
–
+
∫
∫
LP
+ Σ
AGND
HP
S
1/4 LTC1064
–
BP
R1
R2
VIN
R3
R4
1064 F09
CC
RL
RH
RG
NOTCH
EXTERNAL OP AMP OR INPUT
OP AMP OF THE LTC1064,
SIDE A, B, C, D
–
+
Figure 9. Mode 3a: 2nd Order Filter Providing Highpass, Bandpass, Lowpass and Notch
1064 F08Eq
fO =
1 +
; fn =
; Q =
1 +
; HOLP = –
;
fCLK
100
R2
R4
R3
R2
MODE 2 (100:1):
NOTE: THE 50:1 EQUATIONS FOR MODE 2 ARE DIFFERENT FROM THE EQUATIONS
FOR MODE 2 OPERATION OF THE LTC1059, LTC1060 AND LTC1061. START WITH
fO, CALCULATE R2/R4, SET R4; FROM THE Q VALUE, CALCULATE R3:
√
R2
R4
√
R2
R4
√
fO =
1 +
; fn =
; Q =
; HOLP = –
;
fCLK
50
fCLK
50
fCLK
50
MODE 2 (50:1):
R2
R3
R2
16R4
R2
R4
1.005
1 +
√
–
R3
R1
HOBP = –
; HON1(f→ 0) = –
; HON2 = f→
=
R3
16R4
1 –
R2
R4
R3 =
; THEN CALCULATE R1 TO SET THE DESIRED GAIN.
1 +
+
R2
1.005
Q
√
R2
16R4
R2
R1
R2
R4
1 +
R2
R1
–
R2
R1
R2
R4
1 +
R2
R1
R2
R4
1 +
fCLK
2
()
fCLK
2
()
HOBP = –
; HON1(f→ 0) = –
; HON2 f→
= –
R3
R1
R2
R1
R2
R1
R2
R4
1 +
1064 F09Eq
fO =
; fn =
; HOHP =
; HOBP =
fCLK
100
R2
R4
RH
RL
MODE 3a (100:1):
NOTE: THE 50:1 EQUATIONS FOR MODE 3A ARE DIFFERENT FROM
THE EQUATIONS FOR MODE 3A OPERATION OF THE LTC1059,
LTC1060 AND LTC1061. START WITH fO, CALCULATE R2/R4, SET R4;
FROM THE Q VALUE, CALCULATE R3:
√
R2
R4
√
√
fCLK
100
R2
R4
R3 =
; THEN CALCULATE R1 TO
SET THE DESIRED GAIN.
+
R2
1.005
Q
√
R2
16R4
R2
R1
–
R2
R3
R2
16R4
R2
R4
1.005
√
–
R3
R1
HOBP = –
; HOLP(f = 0) =
Q =
R3
16R4
1 –
R4
R1
–
;
R3
R1
–
;
R3
R2
R4
R1
fCLK
2
()
()()
()( )
RH
RL
√
R2
R4
√
fO =
1 +
; fn =
; HOHP f→
=
fCLK
50
fCLK
50
MODE 3a (50:1):
R2
R1
–
;
fCLK
2
()
()
HOLP = –
; HON1(f→ 0) =
; HON2 f→
=
;
HON(f = fO) = Q
HOLP –
HOHP ; Q =
R4
R1
R2
R1
RG
RL
RG
RL
RG
RH
RG
RH



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