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LT1064 Ver la hoja de datos (PDF) - Linear Technology

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LT1064 Datasheet PDF : 16 Pages
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LTC1064
W
U
ODES OF OPERATIO
R1
VIN
R4
R3
R2
+
AGND
N
S
+
Σ
1/4 LTC1064
R2
√ √ MODE 2 (100:1):
fO
=
fCLK
100
1+
R2
R4
; fn =
fCLK
50
;
Q
=
R3
R2
1+
R2
R4
;
HOLP
=
1
R1
+ R2
;
BP
LP
( ) R2
HOBP
=–
R3
R1
;
HON1(f0)
=
1
R1
+ R2
; HON2
f
fCLK
2
=
R2
R1
R4
R4
MODE 2 (50:1):
fO
=
fCLK
50
1+
R2
R4
;
fn
=
fCLK
50
;
Q
1.005
=
R2
R3
1 + R2
R4
R2
16R4
; HOLP = –
R2
R1
1
+
R2
R4
;
1064 F08
( ) R3
R2
HOBP
=
1
R1
R3
16R4
;
HON1(f
0)
=
1
R1
+ R2
R4
;
HON2
=
f
fCLK
2
=
R2
R1
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:
R3 =
R2
; THEN CALCULATE R1 TO SET THE DESIRED GAIN.
1.005 1 + R2 + R2
Q
R4 16R4
1064 F08Eq
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.
R1
VIN
R4
R3
R2
+
AGND
CC
HP S
BP
+–
Σ
1/4 LTC1064
RH
MODE 3a (100:1):
MODE 3a (50:1):
LP
RG
RL
+
NOTCH
EXTERNAL OP AMP OR INPUT
OP AMP OF THE LTC1064,
SIDE A, B, C, D
1064 F09
√ √ fO
=
fCLK
100
R2
R4
;
fn
=
fCLK
100
RH
RL
;
HOHP
=
R2
R1
;
HOBP
=
R3
R1
;
( )( ) ( ) ( )( ) HOLP = –
R4
R1
;
HON1(f
0)
=
RG
RL
R4
R1
;
HON2
f
fCLK
2
=
RG
RH
R2
R1 ;
( ) HON(f = fO) = Q
RG
RL
HOLP
RG
RH
HOHP
;Q=
R3
R2
R2
R4
√ √ ( ) fO
=
fCLK
50
1+
R2
R4
; fn =
fCLK
50
RH
RL
; HOHP
f
fCLK
2
=
R2
R1
;
R3
HOBP
=
1
R1
R3
;
HOLP(f
=
0)
=
R4
R1
;
Q
=
16R4
1.005 R2
R4
R2
R3
R2
16R4
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:
R3 =
R2
; THEN CALCULATE R1 TO
1.005 R2 + R2 SET THE DESIRED GAIN.
Q R4 16R4
1064 F09Eq
Figure 9. Mode 3a: 2nd Order Filter Providing Highpass, Bandpass, Lowpass and Notch
10

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