UAF42AP [BB]

UNIVERSAL ACTIVE FILTER; 通用有源滤波器


型号：	UAF42AP
厂家：	BURR-BROWN CORPORATION
描述：	UNIVERSAL ACTIVE FILTER 通用有源滤波器有源滤波器过滤器光电二极管 LTE
文件：	总14页 (文件大小：571K)
中文：	中文翻译
下载：	下载PDF数据表文档文件

AP P LICATION BULLETIN

Mailing Address: PO Box 11400 • Tucson, AZ 85734 • Street Address: 6730 S. Tucson Blvd. • Tucson, AZ 85706

Tel: (602) 746-1111 • Twx: 910-952-111 • Telex: 066-6491 • FAX (602) 889-1510 • Immediate Product Info: (800) 548-6132

FILTER DESIGN PROGRAM FOR

THE UAF42 UNIVERSAL ACTIVE FILTER

By Johnnie Molina and R. Mark Stitt (602) 746-7592

Although active filters are vital in modern electronics, their

eliminates signals above the cutoff frequency (in the stop-

band), and perfectly passes signals below it (in the pass-

band). In real filters, various trade-offs are made in an

attempt to approximate the ideal. Some filter types are

optimized for gain flatness in the pass-band, some trade-off

gain variation or ripple in the pass-band for a steeper rate of

attenuation between the pass-band and stop-band (in the

transition-band), still others trade-off both flatness and rate

of roll-off in favor of pulse-response fidelity. FILTER42

supports the three most commonly used all-pole filter types:

Butterworth, Chebyshev, and Bessel. The less familiar In-

verse Chebyshev is also supported. If a two-pole band-pass

or notch filter is selected, the program defaults to a resonant-

circuit response.

design and verification can be tedious and time consuming.

To aid in the design of active filters, Burr-Brown provides a

series of FilterPro™ computer-aided design programs. Us-

ing the FILTER42 program and the UAF42 it is easy to

design and implement all kinds of active filters. The UAF42

is a monolithic IC which contains the op amps, matched

resistors, and precision capacitors needed for a state-variable

filter pole-pair. A fourth, uncommitted precision op amp is

also included on the die.

Filters implemented with the UAF42 are time-continuous,

free from the switching noise and aliasing problems of

switched-capacitor filters. Other advantages of the state-

variable topology include low sensitivity of filter parameters

to external component values and simultaneous low-pass,

high-pass, and band-pass outputs. Simple two-pole filters

can be made with a UAF42 and two external resistors—see

Figure 1.

Butterworth (maximally flat magnitude). This filter has the

flattest possible pass-band magnitude response. Attenuation

is –3dB at the design cutoff frequency. Attenuation beyond

the cutoff frequency is a moderately steep –20dB/decade/

pole. The pulse response of the Butterworth filter has mod-

erate overshoot and ringing.

The DOS-compatible program guides you through the de-

sign process and automatically calculates component values.

Low-pass, high-pass, band-pass, and band-reject (or notch)

filters can be designed.

Chebyshev (equal ripple magnitude). (Other transliterations

of the Russian Heby]ov are Tschebychev, Tschebyscheff

or Tchevysheff). This filter response has steeper initial rate

of attenuation beyond the cutoff frequency than Butterworth.

Active filters are designed to approximate an ideal filter

response. For example, an ideal low-pass filter completely

R_F1

R_F2

15.8kΩ

R₁

50kΩ

C₁

R₂

50kΩ

C₂

1000pF

A₂

1000pF

A₁

A₃

V_O

R₃

50kΩ

R₄

50kΩ

V_IN

UAF42

NOTE: A UAF42 and two external resistors make a unity-gain, two-pole, 1.25dB ripple

Chebyshev low-pass filter. With the resistor values shown, cutoff frequency is 10kHz.

FIGURE 1. Two-Pole Low-Pass Filter Using UAF42.

AB-035C

Printed in U.S.A. July, 1993

FILTER RESPONSE vs FREQUENCY

+10

Ripple

–10

–20

–30

–40

–50

–10

–20

–30

–40

–50

4-Pole Chebyshev

3dB Ripple

5-Pole Chebyshev

3dB Ripple

f_C/100

f_C/10

f_C

10f_C

f_C/100

f_C/10

f_C

10f_C

Normalized Frequency

FIGURE 2A. Response vs Frequency for Even-Order (4-

pole) 3dB Ripple Chebyshev Low-Pass Filter

Showing Cutoff at 0dB.

FIGURE 2B. Response vs Frequency for Odd-Order (5-

pole) 3dB Ripple Chebyshev Low-Pass Filter

Showing Cutoff at –3dB.

This advantage comes at the penalty of amplitude variation

(ripple) in the pass-band. Unlike Butterworth and Bessel

responses, which have 3dB attenuation at the cutoff fre-

quency, Chebyshev cutoff frequency is defined as the fre-

quency at which the response falls below the ripple band.

For even-order filters, all ripple is above the dc-normalized

passband gain response, so cutoff is at 0dB (see Figure 2A).

For odd-order filters, all ripple is below the dc-normalized

passband gain response, so cutoff is at –(ripple) dB (see

Figure 2B). For a given number of poles, a steeper cutoff can

be achieved by allowing more pass-band ripple. The

Chebyshev has more ringing in its pulse response than the

Butterworth—especially for high-ripple designs.

Chebyshev. The difference is that the ripple of the Inverse

Chebyshev filter is confined to the stop-band. This filter type

has a steep rate of roll-off and a flat magnitude response in

the pass-band. Cutoff of the Inverse Chebyshev is defined as

the frequency where the response first enters the specified

stop-band—see Figure 3. Step response of the Inverse

Chebyshev is similar to the Butterworth.

Bessel (maximally flat time delay), also called Thomson.

Due to its linear phase response, this filter has excellent

pulse response (minimal overshoot and ringing). For a given

number of poles, its magnitude response is not as flat, nor is

its initial rate of attenuation beyond the –3dB cutoff fre-

quency as steep as the Butterworth. It takes a higher-order

Bessel filter to give a magnitude response similar to a given

Butterworth filter, but the pulse response fidelity of the

Bessel filter may make the added complexity worthwhile.

Inverse Chebyshev (equal minima of attenuation in the stop

band). As its name implies, this filter type is cousin to the

Tuned Circuit (resonant or tuned-circuit response). If a

two-pole band-pass or band-reject (notch) filter is selected,

the program defaults to a tuned circuit response. When band-

pass response is selected, the filter design approximates the

response of a series-connected LC circuit as shown in Figure

4A. When a two-pole band-reject (notch) response is se-

lected, filter design approximates the response of a parallel-

connected LC circuit as shown in Figure 4B.

FILTER RESPONSE vs FREQUENCY

–20

A_MIN

–40

–60

f_STOPBAND

CIRCUIT IMPLEMENTATION

–80

In general, filters designed by this program are implemented

with cascaded filter subcircuits. Subcircuits either have a

two-pole (complex pole-pair) response or a single real-pole

response. The program automatically selects the subcircuits

required based on function and performance. A program

option allows you to override the automatic topology selec-

tion routine to specify either an inverting or noninverting

pole-pair configuration.

–100

f_C/10

f_C

10f_C

100f_C

Normalized Frequency

FIGURE 3. Response vs Frequency for 5-pole, –60dB

Stop-Band, Inverse Chebyshev Low-Pass Filter

Showing Cutoff at –60dB.

The simplest filter circuit consists of a single pole-pair

subcircuit as shown in Figure 5. More complex filters

consist of two or more cascaded subcircuits as shown in

Figure 6. Even-order filters are implemented entirely with

UAF42 pole-pair sections and normally require no external

capacitors. Odd-order filters additionally require one real

pole section which can be implemented with the fourth

uncommitted op amp in the UAF42, an external resistor, and

an external capacitor. The program can be used to design

filters up to tenth order.

V_IN

V_O

FIGURE 4A. n = 2 Band-Pass Filter Using UAF42 (ap-

proximates the response of a series-connected

tuned L, C, R circuit).

The program guides you through the filter design and gen-

erates component values and a block diagram describing the

filter circuit. The Filter Block Diagram program output

shows the subcircuits needed to implement the filter design

labeled by type and connected in the recommended order.

The Filter Component Values program output shows the

values of all external components needed to implement the

filter.

V_IN

V_O

SUMMARY OF FILTER TYPES

FIGURE 4B. n = 2 Band-Reject (Notch) Filter Using

UAF42 (approximates the response of a par-

allel-connected tuned L, C, R circuit).

Butterworth

Advantages:

Maximally flat magnitude

response in the pass-band.

Good all-around performance.

Pulse response better than

Chebyshev.

Subcircuit 1

Rate of attenuation better than

Bessel.

Out⁽²⁾

(1)

V_IN

V_O

Disadvantages: Some overshoot and ringing in

step response.

NOTES:

(1) Subcircuit will be a complex pole-pair (PP1 through PP6)

subcircuit specified on the UAF42 Filter Component Values and

Filter Block Diagram program outputs.

Chebyshev

(2) HP Out, BP Out, LP Out, or Aux Out will be specified on the

UAF42 Filter Block Diagram program output.

Advantages:

Better rate of attenuation

beyond the pass-band than

Butterworth.

FIGURE 5. Simple Filter Made with Single Complex Pole-

Pair Subcircuit.

Disadvantages: Ripple in pass-band.

Considerably more ringing in

step response than Butterworth.

Subcircuit 1

Out⁽²⁾

Subcircuit N

Out⁽²⁾

Inverse Chebyshev

Advantages:

Flat magnitude response in

pass-band with steep rate of

attenuation in transition-band.

(1)

V_IN

V_O

Disadvantages: Ripple in stop-band.

Some overshoot and ringing in

NOTES:

(1) Subcircuit will be a real-pole high-pass (HP), real-pole low-pass

(LP), or complex pole-pair (PP1 through PP6) subcircuit specified

on the UAF42 Filter Component Values and Filter Block Diagram

program outputs.

step response.

Bessel

Advantages:

(2) If the subcircuit is a pole-pair section, HP Out, BP Out, LP Out, or

Aux Out will be specified on the UAF42 Filter Block Diagram

program output.

Best step response—very little

overshoot or ringing.

Disadvantages: Slower initial rate of attenua-

tion beyond the pass-band than

Butterworth.

FIGURE 6. Multiple-Stage Filter Made with Two or More

Subcircuits.

At low frequencies, the value required for the frequency-

setting resistors can be excessive. Resistor values above

about 5MΩ can react with parasitic capacitance causing

poor filter performance. When f_Ois below 10Hz, external

capacitors must be added to keep the value of R_F1and R_F2

below 5MΩ . When f_Ois in the range of about 10Hz to 32Hz,

An external 5.49kΩ resistor, R_2A, is added in parallel with

the internal resistor, R₂, to reduce R_F1and R_F2by √10 and

eliminate the need for external capacitors. At the other

extreme, when f_Ois above 10kHz, R_2A, is added in parallel

with R₂to improve stability.

The program automatically places lower Q stages ahead of

higher Q stages to prevent op amp output saturation due to

gain peaking. Even so, peaking may limit input voltage to

less than ±10V (V_S= ±15V). The maximum input voltage

for each filter design is shown on the filter block diagram.

If the UAF42 is to be operated on reduced supplies, the

maximum input voltage must be derated commensurately.

To use the filter with higher input voltages, you can add an

input attenuator.

The program designs the simplest filter that provides the

desired AC transfer function with a pass-band gain of

1.0V/V. In some cases the program cannot make a unity-

gain filter and the pass-band gain will be less than 1.0V/V.

In any case, overall filter gain is shown on the filter block

diagram. If you want a different gain, you can add an

additional stage for gain or attenuation as required.

External filter gain-set resistors, R_G, are always required

when using an inverting pole-pair configuration or when

using a noninverting configuration with Q < 0.57.

PP1 (Noninverting pole-pair subcircuit using internal gain-

set resistor, R₃)—See Figure 7. In the automatic topology

selection mode, this configuration is used for all band-pass

filter responses. This configuration allows the combination

of unity pass-band gain and high Q (up to 400). Since no

external gain-set resistor is required, external parts count is

minimized.

To build the filter, print-out the block diagram and compo-

nent values. Consider one subcircuit at a time. Match the

subcircuit type referenced on the component print-out to its

corresponding circuit diagram—see the Filter Subcircuits

section of this bulletin.

PP2 (Noninverting pole-pair subcircuit using an external

gain-set resistor, R_G)—See Figure 8. This configuration is

used when the pole-pair Q is less than 0.57.

The UAF42 Filter Component Values print-out has places to

display every possible external component needed for any

subcircuit. Not all of these components will be required for

any specific filter design. When no value is shown for a

component, omit the component. For example, the detailed

schematic diagrams for complex pole-pair subcircuits show

external capacitors in parallel with the 1000pF capacitors in

the UAF42. No external capacitors are required for filters

above approximately 10Hz.

PP3 (Inverting pole-pair subcircuit)—See Figure 9A. In the

automatic topology selection mode, this configuration is

used for the all-pole low-pass and high-pass filter responses.

This configuration requires an external gain-set resistor, R_G.

With R_G= 50kΩ, low-pass and high-pass gain are unity.

PP4 (Noninverting pole-pair/zero subcircuit)—See Figure

10. In addition to a complex pole-pair, this configuration

produces a jω-axis zero (response null) by summing the low-

pass and high-pass outputs using the auxiliary op amp, A₄,

in the UAF42. In the automatic topology selection mode,

this configuration is used for all band-reject (notch) filter

responses and Inverse Chebyshev filter types when

Q > 0.57. This subcircuit option keeps external parts count

low by using the internal gain-set resistor, R₃.

After the subcircuits have been implemented, connect them

in series in the order shown on the filter block diagram.

FILTER SUBCIRCUITS

Filter designs consist of cascaded complex pole-pair and

real-pole subcircuits. Complex pole pair subcircuits are

based on the UAF42 state-variable filter topology. Six varia-

tions of this circuit can be used, PP1 through PP6. Real pole

sections can be implemented with the auxiliary op amp in

the UAF42. High-pass (HP) and low-pass (LP) real-pole

sections can be used. The subcircuits are referenced with a

two or three letter abbreviation on the UAF42 Filter Compo-

nent Values and Filter Block Diagram program outputs.

Descriptions of each subcircuit follow:

PP5 (Noninverting pole-pair/zero subcircuit)—See Figure

11. In addition to a complex pole-pair, this configuration

produces a jω-axis zero (response null) by summing the low-

pass and high-pass outputs using the auxiliary op amp, A₄,

in the UAF42. In the automatic topology selection mode,

this configuration is used for all band-reject (notch) filter

responses and Inverse Chebyshev filter types when

Q < 0.57. This subcircuit option requires an external gain-set

resistor, R_G.

POLE-PAIR (PP) SUBCIRCUITS

PP6 (Inverting pole-pair/zero subcircuit)—See Figure 12. In

addition to a complex pole-pair, this configuration produces

a jω-axis zero (response null) by summing the low-pass and

high-pass outputs using the auxiliary op amp, A₄, in the

UAF42. This subcircuit is only used when you override the

automatic topology selection algorithm and specify the in-

verting pole-pair topology. Then it is used for all band-reject

(notch) filter responses and Inverse Chebyshev filter types.

In general, all complex pole-pair subcircuits use the UAF42

in the state-variable configuration. The two filter parameters

that must be set for the pole-pair are the filter Q and the

natural frequency, f_O. External resistors are used to set these

parameters. Two resistors, R_F1and R_F2, must be used to set

the pole-pair f_O. A third external resistor, R_Q, is usually

needed to set Q.

PP1

HP Out

R_F1

BP Out

R_F2

LP Out

C_1A

C_2A

R_2A

R₁

50kΩ

C₁

R₂

50kΩ

C₂

1000pF

A₂

1000pF

R₃

50kΩ

A₁

A₃

V_IN

R₄

50kΩ

UAF42

R_Q

FIGURE 7. PP1 Noninverting Pole-Pair Subcircuit Using Internal Gain-Set Resistor R₃.

PP2

HP Out

R_F1

BP Out

R_F2

LP Out

C_1A

C_2A

R_2A

R₁

50kΩ

C₁

R₂

50kΩ

C₂

1000pF

A₂

1000pF

A₁

A₃

R_G

V_IN

R₄

50kΩ

R_Q

UAF42

FIGURE 8. PP2 Noninverting Pole-Pair Subcircuit Using External Gain-Set Resistor R_G.

HP Out

R_F1

BP Out

R_F2

LP Out

PP3

C_1A

C_2A

R_G

R_2A

V_IN

R₁

50kΩ

C₁

R₂

50kΩ

C₂

1000pF

A₂

1000pF

A₁

A₃

R₄

50kΩ

R_Q

UAF42

NOTE: If R_Q= 50kΩ when using the PP3 subcircuit, you can

eliminate the external Q-setting resistor by connecting R₃as shown

in Figure 9B.

FIGURE 9A. PP3 Inverting Pole-Pair Subcircuit.

HP Out

R_F1

BP Out

R_F2

LP Out

C_1A

C_2A

R_G

R_2A

V_IN

R₁

50kΩ

C₁

R₂

50kΩ

C₂

1000pF

A₂

1000pF

A₁

A₃

R₃

50kΩ

R₄

50kΩ

UAF42

FIGURE 9B. Inverting Pole-Pair Subcircuit Using R₃to Eliminate External Q-Setting Resistor R_G.

PP4

HP Out

LP Out

R_Z2

C_1A

C_2A

R_2A

R_F1

R_F2

R_Z1

R_Z3

R₁

50kΩ

C₁

R₂

50kΩ

C₂

1000pF

A₂

1000pF

R₃

50kΩ

A₁

A₃

A₄

Aux

Out

V_IN

R₄

50kΩ

UAF42

R_Q

FIGURE 10. PP4 Noninverting Pole-Pair/Zero Subcircuit Using Internal Gain-Set Resistor R₃.

PP5

HP Out

LP Out

R_Z2

C_1A

C_2A

R_2A

R_F1

R_F2

R_Z1

R_Z3

R₁

50kΩ

C₁

R₂

50kΩ

C₂

1000pF

A₂

1000pF

A₁

A₃

A₄

R_G

Aux

Out

V_IN

R₄

50kΩ

R_Q

UAF42

FIGURE 11. PP5 Noninverting Pole-Pair/Zero Subcircuit Using External Gain-Set Resistor R_G.

The information provided herein is believed to be reliable; however, BURR-BROWN assumes no responsibility for inaccuracies or omissions. BURR-BROWN assumes

no responsibility for the use of this information, and all use of such information shall be entirely at the user’s own risk. Prices and specifications are subject to change

without notice. No patent rights or licenses to any of the circuits described herein are implied or granted to any third party. BURR-BROWN does not authorize or warrant

any BURR-BROWN product for use in life support devices and/or systems.

PP6

HP Out

LP Out

R_Z2

C_1A

C_2A

R_G

R_2A

R_F1

R_F2

V_IN

R_Z1

R_Z3

R₁

50kΩ

C₁

R₂

50kΩ

C₂

1000pF

A₂

1000pF

A₁

A₃

A₄

Aux Out

R₄

50kΩ

R_Q

UAF42

FIGURE 12. PP6 Inverting Pole-Pair/Zero Subcircuit.

This subcircuit option requires an external gain-set resistor,

R_G.

ELIMINATING THE LP SUBCIRCUIT

IN ODD-ORDER INVERSE CHEBYSHEV

LOW-PASS FILTERS

LP (Real-pole low-pass subcircuit). The basic low-pass

subcircuit (LP) is shown in Figure 13A. A single pole is

formed by R_Pand C_P. A₂buffers the output to prevent

loading from subsequent stages. If high input impedance is

needed, an optional buffer, A₁, can be added to the input.

Odd-order Inverse Chebyshev low-pass filters can be simpli-

fied by eliminating the LP input section and forming the real

pole in the first pole-pair/zero subcircuit. To form the real

pole in the pole-pair/zero subcircuit, place a capacitor, C₁, in

parallel with the summing amplifier feedback resistor, R_Z3.

The real pole must be at the same frequency as in the LP

subcircuit. One way to achieve this is to set C₁= C_Pand R_Z3

= R_P, where C_Pand R_Pare the values that were specified for

the LP section. Then, to keep the summing amplifier gains

the same, multiply R_Z1and R_Z2by R_P/R_Z3.

For an LP subcircuit with gain, use the optional circuit

shown in Figure 13B.

For an LP subcircuit with inverting gain or attenuation, use

the optional circuit shown in Figure 13C.

HP (Real-pole high-pass subcircuit). The basic high-pass

subcircuit (HP) is shown in Figure 14A. A single pole is

formed by R_Pand C_P. A₂buffers the output to prevent

loading from subsequent stages. If high input impedance is

needed, an optional buffer, A₁, can be added to the input.

Figures 16A and 16B show an example of the modification

of a 3-pole circuit. It is a 347Hz-cutoff inverse Chebyshev

low-pass filter. This example is from an application which

required a low-pass filter with a notch for 400Hz system

power-supply noise. Setting the cutoff at 347Hz produced

the 400Hz notch. The standard filter (Figure 16A) consists

of two subcircuits, an LP section followed by a PP4 section.

For an HP subcircuit with gain, use the optional circuit

shown in Figure 14B.

For an HP subcircuit with inverting gain or attenuation, use

the optional circuit shown in Figure 14C.

In the simplified configuration (Figure 16B), the summing

amplifier feedback resistor, R_Z3is changed from 10kΩ to

130kΩ and paralleled with a 0.01µF capacitor. Notice that

these are the same values used for R_Pand C_Pin the LP

section of Figure 16A. To set correct the summing amplifier

gain, resistors, R_Z1and R_Z2are multiplied by R_P/R_Z3(130kΩ/

10kΩ). R_Z1and R_Z2must be greater than 2kΩ to prevent op

amp output overloading. If necessary, increase R_Z1, R_Z2, and

R_Z3by decreasing C_P.

IF THE AUXILIARY OP AMP

IN A UAF42 IS NOT USED

If the auxiliary op amp in a UAF42 is not used, connect it as

a grounded unity-gain follower as shown in Figure 15. This

will keep its inputs and output in the linear region of

operation to prevent biasing anomalies which may affect the

other op amps in the UAF42.

C_P

A₂

V_O

R_P

A₂

V_O

A₁

V_IN

R_P

C_P

Optional

Buffer

Real Pole

Section

Optional

Buffer

Real Pole

Section

Real pole f_O= f_–3dB= 1/(2π • R_P• C_P) [Hz]

GAIN = 1.0V/V

Real pole f_O= f_–3dB= 1/(2π • R_P• C_P) [Hz]

GAIN = 1.0V/V

(a)

R₁

R₂

R₁

R₂

C_P

A₂

V_O

R_P

A₂

V_O

A₁

V_IN

R_P

C_P

Optional

Buffer

Real Pole

Section

Optional

Buffer

Real Pole

Section

Real pole f_O= f_–3dB= 1/(2π • R_P• C_P) [Hz]

GAIN = 1 + R₂/R₁

Real pole f_O= f_–3dB= 1/(2π • R_P• C_P) [Hz]

GAIN = 1 + R₂/R₁

(b)

C_P

R₂

R_P

C_P

R_P

R₁

A₁

A₂

V_IN

V_O

A₂

V_IN

V_O

Optional

Buffer

Real Pole

Section

Optional

Buffer

Real Pole

Section

Real pole f_O= f_–3dB= 1/(2π • R_P• C_P) [Hz]

GAIN = –R_P/R₁

Real pole f_O= f_–3dB= 1/(2π • R_P• C_P) [Hz]

GAIN = –R₂/R_P

(c)

FIGURE 13. Low-Pass (LP) Subcircuit: (a) Basic; (b) with

Noninverting Gain; (c) with Inverting Gain.

FIGURE 14. High-Pass (HP) Subcircuit: (a) Basic; (b) with

Noninverting Gain; (c) with Inverting Gain.

A₄

UAF42

Fragment

FIGURE 15. Connect Unused Auxiliary Op Amps as

Grounded-Input Unity-Gain Followers.

Q ENHANCEMENT

4A) ENTER FILTER FREQUENCY

When the f_O• Q product required for a pole-pair section is

above ≈100kHz at frequencies above ≈3kHz, op amp gain-

bandwidth limitations can cause Q errors and gain peaking.

To mitigate this effect, the program automatically compen-

sates for the expected error by decreasing the design-Q

according to a Q-compensation algorithm⁽¹⁾. When this

occurs, the value under the Q heading on the UAF42 Filter

Component Values print-out will be marked with an asterisk

indicating that it is the theoretical Q, not the actual design

Q. The actual design Q will be shown under an added

Move the cursor to the Filter Frequency line in the Param-

eters section.

Low-pass/high-pass filter: enter the f_–3dBor cutoff frequency.

Band-pass filter: enter the center frequency, f_CENTER

Band-reject (notch) filter: enter the notch frequency, f_NOTCH

If your filter is low-pass or high-pass, go to step 5.

4B) ENTER FILTER BANDWIDTH

heading labeled Q_COMP

If the filter is a band-pass or band-reject (notch), move the

cursor to the bandwidth line and enter bandwidth.

USING THE FilterPro™ PROGRAM

If you press <ENTER> with no entry on the bandwidth line,

you can enter f_Land f_Hinstead of bandwidth. f_Land f_Hare

the f_–3dBpoints with regard to the center frequency for

Butterworth and Bessel filters. They are the end of the

ripple-band for Chebyshev types. This method of entry may

force a change in center frequency or notch frequency.

With each data entry, the program automatically calculates

filter performance. This allows you to use a “what if”

spreadsheet-type design approach. For example; you can

quickly determine, by trial and error, how many poles are

needed for a desired roll-off.

5) PRINT-OUT COMPONENT VALUES

GETTING STARTED

Press function key <F4> to print-out Filter Component

Values and a Filter Block Diagram. Follow the instructions

in the filter implementation section of this bulletin to as-

semble a working filter.

The first time you use the program, you may want to follow

these suggested steps.

Type FILTER42 <ENTER> to start the program.

Use the arrow keys to move the cursor to the Filter

Response section.

USING THE PLOT FEATURE

A Plot feature allows you to view graphical results of filter

gain and phase vs frequency. This feature is useful for

comparing filter types.

1) SELECT FILTER RESPONSE

Press <ENTER> to toggle through four response choices:

Low-pass

High-pass

To view a plot of the current filter design, press <F2>.

Band-pass

GRAPHIC DISPLAY COMMANDS

Notch (band-reject)

While viewing the graphic display, several commands can

be used to compare filter responses:

When the desired response appears, move the cursor to the

Filter Type section.

<F1> or S—Saves the plot of the current design for future

recall.

<F2> or R—Recalls the Saved plot and plots it along with

the current design.

2) SELECT FILTER TYPE

Move the cursor to the desired filter type and press

<ENTER>. The selected filter type is highlighted and marked

with an asterisk. There are four filter-type choices:

<F3> or Z—Plots a Zero dB reference line.

GRAPHIC DISPLAY CURSOR CONTROL

Butterworth

Chebyshev

Bessel

Inverse Chebyshev

While viewing the graphics display you can also use the

arrow keys to move a cursor and view gain and phase for

plotted filter responses.

If you choose Chebyshev, you must also enter ripple (i.e.

pass-band ripple—see Chebyshev filter description).

If you choose Inverse Chebyshev, you must also enter A_MIN

(i.e. min attenuation or max gain in stop-band—see Inverse

Chebyshev filter description).

RESISTOR VALUES

With each data entry, the program automatically calculates

resistor values. If external capacitors are needed, the pro-

gram selects standard capacitor values and calculates exact

resistor values for the filter you have selected. The 1%

Resistors option in the Display menu can be used to calcu-

late the closest standard 1% resistor values instead of exact

resistor values. To use this feature, move the cursor to the

resistors line in the Filter Response section and press

3) ENTER FILTER ORDER

Move the cursor to the Filter Order line in the Parameters

section. Enter filter order n (from 2 to 10).

(1) L.P. Huelsman and P. E. Allen, Theory and Design of Active

Filters, p. 241.

OP AMP SELECTION GUIDE (In Order of Increasing Slew Rate)

T_A= 25°C, V_S= ±15V, specifications typ, unless otherwise noted, min/max specifications are for high-grade model.

typ

(MHz)

FPR ⁽¹⁾

typ

(kHz)

typ

(V/µs)

V_OS

max

(µV)

V_OS/dT

max

(µV/°C)

NOISE

at 10kHz

(nV/√Hz)

(3)

OP AMP

MODEL

C_CM

(pF)

OPA177

0.6

0.2

1.9

±0.1

±0.6

±5

OPA27

2.7

OPA2107 dual ⁽²⁾

OPA602 ⁽²⁾

4.5

280

500

875

160

500

250

1000

100

5000

±2

4.5

OPA404 quad ⁽²⁾

OPA627 ⁽²⁾

±3 typ

±0.8

±3 typ

UAF42 aux amp ⁽²⁾

NOTES: (1) FPR is full power response at 20Vp-p as calculated from slew rate. (2) These op amps have FET inputs. (3) Common-mode input capacitance.

<ENTER>. The program will toggle between exact resis-

tors and standard 1% resistors.

GAIN = noise gain of the op amp configuration and

f_O= filter f_–3dBor f_CENTERfrequency.

In high-pass and band-reject (notch) applications, the re-

quired op amp bandwidth depends on the upper frequency of

interest. As with most active filters, high-pass filters de-

signed with the UAF42 turn into band-pass filters with an

upper roll-off determined by the op amp bandwidth. Error

due to op amp roll-off can be calculated as follows:

CAPACITOR SELECTION

Even-order filters above 10Hz normally will not require

external capacitors. Odd order filters require one external

capacitor to set the real pole in the LP or HP section.

Capacitor selection is very important for a high-performance

filter. Capacitor behavior can vary significantly from ideal,

introducing series resistance and inductance which limit Q.

Also, nonlinearity of capacitance vs voltage causes distor-

tion. The 1000pF capacitors in the UAF42 are high perfor-

mance types laser trimmed to 0.5%.

% = 100 1 –

(

)

(1 + f²• (NGAIN)²/(UGBW)²)

200 – % • % • UGBW

NGAIN • (% – 100)

f =

If external capacitors are required, the recommended capaci-

tor types are: NPO ceramic, silver mica, metallized polycar-

bonate; and, for temperatures up to 85°C, polypropylene or

polystyrene. Common ceramic capacitors with high dielec-

tric constants, such as “high-K” types should be avoided—

they can cause errors in filter circuits.

Where:

% = Percent gain error f = Frequency of interest (Hz)

NGAIN = Noise gain of op amp (V/V)

= GAIN of noninverting configuration

= 1 + |GAIN| of inverting configuration

UGBW = Unity-gain bandwidth of the op amp (Hz):

GAIN ACCURACY (%)

f (NGAIN)/(UGBW)

OP AMP SELECTION

–29.29

–10.00

–1.00

–0.10

–0.01

1.000

0.484

0.142

0.045

0.014

Normally you can use the uncommitted fourth op amp in the

UAF42 to implement any necessary LP, HP, or gain stages.

If you must use additional op amps, it is important to choose

an op amp that can provide the necessary DC precision,

noise, distortion, and speed.

EXAMPLES OF MEASURED

UAF42 FILTER RESPONSE

OP AMP SLEW RATE

Figures 17 and 18 show actual measured magnitude re-

sponse plots for 5th-order 5kHz Butterworth, 3dB Chebyshev,

–60dB Inverse Chebyshev and Bessel low-pass filters de-

signed with the program and implemented with UAF42s. As

can be seen, the initial roll-off of the Chebyshev filter is the

fastest and the roll-off of the Bessel filter is the slowest.

However, each of the 5th-order all-pole filters ultimately

rolls off at –N • 20dB/decade, where N is the filter order

(–100dB/decade for a 5-pole filter).

The slew rate of the op amp must be greater than

π • V_OPP• BANDWIDTH for adequate full-power response.

For example, operating at 100kHz with 20Vp-p output

requires an op amp slew rate of at least 6.3V/µs. Burr-Brown

offers an excellent selection of op amps which can be used

for high performance active filter sections. The guide above

lists some good choices.

OP AMP BANDWIDTH

The oscilloscope photographs (Figures 19-22) show the step

response for each filter. As expected, the Chebyshev filter

has the most ringing, while the Bessel has the least.

As a rule of thumb, in low-pass and band-pass applications,

op amp bandwidth should be at least 50 • GAIN • f_O, where

(a)

(d)

–10

–20

–30

–40

–50

–60

–70

–80

–90

–3

(a)

–6

(d)

–9

(b)

–12

–15

–18

–21

–24

–27

(c)

(b)

100

10k

50k

100

10k

Frequency (Hz)

FIGURE 17. Gain vs Frequency for Fifth-Order 5kHz (a)

Butterworth, (b) 3dB Chebyshev, (c) –60dB

Inverse Chebyshev, and (d) Bessel Unity-

Gain Low-Pass Filters, Showing Overall Fil-

ter Response.

FIGURE 18. Gain vs Frequency for Fifth-Order 5kHz (a)

Butterworth, (b) 3dB Chebyshev, (c) –60dB

Inverse Chebyshev, and (d) Bessel Unity-

Gain Low-Pass Filters, Showing Transition-

Band Detail.

FIGURE 19. Step Response of Fifth-Order 5kHz

Butterworth Low-Pass Filter.

FIGURE 21. Step Response of Fifth-Order 5kHz, –60dB

Inverse Chebyshev Low-Pass Filter.

FIGURE 20. Step Response of Fifth-Order 5kHz, 3dB

Ripple Chebyshev Low-Pass Filter.

FIGURE 22. Step Response of Fifth-Order 5kHz Bessel

Low-Pass Filter.

UAF42AP [BB]

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