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參數(shù)資料
| 型號： | LMF380CIN |
| 廠商： | NATIONAL SEMICONDUCTOR CORP |
| 元件分類： | 模擬濾波器 |
| 英文描述： | SERIAL ATA SIGNAL CABLE |
| 中文描述： | TRIPLE SWITCHED CAPACITOR FILTER, CHEBYSHEV, BANDPASS, PDIP16 |
| 封裝： | 0.300 INCH, PLASTIC, DIP-16 |
| 文件頁數(shù)： | 8/12頁 |
| 文件大小： | 232K |
| 代理商： | LMF380CIN |
Typical Applications
(Continued)
THIRD-OCTAVE ANALYZER FILTER SET
The circuit shown in Figure 3 uses the LMF380 to imple-
ment a
(/3
-octave filter set for use in ‘‘real time’’ audio pro-
gram analyzers. Ten LMF380s provide all of the bandpass
filtering for the full audio frequency range. The power supply
connections are not shown, but each power supply pin
should be bypassed with a 0.1
m
F ceramic capacitor in par-
allel with a 1
m
F tantalum capacitor.
The first LMF380, at the top ofFigure 3, handles the highest
octave, with center frequencies of 20 kHz, 16 kHz, and
12.6 kHz. It also contains the 1 MHz master clock oscillator
for the entire system. Its Clock Out pin provides a 500 kHz
clock for the second LMF380, which supplies 250 kHz to
the third LMF380, and so on.
If the audio input signal were applied to all of the LMF380
input pins, aliasing might occur in the lower frequency filters
due to audio components near their clock frequencies. For
example, the LMF380 at the bottom ofFigure 3 has a clock
frequency equal to 1.953125 kHz. An input signal at
1.93 kHz will be aliased down to 23.125 Hz, which is near
the band center of the 24.4 Hz bandpass filter and will ap-
pear at the output of that filter.
This problem is solved by two LMF60–100 6th order Butter-
worth low-pass filters serving as anti-aliasing filters, as
shown inFigure 3. The first LMF60–100 is connected to the
input signal. The clock for this LMF60 is 250 kHz and comes
from pin 10 of the second LMF380. The cutoff frequency is
therefore 2.5 kHz. The output of this first LMF60–100 drives
the inputs of the fifth, sixth, and seventh LMF380s. The sev-
enth LMF380 has a 15.625 kHz clock, so aliasing will begin
to become a problem around 15.2 kHz. With a sixth-order,
2.5 kHz low-pass filter preceding this circuit, the attenuation
at 15.2 kHz is theoretically about 94 dB, which prevents
aliasing from occuring at this bandpass filter.
The output of the first LMF60 also drives the input of the
second LMF60, which provides anti-aliasing filtering for the
three LMF380s that handle the lowest part of the audio fre-
quency spectrum.
Note that no anti-aliasing filtering is provided for the four
LMF380s at the top of Figure 3. These devices will not en-
counter aliasing problems for frequencies below about
120 kHz; if higher input frequencies are expected, an addi-
tional low-pass filter at V
IN
may be required.
DETECTORS
In a real-time analyzer, the amplitude of the signal at the
output of each filter is displayed, usually in ‘‘bar-graph’’
form. The AC signal at the output of each bandpass filter
must be converted to a unipolar signal that is appropriate for
driving the display circuit.
The detector can take any of several forms. It can respond
to the peaks of the input signal, to the average value, or to
the rms value. The best type of detector depends on the
application. For example, peak detectors are useful when
monitoring audio program signals that are likely to overdrive
an amplifier. Since the output of the peak detector is propor-
tional to the peak signal voltage, it provides a good indica-
tion of the voltage swing. Generally, the output of the peak
detector must have a moderately fast (about 1 ms) attack
time and a much slower (tens or hundreds of milliseconds)
decay time. The actual attack and decay times depend on
the expected application. An average detector responds to
the average value of the rectified input signal and provides a
good solution when measuring random noise. An average
detector will normally respond relatively slowly to a rapid
change in input amplitude. An rms detector gives an output
that is proportional to signal power, and is therefore useful
in many instrumentation applications, especially those that
involve complex signals.
Peak detectors and average-responding detectors require
precision rectifiers to convert the bipolar input signal into a
unipolar output. Half-wave rectifiers are relatively inexpen-
sive, but respond to only one polarity of input signal; there-
fore, they can potentially ignore information. Full-wave recti-
fiers need more components, but respond to both polarities
of input signal. Examples of half- and full-wave peak- and
average-responding detectors are shown in Figure 4. The
component values shown may need to be adjusted to meet
the requirements of a particular application. For example,
peak detector attack and decay times may be changed by
changing the value of the ‘‘hold’’ capacitor.
The input to each detector should be capacitively-coupled
as shown in Figure 4. This prevents any errors due to volt-
age offsets in the preceding circuitry. The cutoff frequency
of the resulting high-pass filter should be less than half the
center frequency of the band of interest.
Note that a passive low-pass filter is shown at the input to
each detector inFigure 4. These filters attenuate any clock-
frequency signals at the outputs of the third-octave
switched-capacitor filters. The typical clock feedthrough at a
filter output is 10 mV rms, or 40 dB down from a nominal
1 Vrms signal amplitude. When more than 40 dB dynamic
range is needed, a passive low-pass filter with a cutoff fre-
quency about three times the center frequency of the band-
pass will attenuate the clock feedthrough by about 24 dB,
yielding about 64 dB dynamic range. The component values
shown produce a cutoff frequency of 1 kHz; changing the
capacitor value will alter the cutoff frequency in inverse pro-
portion to the capacitance.
The offset voltage of the operational amplifier used in the
detector will also affect the detector’s dynamic range. The
LF353 used in the circuits inFigure 3 is appropriate for sys-
tems requiring up to 40 dB dynamic range.
DISPLAYS
The output of the detector will drive the input of the display
circuit. An example of an LED display driver using the
LM3915 is shown in Figure 5. The LM3915 drives 10 LEDs
with 3 dB steps between LEDs; the total display range for an
LM3915 is therefore 27 dB. Two LM3915s can be cascaded
to yield a total range of 57 dB. See the LM3915 data sheet
for more information.
8
相關(guān)PDF資料 |
PDF描述 |
|---|---|
| LMF380CIV | LMF380 Triple One-Third Octave Switched-Capacitor Active Filter |
| LMF380CMJ | LMF380 Triple One-Third Octave Switched-Capacitor Active Filter |
| LMF90 | 4th-Order Elliptic Notch Filter |
| LMF90CCJ | 4th-Order Elliptic Notch Filter |
| LMF90CCN | 4th-Order Elliptic Notch Filter |
相關(guān)代理商/技術(shù)參數(shù) |
參數(shù)描述 |
|---|---|
| LMF380CIV | 制造商:NSC 制造商全稱:National Semiconductor 功能描述:LMF380 Triple One-Third Octave Switched-Capacitor Active Filter |
| LMF380CMJ | 制造商:NSC 制造商全稱:National Semiconductor 功能描述:LMF380 Triple One-Third Octave Switched-Capacitor Active Filter |
| LMF3A103W2851 | 制造商:Vishay Dale 功能描述:KIT LM F 3 A 103 W02851 E3 - Rail/Tube |
| LMF3B103W2851 | 制造商:Vishay Dale 功能描述:KIT LM F 3 B 103 W02851 E3 - Rail/Tube |
| LMF3D102W2851 | 制造商:Vishay Dale 功能描述:KIT LM F 3 D 102 W02851 E3 - Rail/Tube |
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