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need help on filters - pyroelectric detectors

N

Natty

hi

I need ur help. I want to know wat sort of filtering is done in the
first and in second stage!

I think in the first stage they have used high pass filtering and in
the second stage it is just amplification of the output from the first
op amp, the first stage.

Also, I wud like to know the reason for using a pull down resistor.

http://www.glolab.com/pirparts/appckt.pdf

I wud really apprecite ur help on this. thank you.

Natty.
 
J

John Popelish

Natty said:
hi

I need ur help. I want to know wat sort of filtering is done in the
first and in second stage!

There are a combination of filter effects in both stages.

C3 R4 provide a low pass corner (capacitor in feedback path increases
negative feedback when impedance of capacitor falls below resistor
impedance as frequency rises) at 1/(2*pi*R*C)=1.6 Hz.

C2 R3 provide a second low pass corner by reducing feedback as
impedance of C2 falls below that of R3 as frequency rises, at the same
1.6 Hz.

Then the output of the first stage is coupled to the second stage
through a high pass filter, C4 R5. it rolls off signals below 1.6 Hz.

The feedback of the second stage increases above 1.6 Hz, causing its
gain to roll off at that frequency, for another low pass pole.

The net affect of these 3 low pass poles and one high pass pole is a
band pass filter with a peak response just below 1.6 Hz.
I think in the first stage they have used high pass filtering and in
the second stage it is just amplification of the output from the first
op amp, the first stage.

The first stage has a gain of about 51 at the overall peak response
frequency, and the second stage has a gain of another 50 at that
frequency. Total overall gain of 51*50=2550.
Also, I wud like to know the reason for using a pull down resistor.

The signal is converted to a digital state by two comparators whose
outputs are connected through diodes that only allow the comparators
to pull up. When both comparators output a low voltage, both diodes
are turned off, so the combination would just float if the pull down
resistor were not there to influence the voltage down to ground
(provide a discharge path for the charge stored on the logic chip
input when one of the diodes had previously turned on and charged it
up to almost 5 volts).

By the way, one comparator pulls the output up when the signal goes
positive by more than a diode drop, and one pulls up when the signal
swings negative by more than a diode drop. So any change at about 1.6
Hz from the average level is detected. The diode drop shifts from
average signal are defined by D1 and D2.

If you're interested, here is the data sheet for the timer chip that
cleans up the signal pulses into an "on time":
http://www.fairchildsemi.com/ds/MM/MM74HC4538.pdf
 
B

Ban

John said:
There are a combination of filter effects in both stages.

C3 R4 provide a low pass corner (capacitor in feedback path increases
negative feedback when impedance of capacitor falls below resistor
impedance as frequency rises) at 1/(2*pi*R*C)=1.6 Hz.

C2 R3 provide a second low pass corner by reducing feedback as
impedance of C2 falls below that of R3 as frequency rises, at the same
1.6 Hz.

Then the output of the first stage is coupled to the second stage
through a high pass filter, C4 R5. it rolls off signals below 1.6 Hz.

The feedback of the second stage increases above 1.6 Hz, causing its
gain to roll off at that frequency, for another low pass pole.

The net affect of these 3 low pass poles and one high pass pole is a
band pass filter with a peak response just below 1.6 Hz.


The first stage has a gain of about 51 at the overall peak response
frequency, and the second stage has a gain of another 50 at that
frequency. Total overall gain of 51*50=2550.


The signal is converted to a digital state by two comparators whose
outputs are connected through diodes that only allow the comparators
to pull up. When both comparators output a low voltage, both diodes
are turned off, so the combination would just float if the pull down
resistor were not there to influence the voltage down to ground
(provide a discharge path for the charge stored on the logic chip
input when one of the diodes had previously turned on and charged it
up to almost 5 volts).

By the way, one comparator pulls the output up when the signal goes
positive by more than a diode drop, and one pulls up when the signal
swings negative by more than a diode drop. So any change at about 1.6
Hz from the average level is detected. The diode drop shifts from
average signal are defined by D1 and D2.


If you're interested, here is the data sheet for the timer chip that
cleans up the signal pulses into an "on time":
http://www.fairchildsemi.com/ds/MM/MM74HC4538.pdf

As I see it there are two cascaded bandpass filters with 1.6Hz center
frequency, even if the first stays at -40dB for very low frequencies. The Q
is 0.25, which means the bandwidth is 0.8 to 3.2Hz. the 1C and 1D form a
window comparator, which goes high for > +/-0.5V signal voltage. the
pulldown is needed for this kind of diode/diode logic.
 
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