This document summarizes the design, simulation, and analysis of a Sallen-Key second-order active low-pass filter circuit. Key points:
- The circuit contains two RC networks (R1C1, R2C2) and its roll-off is -40dB/decade above the cut-off frequency, steeper than a first-order filter.
- PSpice was used to simulate the transient response and obtain the frequency response graph showing a -3dB point at the desired cut-off frequency.
- The transfer function was derived and shows a typical second-order low-pass form. Cut-off frequency and quality factor were also calculated.
- Frequency
Sallen and Key Second Order Active Low Pass Filter Transient Analysis
1. Objective:
Our objective for this laboratory was to investigate a Sallen and Key second
order active low pass filter and to obtain the transient analysis using our
modelled circuit and pspicesimulation. The circuit has two RC networks, R1
and C1, R2 and C2. The frequency responseof the second order low pass filter
is similar to the first order type except that the roll-off will be twice that of the
firstorder filters, at 40dB/decade as the operating frequency increases above
the cut-off frequency.
Malik:
Formal Element Report
Junaid Malik
Formal Element,
Signals and Systems 1,
DT008/2 Group A
3. Reference2
R1= 100k R2=100k C1= 820p C2 820p R4=4.7k R3=10k
Vin(s)→ →Vout(s)
Transfer Function
G(s)=
218619869.126
s2+18658.5365854s+148720999.405
Cut-off frequency
fc = 1940.91394015 (Hz)
Quality factor
Q = 0.653594771242
4. Figure 2: This was the layout which we followed while constructing the Sallen and Key Second-
order active. Reference Paul Tobin.
5. Figure 3: This is a good layout example reference Paul Tobin.
6. Deriving the equation:
An active low-pass filter is required to meet the following specification:
The maximum passband loss Amax = 0.5dB
The minimum stopband loss Amin = 12dB
The passband edge frequency ωp = 100 rs−1( f p = ωp/2π = 15.9 Hz)
The stopband edge frequency ωs = 400 rs−1
We had to obtain a Butterworth transfer function so that the Sallen and Key active
filter circuit could meet the required specification.
The filter order is calculated as follows =>
𝑛 =
log10 [
10(0.1𝑥𝐴𝑚𝑖𝑛)
− 1
10(0.1𝑥𝐴𝑚𝑎𝑥) − 1 ]
2𝑙𝑜𝑔10 (
𝑤𝑠
𝑤𝑝
)
𝑛 =
log10 [
10(0.1𝑥12)
− 1
10(0.1𝑥0.5) − 1 ]
2𝑙𝑜𝑔10 (
400
100
)
𝑛 =
log10[
14.8489
0.12207
]
2𝑙𝑜𝑔10(4)
𝑛 =
2.08529
1.204119
𝑛 = 1.731
𝑛 ≈ 2
8. Results:
TableofResults
Frequency Vin Vout Vout/Vin 20log(vout/vin)
1Hz 1 1 0 0 dB
10Hz 1 1.390V 1.390V 2.86 dB
100Hz 1 1.405V 1.405V 2.95 dB
1000Hz 1 1.431V 1.431V 3.11 dB
1.2kHz 1 1.361V 1.361V 2.677 dB
1.6kHz 1 1.269V 1.269V 2.062 dB
1.8kHz 1 1.170V 1.170V 1.363 dB
2.0kHz 1 1.064V 1.064V 0.531 dB
2.2kHz 1 962.3mV 962.3mV -0.33 dB
2.4kHz 1 864mV 864mV -1.269 dB
2.6kHz 1 776.6mV 776.6mV -2.19 dB
2.8kHz 1 695.4mV 695.4mV -3.15 dB
3.0kHz 1 626.4mV 626.4mV -4.06 dB
From this table of results we can see that as the frequency is increased, the out
output voltage is reduced in effect.
9. Graph
First graphoffrequencyagainstvoltage
GRAPH 1: The frequency response above is the same as for a first order filter. The difference this
time is the steepness of the roll-off which is at -40dB/decade.
Secondgraphofvolatgeagainstfrequency
GRAPH 2:
Frequency
1.0Hz 3.0Hz 10Hz 30Hz 100Hz 300Hz 1.0KHz 3.0KHz 10KHz 30KHz 100KHz
DB(V(OUT))
-80
-60
-40
-20
-0
20
Junaid Malik, DT008/2, Group A
passband gain = 1 + ra/rb = 1.47
(23.806K,-40.2dB decade)
(3.1331K,-6.01dB Decade)
Frequency
1.0Hz 3.0Hz 10Hz 30Hz 100Hz 300Hz 1.0KHz 3.0KHz 10KHz 30KHz 100KHz
V(OUT)
0V
0.5V
1.0V
1.5V
Junaid Malik, DT008/2, Group A, 6/11/12
k = 1 +Ra/Rb=1.47k
(1v,1.47k)
10. Conclusion:
In conclusion there are many filter types and ways to implement them but an active low-
pass filter that’s greatly simplified if R1=R2 and the op amp stage is a unity gain follower
(RB=short and RA=open). The Sallen and Key filter attenuates any input signal in the
frequency range above the cut-off frequency to a point, but then the response turns around
and starts to increase in gain with frequency. The response in the stop band should keep
decreasing as the frequency increases. Instead, the response actually will begin rising again
at some high frequency. A properly functioning op amp is needed for the filters operation;
op amps lose voltage gain at some frequency because of their finite bandwidth.
11. References
Reference 1: Paul Tobin
Reference 2: http://sim.okawa-denshi.jp/en/OPstool.php
Reference 3: PSpice forFiltersandTransmissionLinesby Paul Tobin