Measurement and Instrumentation Dr. Tayab Din Memon Assistant Professor Dept of Electronic Engineering, MUET, Jamshoro. ACTIVE FILTERS and its applications
Mar 22, 2016
Measurement and Instrumentation
Dr. Tayab Din Memon
Assistant Professor Dept of Electronic Engineering, MUET, Jamshoro.
ACTIVE FILTERS and its applications
Objectives Discuss about the Active filters,
its use and applications. Types of filters Important terminologies of Active Filters. Order of Filter
Filter Approximations Order of Filter Categories of Filter Responses Active Lowpass Filter
Single Order Lowpass Filter & Double Order Lowpass Filter Unity Gain and Variable Gain
Active Highpass Filter Single order highpass filter, Second order highpass filter Unity gain and variable gain highpass filter.
K Values Table & its discussion Bandpass Filter
Wideband & Narrowband Band stop Filter Session-II Lab Work Design and simulation of circuits.
Filters: An Introduction Filters can be defined as:
filters are electrical networks that have been designed to pass alternating currents generated at only certain frequencies and to block or attenuate all others.
Filters have a wide use in electrical and electronic engineering and are vital elements in many telecommunications and instrumentation systems where the separation of wanted from unwanted signals – including noise – is essential to their success.
Filters Applications
Filter circuits are used in a wide variety of applications. In the field of telecommunication, band-pass filters are used in
the audio frequency range (0 kHz to 20 kHz) for modems and speech processing.
High-frequency band-pass filters (several hundred MHz) are used for channel selection in telephone central offices.
Data acquisition systems usually require anti-aliasing low-pass filters as well as low-pass noise filters in their preceding signal conditioning stages.
System power supplies often use band-rejection filters to suppress the 60-Hz line frequency and high frequency transients.
Types of Filters Passive Filters
Incorporates only passive components like; capacitors, resistors, inductors.
Passive filters are difficult to design. Further inductors are difficult to handle. Not only are they
expensive, bulky and heavy; they are prone to magnetic field radiation unless expensive shielding is used to prevent unwanted coupling
Used for high frequencies (>MHz) Active Filters
Along with passive components capacitors and resistors, Additionally it incorporates active components particularly like; op-amp.
Due to inductor property at low frequencies, active filters are Used at low frequencies.
It overcomes the inductor problems in passive filter.
Important terminologies in Filters
Frequency Response of Filter is the graph of its voltage gain versus frequency.
Passband: Those frequencies that are passed by a filter without attenuation.
Stopband: Those frequencies that are rejected by filter after cutoff.
Transition: The roll-off region between passband and the stopband.
Attenuation: Attenuation refers to the loss of signal.
Order of a Filter
The order of an active filter depends on the number of RC circuits called poles it contains.
If an active filter contains 8 RC circuits, n=8.
In active filters simple way to determine the order is to identify the number of capacitors in the circuit.
n= #of capacitors.
What is the advantage of increasing Order?
Answer!!
Filter Approximation Butterworth Approximation
The butterworth approximation is sometimes called the maximum flat approximation.
Roll off =20n dB/decade An equivalent roll of in terms of octaves is: Roll-off = 6n
dB/octave Chebyshev Approximation
In Chebyshav approximation ripples are present in passband, but its roll off rate is greater than 20dB/decade for a single pole.
The number of ripples in the passband of a Chebyshav filter are equals to the half of the filter order:
#Ripples = n/2 Inverse Chebyshav Approximation
In applications in which flat response is required as well as the fast roll-off, a designer may choose Inverse Chebyshav.
It has flat passband and rippled stopband. Inverse Chebyshav is not a Monotonic (No Stop Band ripples)
Approximation.
Filter approximation Elliptic Approximation
If rippled passband and rippled stopband are accepted designer must choose elliptic approximation.
Its major advantage is its highest roll-off rate in transition region.
Bessel Approximation Bessel approximation has a flat passband and a
monotonic stopband similar to those of the Butterworth approximation.
For the same filter order, however, the roll-off in the transition region is much less with a Bessel filter than with a Butterworth filter.
The major advantage of the Bessel Filter is that it produces the least distortion of non-sinusoidal signals.
No phase change.
Butterworth Approximation
Chebyshav Approximation
Elliptic Approximation Bessel Approximation
Damping Factor
Peaking action at resonant frequency is to use the damping factor defined as:
For Q=10, the damping factor is 0.1.
Q1
Categories of filters Lowpass
It passes frequencies before cutoff. Highpass
It passes all frequencies after cutoff. Bandpass
It passes all the frequencies in a specific band.
Bandstop It rejects all the frequencies of a specific
band.
Response Curves of All types of Filters
Fig. Lowpass Filter
Fig. Highpass Filter
Filter Response Curves of all types
Fig. Bandpass Filter
Fig. Bandstop Filter
First Order Stage
First order stages can only be implemented using Butterworth response.
Why?
Active Lowpass Filter (unity Gain)
Fig. Single pole lowpass filter.
+
-
AC
R1
C1
2
11
1
1CR2
1 fcfrequency Cutoff
1 isGain
fcf
A
Av
Active Lowpass Filter (Variable Gain)
Fig. Single pole lowpass filter.
Rf
+
-
AC
R1
C1
2
11
1
1CR2
1 fcfrequency Cutoff
1 isGain
fcf
A
RiRfAv
Ri
Active Lowpass Inverting with variable gain.
C1
Rf
+
-
AC
2
1
1
1R2C21 fcfrequency Cutoff
isGain
fcf
A
RiRfAv
Ri
Fig. Active Lowpass Inverting Circuit.
Single pole Highpass unity gain Filter
2
1
1
1R1C21 fcfrequency Cutoff
1 isGain
ffc
A
Av
+
-
ACR1
C1
Fig. Single Pole Highpass Filter.
Single pole Highpass with variable gain
Rf
2
1
1
1R1C21 fcfrequency Cutoff
1 isGain
ffc
A
RiR
Av f
+
-
ACR1
C1
Ri
Sallen Key Approach (VCVS) Second order or 2-pole stages are the
most common because they are easy to build and analyze.
Higher order filters are usually made by cascading second order stages. Each second-order stage has a resonant frequency and Q to determined how much peaking occurs.
Sallen Key approach is also known as VCVS (Voltage Controlled Voltage Source) because the opamp is used as a voltage-controlled voltage source.
VCVS Double Pole Lowpass Filter (Butterworth and Bessel)
0.786Kc 0.577,Q :Bessel1Kc 0.707,Q
:Butterwortfc
f1
1A ,CC0.5Q
CCR21 fpfrequency Cutoff
1Av isGain
41
2
21
+
-ACC1
C2
R R
Double Pole Lowpass Peaked Response
Peaked Response can be calculated using following three frequencies:
f0=K0fp
fc=Kcfp
f3dB=K3fp
f0 is the resonant frequency where peaking appears,
fc is the edge frequency, & f3dB is the cutoff frequency.
K values and Ripple depth of Second-Order Stages (Table 1)
Q K0 Kc K3 Ap(dB)
0.577 ---- ---- 1 --0.707 --- 1 1 ---
0.75 0.333 0.471 1.057 0.0540.8 0.476 0.661 1.115 0.2130.9 0.620 0.874 1.206 0.6881 0.78 1 1.277 1.252 0.935 1.322 1.485 6.33 0.972 1.374 1.532 9.664 0.984 1.391 1.537 12.15 0.99 1.4 1.543 14
10 0.998 1.410 1.551 20100 1 1.414 1.554 40
Discussion of the Table
Table gives us K and Ap values versus Q.
The Bessel and Butterworth have not noticeable frequency, So K0 and Ap values does not apply.
When Q is greater than 0.707, a noticeable resonant frequency appears and all K an Ap values are present.
Equal Component Values Second Order Lowpass Filter
+
-AC
R R
C
C
R1
Rf
RCfc
AvQ
Av RRf
21
31
1 1
VCVS Second Order Unity Gain High Pass Filters
AC
+
-
C C
R1
R2
2121
15.0
1
2
RRCfp
RRQ
Av
VCVS Highpass Filter with Voltage gain greater than unity.
AC
+
-
C C
R
R
CRfp
AVQ
RRfAv
21
31
11
Rf
R1
Bandpass Filter
BWfQ
fff
ffBW
0
210
12
When Q is less than 1, the filter has a wideband response. In this case bandpass filter is designed by cascading lowpass and highpass filter. When Q is greater than 1, the filter has a narrowband response and a different approach is used.
A Bandpass filter has a center frequency and a bandwidth.
Solution!
HIGH PASSfc=300Hz
LOWPASSfc=3.3KHzVin Vout
Fig. Wideband Filters uses cascadeof lowpass and highpass stages.
Narrowband Filters When Q is greater than 1, we use Multiple Feedback
(MFB) filter shown in fig. The input signal is at Inverting terminal. Two feedbacks one from capacitor & resistor. Operation: At low frequencies capacitor appears to be
open. Therefore, the input signal cannot reach the opamp, and the output is zero.
At high frequencies, the capacitors appear to be shorted. In this case, the voltage gain is zero because feedback capacitor has zero impedance.
Between the low and high extremes in frequency, there is a band of frequencies where the circuit acts like an inverting amplifier.
Narrowband Filters (cont….)
2121
0
2
1
2
21
0771007070
100tan7070
150
2
C CRRπC
f
is: frequencyThe center. ional to Qly proport is directA
. .Q
-ce, if AFor ins
-A .Q
to: quivalent which is eRR.Q
is: he circuitThe Q of tR
-RAv
v
v
v
Narrowband Filter Typical Circuit
Notch Filter
v
v
AQ
RCf
RRA
25.0
21
1
0
1
2
VCVS Sallen Key Band stop Filter circuit
All pass filters All pass filter is widely used in
industry. This is called phase filter. It shifts the phase of the output
signal without changing the magnitude.
Time delay filter.
Summary
Note that in Inverting and Non-Inverting Opamp modes, feedback is – ve.
The only difference is that; input is applied at different terminals.
Output is 1800 out of phase with input in Inverting whereas in Non-Inverting Output is in phase with Input.