Lecture 7 Active Filters Active Filters 1-1 Agenda Introduction to Active Filters Highlighting differences with respect to passive filters First-order lowpass active filter First-order highpass active filter Active bandpass filter Active bandreject filter Example Active Filters 1-2 Introduction Some limitations of the passive filters 1. cannot generate gain greater than one • passive elements cannot add energy to the network 2. may require bulky and expensive circuit elements in case of using inductors 3. may have source loading 4. no isolation between the input and the output Active Filters 1-3 Introduction Active filters consist of combinations of resistors, capacitors, and Op Amps They offer some advantages over passive RLC filters often smaller and less expensive can provide amplifier gain in addition to providing the same frequency response as RLC filters can be combined with buffer amplifiers (voltage followers) to isolate each stage of the filter from source and load impedance effects • realizing the desired transfer function Active Filters 1-4 First-Order Active Filter • • • The components selected for 𝑍𝑖 and 𝑍𝑓 determine whether the filter is lowpass or highpass, but one of the components must be reactive First order filters have one pole due to the usage of one capacitor, reactive element, besides resistors in the filtering circuit Active filters comprise active circuit components such Op Amps Active Filters 1-5 Active First-Order Lowpass Filter The transfer function 𝐻 𝜔 = 𝑉𝑜 𝑉𝑖 =− 𝑖𝑍𝑓 𝑖𝑅𝑖 i In case of passive filters no gain In case of DC analysis inverting amplifier 𝐻 𝜔 =− 𝑅𝑓 𝑅𝑖 Active Filters 1-6 Active First-Order Lowpass Filter Knowing the transfer function The maximum gain |𝐻 𝜔 | = 𝑅𝑓 𝑅𝑖 in case DC (dc gain) How to find the 3dB cutoff or the corner frequency 𝜔𝑐 ? It is the frequency when the maximum |𝐻 𝜔 | 1 dropped by 2 Then, 𝜔𝑐 = 𝑅 1 𝑓 𝐶𝑓 Active Filters 1-7 Active First-Order Highpass Filter The transfer function In case of high frequencies inverting amplifier 𝐻 𝜔 =− 𝑅𝑓 𝑅𝑖 the 3dB cutoff or the corner frequency 𝜔𝑐 Active Filters 1-8 Active Bandpass Filter Unity gain Unity gain 𝜔2 > 𝜔1 Active Filters 1-9 Active Bandpass Filter Analysis (cascaded Op Amp circuit) Active Filters 1-10 Active Bandpass Filter Analysis (cascaded Op Amp circuit) The lowpass section sets the upper corner frequency as while the highpass section sets the lower corner frequency as Active Filters 1-11 Active Bandpass Filter Analysis (cascaded Op Amp circuit) With the known values of 𝜔1 and 𝜔2 , the center frequency𝜔0 , bandwidth 𝐵, and quality factor 𝑄 the passband gain 𝐾: Active Filters 1-12 Active Bandreject Filter Active Filters 1-13 Active Bandreject Filter Analysis Active Filters 1-14 Active Bandreject Filter Analysis The transfer function In terms of corner frequencies 1 1 𝜔1 = ,𝜔 = 𝐶1 𝑅 2 𝐶2 𝑅 In the two passbands ( 𝜔 → 0 and 𝜔 → ∞) the gain is Active Filters 1-15 Example Design a first-order lowpass active filter with a dc gain of 4 and a corner frequency of 500 Hz (in other words, get values for 𝑅𝑖 𝑅𝑓 𝑎𝑛𝑑 𝐶𝑓 ) Solution • The dc gain • We can assume a value for 𝐶𝑓 • 𝐶𝑓 = 0.2 𝜇𝐹 Active Filters 1-16 Lecture-related Question Design a first-order highpass active filter with a high- frequency gain of 5 and a corner frequency of 2 kHz. Use a 0.1 𝜇𝐹 capacitor in your design. Active Filters 1-17 Lecture Summary Covered material Introduction to Active Filters Highlighting differences with respect to passive filters First-order lowpass active filter First-order highpass active filter Active bandpass filter Active bandreject filter Example Next Week: Mid-term Exam Good Luck Active Filters 1-18