F REQUENCY R ESPONSE & R ESONANT C IRCUITS Filters, frequency response, time domain connection, bode plots, resonant circuits.

O UTLINE AND TOPICS Low-pass filters High-pass filters Other filters Resonance (Ch 20) Ideal op-amps and active filters Decibels & log scales Linear systems and transfer functions Bode plots Reading 1.Boylestad Ch Boylestad Ch

F ILTERS

Any combination of passive ( R, L, and C ) and/or active (transistors or operational amplifiers) elements designed to select or reject a band of frequencies is called a filter. In communication systems, filters are used to pass those frequencies containing the desired information and to reject the remaining frequencies.

FILTERS In general, there are two classifications of filters: Passive filters-gain always<1 Active filters-gain can be >1

FILTERS FIG Defining the four broad categories of filters.

R-C LOW-PASS FILTER FIG Low- pass filter. FIG R-C low- pass filter at low frequencies.

R-C LOW-PASS FILTER FIG R-C low- pass filter at high frequencies. FIG V o versus frequency for a low-pass R-C filter.

R-C LOW-PASS FILTER FIG Normalized plot of Fig

R-C LOW-PASS FILTER FIG Angle by which V o leads V i.

R-C LOW-PASS FILTER FIG Angle by which V o lags V i.

R-C LOW-PASS FILTER FIG Low-pass R- L filter. FIG Example 21.5.

R-C LOW-PASS FILTER FIG Frequency response for the low-pass R-C network in Fig

R-C LOW-PASS FILTER FIG Normalized plot of Fig

R-C HIGH-PASS FILTER FIG High- pass filter.

R-C HIGH-PASS FILTER FIG R-C high-pass filter at very high frequencies. FIG R-C high- pass filter at f = 0 Hz.

R-C HIGH-PASS FILTER FIG V o versus frequency for a high- pass R-C filter.

R-C HIGH-PASS FILTER FIG Normalized plot of Fig

R-C HIGH-PASS FILTER FIG Phase-angle response for the high- pass R-C filter.

R-C HIGH-PASS FILTER FIG High-pass R- L filter.

R-C HIGH-PASS FILTER FIG Normalized plots for a low-pass and a high-pass filter using the same elements.

R-C HIGH-PASS FILTER FIG Phase plots for a low-pass and a high-pass filter using the same elements.

PASS-BAND FILTERS FIG Series resonant pass- band filter.

RLC C IRCUITS - RESONANCE ! The resonant electrical circuit must have both inductance and capacitance. In addition, resistance will always be present due either to the lack of ideal elements or to the control offered on the shape of the resonance curve. When resonance occurs due to the application of the proper frequency ( fr ), the energy absorbed by one reactive element is the same as that released by another reactive element within the system.

SERIES RESONANT CIRCUIT A resonant circuit (series or parallel) must have an inductive and a capacitive element. A resistive element is always present due to the internal resistance of the source ( Rs ), the internal resistance of the inductor ( Rl ), and any added resistance to control the shape of the response curve ( R design).

SERIES RESONANT CIRCUIT FIG Series resonant circuit.

PASS-BAND FILTERS FIG Parallel resonant pass- band filter.

PASS-BAND FILTERS FIG Series resonant pass-band filter for Example 21.7.

PASS-BAND FILTERS FIG Pass-band response for the network.

PASS-BAND FILTERS FIG Normalized plots for the pass-band filter in Fig

PASS-BAND FILTERS FIG Pass- band filter.

PASS-BAND FILTERS FIG Pass-band characteristics.

PASS-BAND FILTERS FIG Pass- band filter. FIG Pass-band characteristics for the filter in Fig

PASS-BAND FILTERS FIG Network of Fig at f = kHz.

BAND-REJECT FILTERS Since the characteristics of a band-reject filter (also called stop-band or notch filter) are the inverse of the pattern obtained for the band-pass filter, a band-reject filter can be designed by simply applying Kirchhoff’s voltage law to each circuit.

BAND-REJECT FILTERS FIG Demonstrating how an applied signal of fixed magnitude can be broken down into a pass-band and band-reject response curve.

BAND-REJECT FILTERS FIG Band-reject filter using a series resonant circuit.

BAND-REJECT FILTERS FIG Band-reject filter using a parallel resonant network.

BAND-REJECT FILTERS FIG Band- reject filter.

BAND-REJECT FILTERS FIG Band-reject characteristics.

O PERATIONAL AMPLIFIERS Active filters

AMPLIFIERS GIVE GAIN Simple amp-1 input and 1 output Gain, A=Vout/Vin

E XAMPLE If the amplifier above gives an output voltage of 1000V with an input voltage of 50V, what is the gain?

IDEAL OPERATIONAL - AMPLIFIER ( OP - AMP ) Inputs draw no current-infinite input impedace Vout=A(Vplus-Vminus) A-open loop gain. A is ideally infinity-How is this useful? Output can provide as much voltage/current as needed-zero output impedance

NEGATIVE FEEDBACK Negative feedback (NF) tries to reduce the difference with NF, Vplus=Vminus ALWAYS summing point constraints virtual ground.

I NVERTING AMPLIFIER Input goes into Vminus input-INVERTING input Gain, Ainv=-R2/R1, gain is negative because inverting

INVERTING AMPLIFIER Vplus=Vminus Inputs draw no current

N ON - INVERTING AMPLIFIER Input goes into Vplus input-NON-INVERTING input Gain, Ainv=1+R2/R1, gain is positive

UNITY GAIN BUFFER Gain is 1 i.e. Vin=Vout Used to isolate one side from the other

R EAL OP - AMPS Output voltage determined by rails (power supply) Open loop gain not infinity Inputs draw small amount of current-nA’s or less Quad LM324 Single LM741

BANDPASS F ILTER AMPLIFIER f1=0.3Hz, f2=10Hz High freq., cap is short, low freq., cap is open

FREQUENCY < F 1 all caps are open. What is the gain?

F1<F REQUENCY <F2 C1 is short. C2 is open. What is the gain?-midband gain.

FREQUENCY > F 2 All caps are shorts What is the gain?

FILTER OP - AMP What is T(s)?

FILTER OP - AMP zero at s=0 poles at 1/R1C1 and 1/R2C2 What happens at the zero? At the poles?

D ECIBELS & B ODE PLOTS The key to amplifiers and control systems.

INTRODUCTION The unit decibel (dB), defined by a logarithmic expression, is used throughout the industry to define levels of audio, voltage gain, energy, field strength, and so on.

INTRODUCTION L OGARITHMS Basic Relationships Let us first examine the relationship between the variables of the logarithmic function. The mathematical expression:

INTRODUCTION L OGARITHMS Some Areas of Application The following are some of the most common applications of the logarithmic function: 1. The response of a system can be plotted for a range of values that may otherwise be impossible or unwieldy with a linear scale. 2. Levels of power, voltage, and the like can be compared without dealing with very large or very small numbers that often cloud the true impact of the difference in magnitudes. 3. A number of systems respond to outside stimuli in a nonlinear logarithmic manner. 4. The response of a cascaded or compound system can be rapidly determined using logarithms if the gain of each stage is known on a logarithmic basis.

INTRODUCTION L OGARITHMS FIG Semilog graph paper.

INTRODUCTION L OGARITHMS FIG Frequency log scale.

INTRODUCTION L OGARITHMS FIG Finding a value on a log plot. FIG Example 21.1.

PROPERTIES OF LOGARITHMS There are a few characteristics of logarithms that should be emphasized: The common or natural logarithm of the number 1 is 0 The log of any number less than 1 is a negative number The log of the product of two numbers is the sum of the logs of the numbers The log of the quotient of two numbers is the log of the numerator minus the log of the denominator The log of a number taken to a power is equal to the product of the power and the log of the number

PROPERTIES OF LOGARITHMS C ALCULATOR F UNCTIONS Using the TI-89 calculator, the common logarithm of a number is determined by first selecting the CATALOG key and then scrolling to find the common logarithm function. The time involved in scrolling through the options can be reduced by first selecting the key with the first letter of the desired function—in this case, L, as shown below, to find the common logarithm of the number 80.

DECIBELS Power Gain Voltage Gain Human Auditory Response

DECIBELS TABLE 21.1

DECIBELS TABLE 21.2 Typical sound levels and their decibel levels.

DECIBELS FIG LRAD (Long Range Acoustic Device) 1000X. (Courtesy of the American Technology Corporation.)

DECIBELS I NSTRUMENTATION FIG Defining the relationship between a dB scale referenced to 1 mW, 600Ω and a 3 V rms voltage scale.

L INEAR SYSTEMS RLC circuits, op-amps are linear circuit elements i.e. a differential equation can describe them. You can add solutions at a given ω i.e. if exp(jωt) and exp(-jωt) are solutions, exp(jωt)+exp(-jωt)=2cos(ωt) is a solution. t t tt

LINEAR SYSTEMS Any voltage signal can be represented by a sum of sinusoidal voltage signals- Fourier/Laplace theorems If s=jω, the input voltage is represented by: V 0 exp(jωt)= V 0 exp(st) Allows us to use algebra instead of differential eqns. RLC circuit, for example. t t tt

T RANSFER FUNCTION Transfer function T(s), or H(s) describes how the output is affected by the input. i.e. T(s)=V o /V i s=jω, so Z C =1/sC and Z L =sL The ‘s’ notation is convenient shorthand, but is also important in the context of Laplace Transforms, which you will see later in the class. Transfer because it describes how voltage is “transferred” from the input to output.

LINEAR SYSTEMS T(s) has zeros when T(s)=0 T(s) has poles when T(s)=infinity

P OLES & ZEROS All transfer functions have poles and zeros. Zeros are when T(s)=0 Poles are when 1/T(s)=0 or T(s)=∞ These contribute very distinct behaviors to the frequency response of a system. For our friend the RC lowpass circuit,

T RANSFER FUNCTION FOR LOW - PASS Again we go to our good friend, the low-pass filter. FIG Example Now, we will redo this in the language of “transfer function”

B ODE PLOTS