Series And Parallel Resonance - Rutgers ECE

School of EngineeringDepartment of Electrical and Computer Engineering332:224 Principlesof ElectricalEngineeringII LaboratoryExperiment 1Series and Parallel Resonance1IntroductionObjectives To introduce frequency response by studying thecharacteristics of two resonant circuits on either side ofresonanceOverviewIn this experiment, the general topic of frequency response is introduced by studying thefrequency-selectivity characteristics of two specific circuit structures. The first is referred toas the series-resonant circuit and the second as the parallel-resonant circuit.The relevant equations and characteristic bell-shaped curves of the frequency responsearound resonance are given in section 2.Prelab exercises are designed to enhance understanding of the concepts and calculateanticipated values subsequently measured in the lab.Current and voltage are then measured in the two resonant circuits as functions of frequencyand characteristic frequencies (resonance and 3-dB points) are experimentally determined. Rutgers UniversityAuthored by P. SannutiLatest revision: December 16, 2005, 2004by P. Panayotatos

PEEII-III-2/122Theory2.1Frequency Domain AnalysisIn electrical engineering and elsewhere, frequency domain analysis or otherwise known asFourier analysis has been predominantly used ever since the work of French physicist JeanBaptiste Joseph Fourier in the early 19th century. The pioneering work of Fourier led towhat are now known as Fourier Series representations of periodic signals and FourierTransform representations of periodic signals. A periodic signal of interest in engineeringcan be represented in terms of a Fourier Series1 which is a weighted linear combination ofsinusoids of harmonically related frequencies. Each frequency among harmonically relatedfrequencies is an integer multiple of a particular frequency known as the fundamentalfrequency. The number of harmonically related sinusoids present in the Fourier Seriesrepresentation of a periodic signal could be finite or countably infinite. Since a periodicsignal can be viewed as being composed of a number of sinusoids, in order to specify aperiodic signal, one could equivalently specify the amplitude and phase of each sinusoidpresent in the signal. Such a specification constitutes the frequency domain description of aperiodic signal. Similarly, in Fourier Transform representation, under some naturalconditions, an aperiodic signal or a signal which is not necessarily periodic can be viewed asbeing composed of uncountably infinite number of sinusoids or a continuum of sinusoids. Inthis case, instead of being a weighted sum of harmonically related sinusoids, an aperiodicsignal is a weighted integral of sinusoids of frequencies which are all not harmonicallyrelated. Again, instead of specifying an aperiodic signal in terms of the time variable t, onecan equivalently specify the amplitude and phase density of each sinusoid of frequency !contained in the signal. Such a description obviously uses the frequency variable ! as anindependent variable, and thus it is said to be the frequency domain or !"domain descriptionof the given time domain signal. In this way, a time domain signal is transformed to afrequency domain signal. Of course, once the frequency domain description of a signal isknown, one can compose all the sinusoids present in the signal to form its time domaindescription. However, it is important to recognize that the frequency domain description issimply a mathematical tool. In engineering, signals exist in a physically meaningful domainsuch as time domain. The frequency domain description only serves to help for the betterunderstanding of certain signal characteristics.1A more detailed treatment can be found in the text starting with section 16.1.

PEEII-III-3/122.2Series ResonanceThe basic series-resonant circuit is shown in fig. 1. Of interest here in how the steady stateamplitude and the phase angle of the current vary with the frequency of the sinusoidalvoltage source. As the frequency of the source changes, the maximum amplitude of thesource voltage (Vm) is held constant. VL- LVs -iVC-C RVR-Vs Vmcos(!t)Fig. 1 The SeriesResonant Circuiti Imcos(!t #)The frequency at which the reactances of the inductance and the capacitance cancel eachother is the resonant frequency (or the unity power factor frequency) of this circuit. Thisoccurs at!o 1LC(1)Since i VR /R, then the current i can be studied by studying the voltage across the resistor.The current i has the expressioni Imcos(!t #)whereIm Vm1 &#R %! L "( !C '2(2A)2and1 ' #L "&#C )! " tan "1 &)R&%)((2B)The bandwidth of the series circuit is defined as the range of frequencies in which theamplitude of the current is equal to or greater than 1 / 2 2 / 2 times its maximum(amplitude, as shown in fig. 2. This yields the bandwidth)B !2-!1 R/L

PEEII-III-4/1221R" R%! 2,1 ' # 2L &LC 2LWhere(3)!2,1 are called the half power frequencies or the 3 dB frequencies, i.e the frequencies at whichthe value of Im equals the maximum possible value divided by 2 1.414 .The quality factorQ !o 1 L B R C(4)Then the maximum value of :! !o!o1- VR occurs at(5A)R 2C1"2L2- VL occurs at!o3- VC occurs at(5B)R 2C1"2L(5C)ImI max VmRI m amx/ 1 .(421)1/24B !1Fig. 2!0RL ! 2 - !1!2Frequency Response of a Series - Resonant Circuit!

PEEII-III-5/122.3Parallel ResonanceThe basic parallel-resonant circuit is shown in fig. 3. Of interest here in how the steady stateamplitude and the phase angle of the output voltage V0 vary with the frequency of thesinusoidal voltage source. !IsRCV0LFig. 3 The ParallelResonant circuit-Is Imcos(!t)If Is Imcos(!t),Vo Vmcos(!t #)thenVm Vo Vmcos(!t #)whereIm1 #1 & !C"%(R2 !L'2(6A)and1 '' ! " tan "1 & R & # C ")% %# L ( )((6B)1LCThe resonant frequency is!o The 3 dB frequencies are:11" 1 %! 2,1 # 2RC '&LC 2RC2The bandwidthThe quality factorB !2 - !1 1/RC.!CQ o RBL(7)(8)

PEEII-III-6/12VmIm RIm RB (2) 1/2!1Fig. 42.4RL ! 2 - !1!2!0!Frequency Response of the Parallel - Resonant CircuitA More Realistic Parallel Resonance CircuitA more realistic parallel-resonant circuit is shown in fig. 5. It is a more realistic modelbecause it accounts for the losses in the inductor through its d.c. resistance RL. RL!IsRV0CLFig. 5 A More RealisticParallel - Resonant Circuit-In this case :!o 1 # RL &"% (LC L 'Z(! o ) and2RLRL RC L(9)(10)

PEEII-III-7/12Vo (! o ) I s (! o )RLRL RC L(11)An analysis of the amplitude of the output voltage as a function of frequency reveals that theamplitude is not maximum at !0. It can be derived that V0 is maximum when! !m (x - y)1/2(12)x (a b)1/2where2RL !a 1 &R %( LC )2 #"12!R 2b # L&" L % LCand!R y # L&" L%2This analysis can be followed by first expressing Vo as a function of !, differentiating thisexpression with respect to ! and then finding the value of ! that makes the derivative zero.3Prelab Exercises3.1Derive equations 1, 2, 3, and 4 for the series-resonant circuit in fig. 1.3.2Derive equations: 5A, 5B, and 5C for the series-resonant circuit in fig. 1.HINT: VR I R where I Im is given by equation 2A. So VR is maximum whenIm R is maximum i.e., Im is maximum (since R is constant). Similarly solve forVL I ZL and VC I ZC .3.3For the series-resonant circuit shown in fig. 6, use equations: 5A, 5B, and 5C to determinethe frequencies at which VR, VC, and VL RL are maximum.

PEEII-III-8/124 ExperimentsSuggested Equipment:Tektronix FG 501A 2MHz Function Generator2Tektronix 504A Counter - TimerHP 54600A or Agilent 54622A OscilloscopeProtek Model B-845 Digital MultimeterLS-400A Inductance Substituter Box620 Ω Resistor0.1 µF CapacitorBreadboardOther circuit elements to be determined by the students.4.1Series ResonanceAny function generator used has internal resistance. Also, the inductor has internal resistance.Both need to be determined since all resistances affect the behavior of the circuit.Function generator resistanceThe internal resistance of the function generator will affect the damping of an RLC circuit towhich it is connected. Check the resistance in the following way:a- With a sine wave output, set the open circuit voltage to some convenient value, say 1V.b- Connect a pure variable resistance load (potentiometer) thus forming a voltage divider.Adjust R until the terminal voltage falls to one-half the open circuit value. At this point thetwo resistances of the voltage divider have to be equal. Therefore, the resistance of thepotentiometer should now be equal to the internal resistance of the function generator.Disconnect the potentiometer from the circuit and measure its resistance.Inductor internal resistanceUse the digital ohmmeter to measure the internal resistance of the inductor used.Measure Rs and RL.Rs 2Ω.RL Ω.NOTE: The oscillator is designed to work for a very wide range of frequencies but may not be stable at very lowfrequencies, say in the order of 100 Hz or 200Hz. To start with it is a good idea to have the circuit working at somemid-range frequency, say in the order of 1K Hz or 2K Hz, and then change the frequency slowly as needed.

PEEII-III-9/12Build the circuit shown in fig. 6 using R 620 Ω, L 100 mH, and C 0.1 µF.Apply a sinusoidal input to the circuit and display both input and output on the screen of theoscilloscope.VL RL RLRsVsL VC-C R -V0-Fig. 6 A Series Resonant CircuitWith the frequency varied from 600 Hz to 2,500 Hz in increments of 100 Hz (using thefrequency counter), measure the rms values of VR, VL RL, and VC using the DVM and thephase angle from the scope (take the phase angle of Vs as the reference). Download thescope trace for your report.The phase angle between two sinusoidal signals of the same frequency can be determined asfollows: Trace both signals on two different channels with the same horizontal sensitivities(the same horizontal scale). To calibrate the horizontal scale in terms of degrees, one canuse the fact that the angular difference between the two successive zero crossing points of asinusoidal signal is 180 degrees. Thus, by measuring the distance between the successivezero crossing points of either sinusoidal signal, one can calibrate the horizontal scale interms of degrees. To determine the phase difference between the two sinusoidal signals,determine the distance between the zero crossing point of one signal to a similar zerocrossing point of another signal and convert it into degrees.Also, to save tedious calculations later, set the rms values of Vs to 1.00 volt before eachreading. Make sure that you use the frequency counter for all frequency measurements, andto note the exact frequencies at which VR, VC, and VL RL are maximum.Once the maximum output voltage (V0 VR) is known, vary the frequency and find the 3 dB(the half power) frequencies, f1,2.Before dismantling the equipment, check your results against those obtained from thetheoretical relationships in eqs 3 & 5. (Make sure to account for the internal resistance of thefunction generator and the d.c. resistance RL of the inductor L in all calculations.)

PEEII-III-10/12f nominal f RVL RL VCParallel ResonanceUsing source transformation, the parallel - resonant circuit in fig. 5 can be represented asshown in fig. 7 where Rs is the internal resistance of the function generator.RVs -Rs RLCV0LFig. 7 A Parallel- Resonant Circuit-Build the circuit of fig. 7 using R 620 Ω, L 100 mH, and C 0.1 µF.Apply a sinusoidal input to the circuit and display both input and output on the scope. Set therms value of Vs 1.00 volts.