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<strong>www</strong>.<strong>GOALias</strong>.<strong>blogspot</strong>.<strong>com</strong>PhysicsThus, the analytical solution for the amplitude and phase of the currentin the circuit agrees with that obtained by the technique of phasors.7.6.3 ResonanceAn interesting characteristic of the series RLC circuit is the phenomenonof resonance. The phenomenon of resonance is <strong>com</strong>mon among systemsthat have a tendency to oscillate at a particular frequency. This frequencyis called the system’s natural frequency. If such a system is driven by anenergy source at a frequency that is near the natural frequency, theamplitude of oscillation is found to be large. A familiar example of thisphenomenon is a child on a swing. The the swing has a natural frequencyfor swinging back and forth like a pendulum. If the child pulls on therope at regular intervals and the frequency of the pulls is almost thesame as the frequency of swinging, the amplitude of the swinging will belarge (Chapter 14, Class XI).For an RLC circuit driven with voltage of amplitude v mand frequencyω, we found that the current amplitude is given byvvZ R X Xmm = =im2 2+ (C−L)with X c= 1/ωC and X L= ω L. So if ω is varied, then at a particular frequencyω 0, X c= X L, and the impedance is minimum ( Z R )2 02 Rfrequency is called the resonant frequency:1Xc= XLor =0Lω Cω0= + = . This1or ω0= (7.35)LCAt resonant frequency, the current amplitude is maximum; i m= v m/R.Figure 7.16 shows the variation of i mwith ω ina RLC series circuit with L = 1.00 mH, C =1.00 nF for two values of R: (i) R = 100 Ωand (ii) R = 200 Ω. For the source applied v m=100 V. ω 0for this case is⎛⎜⎝1 ⎞⎟LC ⎠= 1.00×10 6rad/s.We see that the current amplitude is maximumat the resonant frequency. Since i m= v m/ R atresonance, the current amplitude for case (i) istwice to that for case (ii).FIGURE 7.16 Variation of i Resonant circuits have a variety ofmwith ω for twocases: (i) R = 100 Ω, (ii) R = 200 Ω, applications, for example, in the tuningL = 1.00 mH.mechanism of a radio or a TV set. The antenna ofa radio accepts signals from many broadcastingstations. The signals picked up in the antenna acts as a source in the248tuning circuit of the radio, so the circuit can be driven at many frequencies.

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