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Series and Parallel Resonance Series Resonant circuit L 4.7mH C 0.001µF R 47Ξ© Vin 1V (p-p) fr = ? VC = ? XC = ? VL = ? XL = ? Q=? IT = ? βf = ? Ξ=? Find fr β’ fr = 6.28 1 2π πΏπΆ 1 = 1 6.28 4.7×10β12 = 4.7×10β3 1 1.362×10β5 0.001×10β6 = = 73.412kHz Find reactances β’ XL = 2ΟfL = (6.28)(73.142X103)(4.7X10-6) = 2.168kΞ© β’ 1 1 XC = = 2πππΆ 6.28 73.142×103 0.001×10β6 1 = 2.168kΞ© β4 4.613×10 = Since XC and XL are equal, along with being 180° out of phase, the net reactance is zero which makes the total impedance equal to the resistor β΄ ZT = R Find total current and voltages β’ IT = πππ ππ = πππ π = 0.3535 = 47 7.521mA Since this is a series circuit, the current found for the total will also be the current flowing through the reactive components. β’ VC = (XC)(IT) = (2.168kΞ©)(7.521mA) = 16.306V β’ VL = (XL)(IT) = (2.168kΞ©)(7.521mA) = 16.306V As you can see, the resonant circuit appears to amplify the voltages. Find the Q of the circuit β’ Q= ππΏ ππ ο¨ Since there is no value given for a resistance of the coil, we have to use the only resistance in the circuit to find this value ππΏ 2.168ππΊ β΄Q= = = 46.128 π 47πΊ Solve for Bandwidth and Cutoff frequencies ππ π 73.142ππ»π§ 46.128 β’ βπ = π2 β π1 = = = 1.592kHz ο¨This means the frequency will vary ±796Hz βπ . The entire range is also known as 2 Bandwidth. β’ f2 = βπ fr + = 73.412kHz + 796Hz = 74.208kHz 2 βπ fr - = 73.412kHz - 796Hz = 72.616kHz 2 β’ f1 = β’ ΞΈ = 0° since XL and XC are canceling, which means at resonance the circuit is purely resistive. Parallel Resonant circuit C 162.11pF L 100µH VA 10v(p-p) 50% rs 7.85Ξ© fr = ? IL = ? XL = ? Q=? XC = ? Zeq = ? IC = ? IT = ? βf = ? Solve for fr β’ fr = 6.28 1 2π πΏπΆ 1 = 1 6.28 1.621×10β14 100×10β6 = 1 799×10β9 162.11×10β12 = 1.25MHz = Find the reactances β’ XL = 2ΟfL = (6.28)(1.25X106)(100X10-6) = 785.394Ξ© β’ 1 1 XC = = 2πππΆ 6.28 1.25×106 162.11×10β12 1 = 785.417Ξ© β3 1.273×10 = Since this is a parallel circuit, we presume the applied voltage will be across each reactive component. Find branch currents and the equivalent impedance β’ β’ β’ ππ΄ 10 IC = = = 12.732mA ππ 785.417 ππ΄ 10 IL = = = 12.732mA ππΏ 785.398 ππΏ 785.398 Q= = = 100.051 β ππ 7.85 100 β’ Zeq = QXL = (100.051)(785.398) = 78.58kΞ© ο¨ Since this is the only way we are going to get the total impedance, we now need to use it to find the total current. Find total current β’ IT = ππ΄ πππ = 10 78.58ππΊ = 127.259µA Again, we can see the magnification of the current due to resonance. Solve for Bandwidth and Cutoff frequencies β’ βπ = π2 β π1 = ππ π = 1.25ππ»π§ 100.051 = 12.494kHz ο¨This means the frequency will vary ±6.247kHz β’ f2 = β’ f1 = βπ 2 βπ fr + = 1.25MHz + 6.247kHz = 1.256MHz 2 βπ fr - = 1.25MKz β 6.247kHz = 1.243MHz 2