* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Resonance In both series and parallel RLC circuits, resonance
Buck converter wikipedia , lookup
Electrical substation wikipedia , lookup
Opto-isolator wikipedia , lookup
Resistive opto-isolator wikipedia , lookup
Mechanical filter wikipedia , lookup
Wien bridge oscillator wikipedia , lookup
Two-port network wikipedia , lookup
Fault tolerance wikipedia , lookup
Earthing system wikipedia , lookup
Flexible electronics wikipedia , lookup
Zobel network wikipedia , lookup
Integrated circuit wikipedia , lookup
Circuit breaker wikipedia , lookup
Resonant inductive coupling wikipedia , lookup
Resonance In both series and parallel RLC circuits, resonance occurs when XC = XL. In a series circuit VC = VL at resonance ZT = minimum (purely resistive) IT = maximum Below resonance the circuit is primarily capacitive At resonance the circuit is purely resistive Above resonance the circuit is primarily inductive In a parallel circuit IC = IL at resonance ZT = maximum (purely resistive) IT = minimum Below resonance the circuit is primarily inductive At resonance the circuit is purely resistive Above resonance the circuit is primarily capacitive The shape of a circuit’s resonance response is determined by an important factor called the Q factor. A higher Q translates to a sharper response characteristic. Series Circuit Resonance Curves Parallel Circuit Resonance Curves Series Resonance In a series circuit, Q can be determined by the ratios XL X OR C R R Interestingly, the voltage across both the capacitor and inductor at resonance are directly related to the Q factor, as shown above. Q is also affected by the ratio L . A larger ratio means a larger Q factor. C Parallel Resonance A parallel circuit at resonance behaves slightly differently to a series circuit. A parallel circuit designed to resonate is often referred to as a tank circuit. Tank circuits are used a great deal in communication systems. Ideal tank circuit An ideal tank circuit consists of a capacitive element in parallel with an inductive element, and no resistance. Since there is no resistance the Q of the circuit is theoretically infinite. At resonance, since the capacitor and inductor currents are 180° out of phase, the net circuit current is zero. This means that theoretically no current is supplied to the circuit at resonance. Also, since Z = V/I, the impedance seen by the source is theoretically infinite. Practical tank circuit In a practical tank circuit, there will be some resistance associated with the inductor. Thus the Q of the circuit will not be infinite, and can be determined by the ratio XL . R The simple formula for finding the resonant frequency of a series circuit applies equally to a parallel tank circuit provided it has a Q of 10 or greater. Selectivity and bandwidth Selectivity is a measure of how sharp the response curve of a resonant circuit is. The sharper the response, the more selective the circuit is. The responses shown in the above figure are significant since they demonstrate that a resonant circuit can be used to restrict the passage of frequencies to a small proportion of the total frequency range, centered around the resonant frequency. The circuit therefore behaves as a filter, as it filters out all but the frequencies of interest. This range of frequencies is typically referred to as the bandwidth of the filter. Applications Tuned Amplifiers Antenna input to a receiver TV Receiver