For an RLC series circuit, a constant associated with this phenomenon can be calculated as attenuationdivided by the resonant angular frequency. That constant associated with this phenomenon is given byone-half the resistance times the square root of capacitance over inductance. That constant is usuallysymbolized zeta or xi and is equivalent to one-half the reciprocal of the Q factor. This phenomenon cancreate a function with a quasi-frequency. When there is only one eigenvalue for the differential equationgoverning thi
For an RLC series circuit, a constant associated with this phenomenon can be calculated as attenuationdivided by the resonant angular frequency. That constant associated with this phenomenon is given byone-half the resistance times the square root of capacitance over inductance. That constant is usuallysymbolized zeta or xi and is equivalent to one-half the reciprocal of the Q factor. This phenomenon cancreate a function with a quasi-frequency. When there is only one eigenvalue for the differential equationgoverning this phenomenon, it occurs critically. It usually results in an exponentially-decaying sinusoidalposition-time graph as amplitude decreases. For 10 points, name this phenomenon in which energy is lostduring harmonic oscillations.
For an RLC series circuit, a constant associated with this phenomenon can be calculated as attenuationdivided by the resonant angular frequency.
damping [or word forms]