A quantity that describes this phenomenon is expressed as a linear combination of two matrices denoted M and K in a numerical model named for Rayleigh. Multiplying the strength of this phenomenon by the factor “1 (15[1])minus x squared” creates a system whose behavior is described by Lienard's theorem. The strength of this phenomenon can be (-5[1])quantified by the logarithmic decrement. This phenomenon corresponds to the B term of the (10[1]-5[1])differential equation (-5[2])0 equals (*) A (10[2]-5[3])times x (-5[1])double (10[2]-5[1])prime, plus (10[1])B times x prime, plus C times x. (10[2])“Over” (-5[1])examples of this (10[1])phenomenon (10[2])display no overshooting, (10[2])while “critical” examples (10[1])have a Q-factor of one-half and minimize the time to static (10[4])equilibrium. For 10 points, name this (10[1])phenomenon in which an oscillating system (10[1])loses energy and stops (10[1])oscillating. ■END■