Logarithmic decrement: Difference between revisions

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clarification. Peaks is vague (x0 and x1 imply peak times) amplitude makes this more understandable
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{{Short description|Measure for the damping of an oscillator}}
{{more citations needed|date=February 2012}}
[[File:Dampingratio111.svg|thumb|400px|The logarithmic decrement can be obtained e.g. as ln(''x''<sub>1</sub>/''x''<sub>3</sub>).]]
 
'''Logarithmic decrement''', <math> \delta </math>, is used to find the [[damping ratio]] of an [[underdamped]] system in the time ___domain.
 
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: <math> \delta = \frac{1}{n} \ln \frac{x(t)}{x(t+nT)} </math>
 
where ''x''(''t'') is the overshoot (amplitude - final value) at time ''t'' and {{nowrap|''x''(''t'' + ''nT'')}} is the amplitudeovershoot of the peak ''n'' periods away, where ''n'' is any integer number of successive, positive peaks.
 
The damping ratio is then found from the logarithmic decrement by:
 
: <math> \zeta = \frac{1\delta}{\sqrt{14\pi^2 + (\frac{2\pi}{\delta})^2}} </math>
 
Thus logarithmic decrement also permits evaluation of the [[Q factor]] of the system:
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: <math> Q = \frac{1}{2} \sqrt{1 + \left(\frac{n2\pi}{\ln \frac{x(t)}{x(t+nT)}}\right)^2} </math>
 
The damping ratio can then be used to find the natural frequency ''ω''<sub>''n''</sub> of vibration of the system from the damped natural frequency ''ω''<sub>''d''</sub>'':''
 
: <math> \omega_d = \frac{2\pi}{T} </math>
: <math> \omega_n = \frac{\omega_d}{\sqrt{1 - \zeta^2}} </math>
where ''T,'', the period of the waveform, is the time between two successive amplitude peaks of the underdamped system.
 
==Simplified Variationvariation==
The damping ratio can be found for any two adjacent peaks. This method is used when {{nowrap|1=''n'' = 1}} and is derived from the general method above:
: <math> \zeta = \frac{1}{\sqrt{1 + \left(\frac{2\pi}{\ln \left(\frac{x_0/}{x_1}\right)}}\right)^2}} </math>
 
where ''x''<sub>''0''</sub> and ''x''<sub>''1''</sub> are amplitudes of any two successive peaks.
 
And forFor system where <math> \zeta <<\ll 1 </math> (not too close to the critically damped regime, where <math> \zeta =\approx 1 </math>).
 
: <math> \zeta =\approx \frac{\ln \left(\frac{x_0/}{x_1}\right)}{2\pi} </math>
 
==Method of fractional overshoot==
The method of fractional overshoot can be useful for damping ratios between about 0.5 and 0.8. The fractional overshoot ''{{math|OS''}} is:
 
: <math>\mathrm{ OS} = \frac{x_p - x_f}{x_f} </math>
 
where ''x''<sub>''p''</sub> is the amplitude of the first peak of the step response and ''x''<sub>''f''</sub> is the settling amplitude. Then the damping ratio is
 
: <math> \zeta = \frac{1}{\sqrt{1 + \left(
\frac{\pi}{\ln (\mathrm{OS})}
\right)^2}} </math>
 
== See also ==
* [[Damping]]
* [[Damping factor]]
 
==References==
{{reflist}}
* {{cite book|last=Inman|first=Daniel J.|title=Engineering Vibration|year=2008|publisher=Pearson Education, Inc.|___location=Upper Saddle, NJ|isbn=978-0-13-228173-27|pages=43–48}}
 
[[Category:Kinematic properties]]
[[Category:Logarithms]]