Logarithmic decrement: Difference between revisions

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The damping ratio is then found from the logarithmic decrement by:
 
: <math> \zeta = \frac{1\delta}{\sqrt{14\pi^2 + \left(\frac{2\pi}{\delta}\right)^2}} </math>
 
Thus logarithmic decrement also permits evaluation of the [[Q factor]] of the system:
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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.
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For 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 ==
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==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]]