Logarithmic decrement,
\delta
The method of logarithmic decrement becomes less and less precise as the damping ratio increases past about 0.5; it does not apply at all for a damping ratio greater than 1.0 because the system is overdamped.
The logarithmic decrement is defined as the natural log of the ratio of the amplitudes of any two successive peaks:
\delta=
1 | |
n |
ln
x(t) | |
x(t+nT) |
where x(t) is the overshoot (amplitude - final value) at time t and is the overshoot 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:
\zeta=
\delta | |
\sqrt{4\pi2+\delta2 |
Thus logarithmic decrement also permits evaluation of the Q factor of the system:
Q=
1 | |
2\zeta |
Q=
1 | |
2 |
\sqrt{1+\left(
n2\pi | |||||
|
\right)2}
The damping ratio can then be used to find the natural frequency ωn of vibration of the system from the damped natural frequency ωd:
\omegad=
2\pi | |
T |
\omegan=
\omegad | |
\sqrt{1-\zeta2 |
The damping ratio can be found for any two adjacent peaks. This method is used when and is derived from the general method above:
\zeta=
1 | ||||||||||
|
where x0 and x1 are amplitudes of any two successive peaks.
For system where
\zeta\ll1
\zeta ≈ 1
\zeta ≈
| ||||||
2\pi |
The method of fractional overshoot can be useful for damping ratios between about 0.5 and 0.8. The fractional overshoot is:
OS=
xp-xf | |
xf |
where xp is the amplitude of the first peak of the step response and xf is the settling amplitude. Then the damping ratio is
\zeta=
1 | |||||
|