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Random Vibration Analysis Tool (PSD Input)

Numerical analysis of SDOF random vibration response. Computes response spectrum, response RMS, and 3-sigma values from PSD input in real time. Applicable to vibration durability design for spacecraft, aircraft, and automotive components.

$G_x(f) = |H(f)|^2 \cdot G_f(f)$, $\quad \sigma_{\rm rms} = \sqrt{\displaystyle\int_0^\infty G_x(f)\,df}$
System & Input Parameters
f₀ — Natural Frequency50 Hz
ζ — Damping Ratio0.050
PSD Input Profile
G₀ — PSD Level0.040 g²/Hz
f_min20 Hz
f_max2000 Hz
g
σ_rms Response
g
3σ (99.73%)
g
Miles Equation Estimate
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Resonance Peak Factor
Input PSD / Response PSD / Transfer Function (Log Scale)

Theoretical Background

In random vibration analysis, the response PSD is obtained from the input power spectral density (PSD) and the transfer function of the single-degree-of-freedom system. The response RMS is the square root of the integral of the response PSD.

Transfer function: $|H(f)|^2 = \dfrac{1}{\left[1-\left(\dfrac{f}{f_0}\right)^2\right]^2 + \left[2\zeta\dfrac{f}{f_0}\right]^2}$
Miles equation (flat PSD approximation): $\sigma_{\rm rms} \approx \sqrt{\dfrac{\pi f_0 G_0}{4\zeta}}$
Resonance peak factor: $Q = \dfrac{1}{2\zeta}$ (transfer function maximum $\approx Q^2$)

The Miles equation is an approximate solution that assumes a constant PSD level $G_0$ near $f_0$. When the PSD varies significantly around $f_0$, the numerical integration result is more accurate. Widely used in vibration durability assessment of spacecraft and aircraft components.