Intrinsic (anelastic) attenuation of a seismic wave's amplitude as it travels a distance \(x\) through a medium of quality factor \(Q\) is given by:
\[ \frac{A}{A_0} = \exp\left(-\frac{\pi f x}{Q v}\right) \]where \(f\) is the frequency, \(v\) is the (non-dispersive) wave velocity, and \(x\) is the propagation distance. This form follows from writing the travel time \(t = x/v\) and using the standard temporal attenuation law \(A/A_0 = e^{-\pi f t/Q}\).
Substitute the given values: \(f = 20\ \text{Hz}\), \(x = 10\ \text{km}\), \(Q = 80\), \(v = 5\ \text{km/s}\):
\[ \frac{\pi f x}{Qv} = \frac{\pi \times 20 \times 10}{80 \times 5} = \frac{200\pi}{400} = \frac{\pi}{2} = 1.5708 \]So:
\[ \frac{A}{A_0} = e^{-1.5708} = 0.2079 \]Converting to a percentage:
\[ \frac{A}{A_0} \times 100\% = 20.8\% \]This value of 20.8% lies within the official accepted range of 20 to 21%. Physically, this shows how strongly a 20 Hz P-wave is attenuated by intrinsic damping (Q = 80) over just 10 km -- only about a fifth of the original amplitude survives, which is why higher-frequency seismic signals lose amplitude much faster with distance than lower-frequency ones for the same Q.
\(\boxed{\dfrac{A}{A_0} \approx 20.8\%}\)
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