Depending on the choice of the model to fit, several parameters can
(or should) be provided, e.g. f,q, v, k,
and most importantly, a_0.
If more signals than free parameters are available, the missing
parameters may be estimated during the fit, but without any checks
of quality and meaningfulness. The parameter a_0 will be
defined as 100 times the maximum input amplitude, by default. The
parameters f will be set to 10 Hz, q to 50, v
to 1000 m/s and k to 0.5.
ISSUES: account for non-fixed parameters, especially k
The following amplitude-distance models are available:
"SurfSpreadAtten", Surface waves including geometric
spreading and unelastic attenuation
"BodySpreadAtten", Body waves including geometric
spreading and unelastic attenuation
"SurfBodySpreadAtten", Surface and body waves including
geometric spreading and unelastic attenuation
"SurfSpread", Surface waves including geometric
spreading, only
"BodySpread", Body waves including geometric
spreading, only
"SurfBodySpread", Surface and body waves including
geometric spreading, only
**SurfSpreadAtten**
The model is based on Eq. 17 from Burtin et al. (2016):
$$a_d = a_0 / sqrt(d) * exp(-(pi * f * d) / (q * v))$$
where a_0 is the source amplitude, a_d the amplitude as recorded by a sensor
at distance d, f is the center frequency of the signal, q the ground quality
factor and v the seismic wave velocity.
**BodySpreadAtten**
The model is based on Eq. 16 from Burtin et al. (2016):
$$a_d = a_0 / d * exp(-(pi * f * d) / (q * v))$$
where a_0 is the source amplitude, a_d the amplitude as recorded by a sensor
at distance d, f is the center frequency of the signal, q the ground quality
factor and v the seismic wave velocity.
**SurfBodySpreadAtten**
The model based on Eqs. 16 and 17 from Burtin et al. (2016):
$$a_d = k * a_0 / sqrt(d) * exp(-(pi * f * d) / (q * v)) + (1 - k) * a_0 / d * exp(-(pi * f * d) / (q * v))$$
where a_0 is the source amplitude, a_d the amplitude as recorded by a sensor
at distance d, f is the center frequency of the signal, q the ground quality
factor, v the seismic wave velocity, and n and m two factors determining the
relative contributions of the two wave types, thus summing to 1.
**BodySpread**
The model is simply accounting for geometric spreading
$$a_d = a_0 / d$$
where a_0 is the source amplitude, a_d the amplitude as recorded by a sensor
at distance d.
**SurfSpread**
The model is simply accounting for geometric spreading
$$a_d = a_0 / sqrt(d)$$
where a_0 is the source amplitude, a_d the amplitude as recorded by a sensor
at distance d.
**SurfBodySpread**
The model is simply accounting for geometric spreading
$$a_d = k * (a_0 / d) + (1 - k) * a_d / sqrt(d)$$
where a_0 is the source amplitude, a_d the amplitude as recorded by a sensor
at distance d, and n and m two factors determining the relative
contributions of the two wave types, thus summing to 1.
**References**
- Burtin, A., Hovius, N., and Turowski, J. M.: Seismic monitoring of
torrential and fluvial processes, Earth Surf. Dynam., 4, 285–307,
https://doi.org/10.5194/esurf-4-285-2016, 2016.