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.