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Burridge-Knopoff model

Fig. 4.1. Schematic diagram of the Burridge-Knopoff model of earthquakes. Fig. 4.1. Schematic diagram of the Burridge-Knopoff model of earthquakes.
It may be mentioned here that a recent study (Vasconcelos 1996) of a simple noncooperative (one-block) model of stick-slip motion (described by eqn (4.2) with / o = 0 or eqn (4.4) with k = 0) shows discontinuous velocity-dependent transition in the block displacement, for generic velocity-dependent friction forces. Naive generalisation of this observation for the coupled Burridge-Knopoff model would indicate a possible absence of criticality in the model. [Pg.135]

In another, somewhat more realistic automata model, Olami et al. (1992) (see Perez et al 1996 for a recent review) considered the mapping of the two-dimensional Burridge-Knopoff spring-block model into a cellular automata model. In fact, if one considers the two-dimensional geometry of the Burridge-Knopoff model as shown in Fig. 4.10, one can write for the total elastic force Fij on the block at site (i, j), from (4.4),... [Pg.141]

In the following, we give some details of these studies of response to weak pulses in the BTW model, and of weak periodic pulses in the Burridge-Knopoff model. [Pg.146]

Response of the Burridge-Knopoff model to localised periodic pulses... [Pg.148]

We discuss the various dynamical models of earthquake-like failures in Chapter 4. Specifically, the properties of the Burridge-Knopoff stick-slip model (Burridge and Knopoff 1967) and of the self-organised criticality models, the Guttenberg-Richter type power laws, for the frequency distribution of earthquakes in these models are discussed here. [Pg.4]

Burridge-Knopoff stick-slip model of earthquakes 4.2.1 Laboratory simulation model... [Pg.130]

In their original one-dimensional model for the table top laboratory simulation of earthquakes, Burridge and Knopoff (1967) took a chain of eight massive wooden blocks (of mass around 140 grams each) connected by iden-... [Pg.130]

Fig. 4.2. A typical plot of the time variation of the potential energy (Et) of the spring-block model. Each discontinuity (almost vertical fall) in the potential energy correspond to an earthquake with the magnitude given by the energy release Er) corresponding to the fall. A plot of the frequency n Er) versus energy release (Er) on a log-log scale is indicated in the inset (cf. Burridge and Knopoff 1967). Fig. 4.2. A typical plot of the time variation of the potential energy (Et) of the spring-block model. Each discontinuity (almost vertical fall) in the potential energy correspond to an earthquake with the magnitude given by the energy release Er) corresponding to the fall. A plot of the frequency n Er) versus energy release (Er) on a log-log scale is indicated in the inset (cf. Burridge and Knopoff 1967).

See other pages where Burridge-Knopoff model is mentioned: [Pg.133]    [Pg.142]    [Pg.145]    [Pg.146]    [Pg.148]    [Pg.148]    [Pg.172]    [Pg.133]    [Pg.142]    [Pg.145]    [Pg.146]    [Pg.148]    [Pg.148]    [Pg.172]    [Pg.129]    [Pg.140]    [Pg.258]    [Pg.130]    [Pg.132]    [Pg.374]   
See also in sourсe #XX -- [ Pg.4 , Pg.130 , Pg.131 , Pg.132 , Pg.133 , Pg.134 , Pg.135 , Pg.136 , Pg.137 , Pg.138 , Pg.148 ]




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