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Archaeoseismology and Palaeoseismology in the Alpine ... - Tierra

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1 st INQUA‐IGCP‐567 International Workshop on Earthquake Archaeology <strong>and</strong> <strong>Palaeoseismology</strong><br />

DYNAMIC RESPONSE OF SIMPLE STRUCTURES<br />

47<br />

K.G. H<strong>in</strong>zen (1)<br />

(1) Earthquake Geology Group, Cologne University, V<strong>in</strong>zenz‐Pallotti‐Str. 26, 51429 Bergisch Gladbach. GERMANY.<br />

h<strong>in</strong>zen@uni‐koeln.de<br />

Abstract: Two discrete element models, a three‐part structured column <strong>and</strong> a 52‐block wall, with <strong>the</strong> size of archaeological rema<strong>in</strong>s found <strong>in</strong><br />

Susita, Israel, <strong>and</strong> Sel<strong>in</strong>ute, Italy, are used to study pr<strong>in</strong>cipal aspects of <strong>the</strong> dynamic behaviour dur<strong>in</strong>g earthquake related ground motions.<br />

Systematic variation of frequency <strong>and</strong> maximum amplitude of ground motion shows that <strong>the</strong> impact pattern of a simply structured,<br />

uncemented wall reveals limited <strong>in</strong>formation about <strong>the</strong> nature of <strong>the</strong> ground motion. When activated by modified measured earthquake<br />

ground motion, <strong>the</strong> column model exhibits chaotic behaviour similar to coupled pendulums. Very small changes <strong>in</strong> <strong>in</strong>itial conditions <strong>and</strong>/or<br />

time‐dependent <strong>in</strong>put forces produce unpredictable behaviour. The longer <strong>the</strong> <strong>in</strong>put motion lasts, <strong>the</strong> more complex‐structured <strong>the</strong> resultant<br />

ground motion becomes. Knowledge of <strong>the</strong> mechanics <strong>and</strong> dynamics of build<strong>in</strong>g elements typical for classical archaeological structures is an<br />

essential tool to test <strong>the</strong> seismogenic hypo<strong>the</strong>sis of documented damages.<br />

Key words: Column, Block Wall, Discrete Element Model, <strong>Archaeoseismology</strong>.<br />

INTRODUCTION<br />

One of <strong>the</strong> ma<strong>in</strong> challenges for carry<strong>in</strong>g out archaeo‐<br />

seismic field studies is <strong>the</strong> deduction of damage scenarios.<br />

Even for cases that seem obvious concern<strong>in</strong>g <strong>the</strong> nature<br />

of <strong>the</strong> damag<strong>in</strong>g process, all o<strong>the</strong>r possible scenarios have<br />

to be taken <strong>in</strong>to account. In order to fur<strong>the</strong>r underst<strong>and</strong><br />

<strong>the</strong> reaction of archaeologically excavated structures to<br />

external forces such as earthquakes <strong>and</strong> o<strong>the</strong>r natural<br />

dynamic or anthropogenic sources, we studied simple<br />

structural elements.<br />

Here we present some results from <strong>the</strong> <strong>in</strong>vestigation of<br />

simple columns <strong>and</strong> block walls motivated by <strong>the</strong> toppled<br />

columns of <strong>the</strong> so‐called ‘ca<strong>the</strong>dral’ <strong>in</strong> Susita (Fig. 1a)<br />

above <strong>the</strong> banks of <strong>the</strong> Sea of Galilee <strong>and</strong> <strong>the</strong> toppled<br />

block wall of <strong>the</strong> Triolo temple <strong>in</strong> Sel<strong>in</strong>ute (Fig. 1b), Sicily.<br />

We used similar‐sized structural elements for <strong>the</strong> basic<br />

model.<br />

MODELING PROCEDURE<br />

Several previous studies have shown that much can be<br />

learned from numeric experiments with block structures<br />

us<strong>in</strong>g f<strong>in</strong>ite <strong>and</strong> discrete element techniques (i.e. Augusti<br />

<strong>and</strong> S<strong>in</strong>opoli,1992; Konstant<strong>in</strong>idis <strong>and</strong> Makris, 2005;<br />

Psycharis, 2007; H<strong>in</strong>zen, 2009). While f<strong>in</strong>ite element (FE)<br />

models, a st<strong>and</strong>ard <strong>in</strong> civil eng<strong>in</strong>eer<strong>in</strong>g, are able to predict<br />

dynamic stability <strong>and</strong> failure limits, discrete element (DE)<br />

models are suitable for modell<strong>in</strong>g post failure movements<br />

of build<strong>in</strong>g parts. In archaeoseismology we are forced to<br />

deal with <strong>the</strong> ‘f<strong>in</strong>al result’ of <strong>the</strong> damage process,<br />

(a) (b)<br />

Fig. 1: (a) Row of toppled columns of <strong>the</strong> ‘ca<strong>the</strong>dral’ <strong>in</strong> Susita,<br />

Israel (Photo: H<strong>in</strong>zen); (b) fallen block wall of <strong>the</strong> Triolo<br />

temple at Sel<strong>in</strong>ute, Sicily (from Bottari, 2008)<br />

<strong>the</strong>refore <strong>the</strong> consideration of post failure movements of<br />

build<strong>in</strong>g parts is of special <strong>in</strong>terest <strong>and</strong> speaks for <strong>the</strong> use<br />

of DE models. However, this limits <strong>the</strong> analysis to<br />

situations where <strong>the</strong> elastic properties <strong>and</strong> material<br />

strength are not crucial as for free st<strong>and</strong><strong>in</strong>g columns <strong>and</strong><br />

block structures without mortar or complex clamp<strong>in</strong>g<br />

devices. These are ideal c<strong>and</strong>idates for DE modell<strong>in</strong>g.<br />

The aim of this study is <strong>the</strong> evaluation of <strong>the</strong> pr<strong>in</strong>cipal<br />

behaviour of simple structures, not <strong>the</strong> development of<br />

appropriate scenarios for <strong>the</strong> two archaeological sites.<br />

Therefore, only rough measures were taken from<br />

photographs <strong>and</strong> published plans of <strong>the</strong> church columns<br />

<strong>and</strong> <strong>the</strong> temple wall <strong>and</strong> non site‐specific ground motions<br />

are used.<br />

Column Model<br />

Fig. 2a shows <strong>the</strong> column model <strong>in</strong> two versions, (1)<br />

completely rotational symmetric with round pedestal <strong>and</strong><br />

capital <strong>and</strong> (2) with square base of <strong>the</strong> pedestal <strong>and</strong><br />

capital top like those <strong>in</strong> Figure 1a. Total height is <strong>in</strong> both<br />

cases 5.8 m with contributions of 0.3, 4.7 <strong>and</strong> 0.8 m from<br />

<strong>the</strong> pedestal, <strong>the</strong> shaft <strong>and</strong> <strong>the</strong> capital, respectively. With<br />

a density of 2.7 Mg/m 3 , <strong>the</strong> weight of <strong>the</strong> three parts is<br />

490, 3570, <strong>and</strong> 760 kg. Jo<strong>in</strong>ts between <strong>the</strong> column parts<br />

<strong>and</strong> between <strong>the</strong> pedestal <strong>and</strong> <strong>the</strong> base block have six<br />

degrees of freedom. Contact forces are of stick slip type<br />

with static <strong>and</strong> dynamic coefficients of 0.7 <strong>and</strong> 0.6,<br />

respectively <strong>and</strong> a contact frequency of 200 Hz.<br />

(a) (b)<br />

5.8 m<br />

0.60 m<br />

3.25 m<br />

5.55 m<br />

Fig. 2: Discrete element model of (a) rotational symmetric<br />

three part column (left) <strong>and</strong> a column with square pedestal<br />

<strong>and</strong> capital (right); (b) a 52‐block wall.

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