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441<br />

-— «oaei test<br />

~^^\f^<br />

Horizontal displacement<br />

Smulatian<br />

Model test -<br />

Sinulation<br />

Model test -<br />

^<br />

10 Li 30 2i 30<br />

(s)<br />

Vertical displacement<br />

(s)<br />

Vertical displacenent<br />

FIG. 3.1<br />

MEASURED AND SIMULATED<br />

DISPLACEMENT RESPONSES AT POINT A<br />

OF NON-ISOLATED MODEL<br />

FIG. 3.2<br />

MEASURED AND SIMULATED<br />

DISPLACEMENT RESPONSES AT POINT A<br />

OF ISOLATED MODEL<br />

SIMULATION ANALYSIS FOR A 200M SPAN LATTICED DOME<br />

Analysis Model<br />

As analysis model a single-layer latticed dome of 200m span and 46.63m rise is selected, as shown in<br />

Fig. 4.1. <strong>The</strong> dome is composed of pin-jointed steel pipes and pin-supported on the base isolation<br />

devices at the bottom of a tension ring which is assumed to be so stiff that the isolation devices can be<br />

idealized as a single d. o. f. system movable only in the horizontal x-direction. In Table 4.1 are shown<br />

the principal dimensions of the dome which were so determined as to satisfy the allowable stress<br />

design criteria against the gravity loads, wind loads and temperature change of 40°C (AIJ, 1973).<br />

TABLE 4.1<br />

PRINCIPAL DIMENSIONS OF DOME<br />

FIG. 4.1<br />

ANALYSIS MODEL<br />

Span<br />

Rise<br />

Radius of curvature<br />

Half subtended angle<br />

Gravity load<br />

Total mass of dome<br />

Young's modulus of steel<br />

Poisson's ratio of steel<br />

Section of roof member<br />

Section of tension ring<br />

200m<br />

46.63 m<br />

130.54m<br />

50°<br />

1.96 kN/nr<br />

76701<br />

0.206 MN/mm 3<br />

0.3<br />

0500x20<br />

0900x50

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