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A History of Research and a Review of Recent Developments

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76<br />

Structural loading from distant explosions<br />

Figure 4.1 Blast wave meeting 180° semi-circular arch (from Newmark et al., ref.<br />

4.2).<br />

maximum average pressure on the front <strong>of</strong> the cylinder is 2p, <strong>and</strong> that this<br />

decays linearly until a time 2D/ū. The average side loading is given as<br />

in ref. [4.5], <strong>and</strong> the maximum back surface loading as<br />

p(20D/ū)+C dq(20D/ū).<br />

When a semi-cylindrical, or arched structure is loaded by a shock wave perpendicular<br />

to its longitudinal axis, vortex formations can occur immediately after reflection,<br />

so that a temporary sharp drop can occur before the stagnation pressure is reached.<br />

Subsequently the total pressure, p+C dq, decays in the usual way. The relationship<br />

between p 1, p 2, C d <strong>and</strong> the angle a for a semi-circular arch is shown in Figure 4.1,<br />

where p 1 <strong>and</strong> p 2 are related to p r, the ideal reflected pressure for a free surface.<br />

Since the structural loads are normal to the surface, the total horizontal load on<br />

the structure is formed by summing all horizontal components, <strong>and</strong> Figure 4.1<br />

gives the approximate equivalent net horizontal force.<br />

Many arched structures are not fully semi-cylindrical, <strong>and</strong> for 120° arches<br />

similar relationships to those in Figure 4.1 have been presented (see, for example,<br />

ref. [4.2]). It can be seen from these relationships that C d varies from positive<br />

to negative as the angle increases, <strong>and</strong> is also influenced by the peak incident

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