Crater Formation and Ground Shock

When a nuclear detonation takes place on or near the ground an appreciable amount of the energy is expended in making a crater and, at the same

Crater formation

time, a shock wave is transmitted outwards through the ground.  The effect of a burst in shallow water such as in an estuary, lake  or harbour will be similar to that of ground burst except that the crater will be submerged, quantities of mud and water will be sucked up into the
fireball and much water will be vapourised. A burst in deep water will cause a shock wave to be transmitted through the water at higher speeds and to greater distances than a blast wave in the air.

Crater formation

In a surface burst a considerable quantity of vaporised or pulverised material is sucked up by the ascending fireball and associated air currents. A still larger quantity is gouged out of the crater by the force of the explosion and is deposited around the crater to add to the “lip” formed by the ground which is squeezed up round the edges of the crater. The combined lip formed in this way has a width roughly equal to the radius of the crater and a height of about a quarter of the depth of the crater. The lip dimensions produced by weapons of dilferent powers are shown in the table for nuclear detonations on saturated clay: on dry soil or hard rock the craters are slightly deeper but less extensive.  Scaling laws/ conversion factors for crater dimensions and a formula for calculating the total volume of a crater are listed below the table.
Crater dimensions in metres (feet) for a ground burst in saturated clay
Weapon power 20KT 100KT 0.5MT 1MT 2MT 5MT 10MT
Radius of crater 91 (300) 155 (510) 260 (850) 335 (1,100) 415 (1,360) 518(1,700) 670 (2,200)
Radius of crater lip 183 (600) 310 (1,020) 518 (1,700) 670 (2,200) 830 (2,720) 1,036 (3,400) 1,340 (4,400)
Depth of crater 12.2 (40) 17 (55) 24 (80) 30 (100) 37 (120) 46 (150) 52 (170)

Scaling laws for crater dimensions
A possible civil defence problem might be that of a crater blocking a river, with a few exceptions British rivers are relatively small and it is unlikely that the flooding would extend beyond the area of complete destruction. Furthermore, the radioactivity in the vicinity of the crater would be so intense that no remedial operation such as cutting a channel through the crater lip, except possibly by bombing from the air, would be possible for a considerable time after the nuclear detonation.

Ground shock

The ground shock effects produced by a megaton surface burst are similar to those produced by an earthquake of moderate intensity, but the pressure in the ground shock wave falls off more rapidly with distance. The effects of this ground shock on structures above ground are irrelevant, since they do not occur beyond the distances at which these structures are totally destroyed by blast. Its effects on structures below ground depend upon the ability of the structure to accommodate itself to the accompanying ground movement. Thus, small structures (e.g. shelters below ground, including Royal Observer Corps Posts) would move bodily with the surrounding ground and should be undamaged beyond 2 or 3 crater radii from the burst. Similarly long, flexible underground structures (e. g. underground utilities) should be able to accommodate themselves to the comparatively small relative ground movement, and should be undamaged outside about 3 crater radii (i.e. less than 1.5 miles or 2.5km for a 10 MT bomb).

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