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Pile Design and Construction Practice, Fifth edition

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From �7.5 to �3.0 m: no increase of diameter (i.e. D � 0.61 m)<br />

From �3.0 to �1.5 m: increase of 70 mm (D � 0.68 m)<br />

From �1.5 m to sea bed: increase of 190 mm (D � 0.80 m)<br />

Piling for marine structures 433<br />

Taking Newmark’s values a drag force coefficient of 0.5 is used to calculate the current<br />

<strong>and</strong> wave drag forces, <strong>and</strong> an inertia coefficient of 2.0 is used to calculate the wave inertia<br />

forces. Thus in equation 8.10:<br />

F D � 0.5 � 0.5 � � � V 2 � A n � 0.25V 2 A n kN (for � � 1 mg�m 3 )<br />

In equation 8.9<br />

f � 7.8 � 0.5 � 11(u�c) 2 � 8 � 2 � D� 1 g<br />

The calculated wave <strong>and</strong> current forces are shown in Table 8.4 <strong>and</strong> Figure 8.20. The bending<br />

moments shown in Table 8.4 have been calculated on the assumption of virtual fixity of the<br />

pile at a point 1.5 m below the sea bed in the stiff boulder clay. Scour would not be expected<br />

around the piles in this type of soil. From Table 8.4, the combined wave <strong>and</strong> current forces<br />

produce a maximum bending moment at the point of fixity of 690.57 kN m.<br />

Bending moment due to wind force on deck slab:<br />

� 1<br />

2 � 25 � (15.0 � 1.5) � 206.25 kN m<br />

Total bending moment � 896.82 kNm�pile.<br />

Moment of inertia of pile section � �(0.6100 4 � 0.5846 4 )�64 � 1.063 � 10 �3 m 4 .<br />

Extreme fibre stress of pile �<br />

896.82 � 0.305<br />

1.063 � 10 �3 � 10 3 � 257 MN�m 2 .<br />

The direct stress resulting from the dead load of the deck slab <strong>and</strong> self weight of the pile is<br />

added to the bending stress calculated above. It is also necessary to calculate the susceptibility<br />

of the pile to current-induced oscillations.<br />

Assuming the pile to be filled with fresh water, the effective mass is approximately equal<br />

to the mass of metal plus twice the mass of the displaced water. Therefore<br />

M � 187 � (2 � 1<br />

4��0.61 2 � 1 000) � 771.5 kg�m<br />

When the pile is in an unsupported condition cantilevering from the sea bed, from<br />

equation 8.13:<br />

fN � 0.56<br />

14 2�200 � 109 � 1.063 � 10�3 � 1.50 Hz 771.5<br />

du<br />

·<br />

dt� � 42.9(u�c) 2 � 16D� 1 du<br />

g ·<br />

dt� .<br />

From equation 8.12 critical velocity for onset of cross-flow oscillation � 5.5 � 1.5 � 0.61 �<br />

5 m/sec.<br />

Therefore cross-flow or in-line oscillations should not take place for the flow velocities<br />

shown in Figure 8.20.

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