This preview shows pages 1–3. Sign up to view the full content.
This preview has intentionally blurred sections. Sign up to view the full version.
View Full Document
Unformatted text preview: x y z w w + G w v + G v v u u + G u G y G x G z 6 WATER WAVES 35 6 WATER WAVES Surface waves in water are a superb example of a stationary and ergodic random process. The model of waves as a nearly linear superposition of harmonic components, at random phase, is confirmed by measurements at sea, as well as by the linear theory of waves, the subject of this section. We will skip some elements of uid mechanics where appropriate, and move quickly to the cases of twodimensional, inviscid and irrotational ow. These are the major assumptions that enable the linear wave model. 6.1 Constitutive and Governing Relations First, we know that near the sea surface, water can be considered as incompressible, and that the density is nearly uniform. In this case, a simple form of conservation of mass will hold: u v w + + = 0 , x y z where the Cartesian space is [ x, y, z ], with respective particle velocity vectors [ u, v, w ]. In words, the above equation says that net ow into a differential volume has to equal net ow out of it. Considering a box of dimensions [ x, y, z ], we see that any u across the xdimension, has to be accounted for by v and w : uyz + vxz + wxy = 0 . Next, we invoke Newtons law, in the three directions: u u u u p 2 u 2 u 2 u t + u x + v y + w z = x + x 2 + y 2 + z 2 ; v v v v p 2 v 2 v 2 v t + v x + w y + u z = y + x 2 + y 2 + z 2 ; w w w w p 2 w 2 w 2 w t + w x + u y + v z = z + x 2 + y 2 + z 2 g. T T T T T x x x x y y y y I#!#0T#2#5 I#!#T#2#5 I#!#0T I#!#3 6 WATER WAVES 36 Here the lefthand side of each equation is the acceleration of the uid particle, as it moves u through the differential volume. The terms such as u x capture the fact that the force balance is for a moving particle; the chain rule expansion goes like this in the xdirection: du u u x u y u z = + + + , dt t x t y t z t where u = x/t and so on. On the right side of the three force balance equations above, the differential pressure clearly acts to slow the particle (hence the negative sign), and viscous friction is applied through absolute viscosity . The third equation also has a term for gravity, leading in the case of zero velocities to the familiar relation p ( z ) = gz , where z is taken positive upward from the mean free surface. 6.2 Rotation and Viscous Effects In a uid, unlike for rigid bodies, rotation angle is taken as the average of the angular deections of the faces. Hence, a net rotation only occurs if the deection of each face is additive. If they are opposing, then we have only a shearing of the element, with no rotation....
View Full
Document
 Spring '05
 GeorgeKocur
 Superposition

Click to edit the document details