In many Boussinesq formulations the velocity is used instead of the potential. Writing u=∂xϕu=∂xϕ the equations

with forcing in the velocity become equation(16) {∂tη=1g∂xC2u∂tu=−g∂xη+G3where C2=^−D/k2 is the squared phase velocity operator. By eliminating ηη the second order equation for u   is obtained ∂t2u=−Du+∂tG3This is the same as Eq. (15) for the uni-directional elevation influxing, and G  3 can be specified if the velocity at x  =0 is given, say u(0,t)=s3(t)u(0,t)=s3(t) G3=g(x)f(t)−(∂t−1f(t))A1g(x)withg^(K1(ω))fˇ(ω)=12πVg(K1(ω))sˇ3(ω) In this section the results of the previous R428 in vivo section are generalized to multi-directional waves in 2D in a straightforward way. The notation for the horizontal coordinates is x=(x,y)x=(x,y) and

for the wave vector k=(kx,ky)k=(kx,ky); the lengths of these vectors are written as x=|x|x=|x| and k=|k|=kx2+ky2 respectively. In 2D the spatial transform is η(x)=∫η^(k)eik.xdk,η^(k)=1(2π)2∫η(x)e−ik.xdxThe dispersion relation is the relation between the wave vector kk and the frequency ωω so that the plane waves expi(k.x−ωt) are physical solutions. In 2D a skew-symmetric operator AeAe will Afatinib supplier be defined for given direction vector ee to formulate first order dynamic equations that describe forward or backward wave propagation with respect to the vector ee. Forward propagating wave modes have a wave vector that lies in the positive half-space kk.e>0 while the wave vector of backward propagating modes lies in the negative half-space k.e<0k.e<0. First order in time equations for forward or backward

travelling waves is most useful for wave influxing in a specific part of a half plane, for instance when waves are generated in a hydrodynamic laboratory, Ribonucleotide reductase or when dealing with coastal waves from the deep ocean towards the shore. The embedded forcing in the first order equations will also help us to determine the forcings in second order in time multi-directional equations. The first order in time equations are obtained with an operator AeAe that is defined as the pseudo-differential operator that acts in Fourier space as multiplication as Ae=^iΩ2(k)withΩ2(k)=sign(k.e)Ω(k)As before ω2=Ω(k)2=D(k)ω2=Ω(k)2=D(k), but note that now k=|k|k=|k| in Ω(k)Ω(k) only takes nonnegative values. Since Ω2(k)=−Ω2(−k)Ω2(k)=−Ω2(−k) the operator AeAe is real and skew-symmetric. Observe that Ω2Ω2 has discontinuity along the direction e⊥e⊥ (perpendicular to ee). The 2D forward propagating dispersive wave equation is then given as equation(17) ∂tζ=−Aeζ∂tζ=−Aeζwhich has as basic solutions the plane waves expi(k.x−Ω2(k)t). Without restriction of generality we will take in the following e=(1,0)e=(1,0) so that Ω2(k)=sign(kx)Ω(k)Ω2(k)=sign(kx)Ω(k).