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  1. Period: the time it takes for two successive crests to pass a given point. Frequency: the number of waves passing a point in a given amount of time, usually expressed as waves per second. This is the inverse of the period. Speed: how fast the wave travels, or the distance traveled per unit of time.

  2. Calculate the wave velocity of the ocean wave in the previous figure if the distance between wave crests is 10.0 m and the time for a seagull to bob up and down is 5.00 s. Strategy The values for the wavelength ( λ = 10.0 m ) ( λ = 10.0 m ) and the period ( T = 5.00 s) ( T = 5.00 s) are given and we are asked to find v w v w Therefore, we can ...

  3. On an impervious boundary B (x; y; z; t) = 0, we have KBC: @Á * 3 ́ 3 ́ *v ¢ ^n = rÁ ¢ ^n = = U *x; t ¢ ^n *x; t = Un on B = 0 @n. Alternatively: a particle P on B remains on B, i.e. B is a material surface; e.g. if P is on B at. t = t0, i.e.

  4. Chapter 1 Basic waves To describe ocean waves, we use a right-handed, Cartesian coordinate system in which the z-axis points upward. The x- and y-axes point in horizontal directions at right angles. In the state of rest, the ocean surface coincides with z= 0. When waves are present, the surface is located at z= (x;y;t), where tis time. The ...

  5. 2.1 Equations of motion The phenomena to be modelled are short waves at the free surface between water and air. Here, short means that characteristic wave periods are small compared to the rotation period of the earth. Furthermore, baroclinic features (variation of internal density surfaces) are not essential.

  6. ocw.mit.edu › courses › 12-802-wave-motion-in-the-ocean-and-the-atmosphere-springEquations of Motion - MIT OpenCourseWare

    Thus the period average of the energy equation is: ∂t <E >+∇H •[G c g <E >]=0 Thus we have the important result that the energy in the wave propagates with the group velocity. If the medium is homogeneous, G c g = ∂ω ∂ k (| k |) only and we can write ∂ ∂t <E >+ G c g •∇H <E >=0

  7. WAVES IN WATER. 1 Governing equations for waves on the sea surface. In this chapter we shall model the water as an inviscid and incompressible fluid, and consider waves of infinitesimal amplitude so that the linearized approximation suffices.

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