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  1. The major parameters to describe sea state are the different peak periods (Tp composed of Tp1, Tp2, Tpw), the different mean periods (Tm composed of Tm02, Tm-10), the significant wave heights (Hs composed of Hs1, Hs2, Hsw) and the different peak directions (dp composed of dp1, dp2, dp3).

  2. 5 Φεβ 2005 · Design often requires only a synthesized description of the wave spectra by means of the three main integral wave parameters: significant wave height (H s), mean (zero-upcrossing) wave period (T m), and mean wave direction. Also, validations and comparisons of observations from different sources are often limited to these quantities.

  3. 16 Ιουν 2023 · The disturbance could mean the high and low parts of an ocean wave, or the high and low pressure parts of a sound wave, etc. Periodic means that the disturbance repeats. As an example, consider a graph of y = sin(x).

  4. c = wavelength x frequency. Therefore, the longer the wavelength, the faster the wave. Although waves can travel over great distances, the water itself shows little horizontal movement; it is the energy of the wave that is being transmitted, not the water.

  5. Tm01 = m0/m 1. Tm02 = sqrt(m0/m2) 📌 Note: Tm-10, Tm01 and Tm02 (spectral moment wave periods) correspond to the inverse of f-10, f01 and f02 (spectral moment wave frequencies). Each of these values could be computed on a part of the spectrum or on the whole spectrum.

  6. 16 Ιουλ 2024 · The wave is an up and down disturbance of the water surface. It causes a sea gull to move up and down in simple harmonic motion as the wave crests and troughs (peaks and valleys) pass under the bird. The time for one complete up and down motion is the wave’s period \(T\). The wave’s frequency is \(f=1 / T\), as usual.

  7. 19 Δεκ 2021 · The wave period \(T\) is the time the wave needs to pass the location, the inverse of which is the frequency \(f\), the number of waves passing a fixed location per unit time. When travelling in the ocean at a certain moment in time the wave can be seen as a similar sinusoidal variation of the water surface, see the left hand side of Fig. 3.1.

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