Blood Moon, semi permanent hair dye red - 118 ml - Lunar Tides

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Migrating solar tides [ edit ] Figure 1. Tidal temperature and wind perturbations at 100 km altitude for September 2005 as a function of universal time. The animation is based upon observations from the SABER and TIDI instruments on board the TIMED satellite. It shows the superposition of the most important diurnal and semidiurnal tidal components (migrating and nonmigrating). s {\displaystyle s} and frequency σ {\displaystyle \sigma } . Zonal wavenumber s {\displaystyle s} is a positive

Solar energy is absorbed throughout the atmosphere some of the most significant in this context are [ clarification needed] water vapor at about 0–15km in the troposphere, ozone at about 30–60km in the stratosphere and molecular oxygen and molecular nitrogen at about 120–170km) in the thermosphere. Variations in the global distribution and density of these species result in changes in the amplitude of the solar tides. The tides are also affected by the environment through which they travel. Atmospheric tides are global-scale periodic oscillations of the atmosphere. In many ways they are analogous to ocean tides. Atmospheric tides can be excited by: The reason for this dramatic growth in amplitude from tiny fluctuations near the ground to oscillations that dominate the motion of the mesosphere lies in the fact that the density of the atmosphere decreases with increasing height. As tides or waves propagate upwards, they move into regions of lower and lower density. If the tide or wave is not dissipating, then its kinetic energy density must be conserved. Since the density is decreasing, the amplitude of the tide or wave increases correspondingly so that energy is conserved. Atmospheric tides are also produced through the gravitational effects of the Moon. [4] Lunar (gravitational) tides are much weaker than solar thermal tides and are generated by the motion of the Earth's oceans (caused by the Moon) and to a lesser extent the effect of the Moon's gravitational attraction on the atmosphere. Its maximum pressure amplitude on the ground is about 60 Pa. [5] The largest solar semidiurnal wave is mode (2, 2) with maximum pressure amplitudes at the ground of 120 Pa. It is an internal class 1 wave. Its amplitude increases exponentially with altitude. Although its solar excitation is half of that of mode (1, −2), its amplitude on the ground is larger by a factor of two. This indicates the effect of suppression of external waves, in this case by a factor of four. [9] Vertical structure equation [ edit ]The set of equations can be solved for atmospheric tides, i.e., longitudinally propagating waves of zonal wavenumber The basic characteristics of the atmospheric tides are described by the classical tidal theory. [5] By neglecting mechanical forcing and dissipation, the classical tidal theory assumes that atmospheric wave motions can be considered as linear perturbations of an initially motionless zonal mean state that is horizontally stratified and isothermal. The two major results of the classical theory are Migrating tides are Sun synchronous – from the point of view of a stationary observer on the ground they propagate westwards with the apparent motion of the Sun. As the migrating tides stay fixed relative to the Sun a pattern of excitation is formed that is also fixed relative to the Sun. Changes in the tide observed from a stationary viewpoint on the Earth's surface are caused by the rotation of the Earth with respect to this fixed pattern. Seasonal variations of the tides also occur as the Earth tilts relative to the Sun and so relative to the pattern of excitation. [1] Hence, atmospheric tides are eigenoscillations ( eigenmodes)of Earth's atmosphere with eigenfunctions Θ n {\displaystyle \Theta _{n}} , called Hough functions, and eigenvalues ε n {\displaystyle \varepsilon _{n}} . The latter define the equivalent depth h n {\displaystyle h_{n}} which couples the latitudinal structure of the tides with their vertical structure. The primary source for the 24-hr tide is in the lower atmosphere where surface effects are important. This is reflected in a relatively large non-migrating component seen in longitudinal differences in tidal amplitudes. Largest amplitudes have been observed over South America, Africa and Australia. [3] Lunar atmospheric tides [ edit ]

At ground level, atmospheric tides can be detected as regular but small oscillations in surface pressure with periods of 24 and 12 hours. However, at greater heights, the amplitudes of the tides can become very large. In the mesosphere (heights of about 50–100km (30–60mi; 200,000–300,000ft)) atmospheric tides can reach amplitudes of more than 50m/s and are often the most significant part of the motion of the atmosphere. Figure 3. Pressure amplitudes vs. latitude of the Hough functions of the diurnal tide ( s = 1; ν = −1) (left) and of the semidiurnal tides ( s = 2; ν = −2) (right) on the northern hemisphere. Solid curves: symmetric waves; dashed curves: antisymmetric wavesa cos ⁡ φ ( ∂ u ′ ∂ λ + ∂ ∂ φ ( v ′ cos ⁡ φ ) ) + 1 ϱ o ∂ ∂ z ( ϱ o w ′ ) = 0 {\displaystyle {\frac {1}{a\,\cos \varphi }}\,\left({\frac {\partial u'}{\partial \lambda }}\,+\,{\frac {\partial }{\partial \varphi }}(v'\,\cos \varphi )\right)\,+\,{\frac {1}{\varrho _{o}}}\,{\frac {\partial }{\partial z}}(\varrho _{o}w')=0} Atmospheric tides propagate in an atmosphere where density varies significantly with height. A consequence of this is that their amplitudes naturally increase exponentially as the tide ascends into progressively more rarefied regions of the atmosphere (for an explanation of this phenomenon, see below). In contrast, the density of the oceans varies only slightly with depth and so there the tides do not necessarily vary in amplitude with depth. Longuet-Higgins [8] has completely solved Laplace's equations and has discovered tidal modes with negative eigenvalues ε s Following this growth with height atmospheric tides have much larger amplitudes in the middle and upper atmosphere than they do at ground level.