Semidiurnal tides in an atmosphere with mean wind and dissipation



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Edition Notes

Statementby Siu-Shung Hong.
Classifications
LC ClassificationsMicrofilm 51839 (Q)
The Physical Object
FormatMicroform
Paginationxiv, 180 leaves.
Number of Pages180
ID Numbers
Open LibraryOL2019560M
LC Control Number90954839

The global map of internal tide energy in Niwa and Hibiya () shows that the northwest Pacific Ocean (NWP, which ranges from 0° to 35°N and from ° to °E) is one of the most energetic regions with regard to both diurnal and semidiurnal baroclinic (BC) tides. With double-ridge topography and strong BT tides, the Luzon Strait (LS) is the most energetic source of internal tides and. semidiurnal zonal and meridional wind tides over a range of MLT altitudes (85– km) up to zonal wave number 4 [Oberheide et al., , , ]. Recently, Oberheide and Forbes [a] established the internal consistency of these tidal temperature and wind climatologies within the framework of the tidal theory. Their work was focused on. 1. Introduction. The diurnal solar forcing of the thin Martian atmosphere drives large-amplitude planetary-scale oscillations known as atmospheric thermal tides [Gierasch and Goody, ; Zurek, ; Leovy, ].These tides have been seen in lander records of daily varying surface pressure and near–surface winds [Hess et al., ; Leovy, ; Tillman, ; Murphy et al., Monthly simulations of the thermal diurnal and semidiurnal tides are compared to High-Resolution Doppler Imager (HRDI) and Wind Imaging Interferometer (WINDII) wind and temperature measurements on the Upper-Atmosphere Research Satellite (UARS). There is encouraging agreement between the observations and the linear global mechanistic tidal model results both for the diurnal and semidiurnal.

semidiurnal tide. Contour intervals are 10 m/s. Latitude-height cross-sections of amplitudes of zonal wind pertubations for diurnal and semidiurnal solar tides in July are shown in Fig. 2. These are two of the free global normal modes the atmosphere exhibits . Continuous radar measurements of the wind oscillations caused by the solar diurnal and semidiurnal tides in the 80 to km region of the atmosphere at the geographically conjugate stations of Adelaide (35 S, E) and Kyoto (35 N, E) are compared for the period to At the solstices it is found for both the and hr tides that the NS and EW oscillations tend to be in-phase. s = −1 cycles/sol denotes the westward‐moving diurnal tide, while the wave with s = 1 cycles/sol is the eastward‐moving diurnal tide. At an altitude of 10 km (Figure 2a), the diurnal (s = ±1) and semidiurnal (s = ±2) components are predominant. It is noteworthy that spectral peaks due to diurnal and semidiurnal tides having large zonal wave. Thermal tides and studies to tune the mechanistic tidal model using UARS observations V. A. Yudin1, B. V. Khattatov2, M. A. Geller1, D. A. Ortland3, C. McLandress4, G. G. Shepherd5 1 Institute for Terrestrial and Planetary Atmospheres, State University of New York at Stony Brook, Stony Brook, NY , USA 2 National Center for Atmospheric Research, Boulder, Colorado, P.O. Box , USA.

turbations from tides and planetary waves. Following, for example, Manson et al. (), in winter, westward propa-gating GWs predominate around the mesopause, the mean eastward winds lower down having filtered out the eastward propagating population. Increases in the GW-related wind variances then occur and maximize when the tide perturba-. Internal tides are generated as the surface tides move stratified water up and down sloping topography, which produces a wave in the ocean interior. So internal tides are internal waves at a tidal frequency. The other major source of internal waves is the wind which . sources of the diurnal tide (and to a lesser extent the semidiurnal tide) in the mesosphere and lower thermosphere (MLT) region are those excited in the troposphere and propagated up to the middle and upper atmosphere, includ-JOURNAL OF GEOPHYSICAL RESEARCH, VOL. , NO. 0, /JD,

Semidiurnal tides in an atmosphere with mean wind and dissipation Download PDF EPUB FB2

Diurnal and semidiurnal solar thermal tides play an important role in determining the mean circulation and thermal structure of terrestrial planetary atmospheres (Venus, Earth, and Mars), in addition to their more obvious contributions to variability about the zonal mean state (see review by Forbes ).In Earth's atmosphere, solar tides begin to dominate flow patterns above about 80 by: atmospheric tides on Earth are mainly relevant in the upper atmosphere, on Mars, they dominate temperature variations and winds throughout the atmosphere.

Observations and model simulations to date have suggested that the migrating diurnal tide is the predominant mode in the Martian atmosphere, and that the semidiurnal tide is only relevant inCited by: The Q factor is around 23 for semidiurnal tides so that the dissipation (or alternatively renewal) timescale for these tides is around 2 days.

On the other hand, the Q factor is smaller, about 13 for diurnal tides, with a corresponding dissipation timescale of 2 days also. It is about for Mf, and hence the dissipation timescale is days. Vertical coupling due to the solar semidiurnal tide in Mars's atmosphere, and effects on zonal mean temperature and wind structures, are investigated using a numerical model.

The model provides self-consistent solutions to the coupled zonal mean and tidal equations from the surface to km. Breaking (convective instability) of the semidiurnal tide is parameterized using a linear saturation. Forbes, J. and Hagan, M. () Diurnal propagating tide in the presence of mean winds and dissipation: a numerical investigation.

Planet. Space Sei. 36, Cited by: The results for the mean wind are compared with the Horizontal neutral wind model (HWM), and the results for atmospheric tides are compared with the Global Scale Wave Model (GSWM Climatology of upward propagating diurnal and semidiurnal tides in the thermosphere dynamo electric fields by nonmigrating zonal wind tides [Hagan et al., ; Jin et al., ] although there is thermal atmosphere without mean winds and dissipation.

[tides. [phases are reconstructed as function of latitude, altitude and. Horizontal wind observations over four years from the meteor radar at Esrange (68˚N) are analyzed to determine the variability of the semidiurnal tide. Simultaneous global observations of temperature and geopotential from the SABER satellite instrument are used to construct time series of planetary wave amplitudes and geostrophic mean zonal wind.

middle atmosphere is considered: non-linear interaction between stationary planetary waves and migrating tides, heating due to absorption of solar radiation by ozone distributed in longitude. The vertical propagation of tides is controlled by the background wind.

Due to interactions between the tidal components and the zonal mean wind, they. By atmospheric tides we generally mean those planetary scale oscilla­ tions whose periods are integral fractions Semidiurnal tides in an atmosphere with mean wind and dissipation book a solar or lunar day (diurnal refers to a period of one day, semidiurnal refers to a period of half a day, and terdiurnal refers to a period of one third of a day).

These periods are chosen. We derive the polarization relationships of tides from the primitive equations for perturbations of a dissipation-less atmosphere. The vertical wind tide is found to relate directly to temperature tide, independent of tidal structure and geometric location.

In Section 4 we present diurnal and semidiurnal tides in temperature, zonal wind and. gravitational pull of the Sun. The solar semidiurnal tides are the subset of waves with hour periods that are further characterized by the number of perturbation maxima or minima along a latitude circle, that is, the zonal wave number.

By definition, the migrating semidiurnal tide prop-agates with the apparent motion of the Sun when observed. wind diurnal (Figure 1a) and semidiurnal (Figure 1b) tides for UT days –, centered at UT, along with the rnalamplitudesondays– and are typical, enerally the same as the 9-day mean amplitude, but with more wavy patterns.

The zonal wind diurnal amplitude above 85 km dramatically increased. Figures 3a and 3b show the mean zonal-wind tides at 52°N for July and January after averaging the tides at the same local time over all longitudes. There is a predominant diurnal tide in the stratosphere and lower mesosphere, whereas a semidiurnal tide develops above about hPa (~70 km).

Hamilton () and Zurek () first demonstrated that dissipation of tides could significantly affect the mean wind and thermal structure of Mars' middle atmosphere. A recent illustration of this effect in Fig. 5 is provided by the intense (∼50– ms −1) mean westward jet in the LMD Mars GCM at altitudes 50–90 km over the equator which is especially intense around the equinoxes.

The Orbiter Infrared Radiometer experiment, aboard the Pioneer Venus mission, produced strong evidence for the existence of a semidiurnal solar tide in the mesosphere of Venus 1.

At the same time, measurements in situ of radiative fluxes and cloud particle distribution, in other Pioneer Venus experiments, have provided much information about the structure of the solar heating and infared. Mean wind and dissipation mechanisms are not considered. The present tidal model reveals that the diurnal amplitude peaks in mid to low latitudes, whereas semidiurnal component is stronger at higher latitudes.

The semidiurnal tide is about an order of magnitude weaker than the diurnal tide. Also, semidiurnal wave has longer vertical. where u, v are the zonal and meridional wind measurements, u 0, v 0 are the mean zonal and meridional winds, and represent the zonal and meridional tidal component's corresponding amplitudes and phases, T i is the period for each considered tide (solar diurnal, solar semidiurnal, solar terdiurnal, and lunar semidiurnal; i.e., T 1 = 24 h, T 2.

We discuss the variable mean wind results in light of previous analytic attempts to describe the diurnal tide in the presence of mean winds and dissipation. Our calculations do not explain the interannual tidal variations observed by the High Resolution Doppler Interferometer (HRDI) on the Upper Atmosphere Research Satellite (UARS).

The former deals with how energy input by the atmosphere, principally via wind stress, and by tides, lunar and solar, flows through the ocean. Energy moves in space, from one place to another, and in length and time scales, until ultimate dissipation by molecular viscosity and diffusivity in patches of intense centimeter-scale gradients.

locally enhanced dissipation rates following internal waves of tidal frequency emanating from steep topography occur (Lueck and Mudge, ; Carter et al., ), meaning that momentum transfer from semidiurnal waves to subinertial ow may be signi cant near internal tide generation sites in gen-eral.

The climatology of mean wind, diurnal and semidiurnal tide during the first year () of simultaneous wind observations at Wakkanai (°N, °E) and Yamagawa (°N, °E) is. General characteristics. The largest-amplitude atmospheric tides are mostly generated in the troposphere and stratosphere when the atmosphere is periodically heated, as water vapor and ozone absorb solar radiation during the day.

These tides propagate away from the source regions and ascend into the mesosphere and heric tides can be measured as regular fluctuations in wind. importance in the composite semidiurnal tide during different seasons, we use the lidar-observed monthly mean temperature and zonal wind from the same data set as well as HAMMONIA output to calculate the vertical wave number seasonal variations of the major tidal modes of the migrating semidiurnal tide.

This leads to a qualitative. tion model with a zonal mean flow and zonal wavenumbers 1 and 2 (10). These waves correspond to the diurnal and semi-diurnal tides, but they can also be excited by barotropic or baroclinic instability.

Wavesofhigherwavenumbers andinterac-tions between the waves are neglected; these terms maynot be insignificant. Sym-metry about the equator is. The main physical processes affecting the propagation of tides from the lower to the middle and upper atmosphere are examined along with existing models used to simulate tidal propagation.

Theoretical work is presented which quantifies the effects of mean winds and dissipation on the diurnal propagating tide in the mesosphere and lower thermosphere. In addition, a method is proposed whereby. Depth-integrated dissipation is 3 times greater toward the end of the record, reaching 60 mW m −2 during the last spring tide.

Dissipation near a submarine ridge is strongly tidally modulated, reaching 10 −5 W kg −1 (10–m overturns) during spring tide and appears to be due to breaking lee waves. However, the phasing of the breaking.

CiteSeerX - Document Details (Isaac Councill, Lee Giles, Pradeep Teregowda): Abstract. Monthly simulations of the thermal diurnal and semidiurnal tides are compared to High-Resolution Doppler Imager (HRDI) and Wind Imaging Interferometer (WINDII) wind and temperature measurements on the Upper-Atmosphere Research Satellite (UARS).

There is encouraging agreement between the. They are however only predictions, the actual time and height of the tide is affected by wind and atmospheric pressure. Many shorelines experience semi-diurnal tides—two nearly equal high and low tides each day.

Other locations have a diurnal tide—one high and low tide each day. A "mixed tide"—two uneven magnitude tides a day—is a third regular category. Mean profiles of the turbulent dissipation rate ε and the PDF of log(ε) for both series of casts are shown in Fig.

There is evidence for intensified dissipation during the spring tide, as highlighted by the spring tide PDF of log(ε) being skewed toward higher values compared to the neap tide PDF. About Cookies, including instructions on how to turn off cookies if you wish to do so.

By continuing to browse this site you agree to us using cookies as described in About Cookies. Remove maintenance message.Energetics of semidiurnal barotropic and internal tides in the Bay of Bengal (BoB) and Andaman Sea (AS) are studied using the simulations from a high-resolution ocean general circulation model.Semidiurnal tidal features have been examined in the Mesosphere and Lower Thermosphere (MLT) from the long-term (–) meteor wind data over Maui (°N, °W).