Global Dynamics of the MLT
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The transition between the middle atmosphere and the thermosphere is known as the MLT region (for mesosphere and lower thermosphere). This area has some characteristics that set it apart from other regions of the atmosphere. Most notably, it is the altitude region with the lowest overall temperature and has the unique characteristic that the temperature is much lower in summer than in winter. The summer-to-winter-temperature gradient is the result of adiabatic cooling and warming associated with a vigorous circulation driven primarily by gravity waves. Tides and planetary waves also contribute to the circulation and to the large dynamical variability in the MLT. The past decade has seen much progress in describing and understanding the dynamics of the MLT and the interactions of dynamics with chemistry and radiation. This review describes recent observations and numerical modeling as they relate to understanding the dynamical processes that control the MLT and its variability. Results from the Whole Atmosphere Community Climate Model (WACCM), which is a comprehensive high-top general circulation model with interactive chemistry, are used to illustrate the dynamical processes. Selected observations from the Sounding the Atmosphere with Broadband Emission Radiometry (SABER) instrument are shown for comparison. WACCM simulations of MLT dynamics have some differences with observations. These differences and other questions and discrepancies described in recent papers point to a number of ongoing uncertainties about the MLT dynamical system.
KeywordsMesopause Gravity waves Tides WACCM SABER
The region of transition from the middle atmosphere to the thermosphere is known as the MLT (mesosphere and lower thermosphere). This region exhibits a balance of processes not seen elsewhere in the atmosphere and is often treated as a separate region. Much has been learned about the MLT in recent years through additional observations and improved numerical modeling capabilities. This survey will describe the dynamics of the MLT, with emphasis on recent developments and ongoing questions.
The concepts will be illustrated primarily with the results from simulations made with the Whole Atmosphere Community Climate Model (WACCM). WACCM is a component of the Community Earth System Model, a family of model components at the National Center for Atmospheric Research (NCAR). WACCM is a comprehensive global climate model that extends from the Earth’s surface into the lower thermosphere. It includes interactive chemistry with realistic surface concentrations and trends of natural and anthropogenic trace gases. External forcing by solar variability and energetic particle fluxes is also included. Model results shown here are from extended integrations using WACCM version 3.5. This version does not include interactions between the atmosphere and the oceans; instead, sea surface temperatures are specified using observations from recent decades. Descriptions of the formulation of dynamics and the external forcing in WACCM version 3.5 are given by Garcia et al. (2007), Marsh et al. (2007), Richter et al. (2010), and Smith et al. (2011). Extensive comparisons of WACCM with other models are presented by Eyring et al. (2006) and WMO (2010). There is also an extended version of the model, WACCM-X, that has an upper boundary at 2.5 × 10−9 hPa (∼500 km altitude) (Liu et al. 2010).
The topics covered in this paper are the characteristics of the large-scale winds and temperatures, the balances that maintain the basic state, the description of waves and their interactions, the dynamical coupling between the MLT and the rest of the middle atmosphere, and the response of the MLT dynamical environment to external forcing by anthropogenic composition changes and solar variability. Companion papers by Feofilov and Kutepov (2012) and Sinnhuber (2012) discuss the MLT radiative balance and the response of MLT chemistry to energetic particles, respectively. Although this paper gives many references for observational and theoretical studies, the reference list is not comprehensive. The topics discussed and the interpretation reflect the interests and experience of the author.
For other reviews of MLT dynamics, see Shepherd (2000), Becker (2011), and Smith (2011). Shepherd (2000) addresses the development of our understanding of some key phenomena in the stratosphere and mesosphere since the middle of the twentieth century. Becker (2011) focusses particularly on the mean circulation and the processes that control it. Smith (2011) reviews the processes involved in the interactions between the lower, middle, and upper atmosphere. A review of whole atmosphere models by Akmaev (2011) also discusses current understanding of the role of the MLT in coupling between atmospheric regions.
2 Measurements and Their Limitations
Measurements of the MLT dynamical conditions have been made remotely using ground- and space-based instrumentation and in situ using rockets. None of the instrumentation can give a complete picture, but together they provide a more rounded picture of the basic state and its variations than is possible with any single measurement technique. Ground-based and rocket-borne instruments have limited geographic extent but can provide high vertical resolution. Continuous ground-based observations give a great deal of information about local time variations. Satellite instruments provide a global or near-global picture but have limited local time sampling, and many also have limited spatial resolution. The primary dynamical fields that can be determined from measurements are kinetic temperature, neutral density, vectors of horizontal winds, and small-scale perturbations to airglow emissions caused by waves. Specialized measurements such as turbulence have also been taken.
Passive ground-based observations use light emitted in the MLT to deduce properties of the atmosphere. The light sources used are various airglow emissions which, depending on the chemical processes that produce the light, come from different altitudes. OH Meinel emissions, which originate in a layer near 87 km, are used to deduce temperature and details of the evolution of small-scale waves. Other emissions used are the O2 atmospheric band (91–95 km), the sodium D line (∼90 km), and the oxygen green line (95–100 km). These measurements are limited to nighttime and sky conditions that are clear or have a light overcast. Visible observations of polar mesospheric clouds in high-latitude summer provide a limited duration but striking method of observing waves in the MLT.
Temperature (e.g., Taylor et al. 1999) and wave properties (e.g., Takahashi et al. 2002; Hecht 2004; Simkhada et al. 2009) can be determined from OH nightglow emissions. There is an element of uncertainty because the dynamical perturbations that change the temperature also affect the altitude of the emitting layer, which can move up or down by several kilometers due, for example, to displacement by tides. Long records of measurement of temperature from ground-based OH emissions (Bittner et al. 2002; French and Mulligan 2010; French and Klekociuk 2011) are useful in determining long-term trends (see Sect. 7) There has also been effort to use two or more different types of ground-based instruments at the same site for additional insight into the dynamics (Ejiri et al. 2009; Taori et al. 2011).
Active ground-based observations are made by radar and lidar. Two types of radar are commonly used for winds in the MLT. Meteor radars use the reflection of radio wave pulses by meteor trails (e.g., Mitchell et al. 2002), and medium frequency (MF) radars use reflections by changes in the refractive index in the clear atmosphere (e.g., Vincent et al. 1998). With two or more beams tilted from the vertical, radar signals can be processed to yield horizontal vector winds. Many radar stations operate unattended 24 h per day and are therefore able to give a continuous record that can be used to determine tides, gravity waves, and other high-frequency variations. Density variations detected by lidar can be used to determine temperature. Some lidars also measure horizontal winds (e.g., Baumgarten 2010). Early lidars operated only during night but, with improved technology, some instruments can operate during day as well (She et al. 2002). Their data coverage is less complete than for radar because no signal is obtained under cloudy conditions and also because the instruments are not fully automated. In a comparison of winds from co-located lidar and meteor radar, Franke et al. (2005) found good agreement; they concluded that most of the root-mean-square difference in the radar and lidar winds could be explained by the much higher vertical resolution of the lidar measurements.
Although the network of ground-based stations that observe mesospheric dynamical processes has increased, it is still not sufficient to provide a detailed global view. One major impediment to achieving this is that land covers less than half of the surface of the globe. In addition, some sites over land are not accessible to lidar or passive optical techniques because of persistent cloud cover. Construction of a regional or global climatology by combining data from different ground-based instruments also has to take into account the bias between instruments.
Probing the MLT region by rockets has been performed intermittently. These measurements are most valuable when made as part of organized campaigns with multiple measurements. Rocket soundings are the only technique for in situ sampling on the MLT. Measurements from rockets have another advantage over other techniques that it is possible to achieve very high verticle resolution. As discussed by Lübken (1997), density fluctuation over distances of a few meters allows the determination of turbulent energy dissipation rates. Rockets have also been used in active experiments in which a plume of substance, such as a chemical that fluoresces or bits of reflecting material that leave a visible trail, is released and observed from the ground. Due to the expense, contributions to MLT observations from rocket-borne experiments have been a decreasing part of the available database in recent decades.
Satellite instrumentation for dynamical variables has improved as instrument design has evolved to take advantage of improving sensors and other technology. However, the high cost and long development time strongly limit the number of instruments in orbit. Passive satellite measurements of the MLT rely either on emissions from the radiatively active trace chemical species or on modifications to the light from the sun or other stars as it passes through the atmosphere. Infrared emissions from CO2 are used to determine temperature. Information about temperature can also be deduced from polar mesospheric clouds (PMC) since these clouds only form when the temperature is extremely low. Airglow emissions provide additional information about temperature and also, through Doppler shift, about horizontal winds in the line of sight. Profiles extending over broad vertical depth provide information about dynamical coupling between atmospheric layers.
Limb scanning is used in many satellite observations because of the potential for good vertical resolution (a few km). Data sets that have provided important information about MLT dynamics come from the Solar Mesosphere Explorer (SME), the Upper Atmosphere Research Satellite (UARS; 1991–2005), the Thermosphere Ionosphere Mesosphere Energetics and Dynamics satellite (TIMED; 2002–ongoing), the Envisat satellite (2002–ongoing), and the Cryogenic Infrared Spectrometers and Telescopes for the Atmosphere (CRISTA; November 1994; August 1997) missions. A major gap in information about the dynamics of the MLT could be approaching since TIMED and Envisat are already beyond their original design lifetimes. Successors for these aging but highly successful satellites are not currently under construction.
The term climatology refers to multiyear averages and their seasonal variations. The climatology is useful for predicting general conditions to be seen at a particular location and time of year.
A long-time and well-used reference for the climatology in the mesosphere is the MSIS (mass spectrometer incoherent scatter) empirical model (Hedin 1991). The most recent version is known as NRLMSIS-00 (Picone et al. 2002). Because additional new satellite observations have been accumulating at a rapid rate since this was released in 2000, the MSIS description does not capture many details about the MLT dynamics, composition, and variability. The empirical model used for NRLMSIS-00 includes parameters to represent the changes with season, solar cycle, and geomagnetic activity. The related Horizontal Wind Model (HWM07) gives horizontal wind climatological fields (Drob et al. 2008). The HWM07 includes seasonal and local time variations due to planetary waves and tides during solar quiet times. There is also an option (DWM07) (Emmert et al. 2008) for the upper thermosphere during solar active periods.
The MLT climatology has been evolving in part due to new observations but also because the climate is itself not fixed. The state of the MLT region exhibits year-to-year variations and trends in response to changing external forcing and changing atmospheric composition. The most important sources of trends and interannual variability are due to the anthropogenic changes in atmospheric composition, changes in the energy input from above (ultraviolet radiation from the Sun and energetic particles from the outer parts of the Earth system), and changes in the wave forcing from below. These are discussed in Sect. 7.
The climatological state of the MLT cannot be completely characterized due to the relatively short duration of most measurement records and to the large variability. As of now, there is not enough information to determine definitively how much of the variability is internal and how much is externally forced. In general, the regions below (i.e., the troposphere and stratosphere) have a more important impact on the MLT than vice versa (e.g., Liu et al. 2009). MLT variations forced from below are often considered to be externally forced.
In the lower atmosphere and in much of the middle atmosphere, the basic dynamics varies more with latitude and altitude than with longitude. The latitude × pressure or latitude × altitude view is considered to be the background basic state. Despite some very large amplitude waves in the MLT, particularly diurnal tides, the 2-D view is nevertheless a useful framework to examine seasonal and interannual evolution of the MLT dynamics. This section describes the basic state averaged in longitude and in local time. The important wave processes are described in Sect. 4
3.1 Zonal Mean Temperature and Winds
The simulated average January and July temperatures from the WACCM model are shown in the lower panels of Fig. 1. See Garcia et al. (2007) and Richter et al. (2010) for some discussions of the WACCM simulations. There are a number of differences between the model and the observed temperature. One obvious difference is the temperature at the mesopause. SABER observations indicate that there is a pole-to-pole extension of low temperature around 95–100 km that is seen at both solstice seasons. This low temperature has been seen in other observations as well (e.g., von Zahn et al. 1996).
The mesopause is defined as the coldest point in the vertical profile. In the winter hemisphere and in low latitudes during all seasons, the daily mean altitude of the mesopause is near 100 km (Fig. 1). However, in the summer high latitudes, the mesopause temperature is much lower, and its altitude is lower (von Zahn et al. 1996; Xu et al. 2007a). The global low temperature at 95–100 km is due to the radiative balance there. As elsewhere in the middle atmosphere, CO2 radiative transfer cools the MLT (Fomichev 2009; Feofilov and Kutepov 2012). The primary energy for heating in the MLT is absorption of solar energy by O2. The link between absorption of energy and heating is complex in the MLT due to the loss of energy due to airglow emissions (Mlynczak and Solomon 1993) and the slow rate at which the energy of photolysis is eventually converted to heat. The low temperature is a result of the balance between the weak heating and the efficient radiation to space by CO2. It is evident from Fig. 1 that the energy balance at 100 km simulated by WACCM has significant discrepancies from the SABER observations.
Another source of global heating and cooling is due to dissipating gravity waves and their interaction with the background atmosphere. See Sect. 4 for a brief discussion of the role of gravity wave heating. This contribution is very uncertain because of the lack of comprehensive observations. There are also different estimates of the net heating from different theoretical studies (e.g., Medvedev and Klaasen 2003; Becker 2004).
Leovy (1964) showed that the cold summer mesopause must be maintained by dynamical motion. The adiabatic cooling associated with strong rising motion is necessary to cool this region to temperatures well below the photochemical equilibrium conditions. Since the work of Lindzen (1981) and Holton (1983), the role of gravity wave propagation and dissipation has been accepted as the dominant wave forcing. Although new details have come to light with improved measurements, the basic explanation for the cold summer mesopause is still accepted. Recent developments have given a better description of the circulation with the help of numerical models (see Sect. 3.2) and have allowed a characterization of the differences between the two hemispheres (see Sect. 6.2)
Horizontal winds in the MLT are highly variable. Radar measurements show a very broad spectrum of variations from the annual timescale to short periods that are limited by the instrumental averaging time. Rapid movement of wave-like perturbations can be seen in airglow images. Many of the observed variations are due to propagating waves. Sections 4.1 and 4.3 discuss two of the most important classes of waves: mesoscale gravity waves and tides. Averaging radar data over time, for example taking a monthly average, gives the time-mean wind and, using the assumption that the longitudinal variations of the time-mean fields are small, an estimate of the zonally averaged wind (Mitchell et al. 2002). Satellite observations (Smith 1997; Wang et al. 2000) show that there are planetary-scale variations in the monthly averaged horizontal winds in the MLT. Because of these persistent longitude variations, the time-mean wind at a radar site is likely to differ from the true zonal mean wind.
Multi-year observations from radar measurements in middle and high latitudes (e.g., Dowdy et al. 2007; Hoffmann et al. 2011) indicate that the summer zonal wind changes sign from easterly (from the east) to westerly around 90–95 km. The average winds during winter are westerly and do not change to easterly within the measurement range of the radars (up to 95–100 km). Although there are satellite observations of horizontal winds, some uncertainty remains because of the difficulty of determining the position on the detector that corresponds to zero wind (Burrage et al. 1993). More than a decade of satellite winds are available from the High-Resolution Doppler Imager (HRDI) on the Upper Atmosphere Research Satellite (UARS) and from the Wind Imaging Interferometer (WINDII) on the same satellite. McLandress et al. (1996) presented near-global MLT zonal winds from a combination of HRDI and WINDII data. The zonal wind climatology from WINDII has been updated by Zhang et al. (2007). Zonally averaged zonal and meridional winds from the TIDI instrument on the TIMED satellite have recently become available (Niciejewski et al. 2011).
The HRDI winds for the period 1991–1998 have been collected by the UARS Reference Atmosphere Project (URAP) and are combined with stratospheric winds from assimilation of meteorological data (Swinbank and Ortland 2003). The monthly URAP winds are available as a climatology. In middle latitudes during the solstice periods, the winds are easterly in the summer hemisphere and westerly in the winter hemisphere. Individual wind profiles can be quite variable and, during dynamically active periods, the entire structure can be changed in the winter hemisphere (see Sect. 5.1)
Observations (e.g., Huang et al. 2006; Xu et al. 2007a) also indicate that there is an interannual variation in the zonally averaged temperature in the MLT that is related to the quasi-biennial oscillation (QBO) in tropical lower stratospheric winds and temperature. The driving mechanism for this may be the same as that for the SAO in the MLT, see Sect. 4.1.3. In a study using several decades of data, Ratnam et al. (2008) showed that the relationship between the stratospheric and mesospheric QBO in winds varies with time. However, some of the data they analyzed for this study have limited local time coverage so the analysis results could include aliasing from the diurnal tide, which itself has a substantial QBO variation in amplitude (see Sect. 4.3.1)
3.2 Mean Meridional Circulation
The temperature structure during solstice periods (Fig. 1) is consistent with net upwelling near the summer pole (adiabatic cooling is responsible for the low temperatures) and sinking near the winter pole. However, details of the circulation are difficult to measure directly. For this, we rely on numerical models that include the radiative forcing as well as the dynamical forcing. Throughout the middle atmosphere, the large-scale motion is driven by waves (Andrews et al. 1987).
In principle, the mean atmospheric circulation for monthly or longer time periods can be diagnosed from the diabatic heating (see discussion of the diabatic circulation by Dunkerton 1978). In practice, it is difficult to determine the diabatic heating because the concentrations of radiatively active gases are not well known due to high variability, including rapid diurnal changes, and also because radiative transfer is complex in the MLT because the CO2 emissions responsible for most of the cooling are not in local thermodynamic equilibrium (LTE; see Feofilov and Kutepov 2012). Lieberman et al. (2000) derived the diabatic circulation using temperature measurements from HRDI. The calculated meridional winds did not show consistent agreement with either the meridional winds measured by HRDI or with time average winds measured by radar at several latitudes.
There are indirect ways of verifying that the basic circulation estimated from theory and numerical models is reasonable. First and foremost is the simulation of the temperature structure, particularly the horizontal structure such as the cold summer and warm winter mesopause. As seen by comparing WACCM temperatures with SABER observations (Fig. 1), the qualitative agreement in temperature is good. For example, in both cases, the summer minimum temperatures in both hemispheres are 120–130 K. This implies that the transformed Eulerian mean circulation simulated in WACCM (Fig. 4) is realistic. However, the altitudes of the summer temperature minima are slightly lower in WACCM than in the SABER observations. Another discrepancy is the penetration of warm air to higher altitude in the SH winter (June–July) in WACCM. Since the transformed Eulerian mean circulation is a wave-driven flow, the discrepancies imply that the magnitude or vertical distribution of the wave momentum or energy deposition in WACCM is not completely accurate. The dominant wave process causing the low temperatures in the summer mesopause is forcing by gravity wave dissipation and breaking, which is parameterized in WACCM. Comparisons of the global mean temperatures suggest that the heating due to gravity wave processes may contribute to the discrepancy between the model and the SABER-observed temperature.
Additional validation of the strength and direction of the circulation comes from the simulation of trace species that are affected by transport. As shown by Smith et al. (2011), comparison of the WACCM simulation of the distributions of water and atomic oxygen with observations suggests that the poleward branch of the circulation in NH winter occurs at an altitude that is too low by a few kilometers. Since the circulation is driven primarily by momentum forcing introduced into the model by the gravity wave parameterization, this suggests that the parameterization needs to be modified. There are several parameters that are poorly constrained by observations. These were adjusted to give a good overall representation of the winds and temperature in the entire middle atmosphere. Since each single parameter affects the simulation in all seasons, latitudes and over a broad vertical range, perfect agreement of the simulations with observations is not feasible. Gravity wave parameterizations in numerical models are discussed further in Sect. 4.1
For direct comparison of WACCM simulations with observations in the past decade, the model is run in specified dynamics mode, known as SD-WACCM. In this mode, key tropospheric and stratospheric dynamical variables are constrained by meteorological analyses from weather prediction models that assimilate observations. Marsh (2011) used this version of the model to examine dynamical and chemical evolution during the 2005–2006 NH winter. He found that the evolution of events during this highly active period (see Sect. 5.1) closely followed the observations, even in the upper levels where no constraints were placed on the model. This gives support for the model dynamics in the mesosphere and for the reliability of the mean circulation derived from WACCM. Additional evidence comes from model experiments to investigate chaotic growth of errors using WACCM. Liu et al. (2009) showed that the error growth in the MLT is much reduced when the lower atmosphere is constrained by reinitializing daily.
In general, the term wave is used for a disturbance that propagates in space and time. Three features of waves are important: generation, propagation, and dissipation. The generation will receive less attention in this paper because the bulk of the wave activity in the MLT originates below, in the troposphere or stratosphere. However, secondary waves that are created by the interactions of waves can be generated anywhere in the system, including in the MLT.
Waves will not interact with the background atmosphere unless they are transient or dissipating. This noninteraction theorem, described by Andrews and McIntyre (1976), applies to Rossby waves, gravity waves, and tides. For all of these waves, the propagation conditions depend on characteristics of the wave and also on the background through which the wave propagates. The background zonal wind is particularly important because of its high speed and large seasonal (Fig. 2) and year-to-year variations.
Another concept that is useful for understanding wave behavior is that of critical layer (also called critical level). This is a point in the atmosphere where the phase speed of a wave is equal to the speed of the background wind. Waves cannot propagate through this region; they will be dissipated or, in some circumstances, reflected. The critical layer concept is most useful for predicting the propagation of gravity waves and planetary waves because they have phase speeds whose magnitudes are within the range of middle atmosphere zonal and meridional winds.
4.1 Gravity Waves and Their Forcing of the Background Atmosphere
Although gravity waves are interesting in their own right and have been much studied, the focus of this section is on the impact of gravity waves on the large-scale dynamics of the MLT. For more about the gravity waves themselves, see the review by Fritts and Alexander (2003).
It is now widely accepted that gravity waves provide the bulk of the momentum forcing that drives the circulation in the MLT. This circulation is responsible for the cold summer mesopause and for much of the vertical transport of trace species (Sect. 3.2). This is not a one-way interaction. The generation, propagation, and dissipation of gravity waves depend on the winds and thermal structure of the surrounding environment. Gravity waves present a particular challenge for observations and numerical modeling because the scale of individual waves can be small (tens of km), whereas their cumulative impact is global.
Observations of gravity wave winds and/or temperatures are made by radars, lidars, and airglow imagers. The wave periods that can be seen are constrained on the short end by the time needed to make a measurement and on the long end by the instrument operation and the need to separate the waves from other atmospheric variation. Deducing some aspects of gravity wave structure (for example horizontal wavelength) from ground-based radar or lidar observations relies on theoretical relations such as the dispersion relation. The analysis can be enhanced by simultaneous observations of several coherent wave variables. Lidars that are capable of both wind and temperature data is one tool for this; another is the combination of simultaneous measurements from co-located ground-based instruments. Another type of observation that is especially useful for detecting waves with short wavelengths and periods is airglow imaging (e.g., Taylor et al. 1997; Snively et al. 2010).
Temperature profiles from limb-viewing satellites such as SABER also contain signatures of gravity waves. The gravity waves that can be detected are limited by the inherent spatial averaging of limb viewing and the vertical resolution (Alexander and Barnet 2007). However, if these limitations are properly treated in the analysis, much can be learned about gravity waves due to the near-global coverage of satellite observations. Preusse et al. (2009) calculated temperature variance from SABER data as an indictor of gravity wave activity. Another approach for determining gravity waves from satellite data was used by Chandran et al. (2010). They reported on the horizontal structure of gravity waves derived from satellite images of polar mesospheric clouds.
Despite the improvements in techniques and the accumulating database of gravity wave measurements, the incomplete availability of measurements is one of the main limitations in characterizing the dynamical system in the MLT. This is further complicated because, due to limitations in computing resources, full interactive general circulation models do not currently perform integrations with sufficient resolution to simulate the generation, propagation, and dissipation of the small-scale waves.
4.1.1 Gravity Wave Sources and Conditions for Vertical Propagation
Ideally, observations could be used to follow individual waves from their point of origin in the troposphere to the region where they dissipate in the mesosphere. However, this is not normally practical for several reasons. (1) The amplitudes of gravity waves that are not dissipating grow approximately exponentially with altitude. Waves that are seen in the MLT have very small amplitudes in the troposphere. (2) Individual measuring systems do not cover the entire vertical range. (3) Gravity waves propagate horizontally as well as vertically so they may move beyond the ranges of instrumentation at a fixed location. Despite these limitations, there has been progress in linking gravity waves in the MLT with their sources below.
Sato et al. (2009) used simulations with a high-resolution global model that resolves gravity waves to look at the momentum fluxes in the middle atmosphere. Based on their analysis, they found several preferred regions for gravity wave sources. The locations of these regions are determined by two factors: tropospheric activity that generates the waves (by shear instability, flow over topography, or convection) and wind conditions that affect the ability for the waves to propagate vertically through the middle atmosphere. In the subtropics during summer, convectively forced gravity waves originating in the monsoon regions were important because these waves were able to propagate through the easterly winds in the stratosphere. In winter, gravity waves originated in the middle and high latitudes and propagated vertically and horizontally into the mesospheric jet regions.
Another approach for determining the gravity waves that affect the MLT circulation was taken by Preusse et al. (2009). They used temperature variance observed by SABER to estimate the gravity wave activity in the middle atmosphere. They also used a gravity wave ray tracing model to estimate where gravity waves launched from various spots on the globe would propagate. The ray-tracing approach included the refraction of the waves in the horizontal direction. The refraction depends strongly on the winds in the middle atmosphere and on properties of the gravity waves themselves, for example, horizontal wavelength, phase speed, amplitude. In the Preusse et al. (2009) study, the gravity wave sources were homogeneous and isotropic but, at each launch site, included waves with different characteristics. The results showed a good comparison of the simulations with the observed gravity wave variance. One finding of this study is the importance of latitudinal refraction of gravity waves. In this regard, the Preusse et al. (2009) study supports the finding from the Sato et al. (2009) study. Both studies indicate that horizontal as well as vertical propagation of the gravity waves that drive the MLT circulation should be taken into account. Additional observational evidence for the importance of horizontal propagation was found by Ern et al. (2011). Using the analysis of observations from SABER along with high-resolution observations from the lower and middle stratosphere, they found that the momentum flux from gravity waves generated in the tropical region affected the winds in midlatitudes.
4.1.2 Gravity Wave Processes in Global Models
The challenge of simulating gravity wave impacts in global models stems from the small horizontal scales of the waves compared to the typical grid of a global numerical model and from the deep vertical domain extending from the Earth’s surface to the MLT. Even if the gravity waves themselves can be resolved, the complex dynamics during the wave breakdown requires even finer spatial and temporal resolution. However, proper simulation of the impacts of gravity waves, either through resolving the waves and their interactions with the larger scale or through parameterization, is necessary for all models of the global MLT.
There has been progress in modeling in which the waves themselves are resolved. In the spectral general circulation model (GCM) discussed by Watanabe et al. (2008) and Sato et al. (2009), gravity waves are generated self-consistently by topography at the surface or by dynamical processes in the troposphere. The waves propagate laterally as well as in the vertical direction. The model simulations are useful for investigating the generation of gravity waves and their propagation to the point where they break or dissipate and interact with the background atmosphere. The model top is near 85 km, so it stops short of simulating the full MLT region.
Another global model that resolves gravity waves was described by Becker (2009). This model is primarily focused on gravity waves and simplifies other atmospheric processes. For example, the radiative forcing to the atmosphere is approximated as a linear damping, convection is neglected, and the calendar is held fixed at January. Analysis of the model results shows that warming of the troposphere from anthropogenic climate change leads to a response in the MLT driven by gravity wave processes.
As noted, even a very high-resolution GCM cannot explicitly model the turbulence associated with breaking gravity waves. Some form of diffusivity is necessary to complete the interaction with the background flow when the scale of the perturbation fields of the wave is too small to be resolved by the model. The GCM described by Watanabe et al. (2008) and Sato et al. (2009) uses a Richardson number-based vertical diffusion to account for unresolved dynamical processes. It also includes a horizontal hyper-diffusion that is tuned to give a realistic spectrum of the waves. The Becker (2009) model also includes vertical and horizontal diffusion that plays a role in the interaction of gravity waves with the larger scales. In this model, both diffusivity parameters depend on the Richardson number.
Most global models with resolution too coarse to resolve the important gravity waves account for these processes by a parameterization. Holton (1983) gives an introduction to gravity wave parameterizations, and McLandress and Scinocca (2005) compare some of the parameterizations used in current models. The parameterization used in WACCM is based on the formulation by Lindzen (1981) with several updates (Richter et al. 2010) and uses a discrete spectrum of gravity waves. Figure 6 shows the climatological net zonal momentum forcing. Another parameterization used in several high-top models [the Canadian Middle Atmosphere Model (CMAM; McLandress and Scinocca 2005), the Hamburg Model of the Middle Atmosphere (HAMMONIA; Schmidt et al. 2006), and the Whole Atmosphere Model (WAM; Akmaev 2001b)] is based on work by Hines (1997a, b). Other gravity wave parameterizations have been proposed by Alexander and Dunkerton (1999), Medvedev and Klaasen (2000), and Warner and McIntyre (2001). Kim et al. (2003) discuss the assumptions about gravity wave spectra that go into the various parameterizations schemes.
All of the current gravity wave drag parameterizations are one dimensional (solved for a vertical column only) and include the following: a gravity wave source, a provision for the gravity wave to evolve and/or disappear based on the background through which it propagates, and a provision for the wave to exchange momentum with the background through dissipation and breaking. In the absence of damping, the gravity wave amplitude will grow approximately exponentially with height. Eventually, the amplitude is so large that the net temperature gradient (wave plus background atmosphere) is convectively unstable, and the wave will break. Parameterizations include a discrete or continuous spectrum of gravity wave phase speeds that extend into fast eastward and westward speeds (magnitudes ≥50–80 m/s). Topographically forced gravity waves with zero phase speed are often included as well; these can be important in the troposphere and stratosphere and sometimes penetrate to the mesosphere (Smith et al. 2009b).
In the earliest parameterizations, the tropospheric sources of gravity waves were a spectrum of zonally propagating gravity waves that were uniform at every point on the globe or were a uniform spectrum modified by the winds at the point where the waves were launched. An intermittency factor was needed, specifying that the waves were present for some fraction of the total time. Later, the sources and propagation were modified to take into account the 2-dimensional (meridional as well as zonal) background winds. A more recent development is for gravity wave sources that depend on the model dynamics. For example, in WACCM (Richter et al. 2010), gravity waves are launched when the conditions indicate the presence of fronts or convective activity. The convective source is most important in the tropics although it also plays a role in the summer over land surfaces. The frontal source is most important in middle and high latitudes. With the interactive sources, a specified intermittency factor is no longer needed.
The impact of the background on gravity wave propagation is the single largest factor affecting the seasonal cycle in dynamics in the MLT. As shown in the first global model with a gravity wave parameterization (Holton 1983), the first-order impact is the filtering of gravity waves in the stratosphere by critical layer processes. Investigation by McLandress and Scinocca (2005) indicates that this is still the most important component to the more sophisticated parameterizations currently in use. Waves with a particular phase speed will not be able to propagate vertically through a layer where the wind speed is equal to the wave phase speed. This filtering process explains the momentum fluxes of waves that reach the MLT. The breaking or dissipation of those waves leads to the reversal of the winds from the stratosphere to the mesosphere during the solstice seasons.
The final element in a parameterization is a representation of the impact of a breaking or dissipating gravity wave on the background atmosphere. In all parameterizations, this includes an exchange of momentum between the wave and the background. It is this momentum exchange that drives the winter westerly and summer easterly winds in the MLT.
Gravity wave parameterizations differ in the specification of the wave behavior and in the wave impacts on temperature and the distribution of trace chemical species. One difference is the fate of a wave that reaches breaking amplitude. That could result in damping of the wave to stay at an amplitude that is just below the breaking amplitude; this assumption was used in the formulation of Lindzen (1981) and Holton (1983) and is used in WACCM (Garcia et al. 2007). Another assumption that the wave disappears completely after it breaks was proposed by Alexander and Dunkerton (1999).
The thermal impact of gravity wave dissipation is another process that is treated differently in different gravity wave parameterizations. The potential thermal impacts are convergence of heat flux by the wave, diffusion of heat by turbulence, and heating due to the conversion of kinetic energy to heat. A mix of positive and negative values (heating and cooling) was estimated by Liu (2000) and shown in modeling by Becker and McLandress (2009). Since the radiative heating is relatively weak in the MLT (this weakness is the reason for the very low temperatures there), gravity wave processes can make a substantial contribution to the global mean heating/cooling.
4.1.3 Impact of Gravity Waves on the MLT
The zonal winds in the MLT at middle and high latitudes change in response to interaction with breaking or dissipation of gravity waves. As noted above, the filtering of the gravity wave spectrum by the large background zonal winds in the stratosphere during solstice seasons is the key process that is responsible for the direction of the mesospheric zonal winds. There is evidence that the filtering of gravity waves accounts for other MLT variations as well.
The SAO in tropical upper mesospheric winds (Lieberman et al. 1993; Garcia et al. 1997) is out of phase with the SAO in the upper stratospheric winds. Dunkerton (1982) showed in a simple model that filtering of gravity waves by the stratospheric SAO affects the phase-speed distribution of gravity waves that penetrate to the mesosphere. When these waves break, they drive the mesospheric SAO. This was examined further by Sassi and Garcia (1997) and Ricciardulli and Garcia (2000). They found that dissipation of convectively forced waves by the SAO in the tropical stratosphere could account for the large SAO in the MLT.
Gravity waves can respond to or affect other waves through the sources, the propagation, or the interaction at dissipation. Smith (2003) showed that stationary planetary wave structures in the zonal wind in the MLT were out of phase with those in the stratosphere. The MLT planetary waves had two possible sources: they could propagate up from the stratosphere with a longitude shift due to the vertical wavelength of propagating Rossby waves, or they could be forced in situ by the dissipation of gravity waves that had been filtered by winds in the stratosphere. Numerical simulations indicated that both these processes were occurring.
It has long been known from radar observations that gravity waves vary depending on the phase of the diurnal (24 h) tide. This is primarily due to the same filtering process that affects gravity wave response to mean winds. The impact of gravity waves on the migrating diurnal tide is larger than for other migrating tides because the tidal vertical wavelength is shorter. A shorter vertical wavelength is associated with stronger wind shears and temperature gradients from the tidal perturbations, and so it can have an impact on gravity wave propagation. The gravity wave interaction with tides is noteworthy because the gravity waves can affect the downward propagation of tidal perturbations, thereby altering the wavelength of the tide. Ortland and Alexander (2006) used a model calculation to demonstrate how gravity waves can change the vertical wavelength of the DW1 tide. Watanabe and Miyahara (2009) found a similar impact of gravity waves on the tidal vertical wavelength in a gravity wave-resolving GCM.
Gravity wave interactions can also damp or amplify the tides when the gravity wave breaking occurs during different phases of the tide. Analysis of TIMED observations by Xu et al. (2009a) showed that the impact of unresolved processes (presumed to be gravity waves) is primarily to damp the diurnal migrating tide. Using the same data, Lieberman et al. (2010) found that the most important effect was to shorten the vertical wavelength of the tide.
Although it is acknowledged that diffusion can be important in the MLT, there is not a consensus about the magnitude or distribution of diffusion. One source of the problem is that the term diffusion is used to indicate several different processes.
Molecular diffusion is the name given for the dispersal and mixing of gases due to long pathlengths at the low density of the upper atmosphere. The impact of molecular diffusion increases as the density of the surrounding gas decreases. Molecular diffusion is further affected by molecular mass since the impact of gravity becomes competitive at the low collision rates. As the dispersive tendency based on mass becomes more important in the thermosphere, the dominant gases separate. The result is that lighter gases overlie heavier ones. The term molecular diffusion is used both for the mixing process and for the dispersive effect.
Models and observations indicate that molecular diffusion affects the composition of some gases in the MLT such as CO2 (López Puertas et al. 2000; Beagley et al. 2010) and atomic oxygen (Smith et al. 2011). Molecular diffusion can have a direct effect on the dynamics through the transport of heat. The exchange of molecules from higher levels due to the long mean free path can lead to heat exchange. Transport of atomic oxygen, which releases heat when it is involved in any of several exothermic reactions (see Mlynczak and Solomon 1993), also is an effective means of transporting heat vertically in the MLT.
The term eddy diffusion is used for two different processes; they are likely related although the nature of the relationship is not clear. On the one hand, eddy diffusion indicates turbulent diffusion such as that responsible for the meteor trail dispersion observed by Kelley et al. (2003) or from the trails of chemicals released from a rocket (Bishop et al. 2004). Turbulence measurements have also been made by incoherent scatter radar (Hall and Hoppe 1998). At present, these measurements are not used in global-scale analysis or model evaluation. To do so would require an understanding of how processes on very small spatial scales and short duration are related to large-scale processes. One path for addressing the link may be the use of turbulence models within larger scale simulations. Liu et al. (1999) used a turbulence model along with a gravity wave model in a mesoscale simulation to investigate the transport effects of a breaking gravity wave. They found that the turbulence affected not only the rate of transport but also the propagation of the gravity wave. Areas of turbulence were not uniformly distributed along the wavelength of the wave. The resulting implied eddy diffusion coefficient, based on induced changes to trace gases, was less than that determined from the gravity wave saturation in the Lindzen (1981) formulation.
The term eddy diffusion is also used to include all unresolved processes that mix heat or chemical constituents; see Garcia et al. (2007) for a derivation showing how the heat flux convergence by a dissipating gravity wave can be represented as a vertical diffusion. Gravity waves that are dissipating give a net heat flux convergence that can be positive (heating) or negative (cooling). However, Akmaev (2007) argued that it is not completely accurate to represent the net heat flux convergence by gravity waves with a diffusion coefficient.
A parameter that is used in the diffusion coefficients from gravity wave parameterizations is the equivalent Prandtl number, Pr. The equivalent Prandl number represents the ratio of momentum flux to heat flux. It can be visualized in terms of the local nature of wave breaking (Coy and Fritts 1988). When breaking conditions are found over part of the wave, instead of along its full horizontal wavelength, Pr is greater than 1. A larger equivalent Prandl number means a lower rate of eddy diffusion applied to heat and trace species. The value adapted in models is normally in the range of 3–5. WACCM, for example, uses Pr = 4.
The term “turbopause” refers to the altitude where turbulent motion ceases. Conventionally, it has been considered the altitude where the molecular diffusion coefficient becomes as large as the eddy diffusion coefficient. A related concept, the homopause, refers to the altitude where long-lived gases are no longer well-mixed. Since the molecular diffusion coefficient varies depending on the mass of the chemical species in question, it is now recognized that there is no single homopause.
Offermann et al. (2007) used standard deviations of temperature as a function of altitude in global data to identify a transition they labeled the wave turbopause. The concept behind their analysis is that, in the middle atmosphere where waves are damped by turbulent processes, the variance will not grow with height at the rate for a conserved wave of exp(z/2H), where z is altitude and H is scale height. However, when the damping ceases at the turbopause, the variance can grow much more rapidly. Using this transition as a signature of the wave turbopause, Offermann et al. (2007) found a clearly defined wave turbopause that varied with latitude and season over the range from about 80 to 100 km.
Tides continue to be a major focus of research, not just because of their large amplitudes but also because tidal modes and their variability are still not completely understood. The persistence of questions is in a way curious because the basic processes that account for tides have been long known. The theory for tides forced by solar heating in an isothermal atmosphere at rest and with no damping was well explained by Chapman and Lindzen (1970). This is known as classical tidal theory, and the tides that it predicts are known as classical tides. Although the classical conditions of isothermal and windless are never met in the global atmosphere, the observed tides bear a good resemblance to the classical predictions. However, surprising new things about tides are still coming to light. One new aspect is the recent awareness of the importance of nonmigrating tides (defined below). Another is the teleconnection involved in the global coupling. An ongoing puzzle is that there is no consensus explanation for the large seasonal variability of the migrating diurnal tide.
Atmospheric tides are gravity wave modes whose period is exactly one day or an integral fraction of a day. Most of the tides seen in the MLT region have propagated from below although they can be modified by local conditions. The tidal response to in situ forcing in the MLT by diurnal variations in the heating is very small compared to the tides that propagate from below (Smith et al. 2003).
Tides can lead to very large variations in winds, temperature, density, and many other atmospheric parameters (airglow emissions, densities of trace species, etc.). A major source of tides is the diurnal variation in heating. The heating in the troposphere comes from absorption of sunlight by water vapor and from latent heat release. Heating in the stratosphere is mainly by absorption of ultraviolet radiation by stratospheric ozone.
Before the 1990s, much of the information about tides in the MLT came from radar observations. These are still an important source of information because radars can detect the diurnal cycle of winds at a single geographic location. With data from a single radar, it is not possible to determine the global structure of the observed tides. However, data from simultaneous operation of multiple radars provide some information about latitudinal (Pancheva et al. 2002) or longitudinal (Murphy et al. 2006) variations. With data from precessing satellites such as UARS and TIMED, the global structure of the temperature and horizontal wind variations are now known. Unfortunately, these slowly precessing satellites cannot resolve short-term variations in the tides, which leaves a gap in the present knowledge. Another limitation to relying on satellite data to determine tides is that some tidal modes are aliased in data from polar-orbiting satellites (Oberheide et al. 2003).
Hough functions provide a set of orthogonal global solutions of the classical tidal equation. A given tidal frequency and wavenumber, for example a westward propagating diurnal tide with wavenumber one, will project on to a set of Hough functions. The set of functions for any wavenumber and frequency combination includes symmetric (with respect to the equator) and asymmetric modes. The heating that forces the tide can also be projected onto Hough functions and varies with season as the heating evolves. The largest seasonal difference is between equinox seasons (heating roughly symmetric across the equator) and solstice seasons (maximum heating shifted to the summer hemisphere). In the classical tide case, the Hough mode projections of the heating determine the tidal response. Specifically, the Hough mode projection of the tides follows the Hough mode projection of the heating and is the same at all vertical levels. However, under realistic conditions, the Hough mode projection of the tides varies with altitude in response to damping and to interactions with the background atmosphere or other waves. A mathematical representation of the variations in tidal projections with altitude is the concept of generalized Hough modes (Ortland 2005a, b).
A technique to extract additional information about tides from limited observations using theory together with wind observations was described by Svoboda et al. (2005) and also used by Oberheide and Forbes (2008). They use Hough mode extensions (HMEs), a technique developed by Forbes and Hagan (1982), to create complete global tidal fields of zonal and meridional winds, vertical wind, temperature and density in the mesopause region from the limited amount of horizontal wind data from UARS.
It is useful to distinguish between migrating and nonmigrating tides. Migrating tides follow the motion of the Sun: for example, a wavenumber 1 westward propagation 24-h tide, a wavenumber 2 westward propagation 12-h tide, and so on. All other tides are called nonmigrating. They can be westward or eastward propagating or stationary. A common abbreviation system refers to the tides by a string of three symbols. The first indicates the period: D (diurnal) or S (semidiurnal); the second indicates the direction of phase propagation: E (eastward), W (westward), or S (stationary); and the third is an integer giving the zonal wavenumber. The classical tides are migrating: DW1, SW2, etc. Analysis of global observations from precessing satellites has shown that nonmigrating tides contribute a significant, sometimes dominant, amount to the total tidal amplitude or variability.
Diurnal variations in dynamical fields that are locally forced but do not propagate vertically are referred to as trapped modes. It is not always possible to determine, from observations, whether a disturbance is or is not propagating. Even when a distinction is possible, the nomenclature can be imprecise. An example is the daily temperature perturbations in the stratosphere due to ozone heating. The temperature fluctuations are normally separated into frequencies that are subharmonics of 24-h (diurnal, semidiurnal, etc.) and considered to be tides. Some fraction of these temperature fluctuations maps onto Hough modes that can propagate vertically while quite a bit of the diurnal signal does not. The Hough modes that do not propagate are also called tides and are referred to as trapped modes.
4.3.1 Migrating Diurnal Tide
Various explanations have been proposed for the equinoctial maximum. The proposed mechanisms fall into three categories: semiannual variations in the heating that forces the tide, variations based on the background winds in the tropical stratosphere or mesosphere, and variations due to damping within the middle atmosphere. The tropospheric heating projected onto the leading symmetric Hough mode has maximum during the December solstice period while the heating projected onto the first asymmetric mode has an equinoctial maxima (Lieberman et al. 2003). The magnitude of the seasonal variations in the heating due to absorption of sunlight by water vapor in the troposphere is small compared with the observed seasonal variations in DW1 amplitude. Hagan and Forbes (2002) found that forcing of DW1 by latent heat release in the troposphere has a pronounced semiannual variation with maximum forcing in the equinox months. The diurnal tide forcing by ozone heating in the stratosphere also has seasonal variations (Xu et al. 2010). In this case, maximum forcing of the leading symmetric Hough mode occurs during NH winter. Taken together, the seasonal variations in water vapor heating in the troposphere and ozone heating in the stratosphere do not provide support for the heating being the cause of the observed seasonal cycle in tidal amplitude. On the other hand, seasonal variations of latent heat release are consistent with the observed changes in tidal amplitude and may contribute to the seasonal cycle. Achatz et al. (2008) looked at the possibility that planetary wave interactions affect the annual cycle of the migrating diurnal tide; they found that these have no important impact.
A second proposed explanation for the observed seasonal cycle is that the tidal propagation is affected by the zonal winds through which the tide propagates. McLandress (2002a, b) showed in the CMAM model that the tide varied based on the zonal winds in the middle atmosphere. His analysis showed that there is a strong semiannual variation in the latitudinal gradient of the zonal wind in low latitudes. This gradient introduces a vorticity that is comparable in magnitude to the Coriolis torque and affects the tidal amplitude. In the model, the semiannual variation in net tidal heating also contributed to the simulated seasonal cycle in tidal amplitude.
A third factor to consider is the possibility that tidal damping is larger during the solstice seasons, leading to maximum amplitude during the equinoxes. Analysis of satellite observations by Xu et al. (2009a) show that the damping of the DW1 tide by gravity wave interactions is largest when the tide itself is largest, thus indicating that damping is not responsible for causing the tidal seasonal cycle. Using different analysis of the same satellite observations, Lieberman et al. (2010) came to a different conclusion that the gravity wave interactions affected mainly the DW1 phase and not the amplitude. Neither of these analyses provides evidence that damping by gravity wave interactions is the primary cause of the seasonal cycle in DW1.
A periodicity that appears in investigations of the interannual variability of the DW1 tide is a biennial or quasi-biennial oscillation (QBO) (Burrage et al. 1995; Wu et al. 2008; Xu et al. 2009b). The amplitude of the DW1 tide varies in alternate years and appears to be related to the QBO in the zonal wind in the lower stratosphere. The tidal QBO is most apparent as a variation in the amplitude during the NH vernal equinox season (March/April). It is this link between the interannual and seasonal variations that makes it difficult to distinguish between a biennial or QBO variation when only a limited number of years of data is available. The phase of the tidal QBO is such that the March tidal amplitude is larger when the equatorial zonal wind at 30 hPa is eastward. Explanations for the interannual variability are still not agreed on. They are similar to those for the seasonal cycle except it is evident that variations of the sources within the troposphere do not contribute to the QBO. In a mechanistic numerical model, Mayr and Mengel (2005) found that filtering of gravity waves by winds in the stratosphere was able to transfer the QBO signal to the MLT. It is also possible that winds in the lower stratosphere affect the tidal forcing but mechanisms have not been identified.
Lieberman et al. (2007) investigated the response of the DW1 tide to large-scale interannual changes in the diurnal component of tropospheric water heating associated with an El Niño event in the tropical ocean/atmosphere. The heating changes include both the absorption of radiation by water vapor and latent heat release. They found that the heating changes during 1997–1998 were sufficient to account for a maximum in the diurnal tide amplitude that was observed in low latitudes during that period.
4.3.2 Semidiurnal and Higher-Frequency Tides
The horizontal wind amplitudes of the migrating semidiurnal tide, SW2, tend to be largest in middle to high latitudes (Pancheva et al. 2009a), so they can be the dominant tidal signal in these areas. The latitude differences between the diurnal and semidiurnal tides are readily explained by the Hough mode structures. The heating projects best onto the gravest symmetric Hough mode which, for DW1 temperature, approaches zero in high latitudes. In contrast, the gravest symmetric Hough mode for SW2 extends from pole to pole.
The maximum amplitude of the SW2 tide tends to be above the mesopause, whereas that of the DW1 tide is around 95 km. This difference is likely related to the vertical structure. DW1 has a relatively short vertical wavelength of ∼25 km. This leads to stronger interactions with gravity waves and therefore to stronger damping. Observations indicate that the vertical wavelength of SW2 varies with latitude and season but even the lowest values observed (35 km found by Pancheva et al. 2009a) are longer than that of DW1. A longer vertical wavelength reduces the magnitude of wind and temperature gradients due to the tide and makes it less susceptible to damping by gravity wave interactions.
Analysis of lidar observations at a site in NH midlatitudes by Yuan et al. (2008) indicates that the semidiurnal tide shows seasonal variations in the phase structure. At this site, the tide is vertically propagating during winter and equinox periods and has a vertical wavelength ranging from 50 to 90 km. During summer, the wavelength becomes even longer or becomes evanescent (no wave-like structure in the vertical profile). Yuan et al. (2008) interpret the seasonal changes as resulting from a different superposition of migrating and nonmigrating modes during the different seasons.
While most work has focussed on the diurnal (24-h) and semidiurnal (12-h) tides, higher-frequency tides have also been observed. Taylor et al. (1999) reported a large amplitude terdiurnal (8-h) tide in temperature data from an airglow imager. Younger et al. (2002) showed the terdiurnal tide in radar winds at 68°N. Smith (2000) and Du and Ward (2005) presented the global and seasonal structure of the terdiurnal tide in horizontal winds observed by HRDI and WINDII, respectively. Modeling studies by Smith and Ortland (2001) and Akmaev (2001a) indicated that the mean terdiurnal tide is primarily forced by solar heating although generation by nonlinear interaction between diurnal and semidiurnal migrating tides also contributed.
Tides with even higher frequency are seen in radar observations. For example, Smith et al. (2004) presented observations and modeling of a 6-h tide. Analysis of the high-frequency tides from observations made with a precessing satellite is a challenge because small changes in the amplitude or phase of lower-frequency tides (particularly diurnal and semidiurnal) can affect the analysis.
4.3.3 Nonmigrating Tides
Numerous observations indicate that nonmigrating diurnal (Oberheide et al. 2005, 2006) and semidiurnal (Baumgaertner et al. 2005; Murphy et al. 2006) tides are normal phenomena of the MLT. Nonmigrating tides can be excited by longitudinal variations in the diurnal heating. The most obvious source of heating variations is latent heat release in the tropical region (Hagan and Forbes 2002; Hagan et al. 2009). The presence of a DE3 tide has been attributed to the heating distribution, in particular to the alternating high and low rates of latent heat release due to the alternating continents and ocean with longitude in the equatorial region (Hagan et al. 2009; Akmaev et al. 2008).
Nonmigrating tides can also be excited by nonlinear interactions between the migrating tides and quasi-stationary planetary waves (Oberheide et al. 2002; Lieberman et al. 2004). A nonlinear interaction between two large-scale waves (the parent waves) can produce child waves with related structure. The wavenumber and frequency of the child waves must be the sum or difference of the wavenumbers and frequencies of the parent waves. This mechanism can produce migrating tides as well. For example, the interaction of DW1 and SW2 can generate the migrating terdiurnal tide. Non-migrating tides can be produced by the interaction of migrating tides with planetary waves. The dominant planetary waves in the winter stratosphere are quasi-stationary with low zonal wavenumbers (wavenumbers 1 and 2 are the largest); a quasi-two day wave with zonal wavenumber of 3 or 4 is often seen in the mesosphere.
Observations (Baumgaertner et al. 2005; Murphy et al. 2009) indicate that the SW1 tide is present around the perimeter of Antarctica. Murphy et al. (2009) showed that the temporal variations in SW1 were well correlated with variations in the amplitude of stationary planetary wave 1 in the NH. They also found a link between SW3 and the NH planetary wave. While not conclusive, this robust correlation provides good evidence that the SW1 in the southern summer MLT is caused by a nonlinear interaction between SW2 and a stationary planetary wave 1 in the stratosphere of the winter hemisphere. The relationship can also go in the opposite direction, from the SH winter to the NH summer. Smith et al. (2007) found a correlation between the planetary wave amplitude in the SH at the semidiurnal tide at a single radar site in the NH. In their analysis, with data from a single site, it was not possible to distinguish between the migrating and nonmigrating semidiurnal tides.
The interaction of tides with planetary waves can also generate nonmigrating tidal modes that are seen locally (in the same hemisphere or even at the same latitude as the planetary wave). Such responses were seen by Liu et al. (2007) in northern midlatitudes and Baumgaertner et al. (2006) in the southern hemisphere.
4.4 Planetary Waves
The term planetary waves refers to various phenomena, some of which are components of middle atmosphere dynamics. In general terms, planetary waves are propagating large-scale disturbances with low zonal wavenumbers. Conservation of angular momentum is the restoring force that governs the wave dynamics.
Quasi-stationary Rossby waves are the dominant disturbances in the extratropical winter stratosphere and lower mesosphere. Stationary Rossby waves with low zonal wavenumbers (typically wavenumbers 1–3) can propagate vertically where the background zonally averaged zonal wind is westerly (Charney and Drazin 1961). This condition is usually met in the winter stratosphere and lower mesosphere. The wintertime zonal wind may reverse from westerly to easterly in the upper mesosphere; the altitude where the reversal occurs varies with latitude, season, and can have large interannual variations due to dynamical activity. Quasi-stationary waves are difficult to separate from the background winds and temperatures in radar and lidar observations but can be observed by satellite. Mukhtarov et al. (2010) present observations of the stationary waves in temperature observed by the SABER satellite instrument. The amplitudes are small in the region of the mesopause (∼100 km altitude).
A planetary-scale variation in the small-scale waves that propagate into the mesosphere can exist due to planetary-scale variations in the generation of the small-scale waves. Another means of generating variations is through differences in the filtering or dissipation of the waves due to the differences in winds, temperature, etc. As shown by Smith (2003), planetary waves in stratospheric winds can filter the gravity waves propagating from below, leading to large-scale variations in the gravity wave flux that propagates into the MLT. When the gravity waves break or dissipate, they will generate a planetary wave pattern in the MLT winds and temperature. Quasi-stationary planetary waves have been seen in the winter MLT (1996, 1997; Wang et al. 2000; Xiao et al. 2009). These probably contain a mix of planetary scale disturbances that have propagated from lower altitudes and wavelike variations due to interactions with small scale waves.
Quasi-stationary planetary waves are absent in the summer stratosphere. Normally during the solstice seasons, the mean zonal winds reverse in the mesosphere; the result is westerly winds in summer and easterly winds during winter. As shown originally by Dickinson (1968), under some circumstances, there can be continuous westerly winds across the tropics from the winter stratosphere to the summer mesosphere. This phenomenon known as the mesospheric tropical waveguide, creates a path for propagation of quasi-stationary planetary waves into the summer mesosphere. Depending on characteristics of the winds and waves, the waveguide can also allow the propagation of other waves (for example, planetary waves with nonzero frequency).
The tropical waveguide has been seen in the observations of the zonal wind (e.g., McLandress et al. 1996; Fleming et al. 1996). Wang et al. (2000) and Garcia et al. (2005) reported the observations of stationary planetary waves in the summer mesosphere in winds and temperature, respectively. Forbes et al. (2002) investigated the source of summer waves observed in the MLT and concluded that the propagation of waves from the winter hemisphere was a likely explanation for the presence of the waves in the summer hemisphere.
Traveling planetary-scale waves can achieve high amplitude in the MLT. The periods of traveling waves cluster around periods associated with atmospheric normal modes. One commonly observed mode is the quasi-two day wave, which has a period of about 2 days and a zonal wavenumber of 3 or 4. It is regularly observed in the mesosphere just after solstices and can attain very large amplitudes (meridional wind ∼30 m/s) (Riggin et al. 2004; Limpasuvan and Wu 2009; Offermann et al. 2011a). Other commonly reported periods are 5 day (Riggin et al. 2006), 6.5 day (Lieberman et al. 2003; Liu et al. 2004), 10 day, and 16 day (Day and Mitchell 2010). These waves do not directly transport much momentum. However, they can interact with other waves such as quasi-stationary Rossby waves, gravity waves, and tides and thereby affect the momentum budget and the periodicity of variability in the middle atmosphere. Spectral breakdown of planetary waves in mesospheric observations has been given by Garcia et al. (2005) and Pancheva et al. (2008, 2009b, c).
Equatorially trapped waves are, as the name indicates, limited to the tropics. These waves fall into two categories: Kelvin waves, which propagate eastward, and mixed-Rossby gravity waves, which propagate westward. Planetary-scale Kelvin waves with short periods have large vertical wavelengths. These waves are less rapidly damped in the middle atmosphere than are Kelvin waves with shorter vertical wavelengths. They are also less likely to be dissipated by critical line interactions because of their fast phase speeds. Salby et al. (1984) showed the presence of very fast Kelvin waves in the upper mesosphere. Numerous observations confirm that these waves are a frequent feature of the tropical MLT (e.g., Younger and Mitchell 2006; Takahashi et al. 2007; Forbes et al. 2009; Chang et al. 2010). Kelvin waves with periods of 24 hours contribute to the observed spectrum of eastward propagating tidal motions.
5 Vertical Coupling Between the Stratosphere and MLT
5.1 MLT Variations due to Active Winter Dynamics
Model predictions and observations indicating the interaction of the stratosphere with the MLT during dynamically active winter periods have a long history. Characteristic variations to the mesosphere are associated with strong disturbance in the stratosphere. One topic of particular interest is the MLT response to stratospheric sudden warmings (SSWs). SSWs are extreme events in which there is rapid warming of the polar stratosphere and reversal of the normally westerly winds to easterly in the middle stratosphere. They are caused by interaction of planetary waves with the stratospheric mean flow. Frequent SSWs in the years since 2000 (Charlton and Polvani 2007) have provided opportunity for extensive observations of the MLT response. It is well documented that the symptoms of SSWs are first seen at higher altitudes in the mesosphere and propagate downward over a period of a few days.
Ground-based observations of MLT winds and temperature (Hoffmann et al. 2007) showed clear wind perturbations up to the highest level shown, about 90 km. The observations also indicate that the perturbations in the stratospheric zonal wind affect gravity wave propagation into the MLT. Siskind et al. (2005) found from SABER temperature observations that the mesospheric cooling associated with the stratospheric warming events was confined to the levels below about 85–95 km.
The response through the depth of the middle atmosphere was simulated by Liu and Roble (2002). Their model study showed a broad region of negative temperature perturbation extending to about 110 km that coincides with the stratospheric warming. Using a version of the same model, Yamashita et al. (2010) showed that the simulated MLT response to a SSW was sensitive to the settings in the gravity wave parameterization. The settings influence the model simulation of planetary wave propagation and damping. They can also affect the vertical structure of the MLT response to the stratospheric perturbations, including the vertical domain over which cooling is simulated.
Global observations extending from the lower stratosphere into the upper mesosphere have enabled the documentation of several important ways in which variability in the MLT is driven by variability in the winter stratosphere. Much attention was focused on this topic due to surges of certain trace chemicals into the high latitude middle atmosphere during some active periods during 2004, 2006, and 2009. The flux of tracers was a signature of rapid downwelling from the MLT region to much lower altitudes. These three winter periods all followed strong midwinter SSWs. However, the persistence of an altered state and strong downward transport during the winter occurs only after some, not all, SSWs.
A striking aspect of the unusual dynamics of those winters were shown in the observations of temperature (Manney et al. 2005, 2008, 2009; Orsolini et al. 2010) and simulations of similar events by WACCM (Chandran et al. 2011; Limpasuvan et al. 2011). In those winters, the position of the stratopause, identified as the middle atmosphere temperature maximum, jumped from its average altitude range (45–55 km) to 75–85 km. The warm temperature in the upper mesosphere was a response to downwelling by increased gravity wave activity while the cooler temperatures below indicated gravity wave breaking in that region was suppressed. Observations also indicated perturbations to the distributions of chemical species that are produced in the MLT (e.g., Randall et al. 2009; Smith et al. 2009a; Kvissel et al. 2012).
Because of the limited availability of satellite observations spanning the lower to upper mesosphere in winter high latitudes, the observational record showing the response of the MLT to winter dynamics is still incomplete. Models and analysis of observations point to the importance of gravity waves and their filtering by stratospheric winds in the vertical coupling in this region. This once again highlights the challenges for global models and observations.
5.2 Summer MLT
The changing climate in high southern latitudes, particularly the deep and persistent spring ozone hole over Antarctica, has led to later breakdown of the winter westerly vortex in the SH (Karpetchko et al. 2005; Haigh and Roscoe 2009; Eyring et al. 2010; WMO 2010). The temperature in the lower stratosphere during spring has become lower (Thompson and Solomon 2002; Randel et al. 2009) and the winds more westerly. In the analysis of WACCM by Smith et al. (2010b), the stratospheric changes affected propagation of gravity waves from the troposphere to the mesosphere. On a long (multiyear) timescale, the trend in the temperature at the early summer mesopause (November and December) was traced to the ozone hole development. Lossow et al. (2012) found a similar perturbation in the CMAM model although in that model the trend was seen only during November. Observational confirmation of the relationship, albeit on a shorter interannual timescale, was provided by Hernandez (2004), who found a relationship between the MLT temperature at the South Pole and the size of the Antarctic ozone hole.
On short timescales of a few days, ozone in the stratosphere is affected by dynamics through transport and temperature-dependent photochemistry. The feedback of the ozone changes on dynamics through changes in radiative forcing is not important on this timescale because the radiative timescale is more than a week (Shine 1987). On the other hand, the persistence of a remnant of the winter vortex in the SH long after spring equinox, and even to the summer solstice (Black and McDaniel 2007), could affect the summertime mesospheric circulation. This is because both the mean winds and the planetary waves in the stratosphere affect the propagation of gravity waves that, in turn, drive the mesospheric circulation.
Variations in the timing of the SH stratospheric vortex breakdown introduce a source of variability that can influence the summer mesopause in the SH. Kirkwood et al. (2008) reported a higher position for the mesopause during Novemeber 2007; they attributed this anomaly to the filtering of gravity waves by winds in the middle atmosphere. Gumbel and Karlsson (2011) found that the onset of the season for polar mesospheric clouds in the SH summer of 2010–2011 was delayed by several weeks. This coincided with a delayed breakdown of the westerly jet in the stratosphere during this summer season. The delayed vortex breakdown has important impacts on the filtering of gravity waves that drive the circulation in the mesosphere (e.g., Smith et al. 2011). The eastward gravity waves that drive the upwelling branch of the circulation cannot propagate under these conditions. Adiabatic cooling associated with the upwelling is responsible for cooling the summer mesopause; changes in the gravity wave driving will therefore affect the temperature in the MLT.
The persistence of westerly winds in the stratosphere over Antarctica into the spring and even early summer means also that planetary waves can exist later in the season. Zonal asymmetries in the winds in the stratosphere may, through the filtering of gravity waves, also lead to zonal asymmetries in the wave flux into the mesosphere, as discussed in Sect. 4.4
6 Hemispheric Differences and Interhemispheric Teleconnections
6.1 Interhemispheric Teleconnections
In recent years, some surprising aspects of global teleconnections in the middle atmosphere have come to light. Two phenomena involving the impact that winter variability in the stratosphere has on the upper mesosphere of the summer hemisphere have been documented. In one case, the signal is seen in semidiurnal nonmigrating tides and, in the other, it is evident in mean winds, temperature, and polar mesospheric cloud occurrence frequency. Although both signals are related to dynamical variability in the winter stratosphere, there has been no indication that the hemispheric teleconnection in tides is otherwise related to that in the time-mean fields.
6.1.1 Teleconnections Involving Tides
The dynamics in the northern hemisphere (NH) winter stratosphere are quite variable. Planetary waves and the zonal mean wind and temperature all vary in response to dynamical perturbations propagating from the troposphere. The variations in planetary wave amplitude are correlated with variations in the amplitude of migrating semidiurnal tides in high southern latitudes (Murphy et al. 2009). Since variations in the wave amplitudes, the mean wind, and the temperature in the winter stratosphere are well correlated, observations cannot give a definitive answer about which of these contribute to the tidal response. Smith et al. (2007) observed a similar correlation between NH summer tides and planetary waves in the SH.
There are numerous observations of the nonmigrating SW1 mode in the SH (e.g., Forbes et al. 1995; Portnyagin et al. 1998; Murphy et al. 2003, 2006; Aso 2007; Chang et al. 2009; Hibbins et al. 2010; Iimura et al. 2009). Yamashita et al. (2002) reproduced the relationship between the SH semidiurnal nonmigrating tides and the NH stratospheric planetary waves in an atmospheric circulation model. In their model, Eliassen-Palm fluxes indicated propagation of nonmigrating tides from the winter stratosphere toward the summer mesosphere. Simulation of a sudden stratospheric warming by Liu and Roble (2002) also shows the generation of nonmigrating semidiurnal tides by interaction of a planetary wave with the migrating tide. Xu et al. (2009d) found a correlation between the SH semidiurnal tide measured by radar and the planetary wave 1 in the NH winter but did not find a comparable correlation between the NH semidiurnal tide and the SH winter planetary wave 1. They did not have enough information to separate the tidal variations into migrating and nonmigrating contributions, so the hemispheric comparisons are likely affected by the longitudes of the radars used to determine the tidal variations.
6.1.2 Teleconnections Involving Zonal Mean Winds and Planetary Waves
A teleconnection pattern has also been seen that involves mean states (zonally averaged temperature or zonal winds), planetary waves, and the characteristics or occurrence frequency of polar mesospheric clouds (PMCs). The wintertime variations in planetary waves and the background zonal mean temperature, winds, and circulation are closely coupled. Therefore, it is not possible, using observations or complex general circulation models, to separate the effect of variability of stratospheric planetary waves (such as wave–wave interactions) from those of the mean temperature and winds (such as filtering of gravity waves by the stratospheric winds). The winds and temperature in the winter stratosphere are highly correlated with the waves on multiple timescales (Xu et al. 2009c). Becker et al. (2004) and Becker and Fritts (2006) used model simulations to show that temperature changes observed in the NH summer mesopause were related to dynamical events in the SH winter. Karlsson et al. (2009a) analyzed simulations from the Canadian Middle Atmosphere Model and found that the model reproduces the observed relationship. Karlsson et al. (2007, 2009b) found a link between variability of PMCs and dynamical variations in the opposite (winter) hemisphere stratosphere. Espy et al. (2011) found that the correlation varied with the phase of the QBO in tropical stratospheric zonal wind.
Calculations do not support a direct connection through a global circulation driven by winter planetary waves or by gravity waves that have been filtered by the planetary waves or the associated changes in stratospheric mean wind. While such a circulation could cause upwelling in the tropics, the extension to the summer pole is not supported. Likewise, direct propagation of planetary waves from the winter to summer hemisphere has not been invoked as a primary mechanism in the published studies although propagation of planetary waves into the summer midlatitude MLT has been seen in both observations and models. The mechanism proposed to explain model simulations of the teleconnection pattern (Becker and Fritts 2006; Karlsson et al. 2009a; Kornich and Becker 2010) involves feedbacks among the mean circulation in the latitude-height plane, gravity wave propagation and breaking, and the zonally averaged wind.
To follow this mechanism, consider a case where the stratospheric polar temperature is higher and the zonal wind is weaker than the climatological values. This corresponds to a period of active dynamics, driven by large transient planetary waves and wave-mean flow interaction in the stratosphere. The weak zonal wind in the stratosphere affects the filtering of gravity waves, with the result that the net momentum forcing in the MLT is weaker than the climatological values. This in turn leads to a weaker driving of the poleward circulation in the MLT that brings midlatitude air toward the pole (see Fig. 4). The weaker circulation affects the rising motion in low latitudes and reduces the adiabatic cooling, thus increasing the temperature in the tropical MLT. The increased tropical temperature then increases the temperature gradient between the cold summer pole and the tropics and, through the thermal wind relation, strengthens the summer westerly winds in the MLT. This affects the gravity wave interactions in the summer hemisphere and reduces the driving of the equatorward circulation there. Through changes in the strength of the adiabatic cooling, there is a positive perturbation to the mean temperature in the poles that correlates with the temperature perturbation in the winter stratosphere. Using a simple model, Kornich and Becker (2010) were able to document each of the steps that give rise to this teleconnection pattern.
6.2 Hemispheric Differences
The winds in the winter stratosphere are stronger in the SH, due in large part to weaker quasi-stationary planetary waves that propagate from the troposphere. The stronger eastward winds affect the propagation of gravity waves with westward phase speeds and the filtering of gravity waves with eastward phase speeds. When the gravity waves break or dissipate near the stratopause or in the mesosphere, the net momentum forcing will then be stronger in the SH. This winter difference leads to a stronger circulation in the SH and to a higher winter mesopause temperature. Planetary waves do not play an important role in the summer stratosphere but, nevertheless, there are also hemispheric differences in the stratospheric summer zonal winds.
Both the height and temperature of the mesopause in high-latitude summer have differences between the two hemispheres. As described in Sect. 3, the low temperature and low altitude of the summer mesopause is due to very strong upwelling near the pole. The summer mesopause is colder and at a lower altitude in the NH summer compared to the SH summer (Huaman and Balsley 1999). Chu (2003) and Chu et al. (2006) reported hemispheric differences of about 1 km in the altitude of polar mesospheric clouds (PMC) from lidar measurement. PMC altitudes are sensitive to temperature but also to other variable fields such as water vapor and vertical wind. Xu et al. (2007a) found similar differences in the mesopause height determined from SABER temperature measurements. Hervig and Siskind (2006) found larger differences in mean summer temperature at 65−70° in HALOE data; the SH was warmer by 3–6 K throughout the mesosphere.
The hemispheric asymmetries in mesopause temperatures and altitudes can be seen in Fig. 1, upper panels. This difference is not well simulated in WACCM (Fig. 1, lower panels); the minimum summer temperatures reached in the two hemispheres are similar, but the simulated mesopause altitude is higher during NH summer. Siskind et al. (2003) reported a stronger gravity wave-driven circulation in the NH during July than in the SH during January in simulations using a two-dimensional model, consistent with the WACCM results for those months.
The annual variation in Earth–Sun distance (closest during January) leads to a solar flux change of about 6 %. This difference can also affect hemispheric differences, including the mesopause temperature and altitude (Chu 2003). Simulations made with the thermosphere–ionosphere–mesosphere-electrodynamics global climate model (TIME-GCM) indicated that the mesopause difference is mainly caused by the solar flux differences between January and July (Chu 2003).
Dowdy et al. (2001, 2007) presented hemispheric differences in high-latitude zonal and meridional wind measured by radar (two sites in each hemisphere). They found that winter zonal winds in the SH were stronger and their seasonal variations were more symmetric around the winter solstice than were those in the NH.
Tidal motions also have hemispheric differences that are apparent in global analyses that show the amplitudes in both hemispheres (e.g., McLandress et al. 1996; Xu et al. 2009b; Pancheva et al. 2009a). Pancheva et al. (2009a) noted that the seasonal cycles in the SW2 tidal temperature amplitudes determined from SABER observations are not symmetric. At 90 km, the amplitude of SW2 at both 40°N and 40°S has an annual cycle, but the NH maximum is in winter (December–February) while the SH maximum is in late fall (May). Hemispheric differences in tides are also simulated in global models (for example, see Fig. 9), but there has not been been much effort to catalog and explain these differences.
As discussed in Sect. 4.1, gravity waves are normally difficult to determine from global measurements. Much of the information about large-scale hemispheric differences in MLT gravity waves comes from inferences in global models, particularly the impact of filtering by stratospheric winds. The impact of filtering is large and important, and it appears, to first order, to be well-simulated by the parameterizations in global models.
Although the filtering of gravity waves in the stratosphere is undoubtedly important, the gravity wave sources may also play a role. There are important gaps in knowledge about hemispheric differences in gravity wave sources and in the actual wave propagation (lateral as well as vertical). Coarse-resolution global models are a poor tool for addressing these issues. The new generation of high-resolution GCMs that resolve gravity wave generation and propagation, such as that described by Sato et al. (2009), will be a helpful tool in addressing this question.
On the other hand, interpretation of gravity wave observations by radars at selected NH and SH sites can be complicated because it is difficult to separate local factors from those affecting a broader area. With the limited number of observation sites available, it is not possible to determine to what extent differences such as seasonal changes are affected by the local surface topography, stratospheric planetary waves, etc., rather than the regional mean conditions. Dowdy et al. (2007) compared the gravity wave activity measured at high latitude radar stations in the NH and SH (two radar sites in each; separated in longitude). In both hemispheres, there was a strong seasonal change in wave activity but the seasonal cycles differed between sites and also with altitude. Overall there was a summer maximum in gravity wave activity at all four sites.
7 Trends and Variations on Multiyear Timescales
Trends in the basic state dynamical fields of the MLT are expected from three causes: changes in the composition of radiatively active gases, changes in wave fluxes from below, and changes in energy input associated with solar activity. Diagnosing of trends is affected by the short records of many observing systems and the high natural variability of the MLT.
The second concern with the mismatch between pressure and altitude coordinates is the effect on comparisons between numerical models (usually with pressure as a vertical coordinate) and observations (many give profiles as a function of geometric altitude). A comparison that does not convert the vertical profiles to the same vertical coordinate system is not trustworthy and may be strongly misleading.
For most MLT observations, the trend analysis is affected by the relatively short observational record. Temperature, for example, is expected to be affected simultaneously by trends in anthropogenic greenhouse gases, changes in composition due to other tropospheric gases, and variations in solar flux and composition due to the solar cycle. Because of these competing or reinforcing processes, disentangling the drivers of the trends and variations is not possible using observations alone. While model simulations have their own problems, they are invaluable in giving guidance about the magnitude and basic structure of the mesospheric response to various applied changes.
7.1 Long-term Trends
Attributing changes in the MLT temperature to composition or other changes must be done carefully. One challenge, as discussed above, is the change in the height of pressure surfaces with the temperature in the underlying column. This is particularly an issue for changes in greenhouse gases, whose effects are felt in the troposphere and entire middle atmosphere. Through a modification of the pressure/altitude relation, the influence of greenhouse gases that have negligible concentrations in the MLT, such as methane (CH4) and CFC12 (CF2Cl2), could nevertheless be felt there. Likewise changes in stratospheric ozone can affect wave propagation (see Sect. 5.2) as well as the column temperature (Bremer and Peters 2008). These remote effects are not included in the list of anthropogenic gases that affect the MLT, given below.
Changes in composition can also directly affect the chemistry and radiative balance of the MLT. Several gases that are known to have undergone long-term changes can also affect the MLT basic structure or dynamics.
Infrared emission by CO2 is the most important cooling process in the MLT (Feofilov and Kutepov 2012). CO2 radiative transfer also gives seasonal weak heating at the cold summer mesopause. Higher concentrations of CO2 lead to higher cooling rates. The global tendency associated with this change is for an increase in CO2 to cause increased cooling and lower temperatures.
Methane is produced at the Earth’s surface from natural and anthropogenic sources. Methane that is transported into the middle atmosphere is oxidized in the stratosphere and lower mesosphere. The hydrogen released forms water (two water molecules for each methane) and contributes about half of the total amount of water above the stratopause. Measurements indicate that methane in the lower atmosphere has been increasing in recent decades although the trend is not monotonic.
H 2 O
Photolysis of water is the main source of reactive hydrogen (HOx, defined as the sum of H, OH, and HO2) in the MLT. Middle atmosphere water has been increasing in part due to the increase in CH4 although there are also trends in the water entering from the troposphere to the stratosphere over the past several decades (Fujiwara et al. 2010). Trends in HOx have an important impact on mesospheric ozone, which is important for the radiative balance in the MLT (both as an absorber of solar ultraviolet radiation and as a component in chemical heating). Marsh et al. (2003) showed the response of ozone to trends in water in the mesosphere.
Another potential source of trends in MLT dynamics is from the waves that drive the circulation. There are several reasons to expect that the sources of gravity waves could change as the Earth’s climate changes. An important forcing is by tropical convection in the troposphere. As the thermal structure in the troposphere changes, the forcing of these waves will change as well. Becker (2009) used a gravity wave-resolving model to look at the differences with two different radiative forcings designed to represent the warming of the troposphere due to greenhouse gases. No differences were imposed on any other part of the model. The results of the Becker (2009) simulations showed an increase in gravity wave activity with the climate warming.
There is contradictory information about possible trends in MLT gravity waves. Offermann et al. (2011b) used standard deviation of temperature derived from nighttime airglow emitted at about 87 km as a proxy for gravity wave activity. They found an average seasonal cycle that fit with expectations from WACCM and they also found long-term variations. The long-term variations show different trends at the two different sites and were different for subsets of the 15-year analysis period; it is therefore not evident that there is any connection to long-term climate change. Hoffmann et al. (2011) showed observations of trends in gravity wave activity over a midlatitude site. The gravity wave activity changes were consistent with filtering by changing average winds in the mesosphere. As discussed in Sect. 4.1, filtering is a first-order process controlling the gravity waves that reach the MLT. Unfortunately, with the measurements available today, it is not possible to determine definitively to what extent observed changes in gravity waves are due to filtering by middle atmosphere winds and to what extent changing sources or other changes in local conditions contribute.
Jacobi et al. (2012) and Keuer et al. (2007) also reported on NH midlatitude MLT wind trends. Jacobi et al. (2012) noted the differences in the trends between North America and Europe, suggesting that changes in planetary waves contributed to the trends.
Trends in tidal sources can also occur, due either to tropospheric warming or to stratospheric ozone changes. Tides are excited in part by latent heat release in tropical convection and also have major sources from the solar radiation absorbed by tropospheric water vapor and stratospheric ozone. If the atmosphere warms while the relative humidity stays constant, the column will contain more water, which would imply a stronger tidal source in the troposphere. Stratospheric ozone decrease (and predicted recovery in upcoming decades) due to anthropogenic chlorine and bromine could affect tidal forcing in the stratosphere. In addition, the ozone heating has a solar cycle variation of several percent due to higher ozone and higher ultraviolet flux during solar maximum conditions.
A recent paper by Beig (2011a) summarizes the observations of trends in the MLT. The reported trends in temperature from different regions and different types of instrumentation still are not in agreement. For a global picture, Beig (2011a) emphasizes the trends derived from HALOE satellite observations by Remsberg (2007, 2009), Remsberg et al. (2008). Those observations indicate very weak cooling in the MLT region. However, the duration of the measurements is not long so the uncertainty in the magnitude and structure of the trends is high.
A long-time record that is sometimes used for trends is the frequency of polar mesospheric clouds, PMCs (e.g., Qian et al. 2011). This is particularly true in the NH, where observations go back to the nineteenth century. However, while the presence of PMCs depends sensitively on temperature, it also depends on water vapor content and possibly also on the distribution of cloud condensation nuclei. Therefore, efforts to deduce a temperature trend from these data encounter many uncertainties.
Simulations with global models are important in predicting the magnitude and vertical structure of trends. Because of the highly interactive nature of the energetics of the MLT, such simulations should include interactive chemistry and energetics, even if the goal is to describe the dynamical trends. Garcia et al. (2007) present WACCM simulations of the temperature trend over the period 1950–2003. These simulations include observed sea surface temperature and observed changes in anthropogenic gases and solar flux. The magnitude of the trend in temperature is at a local minimum in the MLT; it is negative with a magnitude of less than 0.5 K/decade. In a study using a mechanistic middle atmosphere, Berger and Lübken (2011) perform several simulations to determine what factors are most important in the trends. They note the importance of ozone loss in the stratosphere and its impact on the temperature. Unfortunately, comparisons of trends between models is difficult because of the different vertical grids: Berger and Lübken (2011) show most of their results on an altitude scale while Garcia et al. (2007) use pressure.
7.2 Variations due to Solar and Charged Particle Forcing
The MLT responds to variations in the solar flux and to variations in energetic particle precipitation into the region. Heating in the MLT can also be affected indirectly by the transport of gases from the thermosphere. Both of these forcing processes vary on long timescales, including the approximate 11-year period of the sunspot cycle. The solar flux in the Schumann-Runge bands and Schumann-Runge continuum varies in phase with the solar cycle. The differences between solar minimum and solar maximum include changes in the temperature, the atmospheric density structure, and the composition.
The flux of energetic particles is intermittent but is more likely to occur when the Sun is active. Events are more common at solar maximum and in the declining phase of the solar cycle. The companion papers by Feofilov and Kutepov (2012) and Sinnhuber (2012) discuss these in more detail.
The mean dynamical response to solar flux variations are coupled with the photochemistry (Marsh et al. 2007). If there were no changes in composition, an increase in flux would lead to additional heating, increasing the mean temperature and the amplitude of the diurnally varying heating rate. Observations of the MLT response to the solar cycle summarized by Beig et al. (2003, 2008) and Beig (2011b) do show that the temperature is higher during periods of high solar activity although the magnitude of the warming differs in different analyses.
As is the case for the response of the atmosphere to anthropogenic gases, models provide guidance about the response of the MLT to solar variability. Model studies by Marsh et al. (2007) and Schmidt et al. (2006) emphasize the interactive chemistry and its contribution to the net trend in temperature. One of the important radiative gases is ozone, which itself has a marked solar cycle response due to the changes in both production and loss rates. The ozone production (a byproduct of O2 photolysis) is positively correlated with the solar ultraviolet flux. The ozone loss rates in the mesosphere due to photolysis and catalytic reactions involving HOx molecules are also positively correlated with the solar ultraviolet flux. As a result, ozone itself can have either a positive or negative correlation, depending on details of the chemistry.
The relative magnitude of the variability of the solar flux varies with the energy in the solar spectrum. The timing also varies; i.e. the timing of the maximum flux shifts with the wavenumber of the radiation. Empirical models relating the variability in each wavenumber interval to an easily observed parameter such as the 10.7-cm flux (with a long record of daily ground-based observations) provide input fields needed for investigating the atmospheric response. Data to put together such models come from spectrally resolved observations from satellite.
The model described by Lean et al. (1997) and Lean (2000) has been used in a number of middle atmosphere models; see for example Eyring et al. (2006). The importance of the model, in particular the spectral makeup of the solar cycle variability, has been the focus of much discussion recently because of new observations from the Spectral Irradiance Monitor (SIM) on the SORCE satellite. SIM solar fluxes for the years 2004–2007 indicate that the solar variability for wavenumbers >200 nm is different than that in the Lean (2000) model (Harder et al. 2009; Fontenla et al. 2011). In particular, during solar maximum conditions the solar flux at 200–400 nm is substantially higher while that at wavenumbers >400 nm has the opposite sign (lower solar flux during solar maximum).
Numerical model studies using solar variability based on the SIM data by Haigh et al. (2010) and Merkel et al. (2011) focussed on the simulation of the solar cycle response of ozone in the stratosphere and lower mesosphere. In both cases, the models indicated expanded altitude ranges where the ozone response was negative (i.e., lower ozone concentrations for higher solar activity). Observational analysis of ozone measures by the Microwave Limb Sounder (MLS) (Haigh et al. 2010) and SABER (Merkel et al. 2011) agreed in some ways and disagreed in others with the simulations using SIM solar variability. Future work to extend the SIM model over a full solar cycle is needed to fully address this question. The response of temperature in the MLT was not presented in the model studies that have been published as of this writing.
Understanding of the dynamics of the MLT region continues to evolve as new measurements and analysis techniques are developed and numerical models include better representations of physical processes. This review paper describes an overview of the basic state and processes involved in large-scale dynamics. The review describes some of the developments in past decade.
The development of several comprehensive whole atmosphere numerical models allows for the investigation of interactions of the MLT with the troposphere and stratosphere below and the thermosphere above, as well as interactions between dynamics and chemistry.
There is now recognition of the importance of nonmigrating tides. The new recognition is based on new observations that have enabled a more complete characterization of the global structure of these tidal modes.
Evidence for connections in tides and mean temperatures between the winter stratosphere and the summer MLT is evidence of global coupling. There are still uncertainties but it appears that the mechanism for the coupling involves wave propagation, background wind and temperature changes, and the large-scale circulation.
The recent publication of new data for the variations of spectrally resolved solar flux with the 11-year solar cycle raises questions about the solar cycle and the atmospheric response.
Observations of temperature and trace species perturbations during active periods in NH winter have shown strong transport and changes in the mesosphere that had not been previously seen. Characterization of the dynamics and transport during these periods has led to the better understanding of the vertical coupling in the polar winter middle atmosphere.
Two long-lived (ongoing) satellites, TIMED and Envisat, have provided global data of the middle atmosphere for better characterization of climatology, interannual variability, and the interactions of dynamics with chemistry. This has been particularly valuable in the past decade because of highly active and variable dynamics in the NH winter middle atmosphere. The existing network of ground-based measurement systems has also increased; the combination of global satellite observations and detailed but localized ground-based data has been exploited in some investigations but holds the potential for further application to characterize and understand coupling across horizontal scales.
Future advances in understanding the MLT will be much reduced if there is an end to, or a gap in, observations by satellite that span the MLT region. This is a major threat to progress that cannot be compensated for by enhanced ground-based observing capabilities and state-of-the-art numerical models.
The National Center for Atmospheric Research is sponsored by the National Science Foundation. This paper benefited from helpful comments by E. Becker, R. R. Garcia, and V. Yudin.
- Akmaev RA (2011) Whole atmosphere modeling: connecting terrestrial and space weather. Rev Geophys 49:RG4004. doi: 10.1029/2011RG000364
- Akmaev RA, Fomichev VI (1998) Cooling of the mesosphere and lower thermosphere due to doubling of CO2. Ann Geophys 16:1501–1512Google Scholar
- Akmaev RA, Fuller-Rowell TJ, Wu F, Forbes JM, Zhang X, Anghel AF, Iredell MD, Moorthi S, Juang HM (2008) Tidal variability in the lower thermosphere: comparison of whole atmosphere model (WAM) simulations with observations from TIMED. Geophys Res Lett 86:L03810. doi: 10.1029/2007GL032584 CrossRefGoogle Scholar
- Andrews DG, Holton JR, Leovy CB (1987) Middle atmosphere dynamics. Academic Press, San DiegoGoogle Scholar
- Aso T (2007) A note on the semidiurnal non-migrating tide at polar latitudes. Earth Planets Space 59:21–24Google Scholar
- Becker E (2011) Dynamical control of the middle atmosphere. Space Sci Rev (Online First) doi: 10.1007/s11214-011-9841-5
- Becker E, Fritts DC (2006) Enhanced gravity-wave activity and interhemispheric coupling during the MaCWAVE/MIDAS northern summer program 2002. Ann Geophys 60:103–118Google Scholar
- Beig G, Keckhut P, Lowe R, Roble R, Mlynczak M, Scheer J, Fomichev V, Offermann D, French W, Shepherd M, Semenov A, Remsberg E, She C, Lubken F, Bremer J, Clemesha B, Stegman J, Sigernes F, Fadnavis S (2003) Review of mesospheric temperature trends. Rev Geophys 41:1015. doi: 10.1029/2002RG000121 CrossRefGoogle Scholar
- Chandran A, Rusch DW, Merkel AW, Palo SE, Thomas GE, Taylor MJ, Bailey SM, Russell JM III (2010) Polar mesospheric cloud structures observed from the cloud imaging and particle size experiment on the aeronomy of ice in the mesosphere spacecraft: atmospheric gravity waves as drivers for longitudinal variability in polar mesospheric cloud occurrence. J Geophys Res 38:D13102. doi: 10.1029/2009JD013185 CrossRefGoogle Scholar
- Chapman S, Lindzen RS (1970) Atmospheric tides. Gordon and Breach, New YorkGoogle Scholar
- Drob DP, Emmert JT, Crowley G, Picone JM, Shepherd GG, Skinner W, Hays P, Niciejewski RJ, Larsen M, She CY, Meriwether JW, Hernandez G, Jarvis MJ, Sipler DP, Tepley CA, OBrien MS, Bowman JR, Wu Q, Murayama Y, Kawamura S, Reid IM, Vincent RA (2008) An empirical model of the earths horizontal wind fields: HWM07. J Geophys Res 113:A12304. doi: 10.1029/2008JA013668 CrossRefGoogle Scholar
- Eyring V, Butchart N, Waugh DW, Akiyoshi H, Austin J, Bekki S, Bodeker GE, Boville BA, Brühl C, Chipperfield MP, Cordero E, Dameris M, Deushi M, Fioletov VE, Frith SM, Garcia RR, Gettelman A, Giorgetta MA, Grewe V, Jourdain L, Kinnison DE, Mancini E, Manzini E, Marchand M, Marsh DR, Nagashima T, Nielsen E, Newman PA, Pawson S, Pitari G, Plummer DA, Rozanov E, Schraner M, Shepherd TG, Shibata K, Stolarski RS, Struthers H, Tian W, Yoshiki M (2006) Assessment of temperature, trace species and ozone in chemistry-climate simulations of the recent past. J Geophys Res 111(D22):D22308. doi: 10.1029/2006JD007327 CrossRefGoogle Scholar
- Eyring V, Shepherd TG, Waugh DW (eds) (2010) SPARC Report on the Evaluation of Chemistry-Climate Models. WCRP-132, WMO/TD-No.1526Google Scholar
- Feofilov AG, Kutepov AA (2012) Infrared radiance in the mesosphere and lower thermosphere. Surv Geophys This issueGoogle Scholar
- Fontenla JM, Harder J, Livingston W, Snow M, Woods T (2011) High-resolution solar spectral irradiance from extreme ultraviolet to far infrared. J Geophys Res 116:D20108. doi: 10.1029/2011JD016032
- Forbes JM, Zhang X, Palo SE, Russell J, Mertens CJ, Mlynczak M (2009) Kelvin waves in stratosphere, mesosphere and lower thermosphere temperatures as observed by TIMED/SABER during 2002–2006. Earth Planets Space 61:447–453Google Scholar
- Fujiwara M, Vomel H, Hasebe F, Ogino S-Y, Iwasaki S, Nishi N, Shibata T, Shimizu K, Nishimoto E, Valverde Canossa JM, Selkirk HB, Oltmans SJ (2010) Seasonal to decadal variations of water vapor in the tropical lower stratosphere observed with balloon-borne cryogenic frost point hygrometers. J Geophys Res 115:D18304. doi: 10.1029/2010JD014179 CrossRefGoogle Scholar
- Garcia RR, Dunkerton TJ, Lieberman RS, Vincent RA (1997) Climatology of the semiannual oscillation of the tropical middle atmosphere. J Geophys Res 102:26,019–26,032Google Scholar
- Grygalashvyly M, Becker E, Sonnemann G (2011) Gravitywave mixing and effective diffusivity for minor chemical constituents in the mesosphere/lower thermosphere. Space Sci Rev (Online First) doi: 10.1007/s11214-011-9857-x
- Iimura H, Palo SE, Wu Q, Killeen TL, Solomon SC, Skinner WR (2009) Structure of the nonmigrating semidiurnal tide above Antarctica observed from the TIMED Doppler Interferometer. J Geophys Res 114:D11102. doi: 10.1029/2008JD010608
- Jacobi C, Hoffmann P, Liu R, Merzlyakov E, Portnyagin Y, Manson A, Meek C (2012) Long-term trends, their changes, and interannual variability of northern hemisphere midlatitude MLT windsl. J Atmos Solar Terr Phys 75–76:81–89. doi: 10.1016/j.jastp.2011.03.016
- Kvissel OK, Orsolini YJ, Stordal F, Limpasuvan V, Richter J, Marsh DR (2012) Mesospheric intrusion and anomalous chemistry during and after a major stratospheric sudden warming. J Atmos Solar Terr Phys 78–79:116–124. doi: 10.1016/j.jastp.2011.08.015
- Lean JL, Rottman GJ, Kyle HL, Woods TN, Hickey JR, Puga LC (1997) Detection and parameterization of variations in solar midand near-ultraviolet radiation (200–400 nm). J Geophys Res 102:29939–29956Google Scholar
- Lieberman RS, Smith AK, Franke SJ, Vincent RA, Isler JR, Manson AH, Meek CE, Fraser GJ, Fahrutdinova A, Thayaparan T, Hocking W, MacDougall J, Nakamura T, Tsuda T (2000) Comparison of mesospheric and lower thermospheric residual wind with High Resolution Doppler Imager, medium frequency, and meteor radar winds. J Geophys Res 105:27,023–27,035Google Scholar
- Limpasuvan V, Richter JH, Orsolini YJ, Stordal F, Kvissel O (2011) The roles of planetary and gravity waves during a major stratospheric sudden warming as characterized in WACCM. J Atmos Solar Terr Phys 73. doi: 10.1016/j.jastp.2011.03.004
- Liu HL (2000) Temperature changes due to gravity wave saturation. J Geophys Res 105:12,329–12,336Google Scholar
- Liu HL, Foster BT, Hagan ME, McInerney JM, Maute A, Qian L, Richmond AD, Roble RG, Solomon SC, Garcia RR, Kinnison D, Marsh DR, Smith AK, Richter J, Sassi F, Oberheide J (2010) Thermosphere extension of the whole atmosphere community climate model. J Geophys Res 115:A12302. doi: 10.1029/2010JA015586 CrossRefGoogle Scholar
- Manney GL, Krüger K, Pawson S, Minschwaner K, Schwartz MJ, Daffer WH, Livesey NJ, Mlynczak MG, Remsberg EE, Russell JM III, Waters JW (2008) The evolution of the stratopause during the 2006 major warming: satellite data and assimilated meteorological analyses. J Geophys Res 113:D11115. doi: 10.1029/2007JD009097 CrossRefGoogle Scholar
- Manney GL, Schwartz MJ, Krüger K, Santee ML, Pawson S, Lee JN, Daffer WH, Fuller RA, Livesey NJ (2009) Aura Microwave Limb Sounder observations of dynamics and transport during the record-breaking 2009 Arctic stratospheric major warming. Geophys Res Lett 36:L12815. doi: 10.1029/2009GL038586 CrossRefGoogle Scholar
- Marsh DR (2011) Chemical-dynamical coupling in the mesosphere and lower thermosphere. In: Abdu M, Pancheva D, Bhattacharyya A (eds) Aeronomy of the Earth’s atmosphere and ionosphere, IAGA Special Sopron Book Ser., vol 2. Springer, DordrechtGoogle Scholar
- McLandress C, Shepherd GG, Solheim BH, Burrage MD, Hays PB, Skinner WR (1996) Combined mesosphere/thermosphere winds using WINDII and HRDI data from the Upper Atmosphere Research Satellite. J Geophys Res 101:10,441–10,453Google Scholar
- Mlynczak MG, Solomon S (1993) A detail evaluation of the heating efficiency in the middle atmosphere. J Geophys Res 98:10,517–10,541Google Scholar
- Murphy DJ, Forbes JM, LWalterscheid R, Hagan ME, Avery SK, Aso T, Fraser GJ, Fritts DC, Jarvis MJ, McDonald AJ, Riggin DM, Tsutsumi M, Vincent RA (2006) A climatology of tides in the Antarctic mesosphere and lower thermosphere. J Geophys Res 111. doi: 10.1029/2005JD006803
- Niciejewski R, Skinner W, Cooper M, Marshall A (2011) Resolving dynamics structure in the MLT: correlative measurements with TIDI and HRDI. Abstract SA33A-07 presented at 2011 Fall meeting, AGU, San Francisco, California, 5–9 DecGoogle Scholar
- Orsolini YJ, Urban J, Murtagh DP, Lossow S, Limpasuvan V (2010) Descent from the polar mesosphere and anomalously high stratopause observed in 8 years of water vapor and temperature satellite observations by the Odin Sub-Millimeter Radiometer. J Geophys Res 115:D12305. doi: 10.1029/2009JD013501 CrossRefGoogle Scholar
- Pancheva D, Merzlyakov E, Mitchell NJ, Portnyagin Y, Manson AH, Jacobi C, Meek CE, Luo Y, Clark RR, Hocking W, MacDougall J, Muller HG, Kurschner D, Jones GOL, Vincent RA, Reid IM, Singer W, Igarashi K, Fahrutdinova GIFNAN, Stepanov AM, Poole LMG, Malinga SB, Kashcheyev BL, Oleynikov AN (2002) Global-scale tidal structure in the mesosphere & lower thermosphere during the PSMOS campaign summer-99 and comparison with the global scale wave model. J Atmos Solar Terr Phys 64:1011–1035CrossRefGoogle Scholar
- Pancheva D, Mukhtarov P, Mitchell NJ, Merzlyakov E, Smith A, Andonov B, Singer W, Hocking W, Meek C, Manson A, Murayama Y (2008) Planetary waves in coupling the stratosphere and mesosphere during the major stratospheric warming in 2003/2004. J Geophys Res 113:D12105. doi: 10.1029/2007JD009011 CrossRefGoogle Scholar
- Pancheva D, Mukhtarov P, Andonov B, Mitchell NJ, Forbes JM (2009a) Planetary waves observed by TIMED/SABER in coupling the stratosphere–mesosphere–lower thermosphere during the winter of 2003/2004: part 1, Comparison with the ukmo temperature results. J Atmos Solar Terr Phys 71:61–74CrossRefGoogle Scholar
- Pancheva D, Mukhtarov P, Andonov B, Mitchell NJ, Forbes JM (2009b) Planetary waves observed by TIMED/SABER in coupling the stratosphere–mesosphere–lower thermosphere during the winter of 2003/2004: part 2, altitude and latitude planetary wave structure. J Atmos Solar Terr Phys 71:75–87CrossRefGoogle Scholar
- Portnyagin YI, Forbes JM, Makarov NA, Merzlyakov EG, Palo S (1998) The summertime 12-hour wind oscillation with zonal wavenumber s = 1 in the lower thermosphere over the South Pole. Ann Geophys 16:828–837Google Scholar
- Remsberg EE, Marshall BT, Garcia-Comas M, Krueger D, Lingenfelser GS, Martin-Torres J, Mlynczak MG, Russell JM III, Smith AK, Zhao Y, Brown C, Gordley LL, Lopez-Gonzalez MJ, Lopez-Puertas M, She CY, Taylor MJ, Thompson RE (2008) Assessment of the quality of the Version 1.07 temperature-versus-pressure profiles of the middle atmosphere from TIMED/SABER. J Geophys Res 113:D17101. doi: 10.1029/2008JD010013 CrossRefGoogle Scholar
- Shine KP (1987) The middle atmosphere in the absence of dynamical heat fluxes. Q J R Meteorol Soc 113:603–633Google Scholar
- Sinnhuber M (2012) Energetic particle precipitation and the chemistry of the mesosphere/lower thermosphere. Surv Geophys This issueGoogle Scholar
- Smith AK (2011) Interactions between the lower, middle and upper atmosphere. Space Sci Rev (Online First) doi: 10.1007/s11214-011-9791-y
- Smith AK, Garcia RR, Marsh DR, Kinnison DE, Richter JH (2010b) Simulations of the response of mesospheric circulation and temperature to the Antarctic ozone hole. Geophys Res Lett 37:L22803. doi: 10.1029/2010GL045255
- Takahashi H, Wrasse CM, Fechine J, Pancheva D, Abdu MA, Batista IS, Lima LM, Batista PP, Clemesha BR, Schuch NJ, Shiokawa K, Gobbi D, Mlynczak MG, Russell JM (2007) Signatures of ultra fast Kelvin waves in the equatorial middle atmosphere and ionosphere. Geophys Res Lett 34:L11108. doi: 10.1029/2007GL029612 CrossRefGoogle Scholar
- Taylor MJ, Pendelton WR Jr, Clark S, Takahashi H, Gobbi D, Goldberg RA (1997) Image measurements of short-period gravity waves at equatorial latitudes. J Geophys Res 102:26,283–26,299Google Scholar
- Taylor MJ, Pendelton WR Jr, Gardner CS, States RJ (1999) Comparison of terdiurnal tidal oscillations in mesospheric OH rotational temperature and Na lidar temperature measurements at mid-latitudes for fall/spring conditions. Earth Planets Space 51:877–885Google Scholar
- WMO (2010) Scientific assessment of ozone depletion: 2010. Global Ozone Research and Monitoring Project-Report No 52. Geneva, SwitzerlandGoogle Scholar
- Wu Q, Ortland DA, Killeen TL, Roble RG, Hagan ME, Liu HL, Solomon SC, Xu J, Skinner WR, Niciejewski RJ (2008) Global distribution and interannual variations of mesospheric and lower thermospheric neutral wind diurnal tide: 1. Migrating tide. J Geophys Res 113:A05308. doi: 10.1029/2007JA012542 CrossRefGoogle Scholar
- Xu J, Liu H, Smith A, Roble R, Mertens C, Russell J III, Mlynczak M (2007a) Mesopause structure from thermosphere, ionosphere, mesosphere, energetics and dynamics (TIMED)/sounding of the atmosphere using broadband emission radiometry (SABER) observations. J Geophys Res 112:D09102. doi: 10.1029/2006JD007711 CrossRefGoogle Scholar
- Xu J, Smith AK, Liu H, Yuan W, Wu Q, Jiang G, Mlynczak MG, Russell J III, Franke SJ (2009) Seasonal and quasi-biennial variations in the migrating diurnal tide observed by thermosphere, ionosphere, mesosphere, energetics and dynamics (TIMED). J Geophys Res 114:D13107. doi: 10.1029/2008JD011298 CrossRefGoogle Scholar
- Younger PT, Pancheva D, Middleton HR, Mitchell NJ (2002) The 8h tide in the Arctic mesosphere and lower thermosphere. J Geophys Res 1420. doi: 10.1029/2001JA005086
- Zhang X, Forbes JM, Hagan ME, Russell III JM, Palo SE, Mertens CJ, Mlynczak MG (2006) Monthly tidal temperatures 20–120 km from TIMED/SABER. J Geophys Res 111. doi: 10.1029/2005JA011504. EID A10S08