Seasonal Variations of Low‐Latitude Migrating and Nonmigrating Diurnal and Semidiurnal Tides in TIMED‐SABER Temperature and Their Relationship With Source Variations
Seasonal and source variations of migrating and nonmigrating tides are studied using Thermosphere‐Ionosphere‐Mesosphere Energetics and Dynamics‐Sounding of the Atmosphere using Broadband Emission Radiometry temperature data at 10°N (5–15°N) for the year 2009. The migrating DW1 shows equinoctial maxi...
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description | Seasonal and source variations of migrating and nonmigrating tides are studied using Thermosphere‐Ionosphere‐Mesosphere Energetics and Dynamics‐Sounding of the Atmosphere using Broadband Emission Radiometry temperature data at 10°N (5–15°N) for the year 2009. The migrating DW1 shows equinoctial maximum and summer minimum at low latitudes. It shows equinoctial asymmetry with larger amplitudes during spring equinox than fall equinox. The migrating semidiurnal tidal amplitude (SW2) shows larger amplitudes (~20 K) during March–October at 30–60°S. Its seasonal variation resembles stratospheric (10 hPa) ozone variations at southern midlatitudes. During the sudden stratospheric warming of 2009, the SW1 shows larger amplitudes over the equator and it is generated due to nonlinear interaction between SW2 and planetary wave of zonal wave number 1. The eastward nonmigrating DE4 and DE3 tides enhance in summer. The DE3 and DE4 appear to be generated due to latent heat release in the troposphere, as their amplitudes in the National Center for Environmental Prediction (NCEP)'s Precipitable water vapor (proxy for latent heat release) enhance at similar times as in mesosphere. The DW2 and DW0 tides are likely to be generated due to nonlinear interaction between DW1 and planetary wave of zonal wave number 1. The SW3 enhancement during the early winter (November‐December) may be due to nonlinear interaction between DW1 and the large‐amplitude DW2. The nonlinear interactions of DW1 with planetary wave and nonmigrating tides explain the summer minimum and equinoctial asymmetry of DW1.
Key Points
The migrating DW1 tide shows semiannual variation with larger amplitudes during equinox months
DE3 and DE4 tides maximize in summer, when DW1 shows less amplitude and they are generated due to latent heat release in tropical convection
The SW2 shows larger amplitudes during March‐October and its seasonal variation resembles that of 10‐hPa ozone at 30–60°S |
doi_str_mv | 10.1029/2018JA026190 |
format | Article |
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Key Points
The migrating DW1 tide shows semiannual variation with larger amplitudes during equinox months
DE3 and DE4 tides maximize in summer, when DW1 shows less amplitude and they are generated due to latent heat release in tropical convection
The SW2 shows larger amplitudes during March‐October and its seasonal variation resembles that of 10‐hPa ozone at 30–60°S</description><identifier>ISSN: 2169-9380</identifier><identifier>EISSN: 2169-9402</identifier><identifier>DOI: 10.1029/2018JA026190</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Amplitudes ; Asymmetry ; Broadband ; Diurnal variations ; Equator ; Equinoxes ; Heat transfer ; Ionosphere ; Latent heat ; Latent heat release ; Latitude ; Mesosphere ; migrating tides ; nonmigrating tides ; Ozone ; Ozone variations ; Planetary waves ; Precipitable water ; Radiometry ; Seasonal variations ; stratospheric ozone ; Stratospheric warming ; Summer ; Temperature ; Temperature data ; Thermosphere ; Tidal amplitude ; Tides ; TIMED‐SABER ; Troposphere ; Water vapor ; Wavelengths ; Zonal waves</subject><ispartof>Journal of geophysical research. Space physics, 2019-05, Vol.124 (5), p.3558-3572</ispartof><rights>2019. American Geophysical Union. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c3077-64807ce939bfa4a97162125fe806506ed81bb1e74d7e3980d64a73e348d870823</citedby><cites>FETCH-LOGICAL-c3077-64807ce939bfa4a97162125fe806506ed81bb1e74d7e3980d64a73e348d870823</cites><orcidid>0000-0002-0327-3085</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1029%2F2018JA026190$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1029%2F2018JA026190$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,780,784,1417,1433,27924,27925,45574,45575,46409,46833</link.rule.ids></links><search><creatorcontrib>Sridharan, S.</creatorcontrib><title>Seasonal Variations of Low‐Latitude Migrating and Nonmigrating Diurnal and Semidiurnal Tides in TIMED‐SABER Temperature and Their Relationship With Source Variations</title><title>Journal of geophysical research. Space physics</title><description>Seasonal and source variations of migrating and nonmigrating tides are studied using Thermosphere‐Ionosphere‐Mesosphere Energetics and Dynamics‐Sounding of the Atmosphere using Broadband Emission Radiometry temperature data at 10°N (5–15°N) for the year 2009. The migrating DW1 shows equinoctial maximum and summer minimum at low latitudes. It shows equinoctial asymmetry with larger amplitudes during spring equinox than fall equinox. The migrating semidiurnal tidal amplitude (SW2) shows larger amplitudes (~20 K) during March–October at 30–60°S. Its seasonal variation resembles stratospheric (10 hPa) ozone variations at southern midlatitudes. During the sudden stratospheric warming of 2009, the SW1 shows larger amplitudes over the equator and it is generated due to nonlinear interaction between SW2 and planetary wave of zonal wave number 1. The eastward nonmigrating DE4 and DE3 tides enhance in summer. The DE3 and DE4 appear to be generated due to latent heat release in the troposphere, as their amplitudes in the National Center for Environmental Prediction (NCEP)'s Precipitable water vapor (proxy for latent heat release) enhance at similar times as in mesosphere. The DW2 and DW0 tides are likely to be generated due to nonlinear interaction between DW1 and planetary wave of zonal wave number 1. The SW3 enhancement during the early winter (November‐December) may be due to nonlinear interaction between DW1 and the large‐amplitude DW2. The nonlinear interactions of DW1 with planetary wave and nonmigrating tides explain the summer minimum and equinoctial asymmetry of DW1.
Key Points
The migrating DW1 tide shows semiannual variation with larger amplitudes during equinox months
DE3 and DE4 tides maximize in summer, when DW1 shows less amplitude and they are generated due to latent heat release in tropical convection
The SW2 shows larger amplitudes during March‐October and its seasonal variation resembles that of 10‐hPa ozone at 30–60°S</description><subject>Amplitudes</subject><subject>Asymmetry</subject><subject>Broadband</subject><subject>Diurnal variations</subject><subject>Equator</subject><subject>Equinoxes</subject><subject>Heat transfer</subject><subject>Ionosphere</subject><subject>Latent heat</subject><subject>Latent heat release</subject><subject>Latitude</subject><subject>Mesosphere</subject><subject>migrating tides</subject><subject>nonmigrating tides</subject><subject>Ozone</subject><subject>Ozone variations</subject><subject>Planetary waves</subject><subject>Precipitable water</subject><subject>Radiometry</subject><subject>Seasonal variations</subject><subject>stratospheric ozone</subject><subject>Stratospheric warming</subject><subject>Summer</subject><subject>Temperature</subject><subject>Temperature data</subject><subject>Thermosphere</subject><subject>Tidal amplitude</subject><subject>Tides</subject><subject>TIMED‐SABER</subject><subject>Troposphere</subject><subject>Water vapor</subject><subject>Wavelengths</subject><subject>Zonal waves</subject><issn>2169-9380</issn><issn>2169-9402</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp9Uc1OAjEQbowmEuTmAzTxKtqf3W17RESEgCaw6nFT2FkogS22bAg3H8HX8LV8EpcfDScnmcz0m--bzmQQuqTkhhKmbhmhstsgLKKKnKAKo5Gqq4Cw09-cS3KOat7PSGmyhGhYQV9D0N7meo5ftTN6ZWzusc1wz66_Pz57JbAqUsB9M3Flnk-wzlP8ZPPFH3BvCrfVbwtDWJj08I5NCh6bHMedfuu-bDZs3LUGOIbFEkpp4WAniadgHB7AfP_31Czxm1lN8dAWbgxHU12gs0zPPdQOsYpeHlpx87Hee253mo1efcyJEPUokESMQXE1ynSglaARoyzMQJIoJBGkko5GFESQCuBKkjQKtODAA5lKQSTjVXS177t09r0Av0pmdreRTxjjSoWclV5F13vW2FnvHWTJ0pmFdpuEkmR7j-T4HiWd7-lrM4fNv9yk2x40wkAqwX8Aw-KOiQ</recordid><startdate>201905</startdate><enddate>201905</enddate><creator>Sridharan, S.</creator><general>Blackwell Publishing Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>8FD</scope><scope>H8D</scope><scope>KL.</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-0327-3085</orcidid></search><sort><creationdate>201905</creationdate><title>Seasonal Variations of Low‐Latitude Migrating and Nonmigrating Diurnal and Semidiurnal Tides in TIMED‐SABER Temperature and Their Relationship With Source Variations</title><author>Sridharan, S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3077-64807ce939bfa4a97162125fe806506ed81bb1e74d7e3980d64a73e348d870823</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Amplitudes</topic><topic>Asymmetry</topic><topic>Broadband</topic><topic>Diurnal variations</topic><topic>Equator</topic><topic>Equinoxes</topic><topic>Heat transfer</topic><topic>Ionosphere</topic><topic>Latent heat</topic><topic>Latent heat release</topic><topic>Latitude</topic><topic>Mesosphere</topic><topic>migrating tides</topic><topic>nonmigrating tides</topic><topic>Ozone</topic><topic>Ozone variations</topic><topic>Planetary waves</topic><topic>Precipitable water</topic><topic>Radiometry</topic><topic>Seasonal variations</topic><topic>stratospheric ozone</topic><topic>Stratospheric warming</topic><topic>Summer</topic><topic>Temperature</topic><topic>Temperature data</topic><topic>Thermosphere</topic><topic>Tidal amplitude</topic><topic>Tides</topic><topic>TIMED‐SABER</topic><topic>Troposphere</topic><topic>Water vapor</topic><topic>Wavelengths</topic><topic>Zonal waves</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sridharan, S.</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of geophysical research. Space physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sridharan, S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Seasonal Variations of Low‐Latitude Migrating and Nonmigrating Diurnal and Semidiurnal Tides in TIMED‐SABER Temperature and Their Relationship With Source Variations</atitle><jtitle>Journal of geophysical research. Space physics</jtitle><date>2019-05</date><risdate>2019</risdate><volume>124</volume><issue>5</issue><spage>3558</spage><epage>3572</epage><pages>3558-3572</pages><issn>2169-9380</issn><eissn>2169-9402</eissn><abstract>Seasonal and source variations of migrating and nonmigrating tides are studied using Thermosphere‐Ionosphere‐Mesosphere Energetics and Dynamics‐Sounding of the Atmosphere using Broadband Emission Radiometry temperature data at 10°N (5–15°N) for the year 2009. The migrating DW1 shows equinoctial maximum and summer minimum at low latitudes. It shows equinoctial asymmetry with larger amplitudes during spring equinox than fall equinox. The migrating semidiurnal tidal amplitude (SW2) shows larger amplitudes (~20 K) during March–October at 30–60°S. Its seasonal variation resembles stratospheric (10 hPa) ozone variations at southern midlatitudes. During the sudden stratospheric warming of 2009, the SW1 shows larger amplitudes over the equator and it is generated due to nonlinear interaction between SW2 and planetary wave of zonal wave number 1. The eastward nonmigrating DE4 and DE3 tides enhance in summer. The DE3 and DE4 appear to be generated due to latent heat release in the troposphere, as their amplitudes in the National Center for Environmental Prediction (NCEP)'s Precipitable water vapor (proxy for latent heat release) enhance at similar times as in mesosphere. The DW2 and DW0 tides are likely to be generated due to nonlinear interaction between DW1 and planetary wave of zonal wave number 1. The SW3 enhancement during the early winter (November‐December) may be due to nonlinear interaction between DW1 and the large‐amplitude DW2. The nonlinear interactions of DW1 with planetary wave and nonmigrating tides explain the summer minimum and equinoctial asymmetry of DW1.
Key Points
The migrating DW1 tide shows semiannual variation with larger amplitudes during equinox months
DE3 and DE4 tides maximize in summer, when DW1 shows less amplitude and they are generated due to latent heat release in tropical convection
The SW2 shows larger amplitudes during March‐October and its seasonal variation resembles that of 10‐hPa ozone at 30–60°S</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2018JA026190</doi><tpages>15</tpages><orcidid>https://orcid.org/0000-0002-0327-3085</orcidid></addata></record> |
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subjects | Amplitudes Asymmetry Broadband Diurnal variations Equator Equinoxes Heat transfer Ionosphere Latent heat Latent heat release Latitude Mesosphere migrating tides nonmigrating tides Ozone Ozone variations Planetary waves Precipitable water Radiometry Seasonal variations stratospheric ozone Stratospheric warming Summer Temperature Temperature data Thermosphere Tidal amplitude Tides TIMED‐SABER Troposphere Water vapor Wavelengths Zonal waves |
title | Seasonal Variations of Low‐Latitude Migrating and Nonmigrating Diurnal and Semidiurnal Tides in TIMED‐SABER Temperature and Their Relationship With Source Variations |
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