a study of a self generated stratospheric sudden warming and its mesospheric lower thermospheric impacts using the coupled time gcm ccm3 1 a stratospheric sudden warming episode was self consistently generated in the coupled national center for atmospheric research thermosphere ionosphere mesosphere and electrodynamics general circulation model climate community model version 3 time gcm ccm3 taking advantage of the unique vertical range of the coupled model ground to 500 km we were able to study the coupling of the lower and upper atmosphere in this warming episode planetary wave 1 is the dominant wave component in this warming event analysis of the wave phase structure and the wave amplitude indicates that the wave may experience resonant amplification prior to the peak warming the mean wind in the high latitude winter stratopause and mesosphere decelerates and reverses to westward due to planetary wave forcing and forms a critical layer near the zero wind lines the wind deceleration and reversal also change the filtering of gravity waves by allowing more eastward gravity waves to propagate into the mesosphere and lower thermosphere mlt which causes eastward forcing and reverses the westward jet in the mlt this also changes the meridional circulation in the upper mesosphere from poleward downward to equatorward upward causing a depletion of the peak atomic oxygen layer at 97 km and significant reduction of green line airglow emission at high latitudes and midlatitudes planetary waves forced in situ by filtered gravity waves in the mlt grow in the warming episode their growth and interaction with tides create diurnal and semidiurnal variabilities in the zonal mean zonal wind

intra annual variation of wave number 4 structure of vertical e b drifts in the equatorial ionosphere seen from rocsat 1 1 this paper studies the intra annual variation of the wave number 4 structure in the equatorial vertical e b drifts at high solar flux level based on of the rocsat 1 observations during the interval from 1999 to 2004 it is found that the daytime longitudinal structure is significant in northern summer and early autumn but weak in northern winter this is consistent with the intra annual variations of the tidal mode de3 at night the intra annual variation of the wave number 4 structure shows some differences from that in daytime which may relate to different dynamo mechanisms operating in different local time we also found that the wave number 4 structure mainly shifts eastward during daytime in most of months which is coincident with the eastward propagation of the de3 tide however it is largely disturbed near sunrise and sunset we attribute this disturbance as the jumping of the main dynamo region between e and f layers as well as the different dynamo mechanisms in different dynamo regions

isotopic constraints on the structural relationships between the lesser himalayan series and the high himalayan crystalline series garhwal himalaya nd and sr isotope systematics may provide important constraints on the location of major thrust systems that separate lithologically similar sedimentary sequences the potential of the technique is illustrated by this isotopic study of the main central thrust system of the himalaya nd isotope data from the garhwal himalaya indicate that metasedimentary rocks from the vaikrita group nd 14 to 19 correlate closely with those from the high himalayan crystalline series which constitutes the hanging wall lithologies of the main central thrust in contrast metasedimentary rocks from the munsiari group nd 23 to 28 show marked similarities to the lesser himalayan series in the footwall of the main central thrust sr isotopes support the correlations in that the vaikrita group shows partial reequilibration at 500 ma whereas the munsiari group has not undergone sr isotope homogenization since 1800 ma thus the vaikrita thrust that juxtaposes these two formations is recognized as the main central thrust in garhwal himalaya the thrust coincides approximately with the location of the kyanite isograd confirming that inverted metamorphism is characteristic of both hanging wall and footwall of the main central thrust along the tons thrust known locally as the srinagar thrust 50 km south of the main central thrust low grade quartzarenites with nd sr isotope and trace element characteristics typical of lesser himalayan formations have been emplaced on phyllites and siltstones with geochemical characteristics of the high himalayan crystalline series the field relationships most probably result from out of sequence thrusting in which lesser himalayan series rocks to the north were emplaced over low grade equivalents of the high himalayan crystalline series preserved in the external part of the orogen this study establishes the value of isotope data for lithostratigraphic correlations within orogenic belts

inverted metamorphism in the intracontinental ductile shear zone during himalayan collision tectonics collision tectonics in the himalaya ca 50 ma remobilized the proterozoic basement and its cover of the indian plate into the higher himalayan crystalline belt this belt displays an inverted metamorphism progressing from a garnet to a sillimanite k feldspar zone toward higher topographic and structural levels because previously hypothesized mechanisms are not sufficient to explain inverted metamorphism we propose that ductile shear displacements along ubiquitous closely spaced s c shear planes may have caused metamorphic inversion across a 15 20 km thick southwest vergent higher himalayan shear zone

wind driven processes controlling oceanic heat delivery to the amundsen sea antarctica variability in the heat delivery by circumpolar deep water cdw is responsible for modulating the basal melting of the amundsen sea ice shelves however the mechanisms controlling the cdw inflow to the region s continental shelf remain little understood here a high resolution regional model is used to assess the processes governing heat delivery to the amundsen sea the key mechanisms are identified by decomposing cdw temperature variability into two components associated with 1 changes in the depth of isopycnals heave hve and 2 changes in the temperature of isopycnals water mass property changes wmp in the dotson getz trough cdw temperature variability is primarily associated with wmp the deeper thermocline and shallower shelf break hinder cdw access to that trough and cdw inflow is regulated by the uplift of isopycnals at the shelf break which is itself controlled by wind driven variations in the speed of an undercurrent flowing eastward along the continental slope in contrast cdw temperature variability in the pine island thwaites trough is mainly linked to hve the shallower thermocline and deeper shelf break there permit cdw to persistently access the continental shelf cdw temperature in the area responds to wind driven modulation of the water mass on shelf volume by changes in the rate of inflow across the shelf break and in ekman pumping induced vertical displacement of isopycnals within the shelf the western and eastern amundsen sea thus represent distinct regimes in which wind forcing governs cdw mediated heat delivery via different dynamics

polyphase metamorphism and the development of the main central thrust along a cross section through the lesser and higher himalayan units at the kishtwar window area north west india a polyphase barrovian type metamorphism has been delineated in relation to the development of the main central thrust mct in the metapelitic mineral assemblages three metamorphic phases have been distinguished a conditions up to amphibolite grade at moderate to high pressures alm rut ilm kya qtz characterize the m1 phase b pressure release and or temperature increase as a result of movement along the mct and the formation of gneiss domes in the higher himalaya as expressed by oriented n70 100 e fibrolite defines the m2 phase and c finally during uplift of the kishtwar window area a retrogressive m3 phase is characterized by the assemblage quartz muscovite chlorite both optically zoned and single stage garnets have been examined with the electron microprobe to determine their element partitioning normal zoning has been found in samples below the mct in the lesser himalaya indicating prograde growth during the m2 phase whereas tectonically above in the higher himalaya unit the garnets reveal double stage growth with a complex zoning pattern due to reaction partitioning during m1 and m2 and reverse zoning at their rims during the retrogressive m3 phase geothermometry on metapelites along a cross section through the mct zone and the higher himalaya imply distinct readjustments of garnet biotite exchange equilibria and indicate isothermal conditions 500 600 c throughout the section during the m3 retrogression pressure calculations gro an kya qtz and alm rut ilm kya qtz suggest a decrease in pressure towards the top of the section 6 7 5 to 4 5 5 kbar as corroborated by fibrolite replacing kyanite the spatially inverse metamorphism exposed within the lesser himalaya of the kishtwar window is regarded as a product of polyphase metamorphism combined with ongoing thrusting and shearing and is reflected by condensed m2 isograds around the kishtwar window

the life cycle of the northern hemisphere sudden stratospheric warmings motivated by recent evidence of strong stratospheric tropospheric coupling during the northern hemisphere winter this study examines the evolution of the atmospheric flow and wave fluxes at levels throughout the stratosphere and troposphere during the composite life cycle of a sudden stratospheric warming the composite comprises 39 major and minor warming events using 44 years of ncep ncar reanalysis data the incipient stage of the life cycle is characterized by preconditioning of the stratospheric zonal flow and anomalous quasistationary wavenumber 1 forcing in both the stratosphere and troposphere as the life cycle intensifies planetary wave driving gives rise to weakening of the stratospheric polar vortex and downward propagation of the attendant easterly wind and positive temperature anomalies when these anomalies reach the tropopause the life cycle is marked by momentum flux and mean meridional circulation anomalies at tropospheric levels that are consistent with the negative phase of the northern hemisphere annular mode the anomalous momentum fluxes are largest over the atlantic half of the hemisphere and are associated primarily with waves of wavenumber 3 and higher

a linear stratified ocean model of the coastal undercurrent the linear stratified ocean model of mccreary 1981 is used to study the wind driven response of the ocean near an eastern coast the model can be regarded as an extension of the inviscid models of lighthill 1969 and of gill clarke 1974 that allows the vertical diffusion of heat and momentum into the deep ocean solutions are still found as expansions of vertical normal modes vertical mixing affects each mode as a linear drag with a drag coefficient that increases rapidly with mode number n a zonally uniform band of steady equatorward winds forces the ocean and the resulting flow field has many features in common with observations at eastern boundaries there is a surface equatorward jet and a poleward coastal undercurrent confined within 10 20 km of the coast both currents extend well poleward of the wind band upwelling does not reach great depths but occurs only above the core of the undercurrent weak downwelling occurs at greater depths there is offshore ekman drift in the surface mixed layer and return flow at a depth slightly above the core of the undercurrent the baroclinic alongshore pressure gradient field and the vertical mixing of heat and momentum are essential elements of the model dynamics but the beta and horizontal mixing are not low order vertical modes n 6 tend toward a two dimensional balance they generate the transverse circulation pattern associated with coastal ekman pumping

shisha pangma leucogranite south tibetan himalaya field relations geochemistry age origin and emplacement the shisha pangma pluton forming most of the xixabangma 8027 m massif in south tibet is one of the 20 larger leucogranite intrusives that mark the highest structural levels of the himalayan metamorphic core the pluton occurs immediately below the shisha pangma detachment a strand of the south tibetan detachment std system a low angle 30 north dipping normal fault placing paleozoic black slates atop sillimanite grade pelites and calc silicate rocks k feldspar augen gneisses containing fibrolite and sillimanite paragneisses along the footwall show strong internal s c fabrics indicative of down to the north extension the shisha pangma leucogranite is a heterogeneous polyphase intrusion with an earlier foliated biotite rich phase and a later tourmaline muscovite rich phase typically containing the assemblage kfs pl qtz ms tur gt bt sil ap the highly peraluminous granites have high 87sr 86sr ratios 0 738 0 750 typical of pelite derived anatectites nd depleted mantle model

wind forced setup of upwelling geographical origins and numerical models the role of bottom drag 1 an analysis is made to determine the properties and scales for the setup of upwelling driven by an impulsively started steady uniform wind of semi infinite fetch the backward edge of the wind field acts as a geographical origin for the generation of coastal trapped waves ctws a perturbation analysis is used to show that prior to the arrival of the nth mode ctw the alongshore velocity is shown to asymptote to a constant value set by bottom drag and over a timescale tn as this viscous limit is achieved the upwelling becomes increasingly confined to the bottom boundary layer and bottom stress balances wind stress interior upwelling is shut down the viscous limit may not be achieved since after the arrival of the nth ctw mode a gradient in the alongshore velocity is set up and its divergence acts to feed the offshore ekman transport and shut the upwelling down numerical results are used to show that the frictional length and timescales predicted by the perturbation analysis are unrealistically small due to an underestimation of thermal wind shear moreover the theory underpredicts the importance of the first ctw mode which is shown to largely determine the setup and shutdown of upwelling a simple first mode model for upwelling is developed and used to evaluate the validity of a numerical open boundary condition in determining the correct degree of upwelling a case study for the chilean shelf is presented

the crystalline units of the high himalayas in the lahul zanskar region northwest india metamorphic tectonic history and geochronology of the collided and imbricated indian plate in the high himalayan belt of northwest india crustal thickening linked to palaeogene collision between india and eurasia has led to the formation of two main crystalline tectonic units separated by the syn metamorphic miyar thrust the high himalayan crystallines sensu stricto hhc at the bottom and the kade unit at the top these units are structurally interposed between the underlying lesser himalaya and the very low grade sediments of the tibetan nappes they consist of paragneisses orthogneisses minor metabasics and chiefly in the hhc leucogranites the hhc registers a polyphase metamorphism with two main stages designated as m1 and m2 a metamorphic zonation with high temperature recrystallization and migmatization at middle structural levels and medium temperature assemblages at upper and lower levels in contrast the kade unit underwent a low temperature metamorphism rb sr and u th pb isotope data point to derivation of the orthogneisses from early palaeozoic granitoids while the leucogranites formed by anatexis of the hhc rocks and were probably emplaced during miocene time most of the complicated metamorphic setting is related to polyphase tectonic stacking of the hhc with the cooler kade unit and lesser himalaya during the himalayan history however a few inconsistencies exist for a purely himalayan age of some ml assemblages of the hhc as regards the crustal derived leucogranites the formation of a first generation mixed with quartzo feldspathic leucosomes was possibly linked to melt lubricated shear zones which favoured rapid crustal displacements at upper levels they intruded during stage m2 and the latest movements along the syn metamorphic miyar thrust but before juxtaposition of the tibetan nappes along the late metamorphic zanskar fault

heat sources for tertiary metamorphism and anatexis in the annapurna manaslu region central nepal following the collision of india with southern tibet crustal rocks of the leading edge of india 1 underwent regional metamorphism to upper amphibolite grade 2 melted locally to produce anatectic granitoids and 3 were sheared and thrust onto lower grade rock along the main central thrust yielding an inverted metamorphic sequence this sequence is exemplified in the annapurna manaslu region we use simple physical calculations to examine the heat sources involved in the different phases of metamorphism the regional metamorphism apparently is due to the burial of the northern edge of india beneath the accretionary prism along the southern edge of tibet the observed temperatures and pressures of this first phase of metamorphism are consistent with the thermal relaxation during the 10 30 m y before slip on the main central thrust began of thickened continental lithosphere whose original surface heat flux was between 50 and 70 mw m 2 the release of water from the footwall of the main central thrust apparently facilitated melting of the overlying crust in the second phase such melting could have occurred in the first million years or so of thrusting if warm 550 650 c crust in the footwall contained the necessary water if melting did not occur in the earliest stages of slip on the main central thrust dissipative heating with shear stresses of 10 to 100 mpa is required for temperatures near the main central thrust to have remained high enough to generate melting above the fault during the underthrusting of cold material the thickness 6 8 km of the zone of inverted isograds associated with the fault if undisrupted and due solely to thermal diffusion implies that the time required to carry the rocks preserving the inverted metamorphism from the surface to depths of 30 40 km was 4 8 m y the apparent inverted temperature gradients about 10 25 c km in this zone can be understood as the combined result of two processes diffusion of heat from hot rock thrust over cold rock expunged the original temperature gradient near the fault and could have created an inverse gradient of 10 20 c km the peak temperatures in such a zone however would not have exceeded about 350 c without an additional source of heat dissipative heating at shear stresses of about 100 mpa can account for peak temperatures in excess of 600 c during slip on the fault and would have contributed as much as 13 c km to the inverse gradient although inversion of metamorphic isograds could have occurred as a result of deformation within the main central thrust zone the high temperatures during slip on this zone still require dissipative heating unless the duration of slip exceeded 25 m y

gravity wave interactions with the diurnal propagating tide observations of the diurnal propagating solar tide in the mesosphere and lower thermosphere 50 150 km indicate substantial annual variations in tidal amplitudes observations and modeling efforts suggest that interactions with internal gravity waves can result in significant modifications of the diurnal tide herein a two dimensional 2 d linear steady state tidal model is used in conjunction with hybrid lindzen matsuno gravity wave parameterization to examine the role of gravity wave interactions in the seasonal variability of the diurnal tide in the mlt the analysis indicates that annual variations of the background atmosphere result in significant annual variations in the eddy diffusion and the diurnal harmonic of the momentum flux divergence wave stress produced by breaking gravity waves the seasonal variability in these two mechanisms can explain the observed semi annual variability in the diurnal tide amplitude minima at solstice and maxima at equinox the relative roles of wave stress and diffusion are examined and it is shown that both play important roles in tidal modification by damping its amplitude the effects of varying inputs to the gravity wave parameterization are explored

long term coastal upwelling over a continental shelf slope abstract long term coastal upwelling over a continental shelf slope with emphasis on the planetary dispersion of rossby waves is studied with numerical models the ocean is forced by a wind stress with a limited longshore extent the thermocline intersects the shelf slope and the internal radius of deformation is smaller than the width of the shelf slope two case studies with and without the effect are studied lie early stage response within a week or so is similar between the two for an f plane case the whole stage response is accounted for by coastal trapped wave dynamics and only equatorward flow exists over the shelf slope at an advanced stage however inclusion of the effect leads to a significant change in the alongshore flow pattern at the advanced stage due to the westward rossby dispersion of the equatorward flow associated with the first and second coastal trapped mode responses the poleward undercurrent develops in the thermocline layer over the shelf the time for the undercurrent

a northern boundary current along australia s southern shelves the flinders current 1 south of australia the monthly mean wind stress curl is positive during both summer and winter and leads to ekman pumping and downwelling throughout the region sverdrup dynamics indicates that this downwelling should lead to a northward transport of around 5 10 sv 1 sv 10 m3 s 1 classical arguments for western boundary currents are adapted to show that this transport should be deflected into an upwelling favorable boundary current that flows from east to west along australia s southern shelves the flinders current support for this proposition is obtained from results of the ocean circulation and climate advanced modelling project occam sverdrup transports and limited observations for the region in addition the occam results show that the northward transport leads to upwelling at depths below 400 m and that the flinders current 1 intensifies from victoria to western australia transport 8 sv with speeds up to 15 cm s 1 2 can extend from the surface to depths of 800 m and 3 is found during both summer and winter during winter the winds are downwelling favorable and lead to a coastal current that flows from west to east and opposes the flinders current further support for the origin and nature of the flinders current is obtained from simple numerical experiments made using a rectangular domain and idealized representations of the summer and winter wind stress

badrinath gangotri plutons garhwal india petrological and geochemical evidence for fractionation processes in a high himalayan leucogranite the gangotri leucogranite is the western end of the badrinath granite one of the largest bodies of the high himalayan leucogranite belt hhl it is a typical fine grained tourmaline muscovite biotite leucogranite the petrography shows a lack of restitic phases the inferred crystallization sequence is characterized by the early appearance of plagioclase quartz and biotite and by the late crystallization of the k feldspar this suggests that in spite of being of near minimum melt composition the granite probably had long crystallization or melting interval in agreement with previous experimental studies tourmaline and muscovite have a mainly magmatic origin even though the major element composition is homogeneous there are several geochemical trends when cao decreases there is an increase in na2o rb sn u b f and a decrease in k2o fe2o3 tio2 sr ba zr ree th which are best explained by a fractionation process with early crystallizing phases experimental solubility models for zircon and monazite in felsic melt support a magmatic origin for these two accessory phases as well rb sr isotope data show this granite to have like other hhl heterogeneous isotopic values for sr initial 87sr 86sr ratios calculated at 20 ma range between 0 765 and 0 785 therefore no mixing i e no convection occurred between the different batches of magma in contrast 18o data show little variation 13 04 0 25 implying a source with homogeneous 18o values differences in timing between fluid infiltration and the onset of melting related to differences in temperature of the source could explain why source homogenization occurred for the gangotri and not for the manaslu granite the use of experimental results for solubility and the position of the accessory minerals during melting predict a low viscosity for the melt during its extraction this in turn explains the lack of restitic phases major and accessory in the granite as well as some field features lensoid shape pronounced magmatic layering based on the petrographic and isotopic studies it is suggested that the mechanism of ascent was not diapiric but rather that the melt ascended along several fractures and the level of emplacement was partialy controlled by the density contrast between the melt and host rocks

ionospheric current system during sudden stratospheric warming events 1 this paper describes ionospheric current systems associated with the counter electrojet during sudden stratospheric warming ssw events in the northern winter months of 2001 2002 and 2002 2003 magnetic data from 20 stations in the east asian region covering both the northern hemisphere and the southern hemisphere are analyzed additional current systems that are superposed on the normal sq current system and related to the counter electrojet during the ssw events show a global semidiurnal current pattern which shifts to later local times approximately by 0 8 hour day the results indicate that abnormally large lunar tidal winds played a main role to produce the additional current system and counter electrojet during the ssw events

excursions of interhemispheric field aligned currents in africa the interhemispheric field aligned currents ihfacs are the most evident currents connecting the solar quiet sq current systems in the northern and southern hemispheres understanding these coupling currents has practical importance for space weather forecast of the magnetosphere ionosphere interactions and their potential impacts on low orbiting spacecraft in this paper we have examined digital magnetic records from september 2008 to august 2009 at nine magnetic data acquisition system magdas stations in order to uniquely determine the variability of ihfacs in terms of their excursions in the african sector by excursions we mean the direction in which the ihfacs are moving as a function of local time or latitude different from theoretical prediction we found prominent positive ihfacs around dusk in february and march equinox a novel feature of this study is the semidiurnal variation control of the coupling between the northern and southern hemispheres in addition we found terdiurnal variation in september with their associated strong diurnal variations from october through december quite unexpectedly in january a significant latitudinal depletion in the intensities of ihfacs was observed from dawn to dusk compared to any other months under investigation accompanied with a marked reduction of the prominent diurnal variations at the magnetic equator addis ababa aab the fact that the excursions of ihfacs in january experience an unusual retardation with respect to their in

neogene foreland basin deposits erosional unroofing and the kinematic history of the himalayan fold thrust belt western nepal sedimentological and provenance data from the lower miocene pliocene dumri formation and siwalik group in western nepal provide new information about the timing of thrust faulting and the links between erosional unroofing of the himalaya and the cenozoic 87 sr 86 sr record of the ocean in western nepal the dumri formation is an 750 1300 m thick fluvial sandstone and overbank mudstone unit the siwalik group is 4200 m thick and consists of a lower member 850 m of 2 12 m thick fluvial channel sandstones and oxidized calcareous paleosols a middle member 2400 m of very thick 20 m channel sandstones and mainly organic rich histosols and an upper member 1000 m composed of gravelly braided river deposits paleocurrent data indicate that middle miocene pliocene rivers in western nepal flowed southward transverse to the thrust belt throughout deposition of the siwalik group no evidence was found for an axial fluvial trunk system i e the paleo ganges river in siwalik group sandstones a major increase in fluvial channel size is recorded by the transition from lower to middle siwalik members at 10 8 ma probably in response to an increase in seasonal discharge modal petrographic data from sandstones in the dumri formation and the siwalik group manifest an upsection enrichment in potassium feldspar carbonate lithic fragments and high grade metamorphic minerals modal petrographic analyses of modern river sands provide some control on potential source terranes for the miocene pliocene sandstones the dumri formation was most likely derived from erosion of sedimentary and low grade metasedimentary rocks in the tibetan tethyan himalayan zone during early miocene emplacement of the main central thrust the presence in dumri sandstones of plagioclase grains suggests exposure of crystalline rocks of the greater himalayan zone perhaps in response to tectonic unroofing by extensional detachment faults of the south tibetan detachment system during deposition of the lower siwalik group 15 11 ma emplacement of the dadeldhura thrust sheet one of the synformal crystalline thrust sheets of the southern himalaya on top of the dumri formation supplied abundant metasedimentary lithic fragments to the foreland basin a steady supply of plagioclase grains and high grade minerals was maintained by deeper erosion into the main central thrust sheet from 11 ma to the present k feldspar sand increased steadily suggesting that granitic source rocks became widely exposed during deposition of the upper part of the lower siwalik group this provenance change was caused by erosion of passively uplifted granites and granitic orthogneisses in the dadeldhura thrust sheet above a large duplex in the lesser himalayan rocks since the onset of deposition of the conglomeratic upper siwalik group 4 5 ma fault slip in this duplex has been fed updip and southward into the main boundary and main frontal thrust systems we obtained 113 u pb ages on detrital zircons from modern rivers and siwalik group sandstones that cluster at 460 530 ma 850 1200 ma 1 8 2 0 ga and 2 5 ga an abundance of cambrian ordovician grains in the siwalik group suggests sources of siwalik detritus in the granites of the dadeldhura thrust sheet and possibly the greater himalayan orthogneisses the older ages are consistent with sources in the greater and lesser himalayan zones an overall upsection increase in zircons older than 1 7 ga suggests increasing aerial exposure of lesser himalayan rocks none of the detrital zircons even in the modern river samples yielded a cenozoic age that might suggest derivation from the cenozoic greater himalayan leucogranites but this may be attributable to the inheritance problems that characterize the u pb geochronology of the leucogranites when compared with recent studies of the 87 sr 86 sr composition of paleosol carbonate nodules and detrital carbonate in paleosols from the siwalik group the provenance data suggest that erosion and weathering of metamorphosed carbonate rocks in the lesser himalayan zone and cambrian ordovician granitic rocks of the crystalline thrust sheets in central and eastern nepal may have played a significant role in elevating the 87 sr 86 sr ratio of middle miocene synorogenic sediments in the indo gangetic foreland basin and the bengal fan as well as global seawater

spatial variability of solar quiet fields along 96 magnetic meridian in africa results from magdas we have used chains of magnetic data acquisition system magdas magnetometer records of the horizontal h and vertical z magnetic field intensities during september 2008 to august 2009 year of deep minimum across africa to study their variability during the quietest international days which coincidently associated with the sudden stratospheric warming ssw event in january 2009 this selection of the most international quiet days is indicative of 80 that are strongly associated with days when unusually strong and prolonged sudden ssw event occurs in january 2009 interestingly in january a significant magnitude depletion of solar quiet sq equivalent current was observed near noon hours around the magnetic equator addis ababa abb compared to any other months along with a consistent significantly reduced value across the northern hemisphere and moderate decrease at the southern hemisphere also we found that nairobi and dar es salaam at the southern hemisphere which are close to abb dip equator are strongly prone to westward electric field compared to the magnetic equator and khartoum at the northern hemisphere significant negative values of msq z magnitudes observed near noon hours at hermanus indicate the presence of induced currents that suggest ocean effects along with reversal to significant positive values in the afternoon which subsided before 1800 lt in almost all the months indicate stronger influence of ionospheric currents on seasonal variability of sq h a slight depression at abb during september equinox is one of the evidences of seasonal sq focus shift latitudinal variability of sq near noon hours was also investigated

a strontium neodymium and oxygen isotope study of hydrothermal metamorphism and crustal anatexis in the trois seigneurs massif pyrenees france nd sr and o isotope analyses have been made on metamorphic and igneous rocks and minerals from a 310 340 ma hercynian age metamorphic terrane in the pyrenees france lower paleozoic shales and phyllites have 87sr 86sr values of 0 707 0 717 at 310 ma but model values at 310 ma of 0 709 0 736 based on assumed depositional age of 450 ma and an initial 87sr 86sr 0 707 on a regional scale 87sr 86sr was homogenized to about 0 713 to 0 717 in the higher grade pelitic schists during metamorphism much of this 87sr 86sr exchange occurred at very low grades below the biotite isograd but significant changes also accompanied the 18o lowering of the phyllites 13 to 16 during their transformation to andalusite and sillimanite grade schists 18o 11 to 12 all of these effects are attributed to pervasive interactions with hydrothermal fluids wickham and taylor 1985 the data also show that a syn metamorphic plutonic complex dominated by a biotite granite body was derived by mixing of a relatively mafic magmatic end member 87sr 86sr 0 7025 0 7050 and 18o 7 5 to 8 0 with two metasedimentary sources both having 87sr 86sr 0 715 and 18o 10 0 to 12 0 but with one being more homogeneous than the other the more homogeneous component and the mantle derived magmatic end member dominate at low structural levels within the complex the less homogeneous end member that dominates at high levels is clearly derived from the local paleozoic pelitic schists a rb sr age of 330 20 ma was obtained on hornblende from a deep level within the complex which fixes this age for the regional metamorphism as well although a post metamorphic granodiorite magma body at trois seigneurs also displays heterogeneities in 18o and 87sr 86sr and thus does not give a clear cut rb sr isochron the data are consistent with an emplacement age between 260 and 310 ma similar to ages of other late granodiorites in the pyrenees 143nd 144nd is very uniform within the hercynian crust both at trois seigneurs nd 3 to 7 and elsewhere in the pyrenees almost all igneous lithologies have depleted mantle mid proterozoic model ages consistent with efficient recycling of crustal material following original crustal accretion in this area at about 1600 ma or earlier rb sr mineral ages exhibit a complex cooling history reflecting late hercynian and mesozoic thermal events our results show that profound homogenization of the 87sr 86sr and 18o 16o ratios of large volumes of the crust can occur during regional metamorphism and crustal anatexis particularly in regions undergoing extensional tectonics such processes can significantly modify the isotopic compositions of the protoliths of granitic magmas this may explain why many peraluminous hercynian granitoids of western europe have anomalously low 87sr 86sr initial values compared to their probable sedimentary parent rocks

metamorphic reactions related to decompression and synkinematic intrusion of leucogranite high himalayan crystallines bhutan the high himalayan crystallines hhc of bhutan were penetratively deformed intruded by leucogranite and metamorphosed during the collision of the indian and asian plates metamorphic reaction textures in the hhc show that it experienced decompression while maintaining a laterally heterogeneous and locally inverted internal temperature range of c 600 750c this thermal structure was produced by thrusting hot migmatitic rocks over lower grade rocks within the hhc and by the advection of heat from the intrusion of leucogranite dykes and sills during decompression a variable velocity field within the hhc during exhumation and extrusion between india and tibet caused the inversion of top to the south sense of shear present throughout most of the hhc to top down to the north shear near its top

on induction effects of geomagnetic daily variations from equatorial electrojet and solar quiet sources at low and middle latitudes 1 we investigate the spatiotemporal behavior of the magnetic vertical component z of the daily ionospheric current systems the equatorial electrojet eej and solar quiet sq variations considering induction in the mantle and oceans the inducing eej and sq current systems are provided by the comprehensive model of sabaka et al 2004 the three dimensional 3 d conductivity model of the earth includes oceans of laterally variable conductance and a spherical conductor 1 d underneath our model studies demonstrate that induction effects in z due to the eej are negligible everywhere inland for all local times at champ altitude 400 km the magnetic signal induced by eej above the oceans does not exceed 2 5 of the external field during local noon this in particular means that considering the induction effects is not necessary when modeling the eej current strength from inland surface magnetic measurements and or satellite data as expected induction in the oceans strongly affects the sq field the model studies show that the anomalous induction effect defined as the difference between results obtained with 1 d and 3 d conductivity models of sq is substantial at champ altitude comprising 50 of the total field it is therefore necessary to consider induction in the oceans when modeling sq variations for both ground based and satellite data finally we demonstrate that the anomalous behavior of the daily variations in z at south indian sites namely a large positive prenoon peak can be explained by 3 d induction of the sq variations with no contribution from the eej

longitudinal variation of the e region electric fields caused by atmospheric tides 1 polarization electric fields created by the e and f region dynamos cause the uplift of f region plasma the subsequent redistribution of that plasma along the magnetic field lines creates the equatorial ionospheric anomaly eia observations of the post sunset eia made by the image and timed satellites are compared here with champ orsted and sac c observations of the noontime equatorial electrojet eej during magnetically quiet periods around equinox the eia and eej show a remarkably similar four peaked wave like longitudinal variation its structure is consistent with the longitudinal variation in the strength of diurnal tides that drive the e region dynamo this indicates a strong vertical coupling between the ionosphere and troposphere because the four peaked tidal structure is driven by tropospheric weather furthermore the dayside ionospheric conditions are found to perform the global scale longitudinal structure of the post sunset ionosphere at low latitudes

anomalous occurrence features of the preliminary impulse of geomagnetic sudden commencement in the south atlantic anomaly region 1 occurrence features of the preliminary impulse pi of geomagnetic sudden commencement sc both in the pacific ocean and south atlantic anomaly saa regions were investigated using the long term magnetic field data obtained from the circum pan pacific magnetometer network cpmn and nict space weather monitoring nswm magnetometer networks the low latitude preliminary reverse impulse pri at okinawa oki dip latitude 37 97 in the pacific ocean region appeared in all the magnetic local time mlt sectors with the peak occurrence rate of 40 around noon on the other hand the pri occurrence rate at santa maria sma dip latitude 34 35 near the center of the saa region showed a significant enhancement in the daytime sector 0800 1600 h mlt with the peak value of 80 which resembles the occurrence feature of the equatorial pri moreover the pri amplitude around noon at sma was about 3 0 times larger than that at oki from the calculation of the ionospheric conductivity derived from the iri 2007 and nrlmsise 00 models it is shown that the height integrated conductivity was more enhanced in the saa region sma where the ambient magnetic field intensity is weak compared with that in the pacific ocean region oki therefore the anomalous increase of the pri occurrence and amplitude is caused by the significant enhancement of the ionospheric conductivity due to the weakness of the ambient magnetic field intensity in the saa region

the 5500 km long boundary flow off western and southern australia 1 the path of the shelf edge flow off southwestern australia is documented using results from satellite altimetry and sea surface temperature sst and a climatogical in situ analysis during austral winter a continuous current is shown to extend from its origin at north west cape to the southern tip of tasmania a distance of 5500 km satellite sst observations and surface buoy tracks confirm the location and continuity of the current trajectory while the leeuwin current is forced by the strong alongshore pressure gradient associated with the meridional portion of the western australian coastal boundary our results suggest that the essentially zonal shelf edge flow along the southern australian coast arises from the setup of coastal sea level by onshore ekman flow driven by the winter westerly wind and possibly a further alongshore pressure gradient the timing of these two different forcing mechanisms means that the west coast pressure gradient delivers the leeuwin current to the south coast just as the winds reverse and are thus able to maintain the eastward passage of the current the shelf edge flow consists of two main water masses a low salinity warm water type of tropical origin associated with the leeuwin current and a high salinity warm water inflow formed on the western end of the great australian bight continental shelf a naming convention is proposed the leeuwin current representing flow from north west cape to the great australian bight gab the south australian current between the eastern gab and western bass strait and the zeehan current off western tasmania

dating the transition of smectite to illite in palaeozoic mudrocks using the rb sr whole rock technique the interpretation of mudrock rb sr whole rock regression ages using stratigraphically well constrained samples from the ordovician and silurian of central wales is re examined two new rb sr whole rock regressions are presented along with k ar and rb sr data from the

wind forced upwelling the role of the surface mixed layer abstract a numerical study is made of the dynamics of the circulation that arises from forcing by a steady uniform alongshore wind over a uniform zonal shelf in the southern hemisphere the results show that most of the upwelling is confined to the region inshore of the shelf break over the slope and within the region of wind forcing the circulation is found to be dominated by the growth of both an anticyclonic and a cyclonic eddy an offshore flow and downwelling two new mechanisms are identified as being responsible for these features of the upwelling circulation first the offshore advection of alongshore momentum 0u x within the surface mixed layer sml is shown to accelerate the alongshore current near the eastern end of the region of wind forcing leading to a sharpening of the cross shelf gradient of sea level and an excess in the alongshore transport this excess transport acts to raise sea level leads to downwelling below the base of the sml and causes the growth of the anticyclonic ed

age of metamorphism in the lesser himalaya and the main central thrust zone garhwal india results of illite crystallinity 40 ar 39 ar fusion and k ar studies

longitudinal variations in the equatorial vertical drift in the topside ionosphere 1 the vertical ion drift is important for understanding and modeling the electrodynamics at low latitudes measurements from the ion drift meter on the defense meteorological satellite program dmsp f15 are used to examine longitudinal variations in the vertical ion drift at the dip equator in the topside ionosphere local time was restricted to 0930 and the data were organized by month for 2001 and 2002 two features were found contributing to the longitudinal variations in the electrodynamics meridional winds contribute to the equatorial vertical ion drift at the 830 km magnetic apex due to their dynamo action at the foot points of the magnetic field lines in the f region at magnetic latitudes near 15 electric fields producing a downward perturbation drift at 0930 are produced by hemispheric differences in the dynamo current due primarily to the different orientation of the magnetic meridian relative to the terminator this produces the seasonally dependent variation as a function of longitude that is observed a wavenumber 4 longitudinal variation also appears to be present throughout the year but is more influential during equinox conditions this variation also shows a seasonal cycle shifting east during northern summer and west during northern winter further analysis would be required to isolate the characteristics of a wavenumber 4 driver from the wavenumber 4 component of the fourier series used here to fit the data

a thin viscous sheet model for continental deformation summary for the purposes of describing its large scale and long term deformation the continental lithosphere is regarded as a continuum obeying a newtonian or a power law rheology the flow of a thin sheet of power law material overlying an inviscid substrate is studied under the assumption that vertical gradients of the horizontal velocity are negligible a numerical model is used to investigate the deformation of such a sheet under conditions approximating those of continent continent collision the material flows in response to forces applied to its boundaries for example the indenting of one continent by another and to forces in its interior arising from gradients in crustal thickness the horizontal divergence of the flow produces changes in the crustal thickness and hence a time dependent form to the flow itself for a given set of boundary conditions the flow depends on the stress exponent in the power law rheology n and on the argand number which is a measure of the ratio between the stress arising from crustal thickness contrasts and the stress required to deform the material at the ambient strain rates when the effective viscosity of the medium is very high ar o crustal thickness variations do not influence the flow if the material is newtonian n l the deformation associated with an influx of material approximating an indenter is of much greater lateral dimension than the width of the indenter whereas when material has a power law rheology n 3 5 are used the deformation is confined to a region of lateral extent comparable to that of the indenter as ar increases the forces arising from crustal thickness contrasts exert more influence on the flow and the maximum crustal thickness that can be sustained by a given influx of material is related by a simple expression to the effective viscosity of the medium at the ambient strain rates in the limit of a very weak medium ar 10 the lithosphere is unable to sustain appreciable crustal elevation contrasts the results of these numerical experiments show that systems in which the effective viscosities are such that the maximum deviatoric stresses are between 1 kbar

isotopic constraints on the age and provenance of the lesser and greater himalayan sequences nepalese himalaya the main central thrust of the central himalaya juxtaposes the lesser himalayan sequence footwall with the greater himalayan sequence hanging wall both of which are regarded as components of the northern passive margin of india considerable uncertainty surrounds their respective ages and sedimentary derivation u pb and sm nd isotopic studies of samples from the langtang area central nepal demonstrate important distinctions between the two rock packages the greater himalayan sequence had a sedimentary provenance that included a major source of 0 8 1 0 ga zircons implying a late proterozoic age the source of the precambrian part of the lesser himalayan sequence contained 1 87 2 60 ga zircons and its depositional age is probably middle proterozoic nd isotopic characteristics of the two sequences are different at 21 ma the greater himalayan rocks had end values between 14 6 and 18 5 while their lesser himalayan counterparts had values between 21 4 and 25 9 giving rise to major differences in their model ages the lesser and greater himalayan sequences at langtang are interpreted as correlative to the lower and upper parts of the vindhyan supergroup currently exposed south of the gangetic plain in northern india on the basis of available age data the exposed hanging wall of the main central thrust in central and eastern nepal contains no archean early proterozoic basement if the fault does root into the basement at depth it must do so farther north than recently published cross sections indicate this implies a total displacement on the fault that is substantially greater than the 140 210 km required by tectonic overlap in the eastern himalayas

quiet ionospheric currents of the southern hemisphere derived from geomagnetic records a special selection of extremely quiet 1965 geomagnetic daily variation records from north america europe central asia and east asia was used to determine monthly spherical harmonic analysis coefficients representing the sq fields from these regions the coefficients permitted a separation of the external and internal contributions to the daily variations month by month behavior of the equivalent external current system and contours of the daily range of this current showed regional differences in amplitude and location of the equivalent ionospheric currents with seasonal change current foci locations reached 35 to 42 geomagnetic latitude in summer and 18 to 35 in winter with a regional dependence the largest daily range of external current was 14 6 104 a in north america 15 3 104 a in europe 13 7 104 a in central asia and 12 3 104 a in east asia continental differences in the behavior of the current seemed to be explained by the relative position of the geographic and geomagnetic poles with respect to these regions

lunar tide in the equatorial f region vertical ion drift velocity vertical ion drift velocity data from jicamarca have been analyzed for a lunar semidiurnal tide using a least squares fitting method amplitudes of up to 6 m s 1 are obtained with phases in agreement with lunar tidal determinations of other associated physical parameters variations between season solar activity and day to night are also examined generally amplitudes are larger in the southern summer much of the phase variation with season is very similar for solar maximum and minimum years there is a summer to winter phase change that is most distinct at solar maximum nighttime a day to night phase reversal can also been seen in some seasons hints of this are also found in the lunar tide in the f region height and in the magnetic variations at huancayo

geothermobarometry and development of inverted metamorphism in the darjeeling sikkim region of the eastern himalayan abstract the darjeeling sikkim region provides a classic example of inverted himalayan metamorphism the different parageneses of pelitic rocks containing chlorite biotite garnet staurolite kyanite sillimanite plagioclase and k feldspar are documented by a variety of textures resulting from continuous and discontinuous reactions in the different zones microprobe data of coexisting minerals show that xmg varies in the order garnet staurolite biotite chlorite white mica is a solid solution between muscovite and phengite garnet is mostly almandine rich and shows normal growth zoning in the lower part of the main central thrust mct zone and reverse zoning in the upper part of the zone chemographical relations and inferred reactions for different zones are portrayed in afm space in the low grade zones oriented chlorites and micas and rolled garnets grew syntectonically and were succeeded by cross cutting chlorites and micas and garnet rims in the upper zones sillimanite kyanite and staurolite crystallized during a static inter kinematic phase p t contitions of metamorphism estimated through different models of geothermobarometry are estimated to have been 580 c for the garnet zone to a maximum of 770 c for the sillimanite zone the preferred values of pressure range from 5 0 kbar to 7 7 kbar models to explain the inverted metamorphism include overthrusting of a hot high himalayan slab along a c 5 km wide ductile mct zone and the syn or post metamorphic folding of isograds

lunar tide in the equatorial electrojet in relation to stratospheric warmings 1 the relationship between sudden stratospheric warmings ssws and large amplitude lunar tides in the equatorial electrojet eej is studied analysis of ground magnetometer data shows that the lunar tide in the eej is maximum during the northern winter season except in the pacific ocean region since ssws are also a northern winter phenomenon it is suggested that the relation between the large lunar tide in the eej and the ssw may possibly be coincidental the lunar tide in the geomagnetic variations at huancayo is anomalously large compared with other eej stations an examination of geomagnetic variations at eej stations during ssw events shows that afternoon counter electrojets are frequently present at new moon and full moon though the relationship is sometimes broken the observation of large lunar eejs when no ssw is present and of various different delay times suggests that other atmospheric processes are likely to be in play

thrust geometries and deep structure of the outer and lesser himalaya kumaon and garhwal india implications for evolution of the himalayan fold and thrust belt the kumaon garhwal region of the himalaya lies near the center of the himalayan fold and thrust belt we have drawn two balanced cross sections 100 km apart through the outer and lesser himalaya the cross sections incorporate all the surface well log and earthquake seismic data currently available from the region two branch line maps showing trailing and leading branch lines and cutoff lines of the major thrusts in the region are also drawn the three dimensional deep structure of the outer and lesser himalaya is interpreted based on the balanced cross sections and the branch line maps deep structure of the higher and tethyan himalaya is extrapolated based on surface geology and is subject to revision as more surface and seismic data become available from these areas a sequential evolutionary model for the kumaon himalaya along the eastern pindari section is proposed according to this model the kumaon himalaya evolved by an overall forelandward progression of thrusting with some reactivation along the munsiari thrust mt the main boundary thrust mbt and the main central thrust mct we use structural stratigraphic and radiometric criteria to place time constraints on the motion of these thrusts earliest motion along the mbt may have occurred in early middle paleocene but the main episode probably started in late eocene and may still be continuing emplacement of the mt had occurred by middle late eocene whereas the mct shows activity around 20 ma thus exhibiting break back thrusting with respect to the mt shortening estimates are obtained from the pindari section minimum shortening in the sedimentary thrust sheets of the outer and lesser himalaya is 161 km or 65 as a first approximation we have also restored the crystalline sheets in order to obtain shortening estimates for the entire himalaya minimum shortening for the himalaya after restoring the mct sheet varies from 354 76 to 421 km 79 these estimates were further combined with published data from the area between the mct sheet and the indus tsangpo suture zone itsz minimum shortening between the indo ganga foreland and the itsz thus obtained lies in the range 687 754 km or 69 72 we compare our shortening estimates with those available from the pakistan and nepal himalaya

subinertial response of a density driven eastern boundary poleward current to wind forcing a high resolution primitive equation numerical model is used to generate a poleward flow along a meridionally oriented eastern boundary slope shelf system by imposing an along coast density gradient as the forcing mechanism wind forcing is applied to the resulting quasi steady current system and the subinertial response is analyzed parallel experiments with no slope poleward flow are conducted for comparison moderately strong upwelling and downwelling favorable week to month scale wind events modify the poleward flow but do not significantly change the density driven current structure at the slope the alongshore transport within the slope region is reduced by 0 2 0 3 sv from 1 2 sv where sv 106 m3 s 21 under the influence of either downwelling or upwelling winds independent of the wind direction the density driven poleward flow always remains surface intensified wind driven shelf currents develop with a considerable degree of independence from the slopepoleward circulation on the shelf the density field is modified by cross shelf buoyancy advection within the boundary layers and by strong vertical mixing the presence of the poleward flow over the slope constitutes an important factor in the behavior of the bottom boundary layer at the shelf break and for the patterns of crossslope circulation

deceleration of a finite width stratified current over a sloping bottom frictional spindown or buoyancy shutdown abstract the deceleration of an unforced two dimensional finite width current over a sloping bottom in a stratified fluid is studied to quantify the relative importance of frictional spindown and buoyancy shutdown when both act simultaneously frictional spindown decelerates the current through ekman suction and pumping at the current edges which transmit stresses into the interior fluid buoyancy shutdown is the process by which lateral advection of density in the bottom boundary layer generates thermal wind shears that reduce the bottom stress thereby halting deceleration a theoretical model of a downwelling current suggests that buoyancy shutdown always reduces the deceleration timescale from that for frictional spindown alone and produces a nonzero steady along isobath current overlying an arrested bottom mixed layer the model is most sensitive to the burger number s n f where n is the buoyancy frequency the bottom slope and f the coriolis parameter larger s produces a stronger steady cu

ionosphere variability during the 2009 ssw influence of the lunar semidiurnal tide and mechanisms producing electron density variability to investigate ionosphere variability during the 2009 sudden stratosphere warming ssw we present simulation results that combine the whole atmosphere community climate model extended version and the thermosphere ionosphere mesosphere electrodynamics general circulation model time gcm the simulations reveal notable enhancements in both the migrating semidiurnal solar sw2 and lunar m2 tides during the ssw the sw2 and m2 amplitudes reach 50 m s 1 and 40 m s 1 respectively in zonal wind at e region altitudes the dramatic increase in the m2 at these altitudes influences the dynamo generation of electric fields and the importance of the m2 on the ionosphere variability during the 2009 ssw is demonstrated by comparing simulations with and without the m2 time gcm simulations that incorporate the m2 are found to be in good agreement with jicamarca incoherent scatter radar vertical plasma drifts and constellation observing system for meteorology ionosphere and climate cosmic observations of the maximum f region electron density the agreement with observations is worse if the m2 is not included in the simulation demonstrating that the lunar tide is an important contributor to the ionosphere variability during the 2009 ssw we additionally investigate sources of the f region electron density variability during the ssw the primary driver of the electron density variability is changes in electric fields changes in meridional neutral winds and thermosphere composition are found to also contribute to the electron density variability during the 2009 ssw the electron density variability for the 2009 ssw is therefore not solely due to variability in electric fields as previously thought

a late miocene pliocene origin for the central himalayan inverted metamorphism abstract perhaps the best known occurrence of an inverted metamorphic sequence is that found immediately beneath the himalayan main central thrust mct generally thought to have been active during the early miocene however in situ 208 pb 232 th dating of monazite inclusions in garnet indicates that peak metamorphic recrystallization of the mct footwall occurred in this portion of the central himalaya at only ca 6 ma the apparent inverted metamorphism appears to have resulted from activation of a broad shear zone beneath the mct which tectonically telescoped the young metamorphic sequence this explanation may resolve some outstanding problems in himalayan tectonics such why the mct and not the more recently initiated thrusts marks the break in slope of the present day mountain range it also renders unnecessary the need for exceptional physical conditions e g high shear stress to explain the generation of the himalayan leucogranites

characterization of seasonal and longitudinal variability of eej in the indian region this paper presents the seasonal and longitudinal variability of the equatorial electrojet eej based on geomagnetic variation data from two electrojet stations in the northern indian ocean at a longitudinal separation of 15 i e at 77 e and at 93 e one complete year of data is used i e from november 2011 to october 2012 at the two longitudes and compared with the climatological model of the equatorial electrojet eejm 2 0 the results of our analysis show that i the monthly averaged hourly values of eej strength at 77 e and 93 e are overall in agreement with global characteristics of eej with significant departures over the year of study ii the monthly average hourly daytime values at campbell bay and vencode show poor correlation r 10 nt 20 nt for 30 of quiet days sorted by planetary index kp 1 and 2 this variability is reflected in monthly average values v mechanisms for persistent differences in eej on day to day basis are sought from perturbation of westward ion drifts by neutral winds caused by the upward propagation of gravity waves from troposphere stratosphere into the mesosphere these mechanisms have been identified theoretically and experimentally the four wave structure of ionospheric current densities obtained by eejm 2 0 and other contemporary models closely resembles atmospheric tidal signatures and has a common origin the magnitude and persistence of these differences at short spatial scales 15 are significant observation these effects are reflected in the monthly and seasonal signatures of eej and contribute to the contemporary models

rb sr geochronology of granites and gneisses from the mount everest region nepal himalaya nineteen samples of granites orthogneisses and paragneisses from the high himalaya basement nappe s of the mount everest region have been dated by the rb sr method the post metamorphic tourmaline leucogranites of the upper imja drangka nuptse lhotse glacier have high initial sr87 sr86 characteristic of an anatectic origin from crustal material a whole rock isochron age of 52 m y early eocene has been obtained for the samples from the granite body of lhotse glacier apparently sr isotopic homogenization was not reached throughout the much larger nuptse granite

investigation on the variability of the geomagnetic daily current during sudden stratospheric warmings the magnetic field records of the magnetometer networks in the american east asian australian and european african sectors were employed in this present work we used them to investigate equatorial electrojet eej counter electrojet cej tidal variability in eej strength and ionospheric current during the 2005 2006 and 2008 2009 sudden stratospheric warming ssw events in addition to the well investigated tidal variability in eej strength over the american and east asian sectors we investigated that of the african sector for the first time interestingly the tidal components in eej strength during both ssw events clearly exhibit marked longitudinal differences with high moderate and low amplitudes in the american east asian and african sectors respectively an exception found around day 71 in the african sector after the 2008 2009 ssw event had higher solar diurnal tidal component as compared to that of the asian sector over the american sector solar and lunar semidiurnal tides were strongly associated with cej current during both ssw events whereas at the african and east asian sectors such variabilities are not evident a solar diurnal tidal component was strongly related to a reduction in the eej strength over the east asian sector in addition a prolonged period of cej occurrence that begins during the ssw precondition and ends when the ssw was evolving characterized the african sector during both ssw events there is a steady shift in phase at later hours when both ssw events are evolving

exact solutions of wind driven coastal upwelling and downwelling over sloping topography abstractthe dynamics of wind driven coastal upwelling and downwelling are studied using a simplified dynamical model exact solutions are examined as a function of time and over a family of sloping topographies assumptions in the two dimensional model include a frictionless ocean interior below the surface ekman layer and no along slope dependence of the variables however dependence in the cross slope and vertical directions is retained density and the along slope component of momentum are advected by the cross slope velocity with thermal wind balance maintained at all times the time dependent initial value problem is solved with constant initial stratification and no initial along slope flow previously this model has been used to study upwelling over flat bottomed ocean but the novel features in this work are the study of exact solutions for a family of sloping topographic profiles for both upwelling and downwelling the exact solutions are compared to numerical solutions from a primitive equat

wind forced downwelling slope currents a numerical study abstract a study is made of the dynamics of slope currents that arise from a steady constant alongshore wind over a uniform shelf over the first 10 20 days the evolution of the downwelled system on an f plane is qualitatively described by linear coastal trapped wave dynamics after this time the thermal wind shear associated with the bottom mixed layer becomes important in the evolution of the undercurrent uc which is shown to be driven by the alongshore pressure gradient due to sea level as the uc over the slope evolves the bottom ekman transport becomes small and negative leading to the detachment of flow near the shelf break localized spreading of isopycnals and further intensification of the uc in contrast to results obtained without bottom drag bottom friction and boundary layer transport are shown to lead to a two to threefold increase in cross shelf interior transport downwelling and thermal wind shear by day 60 the resultant uc has speeds of up to 15 cm s 1 and a net transport of

gravity anomalies flexure of the indian plate and the structure support and evolution of the himalaya and ganga basin bouguer gravity anomalies along four profiles across the western himalaya and ganga basin show large deviations from local isostatic equilibrium a deficit of mass characterizes the ganga basin and an excess underlies the lesser himalaya both can be understood if the indian plate is flexed down by the distributed load of part of the mountains the cross sectional shape of the ganga basin seems to be controlled by the deflection of the indian plate which we compute assuming the indian plate to overlie an inviscid fluid from the shapes of both bouguer anomaly profiles and the basement topography we place bounds on the flexural rigidity of such a plate if the ganga basin is a steady state feature then the age of the basal sediments in a given locality should be proportional to the distance of that locality from the southern edge of the basin if the rate of convergence of india and the himalaya were constant that rate should equal the distance divided by the corresponding age we find a rate of 10 to 15 mm a for the last 15 to 20 ma which is consistent with a large part of the 50 mm a rate of convergence between india and eurasia being absorbed by the eastward extrusion of parts of tibet profiles of bouguer gravity anomalies show only a small peak or plateau over the southern edge of the lesser himalaya implying that the boundary between the light sediments of the ganga basin and the heavier crustal rocks of the lesser himalaya is not sharp and that there exists some light material beneath the range we infer that some sediment deposited in the ganga basin has been underthrust beneath the lesser himalaya but the quantity is small most of this sediment probably is scraped off the indian plate to make the foothills of the range we find that the load of the high himalaya is too large to be supported solely by elastic stress in the indian plate if the flexural rigidity of the plate is constant and if no other external forces act on the plate the observed gradient in bouguer gravity anomalies increases from an average of about 1 mgal km over the ganga basin and lesser himalaya to about 2 mgal km over the high himalaya this increase in the gravity gradient implies that the moho dips more steeply 10 15 beneath the high himalaya than beneath the lesser himalaya 2 3 we interpret this steepening of the moho to be due to a weakening of the plate which allows it to bend more sharply beneath the high himalaya than farther south with the inclusion of a weak segment of indian plate beneath the high himalaya calculated anomalies show a somewhat increased gradient beneath the high himalaya but when the weight of the entire himalaya is used as a load on the plate calculated anomalies are more negative than observed therefore an external force system is needed to support much of the weight of the high himalaya as well as to bend the plate sufficiently beneath the high himalaya the magnitudes of the bending moment and the force per unit length that must be applied to the end of the plate are compatible with their sources being gravity acting on a part of india s mantle lithosphere stripped of its crust and underthrust beneath southern tibet

finite strain calculations of continental deformation 1 method and general results for convergent zones a finite element method is used to calculate stresses and strain rates in a thin viscous sheet representing the continental lithosphere that is bordered in one part by an indenting boundary we calculate solutions for velocity fields crustal thickness distributions strain rates rotation time integrated vorticity and finite strain ellipsoids to show the dependence of these quantities on the controlling parameters the stress strain exponent n and the strength of the sheet relative to the gravitational forces which may be expressed as a dimensionless number the argand number ar for n 3 and ar between 1 and 10 a plateau of thickened crust is formed in front of the indenter the strain histories of individual elements within the viscous sheet may be quite complex and the finite strain at the end of deformation may bear no obvious relation to the principal stress orientations during the deformation the strain rate fields are interpreted in terms of the style of faulting that would be expected in the brittle upper crust if it were coupled to the ductile but stronger upper mantle in general the length scale of deformation increases with ar and time since the start of the collision and decreases with n for ar 3 the increase in length scale is accompanied by a change in the style of deformation from predominantly crustal thickening with thrust faulting in the brittle layer to predominantly transcurrent deformation strike slip faulting in the brittle layer

solar quiet current response in the african sector due to a 2009 sudden stratospheric warming event we present solar quiet sq variation of the horizontal h magnetic field intensity deduced from magnetic data acquisition system magdas records over africa during an unusual strong and prolonged 2009 sudden stratospheric warming ssw event a reduction in the sqh magnitude that enveloped the geomagnetic latitudes between 21 13 n fayum fym in egypt and 39 51 s durban drb in south africa was observed while the stratospheric polar temperature was increasing and got strengthened when the stratospheric temperature reached its maximum another novel feature associated with the hemispheric reduction is the reversal in the north south asymmetry of the sqh which is indicative of higher sqh magnitude in the northern hemisphere compared to the southern hemisphere during ssw peak phase the reversal of the equatorial electrojet eej or the counter electrojet cej was observed after the polar stratospheric temperature reached its maximum the effect of additional currents associated with cej was observed in the southern hemisphere at middle latitude similar changes were observed in the eej at the south america pacific ocean and central asia sectors the effect of the ssw is largest in the south american sector and smallest in the central asian sector

the interpretation of inverted metamorphic isograds using simple physical calculations several zones of major thrust faulting exhibit a juxtaposition of rocks of higher metamorphic grade over rocks of lower grade this configuration may indicate but does not require that temperature gradients were temporarily inverted near the fault we examine the physical conditions under which such a temperature inversion could occur the overthrusting of hotter rock on colder rock can cause a temporarily inverted gradient both above and below the fault only if the time taken to underthrust rock from the land surface to a given depth z on the fault is less than times the characteristic time for diffusion of heat through the block above the fault where is thermal diffusivity an inverted gradient cannot form without heat generation in the fault zone unless v z sin 100 where v is the rate of underthrusting in millimeters per year z is in kilometers and is the dip of the fault this simple criterion is sufficient to demonstrate that several examples of inverted metamorphic gradients cannot be explained simply by the thrusting of hot on cold rock without heat sources in the fault zone dissipative heating accompanying deformation can cause an inverted temperature gradient within and beneath the thrust zone but whereas the overthrusting of hot upon cold rocks cools the fault zone dissipation heats it thus the overthrusting of hot on cold rock and dissipative heating affect the temperature gradient and the maximum temperatures differently we show that the magnitudes of the inverted temperature gradient and of the maximum temperature above the inverted gradient yield independent estimates of the rate of dissipative heating discrepancy between these estimates implies that some additional process must have occurred such as the post thrusting disruption of the isograds if there is such a discrepancy the maximum temperature probably provides the more reliable estimate of the rate of heating at the fault we illustrate this analysis by applying it to reported inverted metamorphic zonation in the pelona schist the st anthony complex the mt everest region of the main central thrust and the olympos thrust petrological inferences of maximum temperatures depths of metamorphism and magnitudes of apparent inverted gradients imply that shear stresses of about 100 mpa accompanied thrust faulting in some of these regions and that some zones of inverted metamorphism have been tectonically thinned after the metamorphism occured

formation and maintenance of shelfbreak fronts in an unstratified flow abstract a depth averaged model with no density variations was used by chapman to describe the formation of a passive tracer front at a shelfbreak the relevance of this frontogenesis mechanism to cases that allow vertical variations is examined by considering the three dimensional structure of a passive tracer front with explicit finite vertical mixing and bottom boundary layer dynamics a three dimensional primitive equation numerical model is configured in a channel with a continental shelf slope and abyssal plain running the length of the channel a vertically and horizontally uniform inflow is imposed over the shelf with a large horizontal velocity shear near the shelfbreak in the primitive equation model the offshore flow is concentrated in the bottom boundary layer while the alongshelf flow distribution is similar to the depth averaged case the presence of the bottom topography maintains a strong horizontal shear near the shelfbreak above the bottom boundary layer this velocity shear causes

coastal upwelling onshore offshore circulation equatorward coastal jet and poleward undercurrent over a continental shelf slope abstract the onshore offshore circulation equatorward coastal jet and poleward undercurrent associated with coastal upwelling are studied with numerical models the model ocean has a continental shelf slope uniform in the longshort direction and is forced by the wind stress with a limited longshore extent the thermocline intersects the shelf slope and the internal radius of deformation is smaller than the width of the shelf slope this may be a typical situation for coastal upwelling regions such as those off oregon and northwest africa as the initial response to the onset of the winds the ekman offshore flow and the compensating onshore flow are induced and the equatorward flow develops over the shelf slope when the first mode coastal trapped wave from the equatorward edge of the forcing region arrives the onshore compensating flow offshore of the coastal area begins to decrease in strength and eventually offshore flow accompanied by downwelling dominates thus the upwelling tends to be confined t

40ar 39ar age constraints on deformation and metamorphism in the main central thrust zone and tibetan slab eastern nepal himalaya in eastern nepal structural and petrologic observations suggest that movement on the main central thrust mct the development of an inverted metamorphic sequence and leucogranite plutonism were genetically related samples from across the mct zone and its hanging wall the tibetan slab were collected from four locations in the everest region for 40ar 39ar studies 1 the mct zone 2 the lower tibetan slab 3 the upper tibetan slab away from intrusive rocks and 4 the upper tibetan slab adjacent to and including leucogranitic material within the mct zone muscovite and hornblende yield cooling ages of 12 0 0 2 ma and 20 9 0 2 ma respectively k feldspar gives a minimum age of 8 0 0 2 ma closure temperature tc 220 15 c in the lower tibetan slab a sample from a sheared pegmatite yields muscovite and biotite isochron ages of 7 7 0 4 ma and 7 5 0 6 ma and a k feldspar minimum age of 6 4 0 8 ma tc 225 20 c an adjacent gneiss yields a 9 1 0 2 ma biotite isochron and a k feldspar minimum age of 3 6 0 2 ma tc 210 50 c in the upper tibetan slab samples collected 200 m from visible intrusives yield a biotite isochron age of 20 2 0 2 ma and a complex hornblende age spectrum suggestive of excess argon at the fourth location an augen gneiss a pegmatite and a tourmaline bearing leucogranite all in mutual contact yield indistinguishable mineral ages the average biotite and muscovite isochron ages for these samples are 17 0 1 4 and 16 6 0 2 ma respectively the minimum age for k feldspar from the leucogranite is 15 5 1 8 ma as thermobarometric data from the mct zone in this area suggest synmetamorphic deformation at temperatures of 500 550 c the mct hornblende tc 500 c dates this event at 21 ma diffusion experiments on hornblendes from the mct zone provide data which support a maximum duration of peak metamorphic temperatures of 2 ma biotite ages as old as 20 ma from the upper tibetan slab near leucogranites indicate that leucogranite intrusion was essentially coeval with deformation and metamorphism in the mct zone very young ages in a ductile shear zone in the lower tibetan slab suggest that there has been deformation within the tibetan slab that postdates major movement on the mct

observations of the antarctic slope undercurrent in the southeastern weddell sea 1 the antarctic slope front presents a dynamical barrier between the cold antarctic shelf waters in contact with ice shelves and the warmer subsurface waters offshore two hydrographic sections with full depth current measurements were undertaken in january and february 2009 across the slope and shelf in the southeastern weddell sea southwestward surface intensified currents of 30 cm s 1 and northeastward undercurrents of 6 9 cm s 1 were in thermal wind balance with the sloping isopycnals across the front which migrated offshore by 30 km in the time interval between the two sections a mid depth undercurrent on february 23 was associated with a 130 m uplift of the main pycnocline bringing warm deep water closer to the shelf break this vertical displacement comparable to that caused by seasonal variations in wind speed implies that undercurrents may affect the exchanges between coastal and deep waters near the antarctic continental margins

geochemical discrimination of clastic sedimentary rock sources abstract factors controlling the geochemistry of a clastic sedimentary rock can include 1 composition of source terrain 2 chemical weathering 3 hydraulic sorting 4 diagenesis 5 metamorphism and 6 hydrothermal alteration a linear solution inferring source terrain composition from geochemistry of the sediment is impossible in this multivariate system as several unknowns will commonly be present the use of graphical analysis of element pairs circumvents the problem chemically immobile elements will maintain invariant ratios during rock mass change caused by either addition or depletion of mobile elements this results in chemically immobile element scattergrams exhibiting linear trends along radians extending from the origin if the major mineral phases of the immobile elements have behaved in a hydrodynamically similar manner as chemically mobile element plots will produce a scatter of points this relationship can be used to test chemical immobility and similarity in hydrodynamic sorting history the constraint on analysis is that the source area must be compositionally uniform or the sediment well mixed prior to delivery to the basin a second technique using sio2 plots has also been developed to investigate element mobility and hydrodynamic behaviour of the mineral phases containing the elements sio2 immobile element plots result in a linear arrangement of points extending towards either 0 or 100 sio2 the 0 intercept position occurs for elements with major mineral phases concentrated in sand the 100 intercept for those concentrated in clays plotting chemically mobile elements produces different patterns and this can be used to gain information on alteration and sorting history elemental ratios for chemically immobile elements with similar hydrodynamic behaviour will be the same as those for the weighted average composition of the source material this provides a powerful tool for deducing source terrain from sediment geochemistry techniques outlined above were tested on archaean metasandstones from superior province canada immobile element ratio diagrams for nb al ti and zr al ti indicate that a calc alkaline extrusive intrusive suite lying to the north of the study area was the source and not five other volcanic suites in the region this conclusion agrees with previous clast lithology studies and accentuates the applicability of the geochemical techniques

longitudinal variation of ionospheric vertical drifts during the 2009 sudden stratospheric warming 1 the whole atmospheric model wam initialized with a data assimilation scheme is capable of simulating real sudden stratospheric warming ssw events the electrodynamics in the coupled thermosphere ionosphere and plasmasphere with electrodynamics model ctipe was driven by the wam thermospheric winds in january 2009 to study the response of ionospheric drifts during the ssw simulation results are compared with observations of the vertical drift at jicamarca and the equatorial electrojet eej in the asian sectors early morning upward drift and afternoon downward drift are reproduced in all longitudes in the simulations and are consistent with the available observations results also show that the occurrence time of the early morning upward drift and afternoon downward drift have significant phase differences between different longitudes simulations suggest that during the ssw the longitude dependence of the amplitude and phase of the equatorial vertical plasma drift is caused by the changing magnitudes of the migrating tides modulated by the geometry of the geomagnetic field some additional day to day variability and modulation of the phase structures at different longitudes in ionospheric vertical drifts during the ssw are possibly produced by the short term changes in the non migrating tides and by planetary waves

isotopic study of the manaslu granite himalaya nepal inferences on the age and source of himalayan leucogranites a detailed isotopic study of the manaslu leucogranite was carried out a u pb age of 25 ma and a whole rock rb sr age isochron of 18 ma were obtained suggesting that the magmatic activity lasted at least 7 ma initial sr isotopic ratios are very high 0 740 to 0 760 and initial nd isotopic ratios are low nd in 13 to 16 and they show the existence of large isotopic variations even at the metre scale these are not the result of perturbations by fluids but rather they reflect the initial isotopic heterogeneity of the source material which has not been obliterated by magmatic processes e g fusion mixing by convection these results also support the crustal origin of this leucogranite the tibetan slab paragneisses whose sr and nd isotopic ratios are very similar to those of the granite at an age of 20 ma are the most probable parental material nd model ages for both the leucogranite and the gneisses are in the range 1 5 2 ga a model of formation of the manaslu granite by coalescence of different batches of magma is in agreement with the present data

longitudinal and interhemispheric ionospheric response to 2009 and 2013 ssw events in the african european and indian east asian sectors

geochemical investigations of the origin of the manaslu leucogranite himalaya nepal the himalayan orogeny is characterized by an intraplate subduction zone the thrusting of the tibetan slab over the foreland is probably responsible for the origin of the manaslu type leucogranites this geochemical study tries to examine the crustal origin of the granite to verify whether the paragneisses of the tibetan slab are the most probable parent material and to determine the subsequent petrogenetic processes the rb sr systematics suggest that 1 1 the scatter of data points in the 87sr86srvs 87rb86sr diagram may be due to the heterogeneity of the initial 87sr86sr ratios 2 2 the initial isotopic ratios are very high 0 730 0 760 and are in agreement with those of the gneisses of the tibetan slab at the time of the melting pb isotopic ratios are homogeneous they are also consistent with a crustal prehistory the ree and th contents are unexpectedly low in comparison with the much higher contents of the parent material monazite left in the residue of melting or more probably extracted in an early stage of the magmatic history may explain the observed ree and th abundances alternatively field observations show that the emplacement of the granite has been accompanied by a very strong hydrothermal activity in consequence the low ree and th contents of the granite could also be due to the loss by solution during prolonged fluid circulation throughout the granitic melt and the sr and pb isotope distribution to the effect of late to post magmatic fluids the isotopic character of which was determined by the underlying tibetan slab

ductile shear as a cause of inverted metamorphism example from the nepal himalaya in many mountain belts metamorphic sequences occur in an inverted arrangement such that rocks of higher metamorphic grade overlie rocks of lower metamorphic grade in some locations such as the main central thrust mct zone of the himalaya the metamorphic inversion is coincident with the zone of ductile thrust deformation although many explanations have been suggested for the metamorphic inversion of the himalaya none are consistent with all of the observed features a new model based on observations from the eastern nepal himalaya consists of inversion of the metamorphic sequence due to ductile shearing of a pre existing zone of right way up metamorphism this simple structural explanation creates an inverted metamorphic sequence consistent with observations of 1 a zone of distributed deformation 2 metamorphic textures overprinted by deformation and 3 metamorphic isograds sub parallel to shear fabric these observations are not all well accounted for by previously proposed models in this st

shelfbreak current over the canadian beaufort sea continental slope wind driven events in january 2005 the shelfbreak current over the beaufort sea continental slope is known to be one of the most energetic features of the beaufort sea hydrography in january 2005 three oceanographic moorings deployed over the canadian eastern beaufort sea continental slope simultaneously recorded two consecutive shelfbreak current events with along slope eastward bottom intensified flow up to 120 cm s 1 both events were generated by the local wind forcing associated with two pacific born cyclones passing north of the beaufort sea continental slope toward the canadian archipelago over the mooring array the associated westerly wind exceeded 15 m s 1 these two cyclones generated storm surges along the beaufort sea coast with sea surface height ssh rising up to 1 4 m following the two westerly wind maxima we suggest that the westerly along slope wind generated a surface ekman onshore transport the associated ssh increase over the shelf produced a cross slope pressure gradient that drove an along slope eastward geostrophic current in the same direction as the wind this wind driven barotropic flow was superimposed on the background baroclinic bottom intensified shelfbreak current that consequently amplified summer fall satellite altimetry data for 1992 2013 show that the ssh gradient in the southeastern beaufort sea is enhanced over the upper continental slope in response to frequent storm surge events because the local wind forcing and or sea ice drift could not explain the reduction of sea ice concentration over the beaufort sea continental slope in january 2005 we speculate that wind driven sea level fluctuations may impact the sea ice cover in winter

the metamorphism in the central himalaya all along the himalayan chain an axis of crystalline rocks has been preserved made of the higher himalaya crystalline and the crystalline nappes of the lesser himalaya the salient points of the metamorphism as deduced from data collected in central himalaya central nepal and kumaun are 1 the higher himalaya crystalline also called the tibetan slab displays a polymetamorphic history with a first stage of barrovian type overprinted by a lower pressure and or higher temperature type metamorphism the metamorphism is due to quick and quasi adiabatic uplift of the tibetan slab by transport along an mct ramp accompanied by thermal refraction effects in the contact zone between the gneisses and their sedimentary cover the resulting metamorphic pattern is an apparent diachronic inverse zonation with the sillimanite zone above the kyanite zone 2 conversely the famous inverted zonation of the lesser himalaya is basically a primary pattern acquired during a one stage prograde metamorphism its origin must be related to the thrusting along the mct with heat supplied from the overlying hot tibetan slab as shown by synmetamorphic microstructures and the close geometrical relationships between the metamorphic isograds and the thrust 3 thermal equilibrium is reached between units above and below the mct far behind the thrust tip there is good agreement between the maximum temperature attained in the hanging wall and the temperature of the tibetan slab during the second metamorphic stage but closer to the mct front the thermal accordance between both sides of the thrust is due to a retrogressive metamorphic episode in the basal part of the tibetan slab

variations of mesospheric neutral winds and tides observed by a meteor radar chain over china during the 2013 sudden stratospheric warming the neutral winds in the mesospheric and lower thermospheric region obtained from a meteor radar chain within the latitudinal range of 18 53 n were decomposed to examine the latitudinal structures of the tides and mean winds during the sudden stratospheric warming ssw event in 2013 the zonal wind reversed from eastward to westward and the westward wind was larger at middle latitudes than that at low latitudes during the ssw meanwhile a sharp increase in the northward wind was noticeable at all stations the amplitudes of the diurnal and semidiurnal tides decreased from 5 to 13 january and increased subsequently at the same time the terdiurnal tides increased in amplitude especially at beijing wuhan and kunming in response to the ssw moreover the tidal phases showed a large shift that corresponded to a great increase in tidal wavelengths in the semidiurnal and terdiurnal components the wavelet analysis further revealed that the quasi 6 day wave oscillations dominated in the winds at kunming and sanya stations as well as the quasi 16 day wave dominated in the zonal wind and the quasi 11 day and 16 day waves were prevailing in the meridional winds at beijing and wuhan in the same vein the quasi 16 day and quasi 11 day waves were prominent in the zonal and meridional winds during 1 18 january at mohe therefore the tide planetary wave interactions played a significant role in modulating the behaviors of the mesospheric and lower thermospheric dynamics during the ssw event

features of global geomagnetic sq field from 1980 to 1990 1 seasonal and year to year variations of geomagnetic sq field were examined using the global equivalent current system for one solar cycle from 1980 to 1990 it was confirmed that the sq current intensity is about half in solar minimum of that in solar maximum and its year to year variation is relatively smooth for each month at 0200 ut vortices in the winter and summer hemispheres shift to the afternoon and morning side respectively but with phase delay by about 1 or 2 months on the contrary at 1400 ut the northern vortex is located in the morning side of the southern vortex in most months of all years and seasonal variation of the location is not so clear as for the morphology of the current system it was found that there are only two types in the shape of the sq current system at 0200 ut that is it shows northern summer type from april to september and northern winter type from october to march and there is no equinox type and it clearly differs in march from that in september this feature is similar to that of the seasonal variation type of the tidal winds in the upper mesosphere

highly localized cooling in daytime mesopause temperature over the dip equator during counter electrojet events first results the first observations of lowering of mesopause temperature during counter electrojet cej events over a narrow region of 150 km centered at around magnetic equator are presented the daytime mesopause temperature is measured over trivandrum 8 5 n 77 e dip lat 0 5 n india using the ground based multiwavelength dayglow photometer the unique meridional scanning capability of the instrument is extensively used in this study a lowering of temperature by as much as 25 k has been observed during certain cej events which includes a few partial cejs the gravity wave tidal interaction through vertically upward wind is proposed to be manifesting as lowering in the mesopause temperature and also as cej these observations are new and address to the issues concerning the vertical coupling processes prevailing in the equatorial mesosphere lower thermosphere ionosphere mlti region citation vineeth c t k pant c v devasia and r sridharan 2007 highly localized cooling in daytime mesopause temperature over the dip equator during counter electrojet events

a structural analysis of the main central thrust zone langtang national park central nepal himalaya the main central thrust mct is one of the most tectonically significant structures in the himalayan orogen detailed geologic mapping and structural analysis of the mct in the langtang national park region of central nepal reveals that this segment of the fault zone experienced multiple episodes of south directed movement under both brittle and ductile conditions during the tertiary period early mid miocene movement resulted in the development of mylonitic fabrics synchronous with amphibolite facies metamorphism the mean orientation of the dominant mylonitic foliation is n28 w 38 ne an associated mineral stretching lineation plunges 40 to n40 e kinematic indicators suggest hanging wall movement to the southwest relative to the footwall along the north dipping fault it is not possible to constrain the magnitude of high temperature displacement on the mct at the longitude of langtang late stage structures in the mct zone at langtang include a series of imbricate brittle thrust faults that separate different lithostratigraphic units and correspond to metamorphic discontinuities we interpret this fault system as a duplex structure muscovite 40 ar 39 ar cooling ages from the mct zone range from 8 9 6 9 ma because the nominal closure temperature of ar diffusion in muscovite approximately 625 k is higher than the apparent temperature conditions under which late brittle deformation occurred we suggest that brittle deformation was a latest miocene pliocene phenomenon another major himalayan fault the main boundary thrust mbt was developing to the south of langtang at approximately the same time we speculate that brittle faulting within the mct zone may have initiated as the mct zone was transported over a ramp in the mbt

flow near submarine canyons driven by constant winds circulation over coastal submarine canyons driven by constant upwelling or downwelling wind stress is simulated and analyzed with a primitive equation ocean model astoria canyon on the west coast of north america is the focus of this study and model results are consistent with most major features of mean canyon circulation observed in astoria canyon near surface flow crosses over the canyon while a closed cyclone occurs within the canyon upwelling prevails within the canyon and is larger than wind driven upwelling along the adjacent shelf break water rises from depths reaching 300 m to the canyon rim and subsequently onto the adjacent shelf onshore flow within the canyon is driven by the onshore pressure gradient force due to the free surface slope created by the upwelling wind and is enhanced by the limitation to alongshore flow by the canyon topography density gradients largely compensate the surface slope with realistic stratification but continual upwelling persists near the edges of the canyon within the upper canyon 50 150 m below the canyon rim a cyclone is created by flow turning into the canyon mouth separating from the upstream edge and advecting toward the downstream rim below this layer the cyclone is created by vortex stretching due to the upwelling downwelling winds create nearly the opposite flow in which compression and momentum advection create a strong anticyclone within the canyon momentum advection is found to be important both in creating strong circulation within the canyon and in allowing the surface flow to cross the canyon undisturbed model results indicate that astoria like submarine canyons produce across shore transport of sufficient volume to flush a continental shelf in a few 2 5 years

origin of the inverted metamorphism of the lower himalayas central nepal abstract the southern slope of the central nepal himalayas is divided geologically by the main central thrust zone into the underlying midland metasediment zone lower himalayas in the south and the overlying himalayan gneiss zone higher himalayas in the north the former zone consists of a thick pile of various kinds of metasediments folded into an anticlinorium and the latter zone consists of high grade crystalline rocks with a north dipping homoclinal structure and is further overlain by the tethys himalayas composed of non or slightly metamorphosed tethyan sediments the main central thrust zone shows a characteristic lithology such as calcareous schist quartzite phyllitic schist and augen gneiss and is intensely mylonitized the mineral composition and paragenesis of the rocks in the present area indicate an inverted metamorphism from the midland metasediment to the main central thrust zones that is the metamorphic grade of the midland metasediment zone increases upward toward the thrust zone from the chlorite to the biotite zones of the greenschist facies and the greenschist amphibolite transitional zone is attained in the thrust zone the himalayan gneiss zone is apparently much higher in metamorphic grade than the thrust zone on the basis of the compositional zoning of garnets and muscovite compositions however it is concluded that the himalayan gneisses suffered a polymetamorphism the younger metamorphism resulted in a retrograde metamorphism of the himalayan gneisses together with the above mentioned inverted metamorphism and an anatectic melting in depth this was caused by shear heating due to the thrust movement along the main central thrust zone during the alpine tectonism the older metamorphism which seems to be precambrian in age was much higher in metamorphic grade than the younger one and formed the pyrope rich cores of garnets in the himalayan gneisses the maximum metamorphic temperature of 550 c estimated from the mineral paragenesis in the thrust zone is compatible with that caused by shear heating due to the thrusting with thrusting velocity of 5 10 cm yr maximum stress of 300 bars and thrusting distance of 250 km bird 1978

variability of circumpolar deep water transport onto the amundsen sea continental shelf through a shelf break trough 1 the presence of warm circumpolar deep water cdw intrusions on the amundsen continental shelf has been linked to recent thinning of the outlet glaciers draining the west antarctic ice sheet into the amundsen sea inflow of the cdw onto the shelf is thought to occur within a series of troughs that intersect the continental shelf break we use observations between 1994 and 2011 and a numerical model to investigate the variability of cdw transport in a trough intersecting the shelf break at 113 w the location of the main cdw inflow into the trough varies between its eastern flank and center while the western part of the trough is filled by a recirculation that commonly entrains cooler water originating further south on the shelf thermocline depth decreases between the early and late 2000s with an indication that the depth of the 1994 thermocline was similar to the later years mooring results show that the cdw layer cools and thins in summer and thickens and warms in winter in addition to a deeper thermocline in summer we observe a stronger presence of lower cdw in the bottom of the trough heat flux onto the shelf is controlled by current velocities rather than cdw temperature and the majority of the heat is carried onto the shelf by background flow rather than episodic events

effect of sudden stratospheric warming on lunar tidal modulation of the equatorial electrojet 1 using the equatorial electrojet eej peak current intensity as deduced from champ magnetic observations from the years 2001 through 2009 we investigated the relationship between sudden stratospheric warming ssw and lunitidal signatures in the tropical ionosphere there is a practically one to one correspondence between midwinter ssw periods and the strongest 13 day modulation of the eej strength as observed by champ that is all the midwinter ssw periods from december 2001 to august 2009 were accompanied by an enhanced 13 day modulation of the eej strength no other geophysical phenomenon brought about as strong a 13 day modulation as those of the midwinter ssw periods during each midwinter ssw period the amplified 13 day modulation of the eej strengths starts roughly within 1 week around the first peak in stratospheric temperature difference an oscillation with a period of 13 26 days is predicted by the lunitidal equation when considering the precession of the champ orbit when fitting the lunitidal equation to the eej modulations during the midwinter ssw periods consistent phase delays of 4 4 0 3 days of the tidal signal emerge for all the cases the results suggest that the pronounced 13 day modulation of the eej strength is related to an enhancement of the lunar tide in the ionosphere by the ssw effect