Record 1 of 34
Author(s): JIN FF; NEELIN JD
Title: MODES OF INTERANNUAL TROPICAL OCEAN-ATMOSPHERE INTERACTION - A UNIFIED VIEW .1. NUMERICAL RESULTS
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1993, Vol 50, Iss 21, pp 3477-3503
No. cited references: 69
KeywordsPlus: SEA-SURFACE TEMPERATURE; GENERAL-CIRCULATION MODELS; SELF-EXCITED OSCILLATIONS; NINO SOUTHERN OSCILLATION; WIND STRESS PATTERNS; EL-NINO; EQUATORIAL OCEAN; COUPLED MODEL; BASIC STATE; ENSO
Abstract: Coupled ocean-atmosphere models exhibit a variety of forms of tropical interannual variability that may be understood as different flow regimes of the coupled system. The parameter dependence of the primary bifurcation is examined in a ''stripped-down'' version of the Zebiak and Cane model using the equatorial band approximation for the sea surface temperature (SST) equation as by Neelin. In Part I of this three-part series, numerical results are obtained for a conventional semispectral version; Parts II and III use an integral formulation to generate analytical results in simplifying limits. In the uncoupled case and in the fast-wave limit (where oceanic adjustment occurs fast compared to SST time scales), distinct sets of modes occur that are primarily related to the time scales of SST change (SST modes) and of oceanic adjustment (ocean-dynamics modes). Elsewhere in the parameter space, the leading modes are best characterized as mixed SST/ocean-dynamics modes; in particular, the continuous surfaces-in parameter space formed by the eigenvalues of each type of mode can join. A regime in the fast-wave limit in which the most unstable mode is purely growing, with SST anomalies in the eastern Pacific, proves to be a useful starting point for describing these mergers. This mode is linked to several oscillatory regimes by surfaces of degeneracy in the parameter space, at which two degrees of freedom merge. Within the fast-wave limit, changes in parameters controlling the strength of the surface layer or the atmospheric structure produce continuous transition of the stationary mode to propagating modes. Away from the fast-wave limit, the stationary mode persists at strong coupling even when time scales of ocean dynamics become important. On the weaker coupling side, the stationary mode joins to an oscillatory mode with mixed properties, with a standing oscillation in SST whose growth and spatial form may be understood from the SST mode at the fast-wave limit but whose period depends on subsurface oceanic dynamics. The oceanic dynamics, however, is only remotely related to that of the uncoupled problem. In fact, this standing-oscillatory mixed mode is insensitive to low-coupling complications involving connections to a sequence of uncoupled ocean modes at different parameter values, most of which are members of a discretized scattering spectrum. The implication that realistic coupled regimes are best understood from strong rather than weak coupling is pursued in Parts II and III. The interpretation of the standing-oscillatory regime as a stationary SST mode perturbed by wave dynamics gives a rigorous basis to the original physical interpretation of a simple model of Suarez and Schopf. However, viewing the connected modes as different regimes of a mixed SST/ocean-dynamics mode allows other simple models to be interpreted as alternate approximations to the same eigensurface; it also makes clear why varying degrees of propagating and standing oscillation can coexist in the same coupled mode.
Cited references: ANDERSON DLT-1985-J-ATMOS-SCI-V42-P615
BARNETT T-1988-SCIENCE-V241-P192
BARNETT TP-1991-J-CLIMATE-V4-P487
BATTISTI DS-1989-J-ATMOS-SCI-V46-P1687
BATTISTI DS-1988-J-ATMOS-SCI-V45-P2889
BATTISTI DS-1989-J-PHYS-OCEANOGR-V19-P551
BJERKNES J-1969-MON-WEATHER-REV-V97-P163
CANE MA-1990-J-ATMOS-SCI-V47-P1562
CANE MA-1981-J-MAR-RES-V39-P651
CANE MA-1979-J-MAR-RES-V37-P233
CANE MA-1979-J-MAR-RES-V37-P253
CANE MA-1977-J-MAR-RES-V35-P395
CANE MA-1981-J-PHYS-OCEANOGR-V11-P1578
CANE MA-1986-NATURE-V321-P827
CANE MA-1985-SCIENCE-V228-P1084
CHAO Y-1993-J-CLIMATE-V6-P450
GHIL M-1991-REV-GEOPHYS-S-V46
GILL AE-1974-DEEP-SEA-RES-V21-P325
GILL AE-1985-ELSEVIER-OCEANOGR-SE-V40
GILL AE-1983-NATURE-V306-P229
GILL AE-1980-Q-J-ROY-METEOR-SOC-V106-P447
GOLUBITSKY M-1988-SINGULARITIES-GROUPS-V2
GOLUBITSKY M-1985-SINGULARITIES-GROUPS-V1
GORDON C-1989-PHILOS-T-ROY-SOC-A-V329-P207
GRAHAM NE-1990-J-PHYS-OCEANOGR-V20-P1935
GRAHAM NE-1988-SCIENCE-V240-P1293
GUCKENHEIMER J-1983-APPLIED-MATH-SCI-V42
HAO Z-1993-J-CLIMATE-V6-P1523
HIRST AC-1988-J-ATMOS-SCI-V45-P830
HIRST AC-1986-J-ATMOS-SCI-V43-P606
IOOSS G-1990-ELEMENTARY-STABILITY
JIN FF-1993-J-ATMOS-SCI-V50-P3523
LATIF A-1993-J-CLIMATE-V6-P700
LATIF M-1990-J-MAR-SYST-V1-P51
LATIF M-1992-J-PHYS-OCEANOGR-V22-P951
LAU KM-1981-J-ATMOS-SCI-V38-P248
LAU NC-1992-J-CLIMATE-V5-P284
LINDZEN RS-1987-J-ATMOS-SCI-V44-P2440
MATSUNO T-1966-J-METEOR-SOC-JAPAN-V44-P25
MCCREARY J-1976-J-PHYS-OCEANOGR-V6-P632
MECHOSO CR-1993-MON-WEATHER-REV-V121-P2062
MEEHL GA-1990-CLIM-DYNAM-V5-P19
MEEHL GA-1990-J-CLIMATE-V3-P72
MOORE DW-1968-THESIS-HARVARD-U-CAM
MUNNICH M-1991-J-ATMOS-SCI-V48-P1238
NAGAI T-1992-J-CLIMATE-V5-P1202
NEELIN JD-1992-CLIM-DYNAM-V7-P73
NEELIN JD-1993-IN-PRESS-J-ATMOS-SCI-V50
NEELIN JD-1991-J-ATMOS-SCI-V48-P584
NEELIN JD-1990-J-ATMOS-SCI-V47-P674
NEELIN JD-1989-J-ATMOS-SCI-V46-P2466
NEELIN JD-1987-MON-WEATHER-REV-V115-P3
NEELIN JD-1989-PHILOS-T-ROY-SOC-A-V329-P189
NEELIN JD-1988-Q-J-ROY-METEOR-SOC-V114-P747
PHILANDER SGH-1984-J-ATMOS-SCI-V41-P604
PHILANDER SGH-1992-J-CLIMATE-V5-P308
PHILANDER SGH-1980-J-GEOPHYS-RES-OC-ATM-V85-P1123
PHILANDER SGH-1981-J-PHYS-OCEANOGR-V11-P176
RASMUSSON EM-1982-MON-WEATHER-REV-V110-P354
SCHOPF PS-1988-J-ATMOS-SCI-V45-P549
SCHOPF PS-1990-J-PHYS-OCEANOGR-V20-P629
SCHOPF PS-1983-J-PHYS-OCEANOGR-V13-P917
SPERBER KR-1991-CLIM-DYNAM-V6-P83
SUAREZ MJ-1988-J-ATMOS-SCI-V45-P3283
WAKATA Y-1991-J-ATMOS-SCI-V48-P2060
YAMAGATA T-1985-ELSEVIER-OCEANOGR-SE-V40-P637
YAMAGATA T-1989-PHILOS-T-ROY-SOC-A-V329-P225
ZEBIAK SE-1987-MON-WEATHER-REV-V115-P2262
ZEBIAK SE-1986-MON-WEATHER-REV-V114-P1263
Times Cited: 40
Source item page count: 27
Publication Date: NOV 1
IDS No.: MF553
29-char source abbrev: J ATMOS SCI



Record 2 of 34
Author(s): HABERLE RM; HOUBEN HC; HERTENSTEIN R; HERDTLE T
Title: A BOUNDARY-LAYER MODEL FOR MARS - COMPARISON WITH VIKING LANDER AND ENTRY DATA
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1993, Vol 50, Iss 11, pp 1544-1559
No. cited references: 45
KeywordsPlus: GLOBAL DUST STORMS; MARTIAN ATMOSPHERE; GENERAL-CIRCULATION; SIMULATIONS; TOPOGRAPHY; EARTH
Abstract: A one-dimensional boundary-layer model for Mars is described, and its results are compared with Viking data. The model equations are similar to Earth boundary-layer models in that they include contributions from Coriolis, pressure gradient, and frictional forces for momentum; and radiation, sensible heat flux convergence, and advection for heat. Turbulent fluxes are computed from the level-2 second-order closure theory of Mellor and Yamada with similarity relations employed for boundary conditions. The pressure gradient force can be specified or computed from a simple slope model. Radiative heating is due to the absorption of solar and infrared radiation by CO2 ps and suspended dust particles. Ground temperatures are computed by solving a surface heat budget using an accurate treatment of conduction into the Martian soil. The data used for comparison were obtained by the Viking 1 and 2 landers for early northern summer. At each site, these data include a single profile of wind and temperature between 1.5 and 4 km and their diurnal variations at 1.6 m above the surface. Model-predicted temperatures are in good agreement with the data, though they show a greater variation at 1.6 m than is evident in the data. Model-predicted winds compare less favorably in that they can match the surface data or the profiles, but not both simultaneously. In addition, best agreement is obtained using a slope magnitude and/or direction that is different from reported values. However, the model can reproduce the shape, phase, and sense of rotation of the surface wind hodograph at each site. Some features of the simulations include low-level nocturnal jets, which may be common on Mars, and a negative feedback between dust and surface stress. The sensitivity of the model to uncertain parameters such as dust load, optical properties, and surface roughness is discussed.
Cited references: ANDRE JC-1978-J-ATMOS-SCI-V35-P1862
ARYA SP-1988-INTRO-MICROMETEOROLO
BALMINO G-1982-J-GEOPHYS-RES-V87-P9735
BLACKADAR AK-1957-B-AM-MET-SOC-V38-P283
BLACKADAR AK-1962-J-GEOPHYS-RES-V67-P3095
BLUMSACK SL-1973-J-ATMOS-SCI-V30-P66
BONNER WD-1968-MON-WEA-REV-V96-P735
COLBURN DS-1989-ICARUS-V79-P159
CRISP D-1986-J-GEOPHYS-RES-ATMOS-V91-P1851
FLASAR FM-1976-PLANET-SPACE-SCI-V24-P161
GIERASCH P-1968-PLANET-SPACE-SCI-V16-P615
GIERASCH PJ-1973-J-ATMOS-SCI-V30-P169
GIERASCH PJ-1972-J-ATMOS-SCI-V29-P400
GOODY RM-1967-PLANET-SPACE-SCI-V15-P247
GREELEY R-1985-WIND-GEOLOGICAL-PROC
HABERLE RM-1991-ICARUS-V90-P187
HABERLE RM-1982-ICARUS-V50-P322
HESS SL-1977-J-GEOPHYSICAL-RES-V82-P4559
HOLTON JR-1967-TELLUS-V19-P199
IVERSEN JD-1976-J-ATMOS-SCI-V33-P2425
KIEFFER HH-1977-J-GEOPHYSICAL-RES-V82-P4249
LEOVY CB-1973-J-ATMOSPHERIC-SCI-V30-P749
LETTAU H-1969-J-APPL-METEOROL-V8-P828
MAGALHAES J-1982-J-GEOPHYS-RES-V87-P9975
MAHRER Y-1977-MON-WEATHER-REV-V105-P1151
MARTIN TZ-1986-ICARUS-V66-P2
MCNIDER RT-1981-J-ATMOS-SCI-V38-P2198
MELLOR GL-1974-J-ATMOS-SCI-V31-P1791
MELLOR GL-1982-REV-GEOPHYS-V20-P851
MONIN AS-1971-STATISTICAL-FLUID-ME-P417
MURPHY JR-1990-J-GEOPHYS-RES-SOLID-V95-P14629
MURPHY JR-1991-THESIS-U-WASHINGTON
PALLMANN AJ-1983-J-GEOPHYS-RES-OC-ATM-V88-P5483
POLLACK JB-1981-J-ATMOS-SCI-V38-P3
POLLACK JB-1979-J-GEOPHYS-RES-V84-P2929
POLLACK JB-1990-J-GEOPHYS-RES-SOLID-V95-P1447
POLLACK JB-1977-J-GEOPHYSICAL-RES-V82-P4479
RYAN JA-1979-J-GEOPHYS-RES-V84-P2821
SEIFF A-1993-IN-PRESS-J-GEOPHYS-R
SEIFF A-1977-J-GEOPHYSICAL-RES-V82-P4364
SUTTON JL-1978-J-ATMOS-SCI-V35-P2346
THORPE AJ-1977-Q-J-ROY-METEOR-SOC-V103-P633
TOON OB-1977-ICARUS-V30-P663
YE ZJ-1990-J-ATMOS-SCI-V47-P612
ZUREK RW-1992-MARS-P835
Times Cited: 14
Source item page count: 16
Publication Date: JUN 1
IDS No.: LG782
29-char source abbrev: J ATMOS SCI



Record 3 of 34
Author(s): GRANT ALM
Title: THE STRUCTURE OF TURBULENCE IN THE NEAR-NEUTRAL ATMOSPHERIC BOUNDARY-LAYER
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1992, Vol 49, Iss 3, pp 226-239
No. cited references: 34
KeywordsPlus: SPECTRAL CHARACTERISTICS; SURFACE-LAYER; WIND; SEA; STRESS
Abstract: In this paper, the idea of local similarity, previously used to study turbulence in the stably stratified boundary layer, is used to investigate the structure of turbulence in the neutral atmospheric boundary layer and to relate this structure to the turbulent kinetic energy balance. It is found that in the lower half of the boundary layer, the turbulence exhibits local similarity and that the turbulence kinetic energy budget is essentially a balance between shear production and dissipation. In the upper half of the boundary layer, where turbulent transport is a significant term in the turbulence kinetic energy balance, local similarity breaks down. This is consistent with the second-order moment equations, which suggest that local similarity arises in situations where the turbulent and pressure transport terms are small. Results from a large-eddy simulation of the neutral boundary layer are also investigated using local similarity. The simulated turbulence agrees well with the observations for the stress-energy ratio and the stress correlation coefficient, which are related to the production of turbulent kinetic energy and the transport of momentum, respectively. However, for the ratios of velocity component variances the agreement is not quite so good. This may be due to the effect of the simulations' relatively low turbulent Reynolds number on the pressure-strain correlations and/or inadequacies in the subgrid parameterization.
Cited references: ANDREN A-1990-J-APPL-METEOROL-V29-P224
BELJAARS ACM-1987-BOUND-LAY-METEOROL-V38-P95
BROST RA-1982-J-ATMOS-SCI-V39-P818
CHOU SH-1986-J-ATMOS-SCI-V43-P547
DERBYSHIRE SH-1990-Q-J-ROY-METEOR-SOC-V116-P127
GEERNAERT GL-1987-J-GEOPHYS-RES-V92
GRANT ALM-1986-Q-J-ROY-METEOR-SOC-V112-P825
HANJALIC K-1972-J-FLUID-MECH-V52-P609
HOGSTROM U-1990-J-ATMOS-SCI-V47-P1949
HOLTSLAG AAM-1986-BOUND-LAY-METEOROL-V36-P201
HORST JW-1988-J-ATMOS-SCI-V45-P606
HUNT JCR-1988-I-MATH-ITS-APPLICATI-V15-P285
KAIMAL JC-1982-J-ATMOS-SCI-V39-P1098
LENSCOW DH-1980-J-ATMOS-SCI-V37-P465
MASON PJ-1987-Q-J-ROY-METEOR-SOC-V113-P413
NICHOLLS S-1983-J-CLIM-APPL-METEOROL-V22-P1637
NICHOLLS S-1981-Q-J-ROY-METEOR-SOC-V107-P591
NICHOLLS S-1979-Q-J-ROY-METEOR-SOC-V105-P785
NICHOLLS S-1983-RESULTS-ROYAL-SOC-JO-P291
NICHOLLS S-1982-THESIS-SOUTHAMPTON-U-P214
NIEUWSTADT FTM-1986-I-MATH-ITS-APPLICATI-V4-P149
NIEUWSTADT FTM-1984-J-ATMOS-SCI-V41-P2202
PANOFSKY HA-1984-ATMOSPHERIC-TURBULEN-P160
PANOFSKY HA-1977-BOUND-LAYER-METEOR-V11-P355
PENNELL WT-1974-J-ATMOS-SCI-V31-P1308
SHAW WJ-1985-J-ATMOS-SCI-V42-P2563
SMITH SD-1974-BOUNDARY-LAYER-METEO-V6-P235
SMITH SD-1984-J-GEOPHYS-RES-OCEANS-V89-P2029
SMITH SD-1980-J-PHYS-OCEANOGR-V10-P709
SMITH SD-1975-Q-J-ROY-METEOR-SOC-V101-P665
TENNEKES H-1972-1ST-COURS-TURB-P68
TOWNSEND AA-1976-STRUCTURE-TURBULENT-P108
WYNGAARD JC-1975-BOUNDARY-LAYER-METEO-V9-P441
WYNGAARD JC-1981-J-APPL-METEOROL-V20-P784
Times Cited: 14
Source item page count: 14
Publication Date: FEB 1
IDS No.: HE665
29-char source abbrev: J ATMOS SCI



Record 4 of 34
Author(s): ANDREN A; MOENG CH
Title: SINGLE-POINT CLOSURES IN A NEUTRALLY STRATIFIED BOUNDARY-LAYER
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1993, Vol 50, Iss 20, pp 3366-3379
No. cited references: 28
KeywordsPlus: LARGE-EDDY SIMULATIONS; TURBULENCE CLOSURE; REYNOLDS-STRESS; MODEL; TRANSPORT; PROGRESS
Abstract: Closure assumptions often employed in single-point closure models for boundary-layer applications are evaluated against a neutrally stratified planetary boundary-layer flow generated by large-eddy simulation. The contributions from slow and rapid terms to fluctuating pressure are calculated directly from simulated fields. The slow pressure terms are compared with Rotta-type return to isotropy assumptions, both for the components of the Reynolds tensor and for a passive scalar. A simple proportionality between the time scales for dissipation of turbulent kinetic energy and for return to isotropy is found to be a good approximation in the upper two-thirds of the boundary layer. In the lower one-third of the layer, however, this ratio is found to increase by a factor of 2. Closure constants depending on anisotropy are examined and their usefulness determined. Significant contributions of the rapid terms are found for all second moments except vertical velocity variance and vertical scalar flux. Two sets of often-used closure assumptions for the rapid terms are compared with the explicitly calculated data. Also, the rapid terms show that the use of constant closure coefficients are for the tested parameterizations to be viewed at best as a first approximation. Length scales for dissipation of turbulent kinetic energy and scalar variance are extracted and compared with commonly used forms.
Cited references: ANDREN A-1990-BOUND-LAY-METEOROL-V56-P207
ANDREN A-1990-J-APPL-METEOROL-V29-P224
GEERNERT GL-1987-J-GEOPHYS-RES-V12-P13127
GIBSON MM-1978-J-FLUID-MECH-V86-P491
GRANT ALM-1986-Q-J-ROY-METEOR-SOC-V112-P825
LAUNDER BE-1975-J-FLUID-MECH-V68-P537
LAUNDER BE-1975-J-FLUID-MECH-V67-P569
LEPENVEN L-1985-FRONTEIRS-FLUID-MECH-P1
LUMLEY JL-1978-ADV-APPLIED-MECHANIC-V18-P123
MANSOUR NN-1988-J-FLUID-MECH-V194-P15
MASON PJ-1992-J-FLUID-MECH-V242-P51
MASON PJ-1987-Q-J-ROY-METEOR-SOC-V113-P413
MELLOR GL-1974-J-ATMOS-SCI-V31-P1791
MELLOR GL-1982-REV-GEOPHYS-V20-P851
MOENG CH-1989-J-ATMOS-SCI-V46-P2311
MOENG CH-1988-J-ATMOS-SCI-V45-P3573
MOENG CH-1986-J-ATMOS-SCI-V43-P2499
MOENG CH-1984-J-ATMOS-SCI-V41-P2052
PANOFSKY EW-1984-MODELS-METHODS-ENG-A
ROGALLO RS-1981-TM81315-NASA-AMES-RE
ROTTA J-1951-Z-PHYSIK-V129-P547
SAVILL AM-1987-ANNU-REV-FLUID-MECH-V19-P531
SHIH TH-1987-J-FLUID-MECH-V180-P93
WEINSTOCK J-1985-J-FLUID-MECH-V154-P429
WYNGAARD JC-1974-ADV-GEOPHYSICS-A-V18-P193
WYNGAARD JC-1982-ATMOSPHERIC-TURBULEN-P69
ZEMAN O-1981-ANNU-REV-FLUID-MECH-V13-P253
ZEMAN O-1975-J-ATMOS-SCI-V32-P1808
Times Cited: 11
Source item page count: 14
Publication Date: OCT 15
IDS No.: MC643
29-char source abbrev: J ATMOS SCI



Record 5 of 34
Author(s): SAMELSON RM
Title: SUPERCRITICAL MARINE-LAYER FLOW ALONG A SMOOTHLY VARYING COASTLINE
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1992, Vol 49, Iss 17, pp 1571-1584
No. cited references: 18
KeywordsPlus: OCEAN DYNAMICS EXPERIMENT; NORTHERN CALIFORNIA; CONTINENTAL-SHELF; BOUNDARY-LAYER; COASTAL; CURRENTS; MODEL
Abstract: A model for hydraulically supercritical atmospheric marine-layer flow along a smoothly varying coastline is formulated and solved numerically. The model is motivated by a recent comparison of CODE observations to a simple hydraulic theory, which suggested the presence of an expansion fan and a compression jump downstream of topographic features. The marine layer is modeled as a homogeneous rotating fluid layer decelerated by surface friction and forced by imposed upper-level pressure gradients. The equations are solved by a characteristic-based gridpoint scheme. The results indicate that the expansion fan is a robust feature that persists under most conditions in the present more realistic model, but is dramatically altered in structure by the presence of friction, while the jump may weaken rapidly offshore due mainly to offshore variations of the layer height upstream of the jump. The agreement between observations and model predictions is good enough to suggest that a first-order description of the dynamics has been attained in which friction dramatically alters the character of the supercritical flow features. The supercritical flow features cause variations in wind stress of 10%-50% over tens of kilometers.
Cited references: BEARDSLEY RC-1987-J-GEOPHYS-RES-OCEANS-V92-P1467
BRINK KH-1987-J-GEOPHYS-RES-OCEANS-V92-P1783
DAVIS RE-1985-J-GEOPHYS-RES-OCEANS-V90-P4756
DORMAN CE-1985-EOS-T-AGU-V66-P914
FRIEHE CA-1983-AIRCRAFT-FLIGHTS-COA
FRIEHE CA-1984-CODE31-U-CAL-IRV-SCH
FRIEHE CA-1985-CODE32-U-CAL-IRV-SCH
FRIEHE CA-1986-CODE41-U-CAL-IRV-DEP
FRIEHE CA-1984-SCRIPPS-I-OCEANOGRAP-V8420
GARVINE RW-1982-TELLUS-V34-P293
IPPEN AT-1951-T-ASCE-V116-P268
KELLY KA-1985-J-GEOPHYS-RES-OCEANS-V90-P1783
KOSRO PM-1987-J-GEOPHYS-RES-OCEANS-V92-P1637
LARGE WG-1982-J-PHYS-OCEANOGR-V12-P464
RUDNICK DL-1988-J-GEOPHYS-RES-OCEANS-V93-P14013
WHITHAM GB-1974-LINEAR-NONLINEAR-WAV
WINANT CD-1988-J-ATMOS-SCI-V45-P3588
ZEMBA J-1987-J-GEOPHYS-RES-OCEANS-V92-P1489
Times Cited: 11
Source item page count: 14
Publication Date: SEP 1
IDS No.: JK166
29-char source abbrev: J ATMOS SCI



Record 6 of 34
Author(s): NAPPO CJ; CHIMONAS G
Title: WAVE EXCHANGE BETWEEN THE GROUND SURFACE AND A BOUNDARY-LAYER CRITICAL-LEVEL
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1992, Vol 49, Iss 13, pp 1075-1091
No. cited references: 54
KeywordsPlus: PAST 3-DIMENSIONAL OBSTACLES; AMPLITUDE MOUNTAIN WAVES; GENERATED LEE VORTICES; GRAVITY-WAVES; DOWNSLOPE WINDSTORMS; FLOW; TURBULENCE; STABILITY; EVOLUTION; MODEL
Abstract: Gravity waves induced by two- and three-dimensional terrain features are examined theoretically in the planetary boundary layer (PBL) using a linear wave model that includes reabsorption at a critical level. The PBL structure is characterized by a constant Brunt-Vaisala frequency and a hyperbolic tangent wind speed profile, which can be adjusted to produce critical levels. It is found that for typical values of wind speed and thermal stratification in the stable PBL and for even mild terrain disturbances, the Reynolds stress and surface drag caused by surface-generated waves can be at least as those conventionally associated with surface friction. The wave drag will act on the PBL flow where wave dissipation occurs, for example, at a critical level or in regions of wave breaking. The drag over a given crosswind section of a two-dimensional ridge is about twice as great as that over a three-dimensional hill of approximately the same horizontal area. An entirely new result is the prediction that over a three-dimensional hill the wave stresses may generate a horizontal layer of counterrotating vortices immediately below a critical level.
Cited references: BACHMEISTER JT-1988-J-ATMOS-SCI-V45-P63
BEAN BR-1973-BOUND-LAY-METEOROL-V4-P449
BLUMEN W-1965-J-ATMOS-SCI-V22-P529
BLUMEN W-1976-TELLUS-V28-P287
BOOKER JR-1967-J-FLUID-MECH-V27-P513
BRETHERTON FP-1969-QUART-J-ROY-METEOROL-V95-P213
BROST RA-1978-J-ATMOS-SCI-V35-P1427
BUSINGER JA-1971-J-ATMOS-SCI-V28-P181
CHIMONAS G-1989-BOUND-LAY-METEOROL-V47-P217
CHIMONAS G-1987-J-ATMOS-SCI-V44-P533
CHIMONAS G-1986-J-GEOPHYS-RES-ATMOS-V91-P1219
CLARK TL-1977-J-ATMOS-SCI-V34-P1715
CLARKE RH-1971-CSIRO19-DIV-MET-PHYS
CLEMENTS WE-1989-J-APPL-METEOROL-V28-P457
COULTER RL-1990-BOUND-LAY-METEOROL-V52-P75
CRAIK ADD-1985-WAVE-INTERACTIONS-TU
DELAGE Y-1974-Q-J-ROY-METEOR-SOC-V100-P351
DURRAN DR-1986-J-ATMOS-SCI-V43-P2527
DURST CS-1933-Q-J-ROY-METEOR-SOC-V54-P131
EINAUDI F-1981-Q-J-ROY-METEOR-SOC-V107-P793
ELIASSEN A-1960-GEOFYS-PUBLIKASJONER-V22-P1
FINNIGAN JJ-1988-J-ATMOS-SCI-V45-P486
GARRATT JR-1983-BOUND-LAY-METEOROL-V26-P69
GIFFORD FA-1952-B-AMS-V33-P373
GOSSARD EE-1985-J-ATMOS-SCI-V42-P2156
GOSSARD EE-1975-WAVES-ATMOSPHERE
HINES CO-1988-J-ATMOS-SCI-V45-P309
HINES CO-1970-J-GEOPHYS-RES-V75-P5956
HOOTMAN BW-1983-MON-WEATHER-REV-V111-P1052
HUNT JCR-1980-J-FLUID-MECH-V96-P671
IZUMI Y-1973-AFCRLTR760038-AIR-FO
KONDO J-1978-J-ATMOS-SCI-V35-P1012
LALAS DP-1976-J-ATMOS-SCI-V33-P1248
LIN YL-1988-J-ATMOS-SCI-V45-P2987
LIN YL-1986-J-ATMOS-SCI-V43-P2736
LYONS R-1964-J-APPL-METEOROL-V3-P136
MAHRT L-1979-BOUND-LAY-METEOROL-V17-P247
MAHRT L-1985-J-ATMOS-SCI-V42-P2333
MILES JW-1961-J-FLUID-MECH-V10-P496
NAPPO CJ-1990-BOUND-LAY-METEOROL-V54-P69
NAPPO CJ-1989-THESIS-GEORGIA-I-TEC
NEFF WD-1986-ATMOS-RES-V20-P279
NIEUWSTADT FTM-1984-BOUND-LAY-METEOROL-V30-P31
PELTIER WR-1979-J-ATMOS-SCI-V36-P1498
RAO KS-1979-BOUND-LAY-METEOROL-V17-P15
ROTTMAN JW-1989-TELLUS-A-V41-P401
SAWYER JS-1959-QUARTERLY-J-ROYAL-ME-V85-P31
SIMARD A-1982-J-ATMOS-SCI-V39-P587
SMITH RB-1979-ADV-GEOPHYSICS-V21-P87
SMITH RB-1989-J-ATMOS-SCI-V46-P3611
SMITH RB-1980-TELLUS-V32-P348
SMOLARKIEWICZ PK-1989-J-ATMOS-SCI-V46-P1154
WYNGAARD JC-1975-BOUNDARY-LAYER-METEO-V9-P441
YAMAMOTO S-1979-J-METEOR-SOC-JAPAN-V57-P423
Times Cited: 11
Source item page count: 17
Publication Date: JUL 1
IDS No.: JC634
29-char source abbrev: J ATMOS SCI



Record 7 of 34
Author(s): CANUTO VM; MINOTTI F; RONCHI C; YPMA RM; ZEMAN O
Title: 2ND-ORDER CLOSURE PBL MODEL WITH NEW 3RD-ORDER MOMENTS - COMPARISON WITH LES DATA
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1994, Vol 51, Iss 12, pp 1605-1618
No. cited references: 32
KeywordsPlus: PLANETARY BOUNDARY-LAYER; REYNOLDS STRESS MODEL; LABORATORY MODEL; TURBULENCE; EVOLUTION; FLOWS
Abstract: This paper contains two parts. In the first part, a new set of diagnostic equations is derived for the third-order moments for a buoyancy-driven flow, by exact inversion of the prognostic equations for the third-order moment equations in the stationary case. The third-order moments exhibit a universal structure: they all are a linear combination of the derivatives of all the second-order moments, w2BAR, wthetaBAR, theta2BAR, and q2BAR. Each term of the sum contains a turbulent diffusivity D(t), which also exhibits a universal structure of the form D(t) = anu(t) + bwthetaBAR. Since the sign of the convective flux changes depending on stable or unstable stratification, D(t) varies according to die type of stratification. Here nu(t) approximately wl (l is a mixing length and w is an rms velocity) represents the ''mechanical'' part, while the ''buoyancy'' part is represented by the convective flux wthetaBAR. The quantities a and b are functions of the variable (Ntau)2, where N2 = galpha partial derivative THETA/partial derivative z and tau is the turbulence time scale. The new expressions for the third-order moments generalize those of Zeman and Lumley, which were subsequently adopted by Sun and Ogura, Chen and Cotton, and Finger and Schmidt in their treatments of the convective boundary layer. In the second part, the new expressions for the third-order moments are used to solve the ensemble average equations describing a purely convective boundary layer heated from below at a constant rate. The computed second- and third-order moments are then compared with the corresponding LES results, most of which are obtained by running a new LES code, and part of which are taken from published results. The ensemble average results compare favorably with the LES data.
Cited references: ANDRE JC-1978-J-ATMOS-SCI-V35-P1861
ANDRE JC-1976-J-ATMOS-SCI-V33-P482
ANDRE JC-1982-TURBULENT-SHEAR-FLOW-V3-P243
BOUGEAULT P-1986-J-ATMOS-SCI-V43-P1574
BOUGEAULT P-1981-J-ATMOS-SCI-V38-P2429
CANUTO VM-1992-ASTROPHYS-J-V392-P218
CANUTO VM-1993-J-ATMOS-SCI-V50-P1925
CHEN C-1983-BOUND-LAY-METEOROL-V32-P205
CLARKE RH-1971-CSIRO19-DIV-MET-PHYS
DEARDORFF JW-1985-BOUND-LAY-METEOROL-V32-P205
DURBIN PA-1993-J-FLUID-MECH-V249-P465
FINGER JE-1986-BEITR-PHYS-ATMOS-V59-P205
HANJALIC K-1976-J-FLUID-MECH-V74-P593
HANJALIC K-1972-J-FLUID-MECH-V52-P609
HOLT SE-1992-J-FLUID-MECH-V237-P499
LUMLEY JL-1978-ADV-APPLIED-MECHANIC-V18-P123
LUMLEY JL-1978-J-FLUID-MECH-V84-P581
MOENG CH-1989-J-ATMOS-SCI-V46-P2311
MOENG CH-1986-J-ATMOS-SCI-V43-P2499
NIEUWSTADT FTM-1986-J-ATMOS-SCI-V43-P532
NIEUWSTADT FTM-1993-TURBULENT-SHEAR-FLOS-V8
SHIH TH-1985-FDA853-CORN-U
SHIH TS-1992-STUDIES-TURBULENCE-P91
SPEZIALE CG-1991-ANNU-REV-FLUID-MECH-V23-P107
SUN WY-1980-J-ATMOS-SCI-V37-P1558
WEINSTOCK J-1987-J-FLUID-MECH-V202-P319
WILLIS GE-1974-J-ATMOS-SCI-V31-P1297
WYNGAARD JC-1974-BOUNDARY-LAYER-METEO-V7-P289
ZEMAN O-1977-J-ATMOS-SCI-V34-P111
ZEMAN O-1976-J-ATMOS-SCI-V33-P1974
ZEMAN O-1975-THESIS-PENNSYLVANIA
ZEMAN O-1979-TURBULENT-SHEAR-FLOW-V1
Times Cited: 10
Source item page count: 14
Publication Date: JUN 15
IDS No.: NQ998
29-char source abbrev: J ATMOS SCI



Record 8 of 34
Author(s): Sun JL; Howell JF; Esbensen SK; Mahrt L; Greb CM; Grossman R; LeMone MA
Title: Scale dependence of air-sea fluxes over the Western Equatorial Pacific
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1996, Vol 53, Iss 21, pp 2997-3012
No. cited references: 30
KeywordsPlus: CONVECTIVE BOUNDARY-LAYER; SQUALL-LINE; TURBULENCE; HEAT; MESOSCALE; ENERGY
Abstract: The goal of this study is to examine the horizontal scale dependence of vertical eddy flux in the tropical marine surface boundary layer and how this scare dependence of flux relates to the bulk aerodynamic relationship and the parameterization of subgrid-scale flux. The fluxes of heat, moisture, and momentum are computed from data collected from 27 NCAR Electra flight legs in TOGA COARE (The Tropical Ocean Global Atmosphere Coupled Ocean-Atmosphere Response Experiment) with flight elevations lower than 40 m and flight runs longer than 60 km. The dependence of the fluxes on two length scales are studied: the cutoff length scale, defining the averaging length over which mean components are obtained in order to partition field variables into mean and perturbation components; and the dux averaging length scare, defining the length over which products of perturbations are averaged in order to estimate vertical fluxes. Based on the characteristics of the scale dependence of fluxes, the total flux of each flight leg is partitioned into ''turbulent,'' ''large eddy,'' and ''mesoscale'' fluxes due to motions smaller than 1 km, between 1 and 5 km, and between 5 km and the flight leg length, respectively. The results show that fluxes are sensitive to the choice of cutoff length scale in the presence of significant mesoscale activity and in the weak wind case where the turbulent fluxes are small. The turbulent momentum Aux decreases with increasing flux averaging length scale due to mesoscale modulation of the turbulent stress vector. Mesoscale heat, moisture, and momentum fluxes for individual flight legs can reach 20% of the turbulent fluxes in the presence of well-organized convective cloud systems even at 35 m above the sea surface. The mesoscale flux is less correlated to the wind speed and bulk air-sea difference than turbulent fluxes. The local mesoscale flux can be upward or downward, and therefore, its average Value is reduced when averaging over a single flight leg and reduced further when compositing over all of the legs. The mesoscale momentum flux is less systematic than the turbulent stress and is more sensitive to the flux averaging scale than the turbulent stress. Sampling and instrumentation problems are briefly discussed particularly with respect to mesoscale motions.
Cited references: *TCIPO-1992-TOGA-COARE-OP-PLAN
BALAJI V-1993-J-ATMOS-SCI-V50-P3571
BALJAARS AC-1991-J-APPL-METEOROL-V30-P327
BARNES G-1980-MON-WEATHER-REV-V108-P349
BETTS AK-1990-BOUND-LAY-METEOROL-V50-P109
CHOU SH-1991-BOUND-LAY-METEOROL-V55-P255
DONELAN M-1973-J-ATMOS-SCI-V30-P444
EMANUEL KA-1983-MESOSCALE-METEOROLOG-P1
ESBENSEN SK-1996-J-CLIMATE-V9-P2307
FRIEHE CA-1991-J-GEOPHYS-RES-OCEANS-V96-P8593
GEERNAERT GL-1987-J-GEOPHYS-RES-OCEANS-V92-P13127
GROSSMAN RL-1973-THESIS-COLORADO-STAT
HAUF T-1989-Q-J-ROY-METEOR-SOC-V115-P309
HOGSTROM U-1990-J-ATMOS-SCI-V47-P1949
HOJSTRUP J-1993-MEAS-SCI-TECHNOL-V4-P153
HOWELL JF-1994-J-ATMOS-SCI-V51-P2165
JOHNSON RH-1983-MON-WEATHER-REV-V111-P308
KHALSA SJS-1977-BOUNDARY-LAYER-METEO-V12-P273
LEMONE MA-1976-J-ATMOS-SCI-V33-P1308
LENSCHOW DH-1986-J-ATMOS-SCI-V43-P1198
MAHRT L-1992-BOUND-LAY-METEOROL-V60-P143
MAHRT L-1996-J-GEOPHYS-RES-OCEANS-V101-P14327
MAHRT L-1991-Q-J-ROY-METEOR-SOC-V117-P151
MOURAD PD-1990-J-ATMOS-SCI-V47-P414
SUN JL-1994-J-APPL-METEOROL-V33-P1341
TOWNSEND AA-1976-STRUCTURE-TURBULENT
WILLIAMS AG-1993-BOUND-LAY-METEOROL-V64-P55
WILLIAMS AG-1996-J-ATMOS-SCI-V53-P1187
YOUNG GS-1992-J-GEOPHYS-RES-OCEANS-V97-P9595
ZIPSER EJ-1977-MON-WEATHER-REV-V105-P1568
Times Cited: 7
Source item page count: 16
Publication Date: NOV 1
IDS No.: VT966
29-char source abbrev: J ATMOS SCI



Record 9 of 34
Author(s): SMITH RB; SMITH DF
Title: PSEUDOINVISCID WAKE FORMATION BY MOUNTAINS IN SHALLOW-WATER FLOW WITH A DRIFTING VORTEX
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1995, Vol 52, Iss 4, pp 436-454
No. cited references: 30
KeywordsPlus: PAST 3-DIMENSIONAL OBSTACLES; GENERATED LEE VORTICES; ISOLATED TOPOGRAPHY; DOWNSLOPE WINDS; DYNAMICS; MOTION
Abstract: Numerical solutions to the shallow-water equations are used to examine the generation of wake vorticity as a cyclone drifts past a mountain. In cases with sufficient vortex strength, mountain height, and vortex-mountain proximity, the flow becomes supercritical over the mountain and hydraulic jumps generate wake vorticity. The dissipative vorticity transport in jumps modifies the usual vorticity integral constraints for inviscid shallow-water flow regarding potential enstrophy, vorticity centroid, and vortex size. The increase in vortex size during wake formation represents a weakening of the vortex. These changes, and the macroscopic flow patterns, are independent of the viscosity coefficient. The generation of vertical vorticity within a viscous jump, and the associated Bernoulli loss, arise from a shear stress induced at the sloping upper interface of the layer and transmitted down through the layer by a secondary flow. Applied to the problem of a typhoon drifting past Taiwan, the shallow-water equations capture many of the observed phenomena such as upstream blocking, downstream sheltering, corner winds, and foehn and secondary vortex formation.
Cited references: ABRAMOPOULOS F-1987-MON-WEA-REV-V116-P650
ARAKAWA A-1980-MON-WEA-REV-V109-P18
AREF H-1983-ANNU-REV-FLUID-MECH-V15-P345
BACMEISTER JT-1988-J-ATMOS-SCI-V45-P63
BATCHELOR GK-1967-INTRO-FLUID-DYNAMICS
CARSLAW HS-1959-CONDUCTION-HEAT-SOLI
CHANG SWJ-1982-MON-WEATHER-REV-V110-P1255
CHESTER W-1966-J-FLUID-MECH-V24-P367
CHOPRA KP-1973-ADV-GEOPHYSICS-V16-P297
CLARK TL-1984-J-ATMOS-SCI-V41-P3122
CRANK J-1975-MATH-DIFFUSION
DURRAN DR-1987-J-ATMOS-SCI-V44-P3402
ETLING D-1989-METEOROL-ATMOS-PHYS-V41-P157
GENT PR-1993-J-ATMOS-SCI-V50-P1323
GRUBISIC V-1995-IN-PRESS-J-ATMOS-SCI
GUSTAFSSON B-1978-SIAM-J-APPL-MATH-V35-P343
HAYES WD-1957-J-FLUID-MECH-V2-P595
POLVANI LM-1992-J-ATMOS-SCI-V49-P462
SADOURNY R-1974-J-ATMOS-SCI-V32-P680
SCHAR C-1993-J-ATMOS-SCI-V50-P1373
SCHAR C-1993-J-ATMOS-SCI-V50-P1401
SCHAR C-1993-J-ATMOS-SCI-V50-P1437
SMITH RB-1989-ADV-GEOPHYS-V31-P1
SMITH RB-1975-GEOL-SOC-AM-BULL-V86-P1601
SMITH RB-1989-J-ATMOS-SCI-V46-P3611
SMITH RB-1985-J-ATMOS-SCI-V42-P2597
SMITH RB-1993-TELLUS-A-V45A-P28
SMOLARKIEWICZ PK-1989-J-ATMOS-SCI-V46-P1154
WANG ST-1989-7758-NAT-SCI-COUNC-T
ZEHNDER JA-1993-J-ATMOS-SCI-V50-P2519
Times Cited: 7
Source item page count: 19
Publication Date: FEB 15
IDS No.: QK453
29-char source abbrev: J ATMOS SCI



Record 10 of 34
Author(s): ROGERSON AM; SAMELSON RM
Title: SYNOPTIC FORCING OF COASTAL-TRAPPED DISTURBANCES IN THE MARINE ATMOSPHERIC BOUNDARY-LAYER
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1995, Vol 52, Iss 11, pp 2025-2040
No. cited references: 16
KeywordsPlus: OCEAN DYNAMICS EXPERIMENT; NORTH-AMERICA; KELVIN WAVES; WEST-COAST; GENERATION
Abstract: Motivated by recent observations along the west coast of the United States, the authors investigate the generation and propagation of coastal-trapped disturbances in the marine atmospheric boundary layer. Analytic solutions are obtained in a linear, shallow water, reduced-gravity model of the flow subject to forcing by upper-level pressure disturbances and dissipation in the form of wind stress at the sea surface. It is found that unless the mean alongshore flow is to the south with speeds larger than the gravity wave phase speed, a northward propagating coastal-trapped response develops. The superposition of cross-shore propagating forcing and the northward propagating response in marine-layer thickness can give rise to surface pressure ridges at the coast with both narrow and broad cross-shore extent. Wind reversals associated with the disturbance lead the change in surface pressure at the coast. The magnitude of the response increases for weaker inversion strength, greater undisturbed marine-layer depth, and, to some extent, with weaker dissipation. For periodic forcing, the near-resonant response propagates steadily up the coast with the inviscid free Kelvin wave phase speed and has a cross-shore length scale equal to the Rossby deformation radius, while the off-resonant response possesses cross-shore length scales that differ from the Rossby radius, and propagates unsteadily up the coast with an average speed determined by forcing parameters. It is also found that the alongshore length scale of the disturbance depends on the propagation speed of the forcing, and may appear more mesoscale-like for fast-moving pressure systems. The results illustrate that unsteady propagation of the coastal-trapped disturbance can result from the linear response to synoptic forcing.
Cited references: BANNON PR-1981-Q-J-ROY-METEOR-SOC-V107-P313
BEARDSLEY RC-1987-J-GEOPHYS-RES-OCEANS-V92-P1467
DORMAN CE-1987-J-GEOPHYS-RES-OCEANS-V92-P1497
DORMAN CE-1988-MON-WEATHER-REV-V116-P2401
DORMAN CE-1985-MON-WEATHER-REV-V113-P827
GILL AE-1977-Q-J-ROY-METEOR-SOC-V103-P431
HALLIWELL GR-1987-J-GEOPHYS-RES-OCEANS-V92-P1861
HERMANN AJ-1990-J-GEOPHYS-RES-OCEANS-V95-P13169
HOLLAND GJ-1986-Q-J-ROY-METEOR-SOC-V112-P731
LARGE WG-1981-J-PHYS-OCEANOGR-V11-P324
MASS CF-1988-MON-WEATHER-REV-V116-P2407
MASS CF-1987-MON-WEATHER-REV-V115-P1707
NGUYEN NA-1981-Q-J-R-METEOROL-SOC-V107-P521
REASON CJC-1992-J-ATMOS-SCI-V49-P1677
REASON CJC-1990-Q-J-ROY-METEOR-SOC-V116-P1133
SEND U-1987-J-GEOPHYS-RES-OCEANS-V92-P1683
Times Cited: 5
Source item page count: 16
Publication Date: JUN 1
IDS No.: RC286
29-char source abbrev: J ATMOS SCI



Record 11 of 34
Author(s): EMANUEL KA
Title: ON THERMALLY DIRECT CIRCULATIONS IN MOIST ATMOSPHERES
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1995, Vol 52, Iss 9, pp 1529-1534
No. cited references: 11
KeywordsPlus: STATE
Abstract: An expression is derived for the critical horizontal gradient of subcloud-layer theta(e) in radiative-convective equilibrium, sufficient for the onset of thermally direct, zonally symmetric circulations. This corresponds to zero absolute vorticity at the tropopause. The expression is then generalized to nonsymmetric flows under the approximation that the corresponding radiative-convective equilibrium state is in geostrophic balance. Scale analysis shows that actual moist entropy distributions cannot be far from critical in large-scale Hadley, Walker, and monsoon circulations. The balanced component of the surface winds can be calculated from the supercriticality of the surface theta(e) distribution, and the secondary circulation can then be estimated from the surface stress.
Cited references: BETTS AK-1982-J-ATMOS-SCI-V39-P1484
EMANUEL KA-1986-J-ATMOS-SCI-V43-P585
EMANUEL KA-1994-Q-J-ROY-METEOR-SOC-V120-P1111
HELD IM-1980-J-ATMOS-SCI-V37-P515
HIDE R-1969-J-ATMOS-SCI-V26-P841
LINDZEN RS-1988-J-ATMOS-SCI-V45-P2416
LINDZEN RS-1987-J-ATMOS-SCI-V44-P2440
PLUMB RA-1992-J-ATMOS-SCI-V49-P1790
SCHNEIDER EK-1977-J-ATMOS-SCI-V34-P280
SCHNEIDER EK-1975-THESIS-HARVARD-U
XU KM-1989-MON-WEATHER-REV-V117-P1471
Times Cited: 5
Source item page count: 6
Publication Date: MAY 1
IDS No.: QW508
29-char source abbrev: J ATMOS SCI



Record 12 of 34
Author(s): KIM JW; MAHRT L
Title: MOMENTUM TRANSPORT BY GRAVITY-WAVES
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1992, Vol 49, Iss 9, pp 735-748
No. cited references: 34
KeywordsPlus: HYDROSTATIC MOUNTAIN WAVES; AIRCRAFT MEASUREMENTS; GENERAL-CIRCULATION; AIR-FLOW; DRAG; SATURATION; MESOSPHERE; SIMULATION; TURBULENCE; FLUX
Abstract: The momentum flux by orographic gravity waves and the turbulent heat flux in wave-breaking regions are estimated from aircraft data from ALPEX. The fluxes on 6 March 1982 are controlled by low-level directional shear of the mean flow and associated critical level with wave stress decreasing toward the critical level. On 25 March 1982 a critical level does not occur and wave stress is approximately constant with height within the observational domain. The calculation of these fluxes appears to be the first direct comparison between simple models of gravity-wave momentum flux and observed atmospheric fluxes. To develop a simple formulation of gravity wave drag for large-scale models, the gravity-wave stress supersaturation theory by Lindzen is generalized for the application to vertically varying mean flows. The wave momentum flux estimated from the generalized model agrees well with the observations for the two ALPEX days. For the 6 March case, the vertical divergence of wave momentum flux below the critical level is comparable to the Coriolis term in the momentum equation. The effective height of the surface topography required for the formulation of the wave momentum flux at the ground surface is estimated from the data and found to agree with the formulation of Stern and Pierrehumbert. Wave breaking below the critical level leads to a convectively unstable region 10-20 km wide where well-organized turbulent-scale convection occurs. The magnitude of the observed upward turbulent heat flux can be approximated by using the flux gradient relationship in which the mixing length and modified shear are derived from the generalized wave-stress supersaturation condition. However, the net turbulent heat flux across the entire width of the mountain waves appears to be small due to cancellation between the upward heat flux in the convectively unstable region and the downward heat flux at the back of the wave. The spatially averaged wave-scale heat flux is also small for the data analyzed here.
Cited references: BLUMEN W-1976-TELLUS-V28-P287
BROWN PRA-1983-Q-J-ROY-METEOR-SOC-V109-P849
CHAO WC-1984-J-ATMOS-SCI-V41-P1893
DELISI DP-1975-J-FLUID-MECH-V69-P445
DRAZIN PG-1961-TELLUS-V13-P239
DUNKERTON TJ-1989-PURE-APPL-GEOPHYS-V130-P373
ELIASSEN A-1960-GEOFYS-PUBLIKASJONER-V22-P1
GAMAGE N-1990-THESIS-OREGON-STATE
HOINKA KP-1985-Q-J-ROY-METEOR-SOC-V111-P199
HOLTON JR-1982-J-ATMOS-SCI-V39-P791
HUNT BG-1990-J-METEOROL-SOC-JPN-V68-P145
JASPERSON WH-1990-J-ATMOS-SCI-V47-P979
KLEMP JB-1978-J-ATMOS-SCI-V35-P78
LENSCHOW DH-1986-J-ATMOS-SCI-V43-P1198
LILLY DK-1979-J-FLUID-MECH-V95-P241
LILLY DK-1982-Q-J-ROY-METEOR-SOC-V108-P625
LINDZEN RS-1988-J-ATMOS-SCI-V45-P705
LINDZEN RS-1981-J-GEOPHYS-RES-OC-ATM-V86-P9707
LONG RR-1953-TELLUS-V5-P42
LUMLEY JL-1964-STRUCTURE-ATMOSPHERI
MAHRT L-1991-J-ATMOS-SCI-V48-P472
MAHRT L-1987-J-ATMOS-SCI-V44-P1106
MCFARLANE NA-1987-J-ATMOS-SCI-V44-P1775
NAPPO CJ-1991-J-ATOMS-SCI
PALMER TN-1986-Q-J-ROY-METEOR-SOC-V112-P1001
PELTIER WR-1979-J-ATMOS-SCI-V36-P1498
PIEREHUMBERT RT-1986-J-ATOMS-SCI-V42-P977
PITTS RO-1990-Q-J-ROY-METEOR-SOC-V116-P363
SMITH RB-1987-J-ATMOS-SCI-V44-P269
SMITH RB-1977-J-ATMOS-SCI-V34-P1634
SMOLARKIEWICZ PK-1989-J-ATMOS-SCI-V46-P1154
STERN WF-1988-8TH-C-NUM-WEATH-PRED-P745
THORPE SA-1973-BOUNDARY-LAYER-METEO-V5-P95
WYNGAARD J-1972-WORKSHOP-MICROMETEOR
Times Cited: 5
Source item page count: 14
Publication Date: MAY 1
IDS No.: HR508
29-char source abbrev: J ATMOS SCI



Record 13 of 34
Author(s): Oncley SP; Friehe CA; Larue JC; Businger JA; Itsweire EC; Chang SS
Title: Surface-layer fluxes, profiles, and turbulence measurements over uniform terrain under near-neutral conditions
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1996, Vol 53, Iss 7, pp 1029-1044
No. cited references: 50
KeywordsPlus: VONKARMAN CONSTANT; KINETIC-ENERGY; 1976 ITCE; FLOW; STRESS; FIELD; HEAT
Abstract: An atmospheric surface-layer experiment over a nearly uniform plowed held was performed to determine the constants in the flux-profile similarity formulas, particularly the von Kaman constant. New instruments were constructed to minimize flow distortion effects on the turbulence measurements and to provide high-resolution gradient measurements. In addition, a hot-wire anemometer directly measured the turbulent kinetic energy dissipation rate. An average value of the von Karman constant of 0.365 +/- 0.015 was obtained from 91 runs (31 h) in near-neutral stability conditions. However, four near-neutral runs when snow covered the ground gave an average value of 0.42. This result suggests that the von Karman constant depends on the roughness Reynolds number, which may resolve some of the differences in previous determinations over different surfaces. The one-dimensional Kolmogorov inertial subrange constant was found to have a value of 0.54 +/- 0.03, slightly larger than previous results. The flux-profile relations for momentum and temperature variance were evaluated, and humidity variance data behaved similarly to temperature. Dissipation of turbulent kinetic energy was found to be less than production under near-neutral conditions, which suggests that turbulent or pressure transport may be significant.
Cited references: BUSCH NE-1973-WORKSHOP-MICROMETEOR-P1
BUSINGER JA-1988-BOUND-LAY-METEOROL-V42-P145
BUSINGER JA-1971-J-ATMOS-SCI-V28-P181
CHAMPAGNE FH-1977-J-ATMOS-SCI-V34-P515
CHAMPAGNE FH-1978-J-FLUID-MECH-V86-P67
CHENEY NR-1990-J-ATMOS-OCEAN-TECH-V7-P504
DESJARDINS RL-1989-BOUND-LAY-METEOROL-V47-P55
DYER AJ-1982-BOUND-LAY-METEOROL-V22-P3
DYER AJ-1982-BOUND-LAY-METEOROL-V22-P137
FRANCEY RJ-1981-J-APPL-METEOROL-V20-P603
FRENZEN P-1992-10TH-S-TURB-DIFF-POR-P157
FRENZEN P-1992-BOUND-LAY-METEOROL-V60-P49
FRIEHE CA-1988-S-LOW-TROP-PROF-NEED-P235
FRITSCHEN LJ-1989-J-APPL-METEOROL-V28-P680
GARRATT JR-1980-Q-J-ROY-METEOR-SOC-V106-P803
HAUGEN DA-1971-Q-J-R-METEO-V97-P168
HESKESTAD G-1965-J-APPL-MECH-V87-P735
HOGSTROM U-1992-10TH-S-TURB-DIFF-POR-P188
HOGSTROM U-1988-BOUND-LAY-METEOROL-V42-P55
HOGSTROM U-1990-J-ATMOS-SCI-V47-P1949
HOGSTROM U-1986-J-ATMOS-SCI-V43-P2130
HOGSTROM U-1985-J-ATMOS-SCI-V42-P263
HOPKINS KC-1989-NATO-ASI-SER-P55
IZUMI Y-1971-AFCRL720041-USAF-AIR
KAIMAL JC-1968-J-APPL-METEOROL-V7-P827
KAIMAL JC-1972-Q-J-R-METEO-V98-P563
KONDO J-1982-J-METEOROL-SOC-JPN-V60-P461
LENSCHOW DH-1978-4-S-MET-OBS-INSTR-DE-P463
LENSCHOW DH-1994-J-ATMOS-OCEAN-TECH-V11-P661
LO AK-1978-J-APPL-METEOROL-V17-P1704
LUMLEY JL-1965-PHYS-FLUIDS-V8-P1056
LUMLEY JL-1964-STRUCTURE-ATMOSPHERI
MACCREADY PB-1964-J-APPL-MET-V3-P182
MCBEAN GA-1979-WMO350
OBUKHOV AM-1971-BOUNDARY-LAYER-METEO-V2-P7
ONCLEY SP-1989-THESIS-U-CALIFORNIA
PLATE EJ-1971-AERODYNAMIC-CHARACTE
ROSE WG-1962-J-APPL-MECH-V1-P554
SCHOLS JLJ-1986-BOUND-LAY-METEOROL-V34-P1
TELFORD JW-1986-J-ATMOS-SCI-V43-P2127
TENNEKES-1968-AIAA-J-V6-P1735
TSUKAMOTO O-1986-J-ATMOS-OCEAN-TECH-V3-P453
WIERINGA J-1980-BOUND-LAY-METEOROL-V18-P411
WILLIAMS RM-1974-THESIS-OREGON-STATE
WYNGAARD JC-1981-J-APPL-METEOROL-V20-P784
WYNGAARD JC-1971-J-ATMOS-SCI-V28-P190
WYNGAARD JC-1973-WORKSHOP-MICROMETEOR-P135
YAGLOM AM-1977-BOUNDARY-LAYER-MET-V11-P89
ZHANG SF-1986-J-ATMOS-OCEAN-TECHNO-V3-P315
ZHANG SF-1988-THESIS-U-WASHINGTON
Times Cited: 4
Source item page count: 16
Publication Date: APR 1
IDS No.: UD085
29-char source abbrev: J ATMOS SCI



Record 14 of 34
Author(s): GRUBISIC V; SMITH RB; SCHAR C
Title: THE EFFECT OF BOTTOM FRICTION ON SHALLOW-WATER FLOW PAST AN ISOLATED OBSTACLE
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1995, Vol 52, Iss 11, pp 1985-2005
No. cited references: 39
KeywordsPlus: FROUDE-NUMBER FLOW; SPATIALLY DEVELOPING FLOWS; GENERATED LEE VORTICES; 3-DIMENSIONAL OBSTACLES; POTENTIAL VORTICITY; ISOLATED TOPOGRAPHY; STRATIFIED FLOW; DENVER CYCLONE; WAKE; SIMULATION
Abstract: The effect of bottom friction on fluid flow past an isolated obstacle is investigated in the shallow-water framework. The controlling parameter for this effect is the nondimensional bottom friction number, defined as a ratio of friction to inertia. With the bottom stress related to the horizontal wind via standard bulk aerodynamic formula, the friction number is proportional to the surface roughness, the horizontal scale of the obstacle, and the inverse of the upstream fluid depth. Thus, under otherwise identical conditions, the flow past larger obstacles will be more ''viscous.'' Bottom friction modifies the vorticity generation in several ways, but under normal conditions, the wake formation remains dominated by a pseudoinviscid process related to the presence of hydraulic jumps. However, friction strongly controls the velocity-deficit region of the wake and thus influences the stability of the steady-state wakes. Predictions of the linear stability analysis are compared with numerical simulations of the eddy-shedding development under the stabilizing effect of friction. For the values of friction parameter for which linear theory predicts that the flow should be absolutely stable, fully nonlinear numerical evolutions indeed reach a stable quasi-stationary state. For a realistic value of bottom friction, the simulation of the flow past the island of Hawaii produces a wake that is consistent with the recent observations.
Cited references: BATCHELOR GK-1967-INTRO-FLUID-DYNAMICS
BLECK R-1984-RIV-METEOR-AERON-V4-P189
BRIGHTON PWM-1978-Q-J-ROY-METEOR-SOC-V104-P289
CHOMAZ JM-1991-STUD-APPL-MATH-V84-P119
CHOPRA KP-1973-ADV-GEOPHYS-V16-P298
CROOK NA-1990-J-ATMOS-SCI-V47-P2725
DAVIES HC-1983-MON-WEATHER-REV-V111-P1002
DRAZIN PG-1981-HYDRODYNAMIC-STABILI
DRAZIN PG-1962-J-FLUID-MECHANICS-V14-P257
ETLING D-1989-METEOROL-ATMOS-PHYS-V41-P157
GARRATT JR-1992-ATMOSPHERIC-BOUNDARY
GARRATT JR-1977-MON-WEATHER-REV-V105-P915
GENT PR-1993-J-ATMOS-SCI-V50-P1323
GILL AE-1982-ATMOSPHERE-OCEAN-DYN
HANNEMANN K-1989-J-FLUID-MECH-V199-P55
HAYNES PH-1987-J-ATMOS-SCI-V44-P828
HOLTON JR-1992-INTRO-DYNAMIC-METEOR
HOSKINS BJ-1989-WCRP27
HUBERT LF-1962-MON-WEA-REV-V90-P457
HUERRE P-1990-ANNU-REV-FLUID-MECH-V22-P473
HUNT JCR-1980-J-FLUID-MECH-V96-P671
PRATT LJ-1986-J-PHYS-OCEANOGR-V16-P1970
RAYLEIGH-1896-THEORY-SOUND-V2
REISNER JM-1994-J-ATMOS-SCI-V51-P117
ROTUNNO R-1995-J-ATMOS-SCI-V52-P320
SCHAR C-1993-J-ATMOS-SCI-V50-P1373
SCHAR C-1993-J-ATMOS-SCI-V50-P1401
SMITH RB-1995-J-ATMOS-SCI-V52-P436
SMITH RB-1993-J-ATMOS-SCI-V50-P3728
SMITH RB-1989-J-ATMOS-SCI-V46-P3611
SMOLARKIEWICZ PK-1989-J-ATMOS-SCI-V46-P1154
SMOLARKIEWICZ PK-1989-J-ATMOS-SCI-V46-P3614
SMOLARKIEWICZ PK-1988-J-ATMOS-SCI-V45-P1872
SMOLARKIEWICZ PK-1984-J-COMPUT-PHYS-V54-P325
SUTHERLAND BR-1992-GEOPHYS-ASTRO-FLUID-V66-P101
THORPE AJ-1993-J-ATMOS-SCI-V50-P1573
TURNER JS-1973-BUOYANCY-EFFECTS-FLU
UEYOSHI K-1991-J-METEOROL-SOC-JPN-V69-P127
WILCZAK JM-1988-MON-WEATHER-REV-V116-P2688
Times Cited: 4
Source item page count: 21
Publication Date: JUN 1
IDS No.: RC286
29-char source abbrev: J ATMOS SCI



Record 15 of 34
Author(s): MADDEN RA; SPETH P
Title: ESTIMATES OF ATMOSPHERIC ANGULAR-MOMENTUM, FRICTION, AND MOUNTAIN TORQUES DURING 1987-1988
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1995, Vol 52, Iss 21, pp 3681-3694
No. cited references: 33
KeywordsPlus: MADDEN-JULIAN OSCILLATION; INTRASEASONAL VARIATIONS; LENGTH; OCEAN
Abstract: Atmospheric angular momentum (M), friction (T-F), and mountain torques (T-M) are estimated from a 13-month period of European Centre for Medium-Range Weather Forecasts (ECMWF) data. Cross-spectrum analysis between M and total torques results in high coherence and one-quarter cycle phase angles (T-F + T-M leading M) for timescales between 5 and 66 days, suggesting that variations of the total torque are reasonably well estimated for these slower variations. However, cross spectra between M and T-F and T-M separately reveal that the relatively high coherence is present between M and T-F only at periods longer than 20 days. Also comparison with other published values and the considerable lack of balance between T-F + T-M and M over a full year implies that our estimates of T-F, based on the parameterization of surface wind stress in short-term forecasts of the ECMWF, are negatively biased. For the 13-month period, the average bias is about -15.2 Hadleys (10(18) kg m(2) s(-2)). During the period there are a few near 50-day oscillations in the M. Similar variations have been reported before and related to tropical intraseasonal oscillations of the same timescale. Two oscillations in M that are coincident with eastward-propagating cloud complexes of tropical intraseasonal oscillations are examined more closely. It is found that T-F and T-M work together to alter the M on the 50-day timescale, but that T-M's contribution is three times larger than that of T-F. During the two oscillations T-F reaches maxima when cloud complexes of tropical intraseasonal oscillations are in the vicinity of 90 degrees E. It then declines but maintains positive anomalies at least until the cloud complexes reach the Central Pacific. The M reaches its maxima shortly thereafter. T-M has sharp minima shortly before the cloud complexes are strongly developed in the Indian Ocean. Contributors to these minima are strong east to west pressure gradients primarily across the Rocky Mountains.
Cited references: ANDERSON JR-1983-J-ATMOS-SCI-V40-P1584
ARPE K-1989-ANN-METEOROL-V26-P128
BELL MJ-1991-PHILOS-T-ROY-SOC-A-V34-P55
DICKEY JO-1991-J-GEOPHYS-RES-ATMOS-V96-P22643
DUCHON CE-1979-J-APPL-METEOROL-V18-P1016
FELDSTEIN SB-1995-J-ATMOS-SCI-V52-P625
FINK A-1995-UNPUB-TEMPORAL-SPATI
GUTZLER DS-1990-J-GEOPHYS-RES-ATMOS-V95-P18679
HAN YJ-1981-26-OR-STAT-U-CLIM-RE
HENDON HH-1994-J-ATMOS-SCI-V52-P2373
HENDON HH-1994-J-GEOPHYS-RES-ATMOS-V99-P8073
KANG IS-1990-J-METEOROL-SOC-JPN-V68-P237
LAU KM-1989-J-GEOPHYS-RES-ATMOS-V94-P6319
MADDEN RA-1988-J-GEOPHYS-RES-ATMOS-V93-P5333
MADDEN RA-1987-J-GEOPHYS-RES-ATMOS-V92-P8391
MADDEN RA-1992-TRENDS-GEOPHYS-RES-C-V1-P263
MUNK WH-1960-ROTATION-EARTH
NEWTON CW-1971-J-ATMOSPHERIC-SCI-V28-P623
NEWTON CW-1972-METEOR-MONOGR-V13-P215
PONTE RM-1993-J-GEOPHYS-RES-ATMOS-V98-P7317
ROSEN RD-1983-J-GEOPHYS-RES-OC-ATM-V88-P5451
ROSEN RD-1987-MON-WEATHER-REV-V115-P2170
SALBY ML-1994-J-ATMOS-SCI-V51-P2207
SALSTEIN DA-1993-B-AM-METEOROL-SOC-V74-P67
SALSTEIN DA-1994-EOS-T-AGU-V75-P111
SALSTEIN DA-1994-SCIENCE-V264-P407
SWINBANK R-1985-Q-J-ROY-METEOR-SOC-V111-P977
TRENBERTH KE-1994-J-GEOPHYS-RES-ATMOS-V99-P23079
TRENBERTH KE-1987-J-GEOPHYS-RES-ATMOS-V92-P14815
TRENBERTH KE-1988-NCAR300STR-TECH-NOT
WEICKMANN KM-1994-J-ATMOS-SCI-V51-P3194
WEICKMANN KM-1992-MON-WEATHER-REV-V120-P2252
WOLF WL-1987-J-ATMOS-SCI-V44-P3656
Times Cited: 3
Source item page count: 14
Publication Date: NOV 1
IDS No.: TD257
29-char source abbrev: J ATMOS SCI



Record 16 of 34
Author(s): HENDON HH
Title: LENGTH OF DAY CHANGES ASSOCIATED WITH THE MADDEN-JULIAN OSCILLATION
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1995, Vol 52, Iss 13, pp 2373-2383
No. cited references: 28
KeywordsPlus: ATMOSPHERIC ANGULAR-MOMENTUM; GRIDPOINT TEMPERATURE ANOMALIES; RADIOSONDE VALIDATION; TROPICAL PACIFIC; CIRCULATION; PRECISION; PERIOD; 40-DAY; MODEL; SCALE
Abstract: The previously reported spectral peak near 50 days in time series of length of day (LOD) is shown to occur in conjunction with episodes of tropical convective activity associated with the Madden-Julian oscillation (MJO). When the convective signal of the MJO is absent, LOD exhibits a red spectrum at intraseasonal timescales. LOD is shown to be in phase with the convective anomaly due to the MJO over the date line and out of phase with the convective anomaly over the Indian Ocean. A composite angular momentum budget, made relative to the convective signal of the MJO, reveals that the zonal surface stress only partially accounts for the observed tendency of LOD. Not only is the amplitude some 50% too weak, the phase is shifted ahead of the LOD tendency by about 1/8 cycle. Hence, in older to balance the angular momentum budget, an additional mountain torque is postulated to occur. This additional torque is required to lag the frictional torque by about 1/4 of a cycle, but be of similar amplitude. The composite surface stress anomalies appear to result predominantly from zonal mean zonal wind anomalies. An important role for the zonally symmetric convective anomaly due to the MJO is suggested. The surface zonal wind anomalies at low latitudes, which exhibit a high degree of equatorial symmetry with zero amplitude on the equator, appear to be accounted for as the linear response to zonal mean convective heating in the presence of strong dissipation. The upper-tropospheric zonal wind anomalies, which mimic the angular momentum anomalies, are not accounted for by simple linear momentum balance. In particular, maximum zonal wind anomaly occurs on the equator, which suggests an important role for eddy fluxes of momentum during the life cycle of the MJO.
Cited references: ANDERSON JR-1987-J-ATMOS-SCI-V44-P2115
ANDERSON JR-1983-J-ATMOS-SCI-V40-P1584
BLACKMAN RB-1958-MEASUREMENT-POWER-SP
DICKEY JO-1991-J-GEOPHYS-RES-ATMOS-V96-P22643
EUBANKS TM-1985-J-GEOPHYS-RES-SOLID-V90-P5385
GILL AE-1980-Q-J-ROY-METEOR-SOC-V106-P447
HAYASHI Y-1987-J-METEOROL-SOC-JPN-V65-P843
HENDON HH-1994-J-ATMOS-SCI-V51-P2225
ITOH H-1994-J-GEOPHYS-RES-ATMOS-V99-P12981
JENKINS GM-1968-SPECTRAL-ANAL-ITS-AP
LAMBECK K-1980-EARTHS-VARIABLE-ROTA
LANGLEY RB-1981-NATURE-V294-P730
MADDEN RA-1972-J-ATMOS-SCI-V29-P1109
MADDEN RA-1971-J-ATMOS-SCI-V28-P702
MADDEN RA-1988-J-GEOPHYS-RES-ATMOS-V93-P5333
MADDEN RA-1987-J-GEOPHYS-RES-ATMOS-V92-P8391
MADDEN RA-1992-TRENDS-GEOPHYS-RES-C-V1-P263
MAGANA V-1991-J-CLIMATE-V4-P180
MAGANA V-1993-J-GEOPHYS-RES-ATMOS-V98-P10441
PONTE RM-1990-J-GEOPHYS-RES-OCEANS-V95-P11369
RISEBY JS-1988-J-ATMOS-SCI-V45-P2026
ROSEN RD-1983-J-GEOPHYS-RES-OC-ATM-V88-P5451
SALBY ML-1994-J-ATMOS-SCI-V51-P2207
SPENCER RW-1992-J-CLIMATE-V5-P847
SPENCER RW-1992-J-CLIMATE-V5-P858
TRENBERTH KE-1989-NCAR338PLUSSTR-TECH
WEICKMANN KM-1994-J-ATMOS-SCI-V51-P3194
WEICKMANN KM-1992-MON-WEATHER-REV-V120-P2252
Times Cited: 3
Source item page count: 11
Publication Date: JUL 1
IDS No.: RG062
29-char source abbrev: J ATMOS SCI



Record 17 of 34
Author(s): ROGERS DP; JOHNSON DW; FRIEHE CA
Title: THE STABLE INTERNAL BOUNDARY-LAYER OVER A COASTAL SEA .2. GRAVITY-WAVES AND THE MOMENTUM BALANCE
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1995, Vol 52, Iss 6, pp 684-696
No. cited references: 30
KeywordsPlus: NORTHERN CALIFORNIA; FLOW; MOUNTAIN; DYNAMICS
Abstract: Observations of the mean and turbulent structure of the marine atmospheric boundary layer (MABL), obtained using the U.K. Meteorological Research Flight C-130 Hercules aircraft, are used to investigate the momentum balance over the Irish Sea when warm air is advected offshore. The marine boundary layer is made up of two layers: a strongly stable internal boundary layer (IBL), and a stable residual layer located between the top of the IBL and the base of the planetary boundary layer inversion. Measurements obtained near the upwind coast indicate that the Bow is highly ageostrophic. Downwind of the Irish coast, there is a transition toward equilibrium between the geostrophic, Coriolis, and friction components of the Bow along part of the flight track. However, another segment of the flight track indicates an imbalance between the pressure gradient and the other measured terms, which may be attributable to gravity waves affecting the adjustment process. This is more apparent in the leg perpendicular to the coast where the pressure gradient is balanced by the observed acceleration with negligible contributions from the Coriolis and friction terms. Gravity waves associated with mountain lee waves propagate along the direction of the mean wind shear in the IBL, which is directed to the right of the wind measured along the flight track perpendicular to the coast at 30-m altitude. The dominant wavelength is about 19 km, which corresponds with the buoyancy frequency of the MABL near the Irish coast and is supported by satellite images of the cloud structure. Farther downstream the buoyancy frequency increases, but the longer wavelength signal remains dominant. An important result of the gravity waves is the modification of the wind field and wind stress within the IBL. The largest effect is observed in the stress direction, but large changes in magnitude are also observed. The results indicate that the direction of the wind stress corresponds to a large degree with the direction of the mean horizontal wind shear.
Cited references: AXFORD DN-1971-Q-J-ROY-METEOROL-SOC-V97-P313
CRUETTE D-1976-TELLUS-V26-P499
DEBAAS AF-1985-BOUND-LAY-METEOROL-V31-P303
DORMAN CE-1987-J-GEOPHYS-RES-OCEANS-V92-P1497
DURRAN DR-1986-J-ATMOS-SCI-V43-P2527
ENRIQUEZ AG-1991-5TH-C-MET-OC-COAST-Z-P102
FRIEHE CA-1991-J-GEOPHYS-RES-OCEANS-V96-P8593
GEERNAERT GL-1988-J-GEOPHYS-RES-OCEANS-V93-P8215
GILL AE-1982-ATMOSPHERE-OCEAN-DYN
GOSSARD EE-1954-J-METEOR-V11-P259
HAURWITZ B-1947-ANN-NY-ACAD-SCI-V48-P727
JOHNSON WB-1966-B-AM-METEOR-SOC-V47-P982
LACKMANN GM-1989-MON-WEATHER-REV-V117-P1817
LILLY DK-1979-J-FLUID-MECH-V95-P241
LONG RR-1959-J-GEOPHYS-RES-V64-P2151
LONG RR-1953-TELLUS-V5-P42
MACKLIN SA-1988-MON-WEATHER-REV-V116-P1289
MILES JW-1968-J-FLUID-MECH-V33-P803
MILES JW-1969-J-FLUID-MECHANICS-V35-P497
MILES JW-1968-J-FLUID-MECHANICS-V32-P549
NICHOLLS S-1984-Q-J-ROY-METEOR-SOC-V110-P783
OGERS DP-1995-J-ATMOS-SCI-V52-P667
OVERLAND JE-1984-MON-WEATHER-REV-V112-P2530
REITER ER-1974-ARCH-METEOR-GEOPHY-A-V23-P101
SCORER RS-1949-QUART-J-ROY-METEOR-S-V75-P41
SMITH RB-1980-TELLUS-V32-P348
WALD L-1984-BOUND-LAY-METEOROL-V28-P309
WALTER BA-1982-MON-WEATHER-REV-V110-P1458
WINANT CD-1988-J-ATMOS-SCI-V45-P3588
ZEMBA J-1987-J-GEOPHYS-RES-OCEANS-V92-P1489
Times Cited: 3
Source item page count: 13
Publication Date: MAR 15
IDS No.: QP834
29-char source abbrev: J ATMOS SCI



Record 18 of 34
Author(s): SMEDMAN AS; TJERNSTROM M; HOGSTROM U
Title: THE NEAR-NEUTRAL MARINE ATMOSPHERIC BOUNDARY-LAYER WITH NO SURFACE SHEARING STRESS - A CASE-STUDY
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1994, Vol 51, Iss 23, pp 3399-3411
No. cited references: 25
KeywordsPlus: TURBULENCE STRUCTURE; AIR-MOTION; AIRCRAFT; PROFILES; FLUX; FLOW; JET
Abstract: Data from a marine coastal experiment over the Baltic Sea, comprising airborne measurements and mast measurements, have been used to highlight the turbulence dynamics of a case with most unusual flow characteristics. The boundary layer had a depth of about 1200 m. The thermal stratification was near neutral, with small positive heat flux below 300 m and equally small negative heat flux above. The entire situation lasted about 6 hours. Turbulence levels were unexpectedly high in view of the fact that momentum flux was negligible (in fact positive) in the layers near the surface, and buoyancy flux was also small. The turbulence was found to scale with the height of the boundary layer, giving rise to velocity spectra having the shape of those characteristic of convectively mixed boundary layers. Analysis of the turbulence budget for the entire planetary boundary layer (PBL) revealed that energy was produced from shear instability in the uppermost parts of the PBL and was distributed to the lower parts of the PBL by pressure transport. Dissipation was found to be evenly distributed throughout the entire PBL. Without data on surface wave characteristics, no firm conclusions concerning air-sea interaction processes can be drawn, but there are clear indications that the dynamical decoupling observed at the surface is due to the effect of decaying sea state conditions (high wave age conditions). In any case, the process of active turbulence production in the layers close to the surface observed in ''ordinary'' near-neutral boundary layers has been effectively turned off here, leaving only turbulence of the ''inactive'' kind, imported by pressure transport from layers above. The results strongly support the findings reported in the recent literature on ''laboratory turbulence'' that the process of strong turbulence and shearing stress production near the wall of boundary layers of very different kinds is virtually independent of forcing from large-scale structures embedded in the flow.
Cited references: BERGSTROM H-1987-DANTEC-INFORMATION-V5-P16
BROWN EN-1983-J-CLIM-APPL-METEOROL-V22-P171
CHAMBERS AJ-1981-J-PHYS-OCEANOGR-V11-P116
DYER AJ-1982-BOUND-LAY-METEOROL-V24-P181
HOGSTROM U-1992-10TH-S-TURB-DIFF-POR-P188
HOGSTROM U-1988-BOUND-LAY-METEOROL-V42-P55
HOGSTROM U-1984-BOUND-LAY-METEOROL-V33-P351
HOGSTROM U-1982-J-APPL-METEOROL-V21-P1838
HOGSTROM U-1990-J-ATMOS-SCI-V47-P1949
KAIMAL JC-1976-J-ATMOS-SCI-V33-P3152
KAIMAL JC-1972-Q-J-R-METEO-V98-P563
KLINE SJ-1989-P-ZORAN-ZARIC-MEMORI-P200
MAHRT L-1992-BOUND-LAY-METEOROL-V60-P143
MAHRT L-1993-IN-PRESS-J-FLUID-MEC
MAKOVA VI-1975-ATMOS-OCEAN-PHYS-V11-P177
RAUPACH MR-1981-J-FLUID-MECH-V108-P363
ROBINSON SK-1991-NASA103858-TECH-MEM
ROBINSON SK-1989-P-ZORAN-ZARIC-MEMORI-P218
SMEDMAN AS-1993-BOUND-LAY-METEOROL-V66-P105
SMEDMAN AS-1991-J-ATMOS-SCI-V48-P856
TJERNSTROM M-1993-J-APPL-METEOROL-V32-P948
TJERNSTROM M-1991-J-ATMOS-OCEAN-TECH-V8-P19
TJERNSTROM M-1993-J-GEOPHYS-RES-OCEANS-V98-P4809
TOWNSEND AA-1961-J-FLUID-MECH-V11-P97
VOLKOV YA-1970-ATMOS-OCEAN-PHYS-V6-P770
Times Cited: 3
Source item page count: 13
Publication Date: DEC 1
IDS No.: PW533
29-char source abbrev: J ATMOS SCI



Record 19 of 34
Author(s): MALGUZZI P
Title: AN ANALYTICAL STUDY ON THE FEEDBACK BETWEEN LARGE-SCALE AND SMALL-SCALE EDDIES
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1993, Vol 50, Iss 10, pp 1429-1436
No. cited references: 21
KeywordsPlus: LOW-FREQUENCY VARIABILITY; OBSERVATIONAL EVIDENCE; BAROCLINIC ATMOSPHERE; COHERENT STRUCTURES; WEATHER REGIMES; BLOCKING; CIRCULATION; MODEL; PROPAGATION
Abstract: The feedback between large-scale stationary Rossby waves and small-scale high-frequency eddies is computed analytically in the framework of a barotropic and frictionless model atmosphere. The Rossby wave is meant to model blocking situations characterized by high-over-low dipoles and flow splitting, while the eddies represent synoptic disturbances propagating in the deformation field of the blocking pattern. Apart from a westward contribution to the phase speed of the large-scale pattern, the eddy forcing (Reynolds stress), averaged in time, turns out to be a nonlinear function of the large-scale stream function amplitude. It is shown that the eddy forcing always determines, in the time average, a steepening of the flow split associated with the block and (possibly) multiple large-scale amplitudes. A comparison between these results and previous studies about eddy forcing of blocking situations is attempted.
Cited references: AUSTIN JF-1980-Q-J-ROY-METEOR-SOC-V106-P327
BENDER CM-1978-ADV-MATH-METHODS-SCI
BENZI R-1986-Q-J-ROY-METEOR-SOC-V112-P661
BERGGREN RB-1949-TELLUS-V1-P14
CHARNEY JG-1979-J-ATMOS-SCI-V36-P1205
GREEN JSA-1976-WEATHER-V32-P120
HANSEN AR-1990-J-ATMOS-SCI-V47-P380
HOSKINS BJ-1983-J-ATMOS-SCI-V40-P1595
ILLARI L-1984-J-ATMOS-SCI-V41-P3518
ILLARI L-1983-J-ATMOS-SCI-V40-P2232
KALLEN E-1988-Q-J-ROY-METEOR-SOC-V114-P269
MACVEAN MK-1985-J-ATMOS-SCI-V42-P1089
MALANOTTERIZZOLI -1987-J-ATMOS-SCI-V44-P2493
MALGUZZI P-1985-J-ATMOS-SCI-V42-P2463
MALGUZZI P-1984-J-ATMOS-SCI-V41-P2620
MOLTENI F-1990-Q-J-ROY-METEOR-SOC-V116-P31
MULLEN SL-1987-J-ATMOS-SCI-V44-P3
ROBINSON WA-1991-J-ATMOS-SCI-V48-P429
SHUTTS GJ-1983-Q-J-ROY-METEOR-SOC-V109-P737
VAUTARD R-1988-J-ATMOS-SCI-V45-P2811
VAUTARD R-1988-J-ATMOS-SCI-V45-P2845
Times Cited: 3
Source item page count: 8
Publication Date: MAY 15
IDS No.: LC407
29-char source abbrev: J ATMOS SCI



Record 20 of 34
Author(s): Jin FF
Title: An equatorial ocean recharge paradigm for ENSO .1. Conceptual model
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1997, Vol 54, Iss 7, pp 811-829
No. cited references: 59
KeywordsPlus: NINO-SOUTHERN-OSCILLATION; SEA-SURFACE TEMPERATURE; FAST-WAVE LIMIT; EL-NINO; TROPICAL OCEAN; ATMOSPHERE INTERACTION; SEASONAL CYCLE; PACIFIC-OCEAN; UNIFIED VIEW; INTERANNUAL OSCILLATIONS
Abstract: A new conceptual model for ENSO has been constructed based upon the positive feedback of tropical ocean-atmosphere interaction proposed by Bjerknes as the growth mechanism and the recharge-discharge of the equatorial heat content as the phase-transition mechanism suggested by Cane and Zebiak and by Wyrtki. This model combines SST dynamics and ocean adjustment dynamics into a coupled basinwide recharge oscillator that relies on the nonequilibrium between the zonal mean equatorial thermocline depth and wind stress. Over a wide range of the relative coupling coefficient, this recharge oscillator can be either self-excited or stochastically sustained. Its period is robust in the range of 3-5 years. This recharge oscillator model clearly depicts the slow physics of ENSO and also embodies the delayed oscillator (Schopf and Suarez; Battisti and Hirst) without requiring an explicit wave delay. It can also be viewed as a mixed SST-ocean dynamics oscillator due to the fact that it arises from the merging of two uncoupled modes, a decaying SST mode and a basinwide ocean adjustment mode, through the tropical ocean-atmosphere coupling. The basic characteristics of this recharge oscillator, including the relationship between the equatorial western Pacific thermocline depth and the eastern Pacific SST anomalies, are in agreement with those of ENSO variability in the observations and simulations with the Zebiak-Cane model.
Cited references: ANDERSON DLT-1985-J-ATMOS-SCI-V42-P615
BARNETT T-1988-SCIENCE-V241-P192
BARNETT TP-1991-J-CLIMATE-V4-P487
BATTISTI DS-1989-J-ATMOS-SCI-V46-P1687
BATTISTI DS-1988-J-ATMOS-SCI-V45-P2889
BJERKNES J-1969-MON-WEATHER-REV-V97-P163
CANE MA-1992-CLIMATE-SYSTEM-MODEL-P583
CANE MA-1992-J-ATMOS-SCI-V49-P1947
CANE MA-1990-J-ATMOS-SCI-V47-P1562
CANE MA-1981-J-MAR-RES-V39-P651
CANE MA-1981-J-PHYS-OCEANOGR-V11-P1578
CANE MA-1986-NATURE-V321-P827
CANE MA-1985-SCIENCE-V228-P1084
CHANG P-1995-J-ATMOS-SCI-V52-P2353
DESER C-1990-J-CLIMATE-V3-P1254
GRAHAM NE-1988-SCIENCE-V240-P1293
HAO Z-1993-J-CLIMATE-V6-P1523
HIRST AC-1988-J-ATMOS-SCI-V45-P830
HIRST AC-1986-J-ATMOS-SCI-V43-P606
IOOSS G-1990-ELEMENTARY-STABILITY
JI M-1994-TELLUS-A-V46-P398
JIN FF-1996-IN-PRESS-PHYSICA-D
JIN FF-1993-J-ATMOS-SCI-V50-P3477
JIN FF-1993-J-ATMOS-SCI-V50-P3523
JIN FF-1990-J-ATMOS-SCI-V47-P3007
JIN FF-1993-P-9-C-ATM-OC-WAV-STA-P424
JIN FF-1994-SCIENCE-V206-P70
KEPPENNE CL-1992-J-GEOPHYS-RES-ATMOS-V97-P20449
LATIF M-1994-CLIM-DYNAM-V9-P167
LAU KM-1985-J-ATMOS-SCI-V42-P1552
LAU KM-1981-J-ATMOS-SCI-V38-P248
LAU NC-1992-J-CLIMATE-V5-P284
LI B-1994-J-PHYS-OCEANOGR-V24-P681
MANTUA NJ-1994-J-PHYS-OCEANOGR-V24-P691
MCWILLIAMS JC-1978-J-ATMOS-SCI-V35-P962
MEEHL GA-1990-J-CLIMATE-V3-P72
NEELIN JD-1994-ANNU-REV-FLUID-MECH-V26-P617
NEELIN JD-1993-J-ATMOS-SCI-V50-P3504
NEELIN JD-1991-J-ATMOS-SCI-V48-P584
NEELIN JD-1995-J-CLIMATE-V8-P1325
PEDLOSKY J-1986-GEOPHYSICAL-FLUID-DY
PENLAND C-1995-J-CLIMATE-V8-P1999
PENLAND C-1994-J-CLIMATE-V7-P1352
PHILANDER SGH-1984-J-ATMOS-SCI-V41-P604
PHILANDER SGH-1992-J-CLIMATE-V5-P308
PHILANDER SGH-1990-NINI-NINA-SO-OSCILLA
RASMUSSON EM-1982-MON-WEATHER-REV-V110-P354
SCHNEIDER EK-1995-J-CLIMATE-V8-P2415
SCHOPF PS-1988-J-ATMOS-SCI-V45-P549
SUAREZ MJ-1988-J-ATMOS-SCI-V45-P3283
TZIPERMAN E-1995-J-ATMOS-SCI-V52-P293
TZIPERMAN EL-1994-SCIENCE-V263-P72
WAKATA Y-1991-J-ATMOS-SCI-V48-P2060
WANG B-1996-J-ATMOS-SCI-V53-P2786
WYRTKI K-1986-J-GEOPHYS-RES-V91-P7129
WYRTKI K-1975-J-PHYS-OCEANOGR-V5-P572
YAMAGATA T-1989-PHILOS-T-ROY-SOC-A-V329-P225
ZEBIAK SE-1989-J-PHYS-OCEANOGR-V19-P475
ZEBIAK SE-1987-MON-WEATHER-REV-V115-P2262
Times Cited: 2
Source item page count: 19
Publication Date: APR 1
IDS No.: WR417
29-char source abbrev: J ATMOS SCI



Record 21 of 34
Author(s): Smith RB; Gleason AC; Gluhosky PA; Grubisic V
Title: The wake of St. Vincent
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1997, Vol 54, Iss 5, pp 606-623
No. cited references: 49
KeywordsPlus: SHALLOW-WATER FLOW; PAST ISOLATED TOPOGRAPHY; FROUDE-NUMBER FLOW; AERIAL OBSERVATIONS; VORTEX; MOUNTAINS; ISLANDS; IMAGERY; WAVES; MODEL
Abstract: The island of St. Vincent and the other Windward Islands in the southeastern Caribbean were chosen as a field site for the study of weak mountain wakes. By the authors' definition, a ''weak wake'' forms when the potential vorticity generated by a mountain is not strong enough to advect itself into eddies; rather, it is simply advected downstream by the ambient flow. GOES-8 and Landsat sunglint images unambiguously revealed that the mountainous Windward Islands have remarkably long straight wakes. The length of St. Vincent's wake exceeds 300 km although its width is only 20 km. Near the islands, the wake structures reflect the details of the island topography. These wakes do not exhibit any obvious diurnal effect. Boat surveys in the lee of St. Vincent confirmed the existence of features seen in the images: the sharp wake boundary, the small valley-induced jet embedded in the near wake, and the absence of any reverse flow. Aircraft surveys gave evidence of descent over the island and showed that the wake air is relatively warm and dry. The length of the wake (L) agrees with the formula L = H/2C(D) (where H is the wake depth and C-D is the surface drag coefficient), implying that the reacceleration of the wake air is caused by the ambient streamwise pressure gradient rather than by lateral entrainment of momentum or geostrophic adjustment. Two numerical models were used to simulate St. Vincent's wake, a single-layer hydrostatic model and a 3D nonhydrostatic model. Both models indicated that air descent, acceleration, wave breaking, and weak potential vorticity generation occur over the island, causing a long straight wake.
Cited references: BARR S-1982-SCIENCE-V216-P1111
BLUMEN W-1972-REV-GEOPHYSICS-SPACE-V10-P485
CHOPRA KP-1973-ADV-GEOPHYS-V16-P298
CLARK TL-1977-J-ATMOS-SCI-V34-P1715
COX C-1954-J-MARINE-RES-V13-P198
COX C-1954-J-OPT-SOC-AM-V44-P838
CRAM R-1974-J-PHYS-OCEANOGR-V4-P594
CROOK NA-1990-J-ATMOS-SCI-V47-P2725
DEARDORFF JW-1976-B-AM-METEOROL-SOC-V57-P1241
DESOUZA RL-1972-THESIS-FLORIDA-STATE
ETLING D-1989-METEOROL-ATMOS-PHYS-V41-P157
FETT RW-1981-8007-NEPRF-V3
FETT RW-1979-J-APPL-METEOROL-V18-P1340
FETT RW-1976-J-PHYS-OCEANOGR-V6-P324
FETT RW-1981-MON-WEATHER-REV-V109-P1527
FLAMMARION C-1874-ATMOSPHERE
FULLER WH-1982-SCIENCE-V216-P1113
GALCHEN T-1975-J-COMPUT-PHYS-V17-P209
GARSTANG M-1975-REV-GEOPHYS-V13-P139
GRUBISIC V-1995-J-ATMOS-SCI-V52-P1985
HUBERT LF-1962-MON-WEA-REV-V90-P457
HUPPERT HE-1969-J-FLUID-MECHANICS-V35-P481
JOHNSON DB-1994-B-AM-METEOROL-SOC-V75-P5
KHATTAK S-1991-REMOTE-SENS-ENVIRON-V37-P101
LILLY DK-1962-TELLUS-V14-P148
MAUL GA-1975-REMOTE-SENSING-ENVIR-V4-P95
MCCLAIN EP-1969-MON-WEA-REV-V97-P875
MIRANDA PMA-1992-Q-J-ROY-METEOR-SOC-V118-P1057
NEEDHAM BH-1976-B-AM-METEOROL-SOC-V57-P444
SADLER JC-1987-TROPICAL-MARINE-CLIM-V1
SCHAR C-1993-J-ATMOS-SCI-V50-P1373
SCHAR C-1993-J-ATMOS-SCI-V50-P1401
SCHAR C-1993-J-ATMOS-SCI-V50-P1437
SIEBESMA AP-1995-J-ATMOS-SCI-V52-P650
SMAGORINSKY J-1963-MON-WEATHER-REV-V91-P99
SMITH RB-1989-ADV-GEOPHYS-V31-P1
SMITH RB-1995-J-ATMOS-SCI-V52-P436
SMITH RB-1993-J-ATMOS-SCI-V50-P3728
SMITH RB-1989-J-ATMOS-SCI-V46-P3611
SMITH RB-1987-J-ATMOS-SCI-V44-P269
SMITH RB-1985-J-ATMOS-SCI-V42-P2597
SMITH RB-1993-TELLUS-A-V45A-P28
SMITH RB-1989-TELLUS-A-V41-P270
SMOLARKIEWICZ PK-1994-APPL-MATH-COMPUT-SCI-V4-P527
SMOLARKIEWICZ PK-1996-IN-PRESS-ATMOS-OCEAN-V34
STEIN J-1992-MON-WEATHER-REV-V120-P2962
STRONG AE-1974-GEOPHYSICAL-RES-LETT-V1-P47
STRONG AE-1970-REMOTE-SENS-ENVIRON-V1-P181
TUNER JS-1973-BUOYANCY-EFFECTS-FLU
Times Cited: 2
Source item page count: 18
Publication Date: MAR 1
IDS No.: WM247
29-char source abbrev: J ATMOS SCI



Record 22 of 34
Author(s): Kleeman R; Moore AM
Title: A theory for the limitation of ENSO predictability due to stochastic atmospheric transients
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1997, Vol 54, Iss 6, pp 753-767
No. cited references: 34
KeywordsPlus: SURFACE TEMPERATURE ANOMALIES; OCEAN MODEL; EL-NINO; DYNAMICS; THERMODYNAMICS; INSTABILITY; FLOWS
Abstract: It is argued that a major fundamental limitation on the predictability of the El Nino-Southern Oscillation phenomenon is provided by the stochastic forcing of the tropical coupled ocean-atmosphere system by atmospheric transients. A new theoretical framework is used to analyze in detail the sensitivity of a skillful coupled forecast model to this stochastic forcing. The central concept in this analysis is the so-called stochastic optimal, which represents the spatial pattern of noise most efficient at causing variance growth within a dynamical system. A number of interesting conclusions are reached. (a) Sensitivity to forcing is greatest during the northern spring season and prior to warm events. (b) There is little sensitivity to meridional windstress noise. (c) A western Pacific dipole pattern in heat flux noise is most efficient in forcing eastern Pacific SST variance. An estimate of the actual wind stress stochastic forcing is obtained from recent ECMWF analyses and it is found that ''unavoidable'' error growth within the model due to this stochastic forcing saturates at approximately 0.5 degrees C in the NINO3 region with very rapid error growth during the first 6 months. The noise projects predominantly onto the first stochastic optimal and, in addition, around 95% of the error growth can be attributed to stochastic forcing with a strong synoptic character.
Cited references: *WGNE-1995-670-WGNE-WMOTD
BALMASEDA MA-1994-TELLUS-A-V46-P497
BATTISTI DS-1988-J-ATMOS-SCI-V45-P2889
BLUMENTHAL MB-1991-J-CLIMATE-V4-P766
CHEN D-1995-SCIENCE-V269-P1699
EGGER J-1984-PREDICTABILITY-FLUID-P149
FARRELL BF-1993-J-ATMOS-SCI-V50-P200
FARRELL BF-1993-J-ATMOS-SCI-V50-P4044
FARRELL BF-1990-J-ATMOS-SCI-V47-P2409
FARRELL BF-1993-PHYS-FLUIDS-A-FLUID-V5-P2600
FREDERIKSEN JS-1982-J-ATMOS-SCI-V39-P969
GARDINER CW-1985-HDB-STOCHASTIC-METHO
GOSWAMI BN-1991-J-CLIMATE-V4-P3
HADLEY G-1961-LINEAR-ALGEBRA
HENDON HH-1997-IN-PRESS-J-CLIMATE
JIN FF-1994-SCIENCE-V264-P70
JONES C-1996-J-CLIMATE-V9-P3086
KLEEMAN R-1988-COMPUTATIONAL-TECHNI
KLEEMAN R-1992-HYBRID-COUPLED-TROPI
KLEEMAN R-1991-J-ATMOS-SCI-V48-P3
KLEEMAN R-1993-J-CLIMATE-V6-P2012
KLEEMAN R-1995-MON-WEATHER-REV-V123-P3103
KLEEMAN R-1994-NOAA-EXPER-LONG-LEAD-V3-P10
KLEEMAN R-1994-TELLUS-A-V46-P529
LIPSCHUTZ S-1974-THEORY-PROBLEMS-LINE
LUKAS R-1987-P-US-TOGA-W-PAC-AIR
MOLTENI F-1993-Q-J-ROY-METEOR-SOC-V119-P269
MOORE AM-1996-Q-J-ROY-METEOR-SOC-V122-P1405
PENLAND C-1995-J-CLIMATE-V8-P1999
PRIESTLEY MB-1981-SPECTRAL-ANAL-TIME-S
REYNOLDS RW-1994-J-CLIMATE-V7-P929
TRENBERTH KE-1992-373-NCAR
ZEBIAK SE-1991-GREENHOUSE-GAS-INDUC-P457
ZEBIAK SE-1987-MON-WEATHER-REV-V115-P2262
Times Cited: 2
Source item page count: 15
Publication Date: MAR 15
IDS No.: WM594
29-char source abbrev: J ATMOS SCI



Record 23 of 34
Author(s): Weickmann KM; Kiladis GN; Sardeshmukh PD
Title: The dynamics of intraseasonal atmospheric angular momentum oscillations
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1997, Vol 54, Iss 11, pp 1445-1461
No. cited references: 37
KeywordsPlus: MADDEN-JULIAN OSCILLATION; CIRCULATION ANOMALIES; TROPICAL PACIFIC; BALANCE; LENGTH; CYCLE; EARTH; CONVECTION; TORQUES; PERIOD
Abstract: The global and zonal atmospheric angular momentum (AAM) budget is computed from seven years of National Centers for Environmental Prediction data and a composite budget of intraseasonal (30-70 day) variations during northern winter is constructed. Regressions on the global AAM tendency are used to produce maps of outgoing longwave radiation, 200-hPa wind, surface stress, and sea level pressure during the composite AAM cycle. The primary synoptic features and surface torques that contribute to the AAM changes are described. In the global budget, the friction and mountain torques contribute about equally to the AAM tendency. The friction torque peaks in phase with subtropical surface easterly wind anomalies in both hemispheres. The mountain torque peaks when anomalies in the midlatitude Northern Hemisphere and subtropical Southern Hemisphere are weak but of the same sign. The picture is different for the zonal mean budget, in which the meridional convergence of the northward relative angular momentum transport and the friction torque are the dominant terms. During the global AAM cycle, zonal AAM anomalies move poleward from the equator to the subtropics primarily in response to momentum transports. These transports are associated with the spatial covariance of the filtered (30-70 day) perturbations with the climatological upper-tropospheric flow. The zonally asymmetric portion of these perturbations develop when convection begins over the Indian Ocean and maximize when convection weakens over the western Pacific Ocean, The 30-70-day zonal mean friction torque results from 1) the surface winds induced by the upper-tropospheric momentum sources and sinks and 2) the direct surface wind response to warm pool convection anomalies. The signal in relative AAM is complemented by one in ''Earth'' AAM associated with meridional redistributions of atmospheric mass. This meridional redistribution occurs preferentially over the Asian land mass and is linked with the 30-70-day eastward moving convective signal. It is preceded by a surface Kelvin-like wave in the equatorial Pacific atmosphere that propagates eastward from the western Pacific region to the South American topography and then moves poleward as an edge wave along the Andes. This produces a mountain torque on the Andes, which also causes the regional and global AAM to change.
Cited references: ANDERSON JR-1983-J-ATMOS-SCI-V40-P1584
BANTZER CH-1996-J-ATMOS-SCI-V53-P3032
DICKEY JO-1991-J-GEOPHYS-RES-ATMOS-V96-P22643
FELDSTEIN SB-1995-J-ATMOS-SCI-V52-P625
HENDON HH-1995-J-ATMOS-SCI-V52-P2373
HENDON HH-1994-J-ATMOS-SCI-V51-P2225
HIDE R-1991-SCIENCE-V253-P629
ITOH H-1994-J-GEOPHYS-RES-ATMOS-V99-P12981
JIN FF-1990-J-ATMOS-SCI-V47-P3007
KANG IS-1994-J-ATMOS-SCI-V51-P1194
KILADIS GN-1992-MON-WEATHER-REV-V120-P1900
KLINKER E-1992-J-ATMOS-SCI-V49-P608
KNUTSON TR-1987-MON-WEATHER-REV-V115-P1407
LANGLEY RB-1981-NATURE-V294-P730
LORENZ EN-1967-WMO-PUBL-V218
MADDEN RA-1995-J-ATMOS-SCI-V52-P3681
MADDEN RA-1972-J-ATMOS-SCI-V29-P1109
MADDEN RA-1971-J-ATMOS-SCI-V28-P702
MADDEN RA-1988-J-GEOPHYS-RES-ATMOS-V93-P5333
MADDEN RA-1987-J-GEOPHYS-RES-ATMOS-V92-P8391
MARCUS SL-1996-J-ATMOS-SCI-V53-P1993
MARCUS SL-1994-J-ATMOS-SCI-V51-P1431
MAYER TA-1988-GENERATION-CCM-FORMA
MILLIFF RF-1996-J-ATMOS-SCI-V53-P586
NEWTON CW-1971-J-ATMOSPHERIC-SCI-V28-P1329
PONTE RM-1990-J-GEOPHYS-RES-OCEANS-V95-P11369
ROSEN RD-1983-J-GEOPHYS-RES-OC-ATM-V88-P5451
ROSEN RD-1990-J-GEOPHYS-RES-SOLID-V95-P265
ROSEN RD-1993-SURV-GEOPHYS-V14-P1
SALBY ML-1994-J-ATMOS-SCI-V51-P2208
SALBY ML-1994-J-ATMOS-SCI-V51-P2344
SWINBANK R-1985-Q-J-ROY-METEOR-SOC-V111-P977
WANG B-1988-J-ATMOS-SCI-V45-P2051
WEICKMANN KM-1994-J-ATMOS-SCI-V51-P3194
WEICKMANN KM-1992-MON-WEATHER-REV-V120-P2252
WHITE GH-1992-137-NOAA-NOS-NGS
WILLIAMSON D-1987-NCARTN285STR-NCAR
Times Cited: 1
Source item page count: 17
Publication Date: JUN 1
IDS No.: XC335
29-char source abbrev: J ATMOS SCI



Record 24 of 34
Author(s): Craig GC; Gray SL
Title: CISK or WISHE as the mechanism for tropical cyclone intensification
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1996, Vol 53, Iss 23, pp 3528-3540
No. cited references: 38
KeywordsPlus: SEA INTERACTION THEORY; NUMERICAL-MODEL; EVOLUTION; CIRCULATIONS; ADJUSTMENT; SIMULATION; SCHEME; VORTEX; LAYER
Abstract: Examination of conditional instability of the second kind (CISK) and wind-induced surface heat exchange (WISHE), two proposed mechanisms for tropical cyclone and polar low intensification, suggests that the sensitivity of the intensification rate of these disturbances to surface properties, such as surface friction and moisture supply, will be different for the two mechanisms. These sensitivities were examined by perturbing the surface characteristics in a numerical model with explicit convection. The intensification rate was found to have a strong positive dependence on the heat and moisture transfer coefficients, while remaining largely insensitive to the frictional drag coefficient. CISK does not predict the observed dependence of vortex intensification rate on the heat and moisture transfer coefficients, nor the insensitivity to the frictional drag coefficient since it anticipates that intensification rate is controlled by frictional convergence in the boundary layer. Since neither conditional instability nor boundary moisture content showed any significant sensitivity to the transfer coefficients, this is true of CISK using both the convective closures of Ooyama and of Charney and Eliassen. In comparison, the WISHE intensification mechanism does predict the observed increase in intensification rate with heat and moisture transfer coefficients, while not anticipating a direct influence from surface friction.
Cited references: BAIK JJ-1990-MON-WEATHER-REV-V118-P513
BARNES GM-1995-MON-WEATHER-REV-V123-P2348
BRATSETH AM-1985-TELLUS-A-V37-P403
CHARNEY JG-1964-J-ATMOS-SCI-V21-P68
CRAIG GC-1996-Q-J-ROY-METEOR-SOC-V122-P415
CRAIG GC-1995-Q-J-ROY-METEOR-SOC-V121-P79
EMANUEL KA-1995-J-ATMOS-SCI-V52-P3960
EMANUEL KA-1989-J-ATMOS-SCI-V46-P3431
EMANUEL KA-1986-J-ATMOS-SCI-V43-P585
EMANUEL KA-1994-Q-J-ROY-METEOR-SOC-V120-P1111
EMANUEL KA-1989-TELLUS-A-V41-P1
FRAEDRICH K-1995-J-ATMOS-SCI-V52-P1914
FRAEDRICH K-1989-J-ATMOS-SCI-V46-P2642
FRANK WM-1977-MON-WEATHER-REV-V105-P1119
GRAY SL-1994-40-JCMM
HANDEL MD-1991-THESIS-MIT
JORDAN CL-1958-J-METEOR-V15-P91
KLEINSCHMIDT E-1951-ARCH-METEOROL-GEOP-A-V4-P53
KUO HL-1974-J-ATMOS-SCI-V31-P1232
KUO HL-1965-J-ATMOS-SCI-V22-P40
LORD SJ-1984-J-ATMOS-SCI-V41-P2836
MALKUS JS-1960-TELLUS-V12-P1
MCGRIDE JL-1995-Q-J-ROY-METEOR-SOC-V121-P783
OOYAMA K-1964-GEOFIS-INTERN-MEXICO-V4-P187
OOYAMA K-1969-J-ATMOS-SCI-V26-P3
OOYAMA KV-1982-J-METEOROL-SOC-JPN-V60-P369
RASMUSSEN E-1989-POLAR-ARTIC-LOWS-P47
RASMUSSEN E-1979-Q-J-ROY-METEOR-SOC-V105-P531
RASMUSSEN E-1987-TELLUS-A-V39-P408
ROGERS EB-1994-J-APPL-METEOROL-V33-P573
ROSENTHAL SL-1971-MON-WEA-REV-V99-P767
ROTUNNO R-1987-J-ATMOS-SCI-V44-P542
SCHUBERT WH-1980-J-ATMOS-SCI-V37-P1464
SMITH SD-1988-J-GEOPHYS-RES-OCEANS-V93-P15467
TRIPOLI GJ-1992-METEOROL-ATMOS-PHYS-V49-P229
WILLOUGHBY HE-1984-J-ATMOS-SCI-V41-P1169
WILLOUGHBY HE-1982-J-ATMOS-SCI-V39-P395
WILLOUGHBY HE-1979-J-GEOPHYS-RES-OC-ATM-V84-P3173
Times Cited: 1
Source item page count: 13
Publication Date: DEC 1
IDS No.: VX673
29-char source abbrev: J ATMOS SCI



Record 25 of 34
Author(s): Wilson DK; Wyngaard JC
Title: Empirical orthogonal function analysis of the weakly convective atmospheric boundary layer .2. Eddy energetics
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1996, Vol 53, Iss 6, pp 824-841
No. cited references: 24
KeywordsPlus: INTERNAL GRAVITY-WAVES; ROLL VORTICES; TURBULENCE; INVERSION
Abstract: Three-dimensional empirical orthogonal functions (EOFs), calculated from a large-eddy simulation of a weakly convective, planetary boundary layer (PBL), are used to decompose statistics for PBL turbulence into contributions from individual structures. The most energetic EOFs, corresponding largely to boundary-layer-spanning eddies, together are responsible for about one-half of the turbulent kinetic energy (TKE) throughout the boundary layer, although they carry a substantial amount of the momentum and heat fluxes only near mid-PBL. Examination of the flux profiles also reveals coupling between large roll structures and inversion-borne gravity waves. By filtering the fields through the EOFs, skewness and intermittency (kurtosis) associated with the different vertical scales are determined. Positive skewness around mid-PBL is found to be attributable to the boundary-layer spanning eddies. Intermittency, however, cannot be attributed to either large- or small-scale structures: it results from interscale interactions. Finally, equations for the flux and energy budgets of individual structures are derived. The budget analyses show clearly that the main source of TKE for large roll structures is shearing stress, while the main loss mechanism is transfer to smaller scales. The inversion-borne gravity waves gain TKE from interscale transfers and buoyant acceleration and lose TKE to shearing effects.
Cited references: BORKOWSKI J-1969-RADIO-SCI-V4-P1351
BRASSEUR JG-1994-PHYS-FLUIDS-V6-P842
CARRUTHERS DJ-1987-J-ATMOS-SCI-V44-P1801
CLARK TL-1986-Q-J-ROY-METEOR-SOC-V112-P899
ETLING D-1993-BOUND-LAY-METEOROL-V65-P215
FINNIGAN JJ-1984-J-ATMOS-SCI-V41-P2409
HAACK T-1992-J-ATMOS-SCI-V49-P1181
HUNT JCR-1988-Q-J-ROY-METEOR-SOC-V114-P827
KUETTNER JP-1987-Q-J-ROY-METEOR-SOC-V113-P445
LENSCHOW DH-1980-BOUND-LAY-METEOROL-V19-P509
LUMLEY JL-1976-J-FLUID-MECH-V74-P433
LUMLEY JL-1964-STRUCTURE-ATMOSPHERI
MASON PJ-1982-Q-J-ROY-METEOR-SOC-V108-P801
MCBEAN GA-1975-J-ATMOS-SCI-V32-P753
MOENG CH-1990-J-ATMOS-SCI-V47-P1149
MOENG CH-1984-J-ATMOS-SCI-V41-P2052
MOSER RD-1994-PHYS-FLUIDS-V6-P794
SCHUMANN U-1991-J-ATMOS-SCI-V48-P1758
SIEGEL A-1995-11-S-BOUND-LAY-TURB-P379
STULL RB-1988-INTRO-BOUNDARY-LAYER
STULL RB-1976-J-ATMOS-SCI-V33-P1279
WILSON DK-1996-J-ATMOS-SCI-V53-P801
WYNGAARD JC-1988-LECTURES-AIR-POLLUTI-P9
YOUNG GS-1988-J-ATMOS-SCI-V45-P2040
Times Cited: 1
Source item page count: 18
Publication Date: MAR 15
IDS No.: UB134
29-char source abbrev: J ATMOS SCI



Record 26 of 34
Author(s): SOUSOUNIS PJ; SHIRER HN
Title: LAKE AGGREGATE MESOSCALE DISTURBANCES .1. LINEAR-ANALYSIS
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1992, Vol 49, Iss 1, pp 80-96
No. cited references: 29
KeywordsPlus: PLANETARY BOUNDARY-LAYER; SEA BREEZE; FLOW; MODEL
Abstract: The steady boundary-layer responses that occur over the Great Lakes region during wintertime cold air outbreaks are examined using a two-dimensional, linear, analytic model. The planetary boundary layer (PBI.) is modeled as an idealized, constantly stratified, viscous, rotating Boussinesq fluid that moves uniformly between two horizontally infinite, rigid, stress-free plates. The heat from the lakes is parameterized in terms of a specified diabatic forcing function. Solution of the governing differential equation yields an integral expression for the vertical motion of the general response. Further assessment of the response is gained by examining closed-form analytic solutions to several limiting cases. Four response types are identified that depend upon the values of the Froude number Fr, the mechanical Ekman number E(r), the thermal Ekman number E(g), and the eddy Prandtl number Pr. Four different flow regimes are found. When 0 < Fr < 1 and Pr > 1, there is a purely exponentially damped response that exists over and on both sides of the heating. A flow characterized approximately by 1 < Fr2 < 1 + E(f)2 + E(k)2 and Pr > 1 yields a purely exponentially damped response that exists only over and downstream of the heating, while a flow characterized approximately by Fr3 > 1 + E(f)2 + E(g)2 and Pr > 1 yields a mixed oscillating-exponentially damped response that exists only over and downstream of the heating. When Pr < 1 and Fr > 1, either of the previous two response types can occur, while when 0 < Fr < 1, a fourth type of response can occur that is mixed oscillating-exponentially damped and exists over and on both sides of the heating. The model is used to demonstrate the effects that rotation, stability, mean flow speed, and mechanical and thermal dissipation have on the PBL responses that occur over the Great Lakes during wintertime cold air outbreaks. The simulation of heating by the lakes of strong flow within a moderately cold, shallow PBL produces a model response with ascent and implied clouds and precipitation extending well downstream of the lakes, as are typically observed soon after such a response develops. The simulation of heating by the lakes of weak flow within a very cold, deep PBL produces a model response with ascent and implied clouds and precipitation that are collocated with the lakes, as are typically observed just before such a response decays.
Cited references: BOUDRA DB-1977-NUMERICAL-STUDY-DESC
DALU GA-1989-J-ATMOS-SCI-V46-P1815
DANARD MB-1972-MON-WEA-REV-V100-P374
DANARD MB-1974-MON-WEATHER-REV-V102-P166
DEWEY KF-1975-J-APPL-METEOROL-V14-P3
DOCKUS KF-1975-NATL-WEA-DIG-V10-P5
FRITSCH JM-1989-12TH-C-WEATH-AN-FOR-P354
HILDEBRAND FB-1976-ADV-CALCULUS-APPLICA
HJELMFELT MR-1990-MON-WEATHER-REV-V118-P138
HSU HM-1987-J-ATMOS-SCI-V44-P186
KELLY RD-1982-J-ATMOS-SCI-V39-P1521
KUO HL-1973-J-ATMOS-SCI-V30-P53
LAVOIE RL-1972-J-ATMOSPHERIC-SCI-V29-P1025
LIN YL-1986-J-ATMOS-SCI-V43-P40
MALKUS JS-1952-J-METEOROL-V10-P30
NERALLA VR-1975-MON-WEATHER-REV-V103-P388
NIZIOL TA-1987-FORECASTING-V2-P310
ORLANSKI I-1974-J-ATMOS-SCI-V31-P965
PANOFSKY HA-1984-ATMOSPHERIC-TURBULEN
PETTERSSEN S-1959-J-METEOROL-V16-P642
PIELKE RA-1975-J-ATMOS-SCI-V32-P2288
ROTUNNO R-1983-J-ATMOS-SCI-V40-P1999
SMITH RC-1957-Q-J-ROY-METEOR-SOC-V83-P248
SOUSOUNIS PJ-1989-12TH-C-WEATHER-ANAL-P358
SOUSOUNIS PJ-1990-THESIS-PENNSYLVANIA
STAGE SA-1981-J-ATMOS-SCI-V38-P2230
WALSH JE-1974-J-ATMOS-SCI-V31-P2012
YOST DA-1982-J-ATMOS-SCI-V39-P114
YUEN CW-1986-J-ATMOS-SCI-V43-P3089
Times Cited: 1
Source item page count: 17
Publication Date: JAN 1
IDS No.: HB817
29-char source abbrev: J ATMOS SCI



Record 27 of 34
Author(s): Colello GD; Grivet C; Sellers PJ; Berry JA
Title: Modeling of energy, water, and CO2 flux in a temperate grassland ecosystem with SiB2: May-October 1987
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1998, Vol 55, Iss 7, pp 1141-1169
No. cited references: 74
KeywordsPlus: GENERAL-CIRCULATION MODEL; SURFACE PARAMETERIZATION SIB2; TERRESTRIAL CARBON METABOLISM; FIELD EXPERIMENT FIFE; SENSIBLE HEAT FLUXES; STOMATAL CONDUCTANCE; LAND-SURFACE; TALLGRASS PRAIRIE; ATMOSPHERIC CO2; CANOPY PHOTOSYNTHESIS
Abstract: The Simple Biosphere Model, version 2 (SiB2), was designed for use within atmospheric general circulation models as a soil-vegetation-atmosphere transfer scheme that includes CO2 flux prediction. A stand-alone version of SiB2 was used to simulate a grassland at Station 16 of the First ISLSCP Field Experiment (FIFE) located near Manhattan, Kansas, for a period of 142 days of the 1987 growing season. Modeled Values of soil temperature and moisture were initialized, using field measurements from the soil profile, and thereafter updated solely by model calculations. The model was driven by half-hourly atmospheric observations and regular observations of canopy biophysics. This arrangement was intended to mimic model forcing in a GCM. Three model Versions are compared: (i) a Control run using parameter values taken from look-up tables used for running the Colorado State University GCM; (ii) a Tuned run with many adjustments to optimize SiB2 to this ecosystem; and (iii) a Calibrated run, which calibrated the Control Version soil to the local site and incorporated two important changes from the Tuned version. Modeled fluxes of latent heat, sensible heat, soil heat, net radiation, and net site CO2 were compared to over 800 half-hourly observations; modeled surface and deep soil temperatures compared to 6500 observations; and three layers of modeled soil water content compared to 15 measurements of the soil water profile. Statistical methods were used to analyze these results. In the absence of water stress all three versions accurately simulated photosynthesis and canopy conductance. However, during episodes of drought, only the Tuned and Calibrated versions accurately simulated physiological control of canopy fluxes. The largest errors were encountered in the simulation of soil respiration. These were traced to problems predicting water content and temperature in the soil profile. These results highlight the need for improved simulation of soil biophysics to obtain accurate estimates of net CO2 balance. The accuracy of the Tuned version was improved by changes that (i) allowed water extraction by roots from all soil layers, (ii) matched the soil texture specification to the site, and (iii) calibrated the expressions used for diffusion of water and heat within the soil profile.
Cited references: AMTHOR JS-1994-AUST-J-PLANT-PHYSIOL-V21-P623
AVISSAR R-1989-MON-WEATHER-REV-V117-P2113
BALDOCCHI D-1994-AGR-FOREST-METEOROL-V67-P291
BALDOCCHI D-1992-BOUND-LAY-METEOROL-V61-P113
BERRY JA-1982-PHOTOSYNTHESIS-DEV-C-V2-P263
BETTS AK-1998-J-ATMOS-SCI-V55-P1091
BETTS AK-1993-Q-J-ROY-METEOR-SOC-V119-P975
BJORKMAN O-1989-PHOTOSYNTHESIS-P45
CHAVES MM-1991-J-EXP-BOT-V42-P1
CHEN DX-1994-AGR-FOREST-METEOROL-V68-P145
CLAPP RB-1978-WATER-RESOUR-RES-V14-P601
COLLATZ GJ-1991-AGR-FOREST-METEOROL-V54-P107
COLLATZ GJ-1992-AUST-J-PLANT-PHYSIOL-V19-P519
COOPER HJ-1995-J-GEOPHYS-RES-ATMOS-V100-P25419
DENNING AS-1995-NATURE-V376-P240
DENNING AS-1996-TELLUS-B-V48-P521
DENNING AS-1996-TELLUS-B-V48-P543
FAMIGLIETTI JS-1992-J-GEOPHYS-RES-ATMOS-V97-P18997
FIELD CB-1988-TRENDS-ECOL-EVOL-V3-P189
GAO W-1994-J-GEOPHYS-RES-ATMOS-V99-P1317
GARRATT JR-1993-J-CLIMATE-V6-P419
GARRATT JR-1993-J-CLIMATE-V6-P1090
GATES WL-1990-CLIMATE-CHANGE-IPCC-P97
GERMANN PF-1985-WATER-RESOUR-RES-V21-P990
GRANT RF-1992-AGR-FOREST-METEOROL-V61-P129
GRANT RF-1993-AGRON-J-V85-P916
HALL FG-1992-J-GEOPHYS-RES-ATMOS-V97-P19061
HENDERSONSELLERS -1995-B-AM-METEOROL-SOC-V76-P489
HOPE AS-1992-J-GEOPHYS-RES-ATMOS-V97-P19023
JOHNSON IR-1991-PLANT-CELL-ENVIRON-V14-P531
KAISER WM-1987-PHYSIOL-PLANTARUM-V71-P142
KIM J-1991-AGR-FOREST-METEOROL-V57-P187
KIM J-1991-AGR-FOREST-METEOROL-V55-P149
KIM J-1990-BOUND-LAY-METEOROL-V52-P135
KIM J-1990-BOUND-LAY-METEOROL-V51-P401
KIM J-1992-J-GEOPHYS-RES-ATMOS-V97-P6057
KIM J-1989-PRELIMINARY-REPORT-L
KNAPP AK-1985-ECOLOGY-V66-P1309
LIANG X-1994-J-GEOPHYS-RES-V99-P14415
MACPHERSON JI-1992-J-GEOPHYS-RES-ATMOS-V97-P18499
MCMURTRIE RE-1992-FOREST-ECOL-MANAG-V52-P261
NORMAN JM-1992-J-GEOPHYS-RES-ATMOS-V97-P18845
PEREIRA JS-1993-WATER-DEFICITS-P237
POLLEY HW-1992-J-GEOPHYS-RES-ATMOS-V97-P18837
QUICK WP-1992-PLANT-CELL-ENVIRON-V15-P25
RANDALL DA-1996-J-CLIMATE-V9-P738
SAUGIER B-1975-P-SUMM-COMP-SIM-C-P945
SELLERS PJ-1988-B-AM-METEOROL-SOC-V69-P22
SELLERS PJ-1993-FIFE-INTERIM-REPORT
SELLERS PJ-1989-J-APPL-METEOROL-V28-P727
SELLERS PJ-1986-J-ATMOS-SCI-V43-P305
SELLERS PJ-1996-J-CLIMATE-V9-P676
SELLERS PJ-1996-J-CLIMATE-V9-P706
SELLERS PJ-1995-J-GEOPHYS-RES-ATMOS-V100-P25607
SELLERS PJ-1992-J-GEOPHYS-RES-ATMOS-V97-P18345
SELLERS PJ-1992-J-GEOPHYS-RES-ATMOS-V97-P19033
SELLERS PJ-1992-J-GEOPHYS-RES-ATMOS-V97-P19091
SELLERS PJ-1992-REMOTE-SENS-ENVIRON-V42-P1
SELLERS PJ-1996-SCIENCE-V271-P1402
SHARKEY TD-1982-PLANTA-V156-P199
STEWART JB-1992-J-GEOPHYS-RES-ATMOS-V97-P18623
STREBEL DE-1994-COLLECTED-DATA-1-ISL-V1
TARDIEU F-1993-PLANT-CELL-ENVIRON-V16-P341
TARDIEU F-1993-PLANT-CELL-ENVIRON-V16-P413
TARDIEU F-1991-PLANT-CELL-ENVIRON-V14-P121
TARDIEU F-1993-WATER-DEFICITS-PLANT-P237
VERMA SB-1989-BOUND-LAY-METEOROL-V46-P53
VERMA SB-1992-J-GEOPHYS-RES-ATMOS-V97-P18629
VERMA SB-1993-REMOTE-SENS-ENVIRON-V44-P103
VINING RC-1992-J-GEOPHYS-RES-ATMOS-V97-P18951
VITERBO P-1995-J-CLIMATE-V8-P2716
WALTERSHEA EA-1992-J-GEOPHYS-RES-ATMOS-V97-P18925
WOFSY SC-1993-SCIENCE-V260-P1314
WOOD EF-1993-J-CLIMATE-V6-P839
Times Cited: 0
Source item page count: 29
Publication Date: APR 1
IDS No.: ZF369
29-char source abbrev: J ATMOS SCI



Record 28 of 34
Author(s): Hendon HH; Liebmann B; Glick JD
Title: Oceanic Kelvin waves and the Madden-Julian oscillation
Source: JOURNAL OF THE ATMOSPHERIC SCIENCES 1998, Vol 55, Iss 1, pp 88-101
No. cited references: 36
KeywordsPlus: OUTGOING LONGWAVE RADIATION; EASTERN EQUATORIAL PACIFIC; EL-NINO; INTRASEASONAL VARIATIONS; TROPICAL PACIFIC; SEA-LEVEL; MODEL; CIRCULATION; WINTER; CYCLE
Abstract: The relationship between the Madden-Julian oscillation (MJO), the dominant mode of intraseasonal variability in the tropical troposphere, and the Kelvin waves that dominate the variability of the equatorial thermocline in the central and eastern Pacific Oceans is explored. The Kelvin waves have period near 70 days, which is distinctly longer than the dominant period of the MJO (40-50 days). Their zonal wavelength is roughly the width of the Pacific basin, which is about twice the zonal scale of the zonal stress anomalies produced by the MJO across the western Pacific. Their eastward phase speed is about 2.3 m s(-1). which is indistinguishable from the gravest baroclinic mode using the observed stratification in the Pacific. The stress anomalies that force the Kelvin waves are shown to be associated with the lower-frequency components of the MJO (i.e., periods greater than about 60 days). These stress anomalies move eastward at less than 5 m s(-1) from the Indian Ocean to the date line, where their local wavelength is about 15 000 km. East of the date line, where the convective component of the MJO weakens, the phase speed of the stress anomalies increases to greater than 10 m s(-1). The similarity of the phase speeds of the MJO west of the date line and of the gravest baroclinic Kelvin wave is shown to result in near-resonant forcing by the relatively weak. but zonally broad, stress anomalies induced by tile MJO. Despite the large increase in phase speed east of the date line, the MJO-induced stress anomalies are shown to continue to positively project onto the Kelvin waves to about 130 degrees W, which is where the observed thermocline perturbations are the largest. East of this longitude, the MJO-induced stress anomalies detract from the amplitude of the Kelvin waves. The large spatial scale of the zonal stress anomalies produced by the MJO and the near-resonant forcing west of the date line helps explain the observed spectral peak near 70 days for the Kelvin waves despite the higher central frequency of the MJO.
Cited references: BRADY EC-1994-J-PHYS-OCEANOGR-V24-P2658
BUSALACCHI AJ-1988-J-PHYS-OCEANOGR-V18-P801
ENFIELD DB-1987-J-PHYS-OCEANOGR-V17-P1860
ERIKSEN CC-1993-J-PHYS-OCEANOGR-V23-P1208
GENT PR-1989-J-COMPUT-PHYS-V81-P444
GIESE BS-1991-J-GEOPHYS-RES-OCEANS-V96-P3239
GIESE BS-1990-J-GEOPHYS-RES-OCEANS-V95-P7289
GILL AE-1974-DEEP-SEA-RES-V21-P325
GRUBER A-1984-B-AM-METEOROL-SOC-V65-P958
HARRISON DE-1988-GEOPHYS-RES-LETT-V15-P804
HAYES SP-1991-B-AM-METEOROL-SOC-V72-P339
HENDON HH-1996-J-ATMOS-SCI-V53-P1751
HENDON HH-1994-J-ATMOS-SCI-V51-P2225
HENDON HH-1997-J-CLIMATE-V10-P647
HENDON HH-1994-J-GEOPHYS-RES-ATMOS-V99-P8073
JOHNSON ES-1993-J-PHYS-OCEANOGR-V23-P608
KESSLER WS-1995-J-CLIMATE-V8-P1757
KESSLER WS-1995-J-GEOPHYS-RES-OCEANS-V100-P10613
KESSLER WS-1987-J-PHYS-OC