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  • 1
    Monograph available for loan
    Monograph available for loan
    New York [u.a.] : Oxford Univ. Press
    Call number: PIK N 456-11-0377
    Description / Table of Contents: Contents: The Frontier Overhead ; Catching Real Storms ; Numerical Simulations Come of Age ; Storm Chasing and Doppler Radar in Major Field Programs ; The State of the Art ; Where We Are Headed ; Appendix A: The Dynamic Pressure ; Appendix B: The Effects of Momentum Transport by an Updraft in a Sheared Environment ; Appendix C: Other Resources
    Type of Medium: Monograph available for loan
    Pages: XII, 180 S. : zahlr. Ill., graph. Darst., Kt.
    ISBN: 0195105524
    Location: A 18 - must be ordered
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  • 2
    Call number: AWI A6-92-0494
    In: Synoptic-Dynamic Meteorology in Midlatitudes, Vol. 1
    Type of Medium: Monograph available for loan
    Pages: XIII, 431 S. , Ill., graph. Darst
    ISBN: 0195062671
    Language: English
    Note: Contents: 1. INTRODUCTION. - 1.1 What is Synoptic Meteorology?. - 1.1.1 Historical background. - 1.1.2 Classification of atmospheric phenomena. - 1.1.3 Atmospheric phenomena as fractals. - 1.1.4 The role of observations and theory. - 1.1.5 The mystery of synoptic meteorology. - 1.1.6 The organization of this text. - 1.2 Units and Variables. - 1.2.1 The MKS system. - 1.2.2 The MTS system. - 1.2.3 Other useful conversion factors. - 1.3 Coordinate Systems. - 1.3.1 Cartesian coordinates. - 1.3.2 Natural coordinates. - 1.3.3 The representation of the wind field. - 1.3.4 Pressure coordinates. - 1.3.5 Isentropic coordinates. - 1.3.6 σ coordinates. - 1.3.7 Invariance. - 1.3.8 The total derivative. - Note. - References. - 2. SCALAR FIELDS AND THEIR KINEMATICS. - 2.1 The Pressure (Height) Field. - 2.1.1 What is kinematics?. - 2.1.2 A description of features in the pressure (height) field. - 2.1.3 Analysis of the pressure (height) field. - 2.1.4 Kinematics of the pressure (height) field. - 2.1.5 The hydrostatic equation and the reduction of pressure to a reference level. - 2.2 The Temperature and Moisture Fields. - 2.3 The Measurement of Scalar Fields. - 2.3.1 Introduction. - 2.3.2 The measurement of pressure. - 2.3.3 The measurement of height. - 2.3.4 The measurement of temperature. - 2.3.5 The measurement of humidity. - 2.3.6 Clouds. - 2.3.7 The measurement of precipitation. - 2.3.8 Instrument platforms. - Notes. - References. - Problems. - 3. KINEMATICS OF THE WIND FIELD. - 3.1 Properties of the Horizontal Wind Field. - 3.1.1 The decomposition of a linear wind field. - 3.1.2 Translation. - 3.1.3 Divergence. - 3.1.4 Vorticity. - 3.1.5 Deformation. - 3.1.6 Summary. - 3.1.7 Trajectories. - 3.2 The Computation of Divergence, Vorticity, and Deformation. - 3.2.1 The expressions for divergence, vorticity, and deformation on the Earth's surface. - 3.2.2 Finite-difference computations. - 3.2.3 Integral computations of divergence, vorticity, and deformation. - 3.2.4 The linear vector point function method. - 3.3 Properties of the Three-Dimensional Wind Field. - 3.4 Measuring the Wind Field. - 3.4.1 Introduction. - 3.4.2 Wind-measuring instruments: Dependence of the properties of an object upon wind speed. - 3.4.3 Wind-measuring instruments: The tracking of tracers moving with the horizontal component of the wind. - Notes. - References. - Problems. - 4. ELEMENTARY ATMOSPHERIC DYNAMICS AND THERMODYNAMICS. - 4.1 The Law of Motion. - 4.1.1 The equation of fluid motion on a rotating sphere: Vector form. - 4.1.2 The equations of fluid motion on a rotating sphere: Scalar form. - 4.1.3 The geostrophic wind. - 4.1.4 The isallobaric wind and the inertial-advective wind. - 4.1.5 The equations of motion in natural coordinates. - 4.1.6 The thermal wind. - 4.2 The Equation of Continuity. - 4.2.1 The equation of continuity in height coordinates. - 4.2.2 The equation of continuity in pressure coordinates. - 4.2.3 The equation of continuity in isentropic coordinates. - 4.2.4 The kinematic boundary condition. - 4.2.5 The dynamic boundary condition. - 4.3 The Thermodynamic Equation. - 4.3.1 Dry thermodynamics. - 4.3.2 Moist thermodynamics. - 4.4 Friction. - 4.4.1 Molecular friction. - 4.4.2 Turbulent friction. - 4.4.3 The surface boundary layer. - 4.4.4 The friction layer. - 4.4.5 The turbulent transport of general quantities. - 4.4.6 The antitriptic wind. - 4.5 The Vorticity Equation. - 4.5.1 Derivation of the vorticity equation in height coordinates. - 4.5.2 The Bjerknes and Kelvin circulation theorems. - 4.5.3 Physical interpretation of the vorticity equation and the circulation theorems. - 4.5.4 The vorticity equation in pressure coordinates. - 4.5.5 The vorticity equation in isentropic coordinates and Ertel's potential vorticity. - 4.5.6 The horizontal vorticity equation. - 4.5.7 The three-dimensional vorticity equation in a compressible atmosphere. - 4.6 Energetics. - 4.7 Thermodynamic Retrieval. - References. - Problems. - 5. QUASIGEOSTROPHIC THEORY. - 5.1 Introduction. - 5.2 Estimating the Terms in the Vorticity and Thermodynamic Equations. - 5.2.1 Substitution of the analytical-model equations into the vorticity and thermodynamic equations. - 5.2.2 The relationship between w and ω. - 5.2.3 The kinematic boundary conditions for midlatitude, synoptic-scale systems. - 5.2.4 A simplified vorticity equation. - 5.2.5 The thermodynamic equation for synoptic-scale systems in the midlatitudes. - 5.2.6 The effects of diabatic heating and static stability. - 5.3 Estimating Vertical Motion from the Observed Wind and Mass Fields. - 5.3.1 The kinematic method. - 5.3.2 The adiabatic method. - 5.3.3 The vorticity method. - 5.3.4 Satellite infrared photograph technique. - 5.4 Estimating Local Height Tendencies from the Observed Wind and Mass Fields. - 5.5 The Quasigeostrophic Vorticity and Thermodynamic Equations. - 5.5.1 The quasigeostrophic approximation. - 5.5.2 The quasigeostrophic vorticity and thermodynamic equations. - 5.5.3 The quasigeostrophic equations of motion. - 5.6 Derivation of the Quasigeostrophic ω and Height-tendency Equations. - 5.6.1 The quasigeostrophic vorticity and thermodynamic equations expressed in terms of the height field. - 5.6.2 The quasigeostrophic ω equation. - 5.6.3 The quasigeostrophic height-tendency equation. - 5.6.4 The quasigeostrophic ω equation and height-tendency equation with diabatic heating and friction. - 5.7 Interpretation of the Quasigeostrophic ω-Equation. - 5.7.1 Mathematical interpretation. - 5.7.2 Physical interpretation. - 5.7.3 The Trenberth formulation of the quasigeostrophic ω equation. - 5.7.4 The Q-vector representation of the quasigeostrophic ω equation. - 5.7.5 Comparison of the different quasigeostrophic ω equations. - 5.8 The Quasigeostrophic Potential Vorticity Form of the Height-Tendency Equation. - 5.9 Static-Stability Effects on Vertical Motion. - 5.9.1 The effects of horizontal variations in static stability on vertical motion. - 5.9.2 Effective static stability. - 5.10 Interpretation of the Quasigeostrophic Height-Tendency Equation. - 5.10.1 Mathematical interpretation. - 5.10.2 Physical interpretation. - 5.11 The Effects of Vertical Variations in Static Stability on the Geopotential-Height Tendency. - Note. - References. - Problems. - Selected Answers to Problems. - Appendix 1. Review of Vector Notation. - Appendix 2. Implications of Hydrostatic Balance for the Horizontal and Vertical Scales of Meteoro­logical Phenomena. - Appendix 3. Matrix Notation. - Index.
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  • 3
    Publication Date: 2001-11-01
    Description: No Abstract available.
    Print ISSN: 0065-9401
    Electronic ISSN: 1943-3646
    Topics: Geography , Geosciences , Physics
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  • 4
    Publication Date: 2003-08-01
    Print ISSN: 0065-9401
    Electronic ISSN: 1943-3646
    Topics: Geography , Geosciences , Physics
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  • 5
    Publication Date: 2008-11-01
    Description: A case study of a double dryline on 22 May 2002 is presented. Mobile, 3-mm-wavelength Doppler radars from the University of Massachusetts and the University of Wyoming (Wyoming cloud radar) were used to collect very fine resolution vertical-velocity data in the vicinity of each of the moisture gradients associated with the drylines. Very narrow (50–100 m wide) channels of strong upward vertical velocity (up to 8 m s–1) were measured in the convergence zone of the easternmost dryline, larger in magnitude than reported with previous drylines. Distinct areas of descending motion were evident to the east and west of both drylines. Radar data are interpreted in the context of other observational platforms available during the International H2O Project (IHOP-2002). a variational ground-based mobile radar data processing technique was developed and applied to pseudo-dual-Doppler data collected during a rolling range-height indicator deployment. It was found that there was a secondary (vertical) circulation normal to the easternmost moisture gradient; the circulation comprised an easterly component near-surface flow to the east, a strong upward vertical component in the convergence zone, a westerly return, flow above the convective boundary layer, and numerous regions of descending motion, the most prominent approximately 3–5 km to the east of the surface convergence zone.
    Print ISSN: 0065-9401
    Electronic ISSN: 1943-3646
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  • 6
    Publication Date: 2008-11-01
    Description: The nature of the different types of surface boundaries that appear in the southern plains of the United States during the convectively active season is reviewed. The following boundaries are discussed: fronts, the dryline, troughs, and outflow boundaries, The boundaries are related to their environment and to local topography. The role these boundaries might play in the initiation of convective storms is emphasized. The various types of boundary-related vertical circulations and their dynamics are discussed. In particular, quasigeostrophic and semigeostrophic dynamics, and the dynamics of solenoidal circulations, density currents, boundary layers, and gravity waves are considered. Miscellaneous topics pertinent to convective storms and their relationship to surface boundaries such as along-the-boundary variability, boundary collisions, and the role of vertical shear are also discussed. Although some cases of storm initiation along surface boundaries have been well documented using research datasets collected during comprehensive field experiments, much of what we know is based only on empirical forecasting and nowcasting experience. It is suggested that many problems relating to convective-storm formation need to be explored in detail using real datasets with new observing systems and techniques, in conjunction with numerical simulation studies, and through climatological studies.
    Print ISSN: 0065-9401
    Electronic ISSN: 1943-3646
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  • 7
    Publication Date: 2018-07-24
    Description: This study documents the formation and evolution of secondary vortices associated within a large, violent tornado in Oklahoma based on data from a close-range, mobile, polarimetric, rapid-scan, X-band Doppler radar. Secondary vortices were tracked relative to the parent circulation using data collected every 2 s. It was found that most long-lived vortices (those that could be tracked for ≥15 s) formed within the radius of maximum wind (RMW), mainly in the left-rear quadrant (with respect to parent tornado motion), passing around the center of the parent tornado and dissipating closer to the center in the right-forward and left-forward quadrants. Some secondary vortices persisted for at least 1 min. When a Burgers–Rott vortex is fit to the Doppler radar data, and the vortex is assumed to be axisymmetric, the secondary vortices propagated slowly against the mean azimuthal flow; if the vortex is not assumed to be axisymmetric as a result of a strong rear-flank gust front on one side of it, then the secondary vortices moved along approximately with the wind.
    Print ISSN: 0027-0644
    Electronic ISSN: 1520-0493
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  • 8
    Publication Date: 2018-02-01
    Print ISSN: 0027-0644
    Electronic ISSN: 1520-0493
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  • 9
    Publication Date: 2016-06-27
    Description: Past numerical simulation studies found that debris loading from sand-sized particles may substantially affect tornado dynamics, causing reductions in near-surface wind speeds up to 50%. To further examine debris loading effects, simulations are performed using a large-eddy simulation model with a two-way drag force coupling between air and sand. Simulations encompass a large range of surface debris fluxes that cause negligible to substantial impact on tornado dynamics for a high-swirl tornado vortex simulation. Simulations are considered for a specific case with a single vortex flow type (swirl ratio, intensity, and translation velocity) and a fixed set of debris and aerodynamic parameters. Thus, it is stressed that these findings apply to the specific flow and debris parameters herein and would likely vary for different flows or debris parameters. For this specific case, initial surface debris fluxes are varied over a factor of 16 384, and debris cloud mass varies by only 42% of this range because a negative feedback reduces near-surface horizontal velocities. Debris loading effects on the axisymmetric mean flow are evident when maximum debris loading exceeds 0.1 kg kg−1, but instantaneous maximum wind speed and TKE exhibit small changes at smaller debris loadings (greater than 0.01 kg kg−1). Initially, wind speeds are reduced in a shallow, near-surface layer, but the magnitude and depth of these changes increases with higher debris loading. At high debris loading, near-surface horizontal wind speeds are reduced by 30%–60% in the lowest 10 m AGL. In moderate and high debris loading scenarios, the number and intensity of subvortices also decrease close to the surface.
    Print ISSN: 0022-4928
    Electronic ISSN: 1520-0469
    Topics: Geography , Geosciences , Physics
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  • 10
    Publication Date: 2016-01-01
    Description: Several data assimilation and forecast experiments are undertaken to determine the impact of special observations taken during the second Verification of the Origins of Rotation in Tornadoes Experiment (VORTEX2) on forecasts of the 5 June 2009 Goshen County, Wyoming, supercell. The data used in these experiments are those from the Mobile Weather Radar, 2005 X-band, Phased Array (MWR-05XP); two mobile mesonets (MM); and several mobile sounding units. Data sources are divided into “routine,” including those from operational Weather Surveillance Radar-1988 Dopplers (WSR-88Ds) and the Automated Surface Observing System (ASOS) network, and “special” observations from the VORTEX2 project. VORTEX2 data sources are denied individually from a total of six ensemble square root filter (EnSRF) data assimilation and forecasting experiments. The EnSRF data assimilation uses 40 ensemble members on a 1-km grid nested inside a 3-km grid. Each experiment assimilates data every 5 min for 1 h, followed by a 1-h forecast. All experiments are able to reproduce the basic evolution of the supercell, though the impact of the VORTEX2 observations was mixed. The VORTEX2 sounding data decreased the mesocyclone intensity in the latter stages of the forecast, consistent with observations. The MWR-05XP data increased the forecast vorticity above approximately 1 km AGL in all experiments and had little impact on forecast vorticity below 1 km AGL. The MM data had negative impacts on the intensity of the low-level mesocyclone, by decreasing the vertical vorticity and indirectly by decreasing the buoyancy of the inflow.
    Print ISSN: 0027-0644
    Electronic ISSN: 1520-0493
    Topics: Geography , Geosciences , Physics
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