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  • 1
    Monograph available for loan
    Monograph available for loan
    Cambridge [u.a.] : Cambridge Univ. Press
    Associated volumes
    Call number: AWI A10-00-0209
    In: Cambridge atmospheric and space science series
    Description / Table of Contents: Contents: List of Illustrations. - Preface. - Acknowledgments. - 1 Basic Properties of Radiation, Atmospheres, and Oceans. - 1.1 lntroduction. - 1.2 Parts of the Spectrum. - 1.2.1 Extraterrestrial Solar Flux. - 1.2.2 Terrestrial lnfrared Flux. - 1.3 Radiative Interaction with Planetary Media. - 1.3.1 Feedback Processes. - 1.3.2 Types of Matter that Affect Radiation. - 1.4 Vertical Structure of Planetary Atmospheres. - 1.4.1 Hydrostatic and Ideal Gas Laws. - 1.4.2 Minor Species in the Atmosphere. - 1.4.3 Optical Line-of-Sight Paths. - 1.4.4 Radiative Equilibrium and the Thermal Structure of Atmospheres. - 1.4.5 Climate Change: Radiative Forcing and Feedbacks. - 1.5 Density Structure of the Ocean. - 1.6 Vertical Structure of the Ocean. - 1.6.1 The Mixed Layer and the Deep Ocean. - 1 .6.2 Seasonal Variations of Ocean Properties. - 1.6.3 Sea-Surface Temperature. - 1.6.4 Ocean Spectral Reflectance and Opacity. - 1.7 Remarks on Nomenclature, Notation, and Units. - 1.8 Summary. - 2 Basic State Variables and the Radiative Transfer Equation. - 2.1 Introduction.- 2.2 Geometrical Optics. - 2.3 Radiative Flux or Irradiance. - 2.4 Spectral Intensity and Its Angular Moments. - 2.4.1 Relationship between Flux and Intensity. - 2.4.2 Average Intensity and Energy Density. - 2.5 Some Theorems on Intensity. - 2.5.1 lntensity and Flux from an Extended Source. - 2.6 Perception of Brightness: Analogy with Radiance. - 2.7 The Extinction Law. - 2.7.1 Extinction = Scattering + Absorption. - 2.8 The Differential Equation of Radiative Transfer. - 2.9 Summary. - 3 Basic Scattering Processes. - 3.1 Introduction. - 3.2 Lorentz Theory for Radiation- Matter Interactions. - 3.2.1 Scattering and Collective Effects in a Uniform Medium. - 3.2.2 Scattering from Density Irregularities. - 3.2.3 Scattering in Random Media. - 3.2.4 First-Order and Multiple Scattering. - 3.3 Scattering from a Damped Simple Harmonic Oscillator. - 3.3.1 Case ( 1 ): Resonance Scattering and the Lorentz Profile. - 3.3.2 Conservative and Nonconservative Scattering. - 3.3.3 Natural Broadening. - 3.3.4 Pressure Broadening. - 3.3.5 Doppler Broadening. - 3.3.6 Realistic Line-Broadening Processes. - 3.3.7 Case (2): Rayleigh Scattering. - 3.4 The Scattering Phase Function. - 3.4.1 Rayleigh-Scattering Phase Function. - 3.5 Mie-Debye Scattering. - 3.6 Summary. - 4 Absorption by Solid, Aqueous, and Gaseous Media. - 4.1 Introduction. - 4.2 Absorption on Surfaces, on Aerosols, and within Aqueous Media. - 4.2.1 Solids. - 4.2.2 Aerosols. - 4.2.3 Liquids. - 4.3 Molecular Absorption in Gases. - 4.3.1 Thermal Emission and Radiation Laws. - 4.3.2 Planck's Spectral Distribution Law. - 4.3.3 Radiative Excitation Processes in Molecules. - 4.3.4 Inelastic Collisional Processes. - 4.3.5 Maintenance of Thermal Equilibrium Distributions. - 4.4 The Two-Level Atom. - 4.4.1 Microscopic Radiative Transfer Equation. - 4.4.2 Effects of Collisions on State Populations. - 4.5 Absorption in Molecular Lines and Bands. - 4.5.1 Molecular Rotation: The Rigid Rotator. - 4.5.2 Molecular Vibration and Rotation: The Vibrating Rotator. - 4.5.3 Line Strengths. - 4.6 Absorption Processes in the UV/Visible. - 4.7 Summary. - 5 Principles of Radiative Transfer. - 5.1 Introduction. - 5.2 Boundary Properties of Planetary Media. - 5.2.1 Thermal Emission from a Surface. - 5.2.2 Absorption by a Surface. - 5.2.3 Kirchhoff's Law for Surfaces. - 5.2.4 Surface Reflection: The BRDF. - 5.2.5 Albedo for Collimated lncidence. - 5.2.6 The Flux Reflectance, or Albedo: Diffuse Incidence. - 5.2.7 Analytic Reflectance Expressions. - 5.2.8 The Opposition Effect. - 5.2.9 Specular Reflection from the Sea Surface. - 5.2.10 Transmission through a Slab Medium. - 5.2.11 Spherical, or Bond Albedo. - 5.3 Absorption and Scattering in Planetary Media. - 5.3.1 Kirchhoff's Law for Volume Absorption and Emission. - 5.3.2 Differential Equation of Radiative Transfer. - 5.4 Solution of the Radiative Transfer Equation for Zero Scattering. - 5.4.1 Solution with Zero Scattering in Slab Geometry. - 5.4.2 Half-Range Quantities in a Slab Geometry. - 5.4.3 Formal Solution in a Slab Geometry. - 5.5 Gray Slab Medium in Local Thermodynamic Equilibrium. - 5.6 Formal Solution Including Scattering and Emission. - 5.7 Radiative Heating Rate. - 5.7.1 Generalized Gershun's Law. - 5.7.2 Warming Rate, or the Temperature Tendency. - 5.7.3 Actinic Radiation, Photolysis Rate, and Dose Rate. - 5.8 Summary. - 6 Formulation of Radiative Transfer Problems. - 6.1 Introduction. - 6.2 Separation into Diffuse and Direct (Solar) Components. - 6.2.1 Lower Boundary Conditions. - 6.2.2 Multiple Scattering. - 6.2.3 Azimuth lndependence of Flux and Mean Intensity. - 6.3 Azimuthal Dependence of the Radiation Field. - 6.4 Spherical Shell Geometry. - 6.5 Nonstratified Media. - 6.6 Radiative Transfer in the Atmosphere-Ocean System. - 6.6.1 Two Stratified Media with Different Indices of Refraction. - 6.7 Examples of Phase Functions. - 6.7.1 Rayleigh Phase Function. - 6.7.2 The Mie-Debye Phase Function. - 6.8 Scaling Transformations Useful for Anisotropic Scattering. - 6.8.1The [Delta]-Isotropic Approximation. - 6.8.2 The [Delta]- Two-Term Approximation. - 6.8.3 Remarks on Low-Order Scaling Approximations. - 6.8.4 The [Delta]-N Approximation: Arbitrary N. - 6.8.5 Mathematical and Physical Meaning of the Scaling. - 6.9 Prototype Problems in Radiative Transfer Theory. - 6.9.1 Prototype Problem 1: Uniform Illumination. - 6.9.2 Prototype Problem 2: Constant lmbedded Source. - 6.9.3 Prototype Problem 3: Diffuse Reflection Problem. - 6.9.4 Boundary Conditions: Reflecting and Emitting Surface. - 6.10 Reciprocity, Duality, and Inhomogeneaus Media. - 6.11 Effects of Surface Reflection on the Radiation Field. - 6.12 Integral Equation Formulation of Radiative Transfer. - 6.13 Probabilistic Aspects of Radiative Transfer. - 6.13.1 The Escape Probability. - 6.14 Summary. - 7 Approximate Salutions of Prototype Problems. - 7.1 Introduction. - 7.2 Separation of the Radiation Field into Orders of Scattering. - 7.2.1 Lambda Iteration: The Multiple-Scaltering Series. - 7.2.2 Single-Scattered Contribution from Ground Reflection: The Planetary Problem. - 7.3 The Two-Stream Approximation: Isotropic Scattering. - 7.3.1 Approximate Differential Equations. - 7.3.2 The Mean lnclination: Possible Choices for [My]. - 7.3.3 Prototype Problem 1: Differential-Equation Approach. - 7.3.4 Prototype Problem 2: lmbedded Source. - 7.3.5 Prototype Problem 3: Beam Incidence. - 7.4 Conservative Scattering in a Finite Slab. - 7.5 Anisotropic Scattering. - 7.5.1 Two-Stream Versus Eddington Approximations. - 7.5.2 The Backscattering Coefficients. - 7.5.3 Two-Stream Salutions for Anisotropic Scattering. - 7.5.4 Scaling Approximations for Anisotropic Scattering. - 7.5.5 Generalized Two-Stream Equations. - 7.6 Accuracy of the Two-Stream Method. - 7.7 Final Comments on the Two-Stream Method. - 7.8 Summary. - 8 Accurate Numerical Salutions of Prototype Problems. - 8.1 Introduction. - 8.2 Discrete-Ordinate Method - Isotropic Scattering. - 8.2.1 Quadrature Formulas. - 8.2.2 The Double-Gauss Method. - 8.3 Anisotropic Scattering. - 8.3.1 General Considerations. - 8.3.2 Quadrature Rule. - 8.4 Matrix Formulation of the Discrete-Ordinate Method. - 8.4.1 Two- and Four-Stream Approximations. - 8.4.2 Multistream Approximation ( N Arbitrary). - 8.5 Matrix Eigensolutions. - 8.5.1 Two-Stream Salutions ( N = 1). - 8.5.2 Multistream Solutions ( N Arbitrary). - 8.5.3 Inhomogeneous Solution. - 8.5.4 General Solution. - 8.6 Source Function and Angular Distributions. - 8.7 Boundary Conditions - Removal of Ill-Conditioning. - 8.7.1 Boundary Conditions. - 8.7.2 Removal of Numerical lll-Conditioning. - 8.8 Inhomogeneous Multilayered Media. - 8.8.1 General Solution - Boundary and Layer Interface Conditions. - 8.8.2 Source Functions and Angular Distributions. - 8.8.3 Numerical lmplementation of the Discrete-Ordinate Method. - 8.9 Correction of the Truncated Intensity Field. - 8.9.1 The Nakajima-Tanaka Correction Procedure. - 8.9.2 Computed lntensity Distributions for the Standard Problem. - 8.10 The Coupled Atmosphere-Ocean Problem. - 8.10.1 Discretized Equations for the Atmosphere-Ocean System. - 8.10.2 Quadrature and General Solution. - 8.10.3 Boundary, Continuity, and Atmosphere-Ocean Interface Conditions. - 8.11 The Doubling-Adding and the Matrix Operator Methods. - 8.11.1 Matrix-Exponential Solution - Formal Derivation of Doubling Rules. - 8.11.2 Connection between Doubling and Discrete-Ordinate Methods. - 8.11.3 Intuitive Derivation of the Doubling Rules - Adding of Dissimilar Layers. - 8.12 Other Accurate Methods. - 8.12.1 The Spherical-Harmonics Method. - 8.12.2 Invariant lmbedding. - 8.12.3 Iteration Methods. - 8.12.4 The Feautrier Method. - 8.12.5 Integral Equation Approach. - 8.12.6 Monte Carlo Methods. - 8.13 Summary. - 9 Shortwave Radiative Transfer. - 9.1 Introduction. - 9.2 Solar Radiation. - 9.3 Optical Properties of the Earth-Atmosphere System. - 9.3.1 Gaseaus Absorption and Penetration Depth. - 9.3.2 Optical Properlies of Atmospheric Aerosols. - 9.3.3 Optical Properties of Warm (Liquid Water) Clouds. - 9.3.4 Optical Properties of Ice Clouds. - 9.3.5 Optical Properties of the Ocean. - 9.3.6 Optical Properties of Snow and Ice. - 9.4 Modeling of Shortwave Radiative Effects in the Atmosphere. - 9.4.1 Spectral Averaging Procedure: The Chandrasekhar Mean. - 9.4.2 Solar Warming Rates Due to Ozone, Aerosols, and Clouds. - 9.4.3 Computation of Photolysis Rates. - 9.4.4 UV Transmission: Relation to Ozone Abundance. - 9.4.5 UV Transmission and Dose Rates at the Earth 's Surface. - 9.4.6 Comparisan of Measured and Computed UV Irradiance at the Surface. - 9.5 Modeling of Shortwave Radiation in the Ocean. - 9.5.1 Diffuse Radiation: Attenuation in the Ocean. - 9.5.2 Two-Stream Model Appropriate for Deep Water. - 9.5.3 Backscattering by Ocean Particles: The Role of Shape Factars. - 9.5.4 Approximate Expressions for the Remotely Sensed Reflectance. - 9.5.5 Modefing the UV Transmission into the Ocean. - 9.5.6 Measured and Computed UV Irradiance in the Ocean. - 9.6 Interaction of Solar Radiation with Snow and Ice. - 9.7 Summary. - 1 0 Transmission in Spectrally Complex Media. - 10.1 Introduction. - 10.2 Transmission in an Isolated Line. - 10.2.1 Isolated Lorentz Line. - 10.3 Band Models. - 10.3.1 The Elsasser Band Model. - 10.3.2 Distributed Line lntensities. - 10.3.3 Random Band Model. - 10.3.4 MODTRAN: A Moderate-Resolution Band Model. - 10.4 Spectral Mapping Transformations for Homogeneous Media. - 10.4.1 Method of the k-Distribution. - 10.4.2 k-Distribution for the Malkmus Band Model. - 10.5 Transmission in Nongray Inhomogeneaus Media. - 10.5.1 The H- C-G Scaling Approximation. - 10.5.2 LBL Transmission Computation: Inhomogeneaus Paths. - 10.5.3 Inclusion of Multiple Scattering in LBL Computations. - 10.5.4 The Correlated-k Method. - 10.5.5 Inclusion of Multiple Scattering in the Correlated-k Method. - 10.6 Summary. - 11 Radiative Transfer in Nongray Media. - 11.1 lntroduction. - 11.2 Radiative Flux and Heating Rate: Clear-Sky Conditions. - 11.2.1 Monochromatic Flux Equations. - 11.2.2 Wide-Band Emittance Models. - 11.2.3 Narrow-Band Absorption Model. - 11.2.4 Band Overlap. - 11.2.5 The Diffusivity Approximation. - 11.2.6 Equationsfor the Heating Rate. - 11.2.7 Clear-Sky Radiative Cooling: Nonisothermal Medium. - 11.2.8 Computations of Terrestrial Cooling Rates. - 11.3 The IR Radiative Impact of Clouds and Aerosols. - 11.3.1Heating Rate in an Idealized Cloud. - 11.3.2 Detailed Longwave Radiative Effects of Clouds. - 11.3.3 Accurate Treatment Including Scattering. - 11.4 Summary. - 12 The Role of Radiation in Climate. - 12.1 Introduction. - 12.2 Radiative Equilibrium with Zero Visible Opacity. - 12.3 Radiative Equilibrium with Finite Visible Opacity. - 12.4 Radiative-Convective Equilibrium. - 12.5 The Concept of the Emission Height. - 12.6 Effects of spectral window. - 12.7 Radiative forcing. - 12.8 Climate impact of clouds. - 12.8.1 Longwave Effects of water clouds. - 12.8.2 Shortwave effects of water clouds. - 12.8.3 Combined shortwave and longewave effects of clouds. - 12.9 Climate impact of cloud height. - 12.10 Cloud and aerosol forcing. - 12.10.1 Aerosol forcing. - 12.11 Water-Vapor Feedback. - 12.12 Effects of carbon dioxide changes. - 12.13 Greenhouse effect from individual gas species. - 12.14 Summary. - Appendices. - A Nomenclature: Glossary of symbols. - B Physical constants. - C Model atmospheres. - D Ocean optics nomenclature. - E Reflectance and transmittance at an interface. - Index.
    Description / Table of Contents: Radiative transfer is important to a range of disciplines, from the study of greenhause warming to stellar atmospheres and ocean optics. This text provides a foundation of the theoretical and practical aspects of radiative transfer for senior undergraduate and graduate students of atmospheric, oceanic, and environmental sciences. With an emphasis on formulation, judicial approximations and numerical solutions of the radiative transfer equation, Radiative Transfer in the Atmosphere and Ocean fills a gap between descriptive texts covering the physical processes and the practical numerical approaches needed in research. Designed to convey physical insight into the transfer process, it can also be used as a self-contained manual for practitioners who require accurate modeling of the effects of solar and infrared radiation on natural systems. Radiative Transfer in the Atmosphere and Ocean includes a unified treatment of radiation within both the atmosphere and ocean, boundary properties (such as reflectionand absorptance of solid surfaces), heuristic models (Lorentzatom, two-level atom, rotating vibrator), and extensive use of two-stream and approximate methods. State of the-art computational methods are illustrated by a thorough treatment of the discrete-ordinates technique and the correlated-k band absorption method. Exercises and problem sets provide practice in both formulation and solution techniques. Applications to the subjects of solar UV penetration of the atmosphere / ocean system and the greenhause effect serve to illustrate the use of such techniques in modern research. This self-contained, systematic treatment will prepare the student in solving radiative transfer problems across a broad range of subjects.
    Type of Medium: Monograph available for loan
    Pages: XXVI, 517 S. : graph. Darst.
    Edition: 1. publ.
    ISBN: 0521401240
    Series Statement: Cambridge atmospheric and space science series
    Branch Library: AWI Library
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Analytical chemistry 47 (1975), S. 2357-2360 
    ISSN: 1520-6882
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 3
    ISSN: 1420-9136
    Keywords: Solar Mesosphere Explorer ; Ozone ; Water vapor ; Solar ultraviolet monitor ; Limb radiance
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract The 1981–82 Solar Mesosphere Explorer (SME) mission is described. The SME experiment will provide a comprehensive study of mesospheric ozone and the processes which form and destroy it. Five instruments will be carried on the spinning spacecraft to measure the ozone density and its altitude distribution from 30 to 80 km, monitor the incoming solar ultraviolet radiation, and measure other atmospheric constituent which affect ozone. The polar-orbiting spacecraft will be placed into a 3pm-3 am Sun-synchronous orbit. The atmospheric measurements will scan the Earth's limb and measure: (1) the mesospheric and stratospheric ozone density distribution by inversion of Rayleigh-scattered ultraviolet limb radiance, and the thermal emission from ozone at 9.6 μm; (2) the water vapor density distribution by inversion of thermal emission at 6.3 μm; (3) the ozone photolysis rate by inversion of the O2(1Δg) 1.27 μm limb radiance; (4) the temperature profile by a combination of narrow-band and wide-band measurements of the 15 μm thermal emission by CO2; and, (5) theNO2 density distribution by inversion of Rayleighscattered limb radiance at 0.439 μm. The solar ultraviolet monitor will measure both the 0.2–0.31 μm spectral region and the Lyman-alpha (0.1216 μm) contribution to the solar irradiance. This combination of measurements will provide a rigorous test of the photochemical equilibrium theory of the mesospheric oxygen-hydrogen system, will determine what changes occur in the ozone distribution as a result of changes in the incoming solar radiation, and will detect changes that may occur as a result of meteorological disturbances.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 3 (1996), S. 771-780 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The modal structure for linearized waves in a magnetron or a crossed-field amplifier (CFA) is shown to be very sensitive to the profile of the electron density at the edge of the electron sheath. As is well known, with the classical Brillouin density profile, no propagating diocotron mode can exist. Furthermore, in the parameter regime at which these devices operate (ω=kvd where ω is the frequency, k is the wave vector and vd is the drift velocity at the top of the sheath), there are no unstable modes. However if we replace the Brillouin density profile with a "ramped'' density profile (where the discontinuity is replaced by a finite, but large, negative density gradient), then we can show that any mode in the operating regime will become weakly unstable. However these weakly unstable modes in the presence of the strong density gradient at the edge of the ramped density profile combine to generate a quasilinear diffusion of order unity. Thus, after a time on the order of a few cyclotron periods, the original density profile will become modified. This modification is expected to generate a plateau on the edge of the sheath at which time a resonant propagating diocotron mode can exist. Implications of these results and their predictions for magnetron and CFA operation are discussed. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 4 (1992), S. 2640-2644 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The linearized Vlasov–Poisson equations are obtained for the planar magnetron in the form ∂2yφˆ1+(V−k2)φˆ1=0, where V∝(∂yn0)Z(ζ), (∂yn0) is the density gradient and Z(ζ) is usual plasma dispersion function. The form for ζ, the ratio of the shifted phase velocity to the thermal velocity, is very strongly density dependent. One may understand this by considering the thermal velocity to be density dependent. In the interior of the sheath, the wave–particle resonance is very broad, corresponding to a high effective temperature. Just outside the sheath, this effective temperature drops to very low values (proportional to the electron density), leaving very narrow wave–particle resonances. The cold-fluid limit of this equation is also obtained.
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  • 6
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A method is presented for the linear stability analysis of the Vlasov–Poisson equations in high density, finite temperature plasmas in the presence of inhomogeneous crossed fields and density gradients. The method is more general than earlier studies of high-β inhomogeneous plasmas in that various approximations employed therein such as the local approximation (JWKB), low-frequency, or small wavelength restrictions are not employed here. Although only the nonrelativistic electrostatic planar case is treated, the method, with due modification, could be extended into the relativistic electromagnetic regime. The method uses a singular perturbation expansion to construct the unperturbed single particle orbits. Then with these orbits the "integration over the unperturbed orbits'' necessary for determining the perturbed distribution function is performed. The initial distribution function may be quite general, but the expansions used do assume a distribution close to that of a sheared laminar flow. The perturbed distribution function is obtained as a singular perturbation expansion also. Lastly, the application of the method is demonstrated by reducing the linearized Vlasov–Poisson equations, with inhomogeneous electric fields and density gradients, to a second-order ordinary differential equation where the frequency is an eigenvalue. Similarities to and differences from the cold-fluid equations are pointed out.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 31 (1988), S. 2362-2365 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The distribution function f=N exp[−βyw−(βx−βy)p2 x/(2m) −(βz−βy)p2z/(2m)], where w is the single-particle energy, px is the single-particle canonical momentum parallel to the cathode and perpendicular to the magnetic field, and pz is the single-particle canonical momentum parallel to the magnetic field, has been proposed as a model of the distribution of electrons in a planar magnetron [Phys. Fluids 29, 1746 (1986)]. The scalings of this model and the resulting density of electrons are determined by means of a singular perturbation expansion, carried out to second order.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 71 (1992), S. 5752-5759 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Studies of the nonlinear evolution of the electron-density profile in crossed-field devices indicate the classical Brillouin profile to be inadequate for the explanation of the operation of such devices. Instead, the existence of a density plateau at the edge of the electron sheath is found to be essential in the operation of such a device. Such a plateau placed at the edge of a classical Brillouin profile creates a double-box profile. The operational theory for crossed-field devices based on this double-box density profile is presented. It is shown that this profile generates an operating voltage range that agrees quite well with the actual voltage operating range of such devices, except for high magnetic fields.
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  • 9
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] The hypothesis that upper atmospheric water vapour is increasing because of increases in methane is testable by the consequent effect on noctilucent-cloud (NLC) brightness, which has been recorded for over a century. Our model5 of NLC ice-particle formation and growth shows quantitatively that ...
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  • 10
    Publication Date: 1982-11-01
    Print ISSN: 0021-8979
    Electronic ISSN: 1089-7550
    Topics: Physics
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