20,044 research outputs found

    The Use of a Logarithmic Amplifier in Data Processing of Analog Signals

    Get PDF
    Logarithmic amplifier used in data processing of analog signal

    Circuit breaker utilizing magnetic latching relays Patent

    Get PDF
    Relay circuit breaker with magnetic latching to provide conductive and nonconductive paths for current device

    Numerical solutions of free-molecule flow in converging and diverging tubes and slots

    Get PDF
    Numerical solutions of free molecular flow in converging and diverging tubes and slot

    Condensation on spacecraft surfaces downstream of a Kaufman thruster

    Get PDF
    Thruster exhaust products condensation on surfaces downstream of mercury electron bombardment ion thruste

    HEAT TRANSFER WITH LAMINAR FLOW IN CONCENTRIC ANNULI WITH CONSTANT AND VARIABLE WALL TEMPERATURE AND HEAT FLUX

    Get PDF
    Heat transfer with laminar flow in concentric annuli with constant and variable wall temperature and heat flu

    Mixing of a passive scalar in isotropic and sheared homogeneous turbulence

    Get PDF
    In order to calculate the velocity and scalar fields, the three dimensional, time-dependent equations of motion and the diffusion equation were solved numerically. The following cases were treated: isotropic, homogeneous turbulence with decay of a passive scalar; and homogeneous turbulent shear flow with a passive scalar whose mean varies linearly in the spanwise direction. The solutions were obtained at relatively low Reynolds numbers so that all of the turbulent scales could be resolved without modeling. Turbulent statistics such as integral length scales, Taylor microscales, Kolmogorov length scale, one- and two-point correlations of velocity-velocity and velocity-scalar, turbulent Prandtl/Schmidt number, r.m.s. values of velocities, the scalar quantity and pressure, skewness, decay rates, and decay exponents were calculated. The results are compared with the available expermental results, and good agreement is obtained

    Evolution of Cooperative Thought, Theory, and Purpose

    Get PDF
    The evolution of agricultural cooperative thought, theory, and purpose in the United States is reviewed from the standpoint of the reemergence of interest in how cooperatives can provide some of the security and benefits that might be lost with gradual phasing out of federal government farm support programs. By accomplishing group action for self-help, the early development of cooperatives drew considerable attention from economists, social theorists, and politicians. Alternative schools of cooperative thought developed, but most proponents of cooperatives regarded them as having enormous potential to provide a public service role in building a more economically stable and democratic society This paper also surveys how cooperative theory was developed more rigorously in the post-WWII period. It has provided better analytical tools for understanding how and why cooperatives have changed in response to technological and economic developments, as well as to social trends, like individualism. Given the new perspectives on cooperative theory and the scope of changes in how cooperatives operate and are structured, cooperatives have even greater potential for coordinating self-help actions, but this potential needs the support of cooperative education services.Agribusiness,

    Letter from E. W. Reynolds to John Henry Jenks; September 2, 1863

    Get PDF
    A reproduction of the original and typed transcription of a letter from E. W. Reynolds Jenks to John Henry Jenks, written on September 2, 1863, from Swanzey, New Hampshire, during John Henry Jenks\u27 Civil War service with the 14th New Hampshire Volunteer Infantry

    A computer operated mass spectrometer system

    Get PDF
    Digital computer system for processing mass spectrometer output dat

    Scalar entrainment in the mixing layer

    Get PDF
    New definitions of entrainment and mixing based on the passive scalar field in the plane mixing layer are proposed. The definitions distinguish clearly between three fluid states: (1) unmixed fluid, (2) fluid engulfed in the mixing layer, trapped between two scalar contours, and (3) mixed fluid. The difference betwen (2) and (3) is the amount of fluid which has been engulfed during the pairing process, but has not yet mixed. Trends are identified from direct numerical simulations and extensions to high Reynolds number mixing layers are made in terms of the Broadwell-Breidenthal mixing model. In the limit of high Peclet number (Pe = ReSc) it is speculated that engulfed fluid rises in steps associated with pairings, introducing unmixed fluid into the large scale structures, where it is eventually mixed at the Kolmogorov scale. From this viewpoint, pairing is a prerequisite for mixing in the turbulent plane mixing layer
    corecore