7,149 research outputs found
Numerical analysis of transient combustion response to acoustic oscillations in axisymmetric rocket motors
A numerical analysis of unsteady motions in solid
rocket motors with a nozzle has been conducted. The
formulation treats the complete conservation equations
for the gas phase and the one-dimensional equations in
the radial direction for the condensed phase. A fully
coupled implicit scheme based on a dual time-stepping
integration algorithm has been adopted to solve the governing equations and associated boundary conditions.
After obtaining a steady state solution, periodic pressure
oscillations are imposed at the head end to simulate acoustic oscillations of a traveling-wave motion in
the combustion chamber. The amplitude of the pressure
oscillation is 1.0 % of the mean pressure and the
frequency is 1790 Hz, corresponding to the twice of the
fundamental frequency of the chamber. Magnitude and
phase of pressure and axial velocity fluctuations are influenced by the upstream reflecting wave from the nozzle
wall. Axial velocity near surface region oscillates
in phase advance manner with reference to the acoustic
pressure. Large vorticity fluctuations are observed in
near surface region. The mass-flow-rate at the nozzle
exit periodically oscillates with a time delay compared
to the imposed pressure oscillations at the head end
Applications of Various Methods of Analysis to Combustion Instabilities in Solid Propellant Rockets
Instabilities of motions in a combustion chamber are consequences of the coupled dynamics of
combustion processes and of the flow in the chamber. The extreme complexities of the problem
always require approximations of various sorts to make progress in understanding the
mechanisms and behavior of combustion instabilities. This paper covers recent progress in the
subject, mainly summarizing efforts in two areas: approximate analysis based on a form of
Galerkin's method, particularly useful for understanding the global linear and nonlinear
dynamics of combustion instabilities and numerical simulations intended to accommodate as
fully as possible fundamental chemical processes in both the condensed and gaseous phases.
One purpose of current work is to bring closer together these approaches to produce more
comprehensive and detailed realistic results applicable to the interpretation of observations
and for design of new rockets for both space and military applications. Particularly important
are the goals of determining the connections between chemical composition and instabilities;
and the influences of geometry on nonlinear behavior
Transient combustion responses of homogeneous propellants to acoustic oscillations in axisymmetric rocket motors
A numerical analysis of unsteady motions in solid
rocket motors has been conducted. The formulation
considers a 2-D axisymmetric combustion chamber and
a choke nozzle, and treats the complete conservation
equations accounting for turbulence closure and finiterate
chemical kinetics in the gas phase and subsurface reactions.
A fully coupled implicit scheme based on a dual
time-stepping integration algorithm has been adopted
to solve the governing equations and associated boundary
conditions. Results of the steady-state calculations
indicate that the distributions of pressure in the motor
and Mach number in the nozzle are one-dimensional
along the axial direction. Vorticity contours show similar
pattern to those of Mach number in the combustion
chamber. The nozzle has an influence on the flow and
temperature fields in the combustion chamber. A narrow
pressure pulse is imposed at the head end to simulate
unsteady acoustic oscillations in the combustion
chamber. When the front of the pulse reaches near the
nozzle throat, pressure near the nozzle throat increases
and blocks the hot gas flow from passing through the
nozzle throat. Self-generated oscillations have similar
frequencies to those of standing waves of the combustion
chamber. Large vorticity fluctuations are observed
in near surface region. The luminous flame zone responds
to low-frequency pressure wave rather than highfrequency
one. Temperature fluctuations in the primary
flame zone of the head end oscillates independently of
the imposed pressure oscillations while temperature fluctuations
in downstream region show pressure-dependent
oscillations
Numerical study of acoustic oscillations and combustion instabilities in solid propellant rocket
A numerical analysis of unsteady motions in solid rocket motors has been conducted. A fully coupled
implicit scheme based on a dual time-stepping integration algorithm has been adopted to solve the governing
equations and associated boundary conditions. A narrow pressure pulse is imposed at the head end to
simulate unsteady acoustic oscillations in the combustion chamber. Pressure increases when the front of the
pulse reaches near the nozzle area. Self-generated oscillations with frequency of standing wave propagates
upstream in the combustion chamber. Investigation of transient response of gas-phase dynamics to traveling
pressure wave and its effects on propellant combustion reveals several aspects: Combustion responses have
a strong relationship with vorticity fluctuations in case of high turbulent intensity on the propellant surface.
Temperature fluctuations of the propellant surface in the head end region seem to be very unstable and
independent of the pressure wave. Surface temperature without turbulence effect looks more sensitive to
temperature fluctuations in the primary flame zone. Stability of surface temperature is strongly related to
turbulent intensity on the propellant surface
Cloning and expression pattern of bovine adipogenin isoform
The fauna and distribution of chironomid midges in Ueda City were investigated based on the collections of adults attracted to automatic vending machines at 108 stations in the summer and at 103 stations in the fall of 1997. A total of 3,371 chironomid midges, 1,346 males and 2,025 females, was collected from the stations in both seasons. All of these chironomid midges were classified into 97 species belonging to four subfamilies, i. e., 61 species of Chironominae, one species of Diamesinae, 29 species of Orthocladiinae and six species of Tanypodinae. The most abundant species was Polypedilum nubifer (Skuze), which was collected at 60 stations, followed by Chironomus kiiensis Tokunaga (53 stations), Cricotopus triannulatus (Macquart) (52 stations) and Cryptochironomus albofasciatus (Staeger) (50 stations) in summer. On the other hand, in fall, the most abundant species was Smittia aterrima (Meigen), which was collected at 75 stations, followed by P. convictum (Walker) (52 stations). The collected chironomid midges reflected the environmental condition of the collection site. Thus, the number of species collected in summer was larger than that in fall, and the respective number of terrestrial species was increased in fall. In addition, the fauna of chironomid midges and their distribution patterns in Ueda City changed during both seasons.ArticleJOURNAL OF ANIMAL SCIENCE. 85(Suppl.1): 295-295 (2007)journal articl
Electronic Structure of Electron-doped Sm1.86Ce0.14CuO4: Strong `Pseudo-Gap' Effects, Nodeless Gap and Signatures of Short Range Order
Angle resolved photoemission (ARPES) data from the electron doped cuprate
superconductor SmCeCuO shows a much stronger pseudo-gap
or "hot-spot" effect than that observed in other optimally doped -type
cuprates. Importantly, these effects are strong enough to drive the
zone-diagonal states below the chemical potential, implying that d-wave
superconductivity in this compound would be of a novel "nodeless" gap variety.
The gross features of the Fermi surface topology and low energy electronic
structure are found to be well described by reconstruction of bands by a
order. Comparison of the ARPES and optical data from
the sample shows that the pseudo-gap energy observed in optical data is
consistent with the inter-band transition energy of the model, allowing us to
have a unified picture of pseudo-gap effects. However, the high energy
electronic structure is found to be inconsistent with such a scenario. We show
that a number of these model inconsistencies can be resolved by considering a
short range ordering or inhomogeneous state.Comment: 5 pages, 4 figure
Properties of the symplectic structure of General Relativity for spatially bounded spacetime regions
We continue a previous analysis of the covariant Hamiltonian symplectic
structure of General Relativity for spatially bounded regions of spacetime. To
allow for near complete generality, the Hamiltonian is formulated using any
fixed hypersurface, with a boundary given by a closed spacelike 2-surface. A
main result is that we obtain Hamiltonians associated to Dirichlet and Neumann
boundary conditions on the gravitational field coupled to matter sources, in
particular a Klein-Gordon field, an electromagnetic field, and a set of
Yang-Mills-Higgs fields. The Hamiltonians are given by a covariant form of the
Arnowitt-Deser-Misner Hamiltonian modified by a surface integral term that
depends on the particular boundary conditions. The general form of this surface
integral involves an underlying ``energy-momentum'' vector in the spacetime
tangent space at the spatial boundary 2-surface. We give examples of the
resulting Dirichlet and Neumann vectors for topologically spherical 2-surfaces
in Minkowski spacetime, spherically symmetric spacetimes, and stationary
axisymmetric spacetimes. Moreover, we show the relation between these vectors
and the ADM energy-momentum vector for a 2-surface taken in a limit to be
spatial infinity in asymptotically flat spacetimes. We also discuss the
geometrical properties of the Dirichlet and Neumann vectors and obtain several
striking results relating these vectors to the mean curvature and normal
curvature connection of the 2-surface. Most significantly, the part of the
Dirichlet vector normal to the 2-surface depends only the spacetime metric at
this surface and thereby defines a geometrical normal vector field on the
2-surface. Properties and examples of this normal vector are discussed.Comment: 46 pages; minor errata corrected in Eqs. (3.15), (3.24), (4.37) and
in discussion of examples in sections IV B,
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