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For most of this book we have treated collisionless shocks as planar infinitely extended discontinuities with upstream plasma parameters characteristic for the solar wind, possibly corrugated by instabilities. However, all shocks in the solar system are curved and consequently the angles θBn, between the magnetic field and shock normal, and θVn, between the upstream plasma flow and shock normal, change along the shock surface. Ions backstreaming from a certain part of a shock can excite upstream waves which can be convected into other parts of the shock, where they may influence the shock structure. This is of particular importance for planetary bow shocks, where the region upstream of the quasi-perpendicular part of the shock can interact further downstream with the quasi-parallel part of the shock. In addition, the decrease in θVn, toward the flanks results in considerable variation of the shock strength along the bow shock. In Section 9.2 we will discuss results on global bow shock simulations and, in Section 9.3, the influence of bow shock curvature on upstream escaping electrons.
In Chapter 6 it was described how particles can be accelerated to very high energies by the converging flows in shocks. The maximum energy is ultimately only limited by the finite spatial extent of the shock or by the maximum time available for the diffusive shock acceleration mechanism to work. The pressure in the accelerated particles in the upstream region can become very high and can even exceed the thermal particle pressure. This will lead to considerable modification of the shock structure. Although probably not important for shocks in the solar system, we will briefly outline in Section 9.4 the methods which have been used in order to treat shocks mediated by energetic particles which have, in turn, been produced by these shocks. As stated before, we are not so much concerned with the energetic particles (cosmic rays), but with the influence these may have on the shock structure.
Before reaching the heliopause where the solar wind pressure is balanced by the pressure of the local interstellar medium, the solar wind is slowed from a super-fast mode speed flow to a sub-fast mode speed flow at the heliospheric termination shock. The structure of the heliospheric termination shock might not be expected to be so different from other shocks in the solar system, if the upstream medium were much like the solar wind in the inner heliosphere. But the solar wind in the region of the termination shock carries with it a high percentage of pickup protons.
The accumulation of observations of the quasi-perpendicular, high Mach number terrestrial bow shock has led to a consensus view that the main features of shock heating can be explained by a time-stationary macroscopic model for the shock fields: specular reflection of some fraction of the ions produces the bulk of the heating required by the shock jump conditions, and the macroscopic profile of electric and magnetic field adjusts to provide the required reflected fraction; the electron heating is mediated by the cross-shock electric potential in the de Hoffmann–Teller frame. However, as discussed in Chapter 3, although the emphasis is on the macroscopic fields, small-scale fluctuations are vital for a convincing and self-consistent shock model, even on a conceptual basis. Wave–particle coupling in turbulent fluctuations is required to explain ion isotropization, the infilling of the electron distribution function, and, perhaps most importantly, time irreversibility and entropy increase at the shock, all of which a static macrostructure is incapable of providing.
In this chapter we discuss the various sources of microstructure at the quasi-perpendicular shock, concentrating on the high Mach number regime. Of course, there is a certain degree of arbitrariness in the distinction between macro-and microstructure. At one extreme one could assign the heating and dissipation at the shock entirely to the effects of inhomogeneous fluctuations, and then the macro-scopic structure would take whatever form was dictated by a particular choice of spatial and temporal averages. However, the usual approach is to assume that there exists a well-defined underlying macrostructure, which can be related to a multi-fluid model of reflected and transmitted ions, producing the canonical foot–ramp–overshoot structure in the magnetic field. Once the macroscopic structure has been removed, the ensemble of plasma and field fluctuations which remains can give rise to anomalous dissipation and particle heating, acceleration of particles, shock ramp broadening and temporal/spatial changes of the shock structure.
Surveying the data from an Earth-orbiting spacecraft the differences between crossings of the quasi-parallel and quasi-perpendicular bow shock are usually easy to distinguish by their characteristic appearance in the magnetic field. Compared with the extended, turbulent transition of the quasi-parallel shock, the abrupt transition of the quasi-perpendicular shock resembles the idealized MHD shock discontinuity. The apparent simplicity of the quasi-perpendicular shock has produced a large body of observational work, which has focused on the average time-steady structure of the shock transition – the macrostructure of the shock. For most solar wind conditions the Mach number at the Earth's bow shock (and similarly for other solar system shocks) is strong enough to be greater than the critical Mach number found in MHD when resistivity is the dominant dissipation mechanism (see Section 2.4). At such supercritical shocks it is found that ion reflection is a characteristic feature, even though it is a consequence of the kinetics of particles in the shock fields. In this chapter we describe the macrostructure of supercritical quasi-perpendicular shocks, as found at the Earth's bow shock. This is by no means the complete picture, since, as well as the macrostructure, fluctuations are also present across the entire range of plasma time scales, from below the ion cyclotron frequency to above the electron plasma frequency. In Chapter 4 we discuss the microstructure of the quasi-perpendicular shock and its various causes.
The bow shock is observed when it passes over a spacecraft, since the spacecraft motion is generally much slower than that of the bow shock, in the Earth frame. The bow shock position varies in response to changes in the solar wind, and moves with a velocity up to several tens of kilometres per second, both outwards from the Earth and inwards towards the Earth. In a time series of data the bow shock is seen either as a transition from solar wind to magnetosheath (‘inward’ crossing) or from magnetosheath to solar wind (‘outward’ crossing). The quasi-perpendicular shock is characterized as ‘abrupt’, but what is actually observed in the time series will depend on the physical size of the transition, the sample cadence or averaging (i.e, the time resolution) of the data, and the bow shock speed relative to the spacecraft.
A shock is an abrupt transition between supersonic and subsonic flows. The best-known example is that formed by an obstacle, such as an aircraft, travelling through air faster than the speed of sound. For the aircraft to move forward the air ahead of it must be diverted around it, and there has to be a layer of subsonic flow adjacent to the obstacle. If this were not the case the influence of the pressure force, which propagates away from the obstacle at the sound speed, would be swept downstream and could not affect the flow ahead of the obstacle. Relative to the obstacle the distant flow is supersonic, so there has to be a transition to the subsonic flow close to the obstacle.
Considering such transitions within the framework of gas dynamics leads to the study of discontinuous, or near-discontinuous, solutions which must satisfy governing equations such as conservation of mass, momentum and energy. These solutions represent abrupt, well-defined changes in flow state, with so called ‘jumpconditions’ which describe the supersonic to subsonic transition. Two defining qualities can be extracted from this framework. Firstly, at a shock the flow speed changes, but also the temperature increases due to dissipation, so that the shock mediates a transfer of bulk kinetic energy in the upstream flow into thermal energy downstream. The presence of dissipation means that the change of state at a shock corresponds to an entropy increase, and it is irreversible. Secondly, by their nature,shock solutions are fundamentally nonlinear, since not only do they accomplish achange of state, but they can also be thought of as a ‘wave’ whose propagation speed is determined by the supersonic flow speed, i.e., faster than any small-amplitude linear wave. It is nonlinearity which leads to wave steepening at the shock, and the importance of discontinuous solutions.
Shocks have been explored in laboratory plasmas since the 1950s, but the discovery of shocks in interplanetary space, and the confirmation that they are relatively stable structures, has been one of the major advances of space physics. Neverthe-less, the study of shocks in plasmas which are essentially collisionless poses some fundamental problems.
We present the first analysis of spectroscopic and photometric observations of the two southern eclipsing binary stars, V349 Ara and V4403 Sgr. Radial velocity curves of these two systems obtained at the South African Astronomical Observatory and their V light curves from the All Sky Automated Survey were solved simultaneously using the Wilson–Devinney code. Our photometric models describe these two systems as Algol-like binary stars with detached configurations. The masses and radii were found to be 2.59 ± 0.07 M⊙, 3.60 ± 0.07 R⊙ and 2.51 ± 0.06 M⊙, 4.15 ± 0.07 R⊙ for the primary and secondary components of V349 Ara, respectively. Those of V4403 Sgr were derived to be 1.33 ± 0.02 M⊙, 1.74 ± 0.02 R⊙ and 1.59 ± 0.03 M⊙, 2.50 ± 0.03 R⊙ for the primary and secondary components, respectively. The distances to V349 Ara and V4403 Sgr were computed to be 677 ± 36 and 199 ± 10 pc from the dynamic parallax, respectively, taking into account interstellar extinction. The evolution cases of these two systems are also examined. Both components of these two systems are evolved main-sequence stars, and the dynamic ages were estimated as approximately 0.67 and 2.29 Gyr for V349 Ara and V4403 Sgr, respectively, when compared to Geneva theoretical evolution models.
The Lyman alpha emission line (Lyα) of neutral hydrogen (Hi) is intrinsically the brightest emission feature in the spectrum of astrophysical nebulae, making it a very attractive observational feature with which to survey galaxies. Moreover as an ultraviolet resonance line, Lyα possesses several unique characteristics that make it useful to study the properties of the interstellar medium and ionising stellar population at all cosmic epochs. In this review, I present a summary of Lyα observations of galaxies in the nearby universe. By ultraviolet continuum selection, at the magnitudes reachable with current facilities, only ≈ 5% of the local galaxy population shows a Lyα equivalent width (WLyα) that exceeds 20 Å. This fraction increases dramatically at higher redshifts, but only in the local universe can we study galaxies in detail and assemble unprecedented multi-wavelength datasets. I discuss many local Lyα observations, showing that when galaxies show net Lyα emission, they ubiquitously also produce large-scale halos of scattered Lyα, that dominate the integrated luminosity. Concerning global measurements, we discuss how WLyα and the Lyα escape fraction (fLyαesc) are higher (WLyα ≳ 20 Å and fLyαesc ≳ 10%) in galaxies that represent the less massive and younger end of the distribution for local objects. This is connected with various properties, such that Lyα-emitting galaxies have lower metal abundances (median value of 12 + log(O/H) ~ 8.1) and dust reddening. However, the presence of galactic outflows/winds is also vital to Doppler shift the Lyα line out of resonance with the atomic gas, and high WLyα is found only among galaxies with winds faster than ~ 50 km s−1. The empirical evidence is then assembled into a coherent picture, and the requirement for star-formation-driven feedback is discussed in the context of an evolutionary sequence where the interstellar medium is accelerated and/or subject to hydrodynamical instabilities, which reduce the scattering of Lyα. Concluding remarks take the form of perspectives upon future developments, and the most pressing questions that can be answered by observation.
In the original publication of “Image Simulation for Mingantu Ultrawide Spectral Radioheliograph in the Decimetre Wave Range,” by Jing Du, Yihua Yan, Wei Wang, and Donghao Liu, there were concerns regarding ambiguity of a few statements. To clarify, the authors have submitted an update regarding Table 6 (p. 12) and the supporting language (p. 13):
GLEAM, the GaLactic and Extragalactic All-sky MWA survey, is a survey of the entire radio sky south of declination + 25° at frequencies between 72 and 231 MHz, made with the MWA using a drift scan method that makes efficient use of the MWA’s very large field-of-view. We present the observation details, imaging strategies, and theoretical sensitivity for GLEAM. The survey ran for two years, the first year using 40-kHz frequency resolution and 0.5-s time resolution; the second year using 10-kHz frequency resolution and 2 s time resolution. The resulting image resolution and sensitivity depends on observing frequency, sky pointing, and image weighting scheme. At 154 MHz, the image resolution is approximately 2.5 × 2.2/cos (δ + 26.7°) arcmin with sensitivity to structures up to ~ 10° in angular size. We provide tables to calculate the expected thermal noise for GLEAM mosaics depending on pointing and frequency and discuss limitations to achieving theoretical noise in Stokes I images. We discuss challenges, and their solutions, that arise for GLEAM including ionospheric effects on source positions and linearly polarised emission, and the instrumental polarisation effects inherent to the MWA’s primary beam.
We present a complete spatial and dynamical study of the poorly populated stellar system ESO65SC03. The radial distribution of the system gives a core and cluster radii of 1.10±0.63 and 5.36±0.24 arcmin, respectively. The SNDP does not show any clear enhancement of the surface stellar number density between the stars of the system and the field regions. We derive the optimum isochrone solution for a particular grid size in the CMD using the statistical cleaning procedure. Using the statistically cleaned CMDs, we find the distance modulus, (m − M)0, and reddening, E(B − V), of the system to be 11.8±0.2 and 0.45 mag, respectively. The mean proper motion of this system is − 5.37±0.81 mas yr−1 and 0.31±0.40 in RA and DEC directions, respectively. The mean proper motion of this system is found to be almost similar to the field region. The mass function for the brighter stars is found to be too high for the system to be an open cluster. These combined results place constraints on whether stellar system ESO65SC03 is a POCR or an Asterism. Our understanding is that the ESO65SC03 is in a stage of POCR by losing their main-sequence stars in the dynamic evolution processes.
We carried out light curve solutions of ten detached eclipsing eccentric binaries observed by Kepler. The formal errors of the derived parameters from the light curve solutions are below 1%. Our results give indications that the components of the eccentric binaries (especially those with mass ratios below 0.5) do not follow precisely the empirical relations between the stellar parameters derived from the study of circular-orbit binaries. We found the following peculiarities of the targets: (a) the components of KIC 9474969 have almost the same temperatures while their radii and masses differ by a factor around 2.5; (b) KIC 6949550 reveals semi-regular light variations with an amplitude of 0.004 and a period around 7 d which are modulated by long-term variations; (c) KIC 6220470, KIC 11071207, and KIC 9474969 exhibit tidally induced ‘hump’ around the periastron. These are the targets with the biggest relative radii of our sample. We derived the dependence of the hump amplitude on the relative stellar radii, eccentricity, and mass ratio of eccentric binary consisting of MS stars.
The MUSER is a solar-dedicated radio interferometric array, which will observe the Sun over a wide range of radio frequencies (0.4–15 GHz), and make high time, space and frequency resolution images of the Sun simultaneously. MUSER is located in Mingantu Station in Inner Mongolia of China, which is about 400 kilometres away from Beijing. MUSER consists of two arrays: MUSER-I and MUSER-II. MUSER-I contains 40 antennas with 4.5-m aperture operating at 400 MHz to 2 GHz. MUSER-II contains 60 antennas with 2-m aperture operating at 2 to 15 GHz. Currently, MUSER has already been established and entered into the stage of test observation. This work is focus on the imaging performance of MUSER-I. This paper introduces MUSER-I briefly, presents the analysis of the array configurations, and evaluates the image quality mainly using the dynamic range, fidelity index, and the peak signal-to-noise ratio, also make some actual solar model simulations with CASA, the results will be shown below.
Results from long-term multicolour optical photometric observations of the pre-main-sequence stars FHO 26, FHO 27, FHO 28, FHO 29, and V1929 Cyg collected during the period from 1997 June to 2014 December are presented. The objects are located in the dense molecular cloud L935, named ‘Gulf of Mexico’, in the field between the North America and Pelican nebulae. All stars from our study exhibit strong photometric variability in all optical passbands. Using our BVRI observations and data published by other authors, we tried to define the reasons for the observed brightness variations. The presented paper is a part of our long-term photometric study of the young stellar objects in the region of ‘Gulf of Mexico’.
We present observations of the first 10° of longitude in the Mopra CO survey of the southern Galactic plane, covering Galactic longitude l = 320–330° and latitude b = ±0.5°, and l = 327–330°, b = +0.5–1.0°. These data have been taken at 35-arcsec spatial resolution and 0.1 km s−1 spectral resolution, providing an unprecedented view of the molecular clouds and gas of the southern Galactic plane in the 109–115 GHz J = 1–0 transitions of 12CO, 13CO, C18O, and C17O. Together with information about the noise statistics from the Mopra telescope, these data can be retrieved from the Mopra CO website and the CSIRO-ATNF data archive.
Mapping the diversity of SNe to progenitor properties is key to our understanding of stellar evolution and explosive stellar death. Investigations of the immediate environments of SNe allow statistical constraints to be made on progenitor properties such as mass and metallicity. Here, we review the progress that has been made in this field. Pixel statistics using tracers of e.g. star formation within galaxies show intriguing differences in the explosion sites of, in particular SNe types II and Ibc (SNe II and SNe Ibc respectively), suggesting statistical differences in population ages. Of particular interest is that SNe Ic are significantly more associated with host galaxy Hα emission than SNe Ib, implying shorter lifetimes for the former. In addition, such studies have shown (unexpectedly) that the interacting SNe IIn do not explode in regions containing the most massive stars, which suggests that at least a significant fraction of their progenitors arise from the lower end of the core-collapse SN mass range. Host H ii region spectroscopy has been obtained for a significant number of core-collapse events, however definitive conclusions on differences between distinct SN types have to-date been elusive. Single stellar evolution models predict that the relative fraction of SNe Ibc to SNe II should increase with increasing metallicity, due to the dependence of mass-loss rates on progenitor metallicity. We present a meta-analysis of all current host H ii region oxygen abundances for CC SNe. It is concluded that the SN II to SN Ibc ratio shows little variation with oxygen abundance, with only a suggestion that the ratio increases in the lowest bin. Radial distributions of different SNe are discussed, where a central excess of SNe Ibc has been observed within disturbed galaxy systems, which is difficult to ascribe to metallicity or selection effects. Environment studies are also being undertaken for SNe Ia, where constraints can be made on the shortest delay times of progenitor systems. It is shown that ‘redder’ SNe Ia are more often found within star-forming regions. Environment studies are evolving to enable studies at higher spatial resolutions than previously possible, while in addition the advent of wide-field integral field unit instruments allows galaxy-wide spectral analyses which will provide fruitful results to this field. Some example contemporary results are shown in that direction.
We propose that observations of ‘hidden’ magnetars in central compact objects can be used to probe crustal activity of neutron stars with large internal magnetic fields. Estimates based on calculations by Perna & Pons, Pons & Rea and Kaminker et al. suggest that central compact objects, which are proposed to be ‘hidden’ magnetars, must demonstrate flux variations on the time scale of months–years. However, the most prominent candidate for the ‘hidden’ magnetars — CXO J1852.6+0040 in Kes 79 — shows constant (within error bars) flux. This can be interpreted by lower variable crustal activity than in typical magnetars. Alternatively, CXO J1852.6+0040 can be in a high state of variable activity during the whole period of observations. Then we consider the source 1E161348 − 5055 in RCW103 as another candidate. Employing a simple 2D-modelling we argue that properties of the source can be explained by the crustal activity of the magnetar type. Thus, this object may be supplemented for the three known candidates for the ‘hidden’ magnetars among central compact objects discussed in literature.
The conversion of a former 100-foot (30-m) telecommunications antenna (Earth Station) in New Zealand into a radio telescope is described. A specification of the antenna and the priorities for its actual conversion are initially presented. In describing the actual conversion, particular emphasis is given to mechanical and electrical components, as well as to the design of the telescope control system, telescope networking for VLBI operations, and telescope maintenance. Plans for RF, front- and back-end developments based upon radio astronomical priorities are outlined.