3,379 research outputs found

    On Reflection of Shock Waves from Boundary Layers

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    Measurements of the reflection characteristics of shock waves from a flat surface with a laminar and turbulent boundary layer are presented. The investigations were carried out at Mach numbers from about 1.3 to 1.5 and a Reynolds number of 0.9 x 10^4. THe difference in the shock-wave interaction with laminar and turbulent boundary layers, first found in transonic flow is confirmed and ,investigated in detail for supersonic flow. The relative upstream influence of a shock wave impinging on a given boundary layer has been measured for both laminar and turbulent layers. The upstream influence of a shock wave in the laminar layer is found to be of the order of 50 bounday-layer thicknesses as compared with about 5 in the turbulent case. Separation almost always occurs in the laminar boundary layer. The separation is restricted to a region of finite extent upstream of the the shock wave. In the turbulent case no separation was found. A model of the flow near the point of impingement of the shock wave on the boundary layer is given for both cases. The difference between impulse-type and step-type shock waves is discussed and their interactions with the boundary layer are compared. Some general considerations on the experimental production of shock waves from wedges and cones are presented, as well as a discussion of boundary layer in supersonic flow. A few exampies of reflection of shock waves from supersonic shear layers are also presented

    Thermal equilibrium of a Brownian particle with coordinate dependent diffusion: comparison of Boltzmann and modified Boltzmann distributions with experimental results

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    In this paper we compare the Boltzmann distribution with a modified Boltzmann distribution, that results from an It\^o-process considering thermal equilibrium of a Brownian particle with coordinate dependent diffusion, in the light of an existing experiment. The experiment was reported in 1994 by Faucheux and Libchaber. The experiment made use of direct tracking of diffusion of Brownian particles near a wall. Results of this experiment allows us to compare the Boltzmann and the modified Boltzmann distribution without making use of any adjustable parameter. A comparison of these two distributions with the experimental results lends support to the consideration of thermodynamic equilibrium of a Brownian particle with coordinate-dependent diffusion to be an It\^o-process.Comment: 10 pages, 5 figure

    Limits on stable iron in Type \,Ia supernovae from NIR spectroscopy

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    We obtained optical and near-infrared spectra of Type \,Ia supernovae (SNe \,Ia) at epochs ranging from 224 to 496 days after the explosion. The spectra show emission lines from forbidden transitions of singly ionised iron and cobalt atoms. We used non-local thermodynamic equilibrium (NLTE) modelling of the first and second ionisation stages of iron, nickel, and cobalt to fit the spectra using a sampling algorithm allowing us to probe a broad parameter space. We derive velocity shifts, line widths, and abundance ratios for iron and cobalt. The measured line widths and velocity shifts of the singly ionised ions suggest a shared emitting region. Our data are fully compatible with radioactive 56^{56}Ni decay as the origin for cobalt and iron. We compare the measured abundance ratios of iron and cobalt to theoretical predictions of various SN \,Ia explosion models. These models include, in addition to 56^{56}Ni, different amounts of 57^{57}Ni and stable 54,56^{54,56}Fe. We can exclude models that produced only 54,56^{54,56}Fe or only 57^{57}Ni in addition to 56^{56}Ni. If we consider a model that has 56^{56}Ni, 57^{57}Ni, and 54,56^{54,56}Fe then our data imply that these ratios are 54,56^{54,56}Fe / 56^{56}Ni =0.272±0.086=0.272\pm0.086 and 57^{57}Ni / 56^{56}Ni =0.032±0.011=0.032\pm0.011.Comment: 10 pages, 7 figures, Accepted for publication in A&

    iPTF16abc and the population of Type Ia supernovae: Comparing the photospheric, transitional and nebular phases

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    Key information about the progenitor system and the explosion mechanism of Type Ia supernovae (SNe~Ia) can be obtained from early observations, within a few days from explosion. iPTF16abc was discovered as a young SN~Ia with excellent early time data. Here, we present photometry and spectroscopy of the SN in the nebular phase. A comparison of the early time data with a sample of SNe~Ia shows distinct features, differing from normal SNe~Ia at early phases but similar to normal SNe~Ia at a few weeks after maximum light (i.e. the transitional phase) and well into the nebular phase. The transparency timescales (t0t_0) for this sample of SNe~Ia range between ∼\sim 25 and 41 days indicating a diversity in the ejecta masses. t0t_0 also weakly correlates with the peak bolometric luminosity, consistent with the interpretation that SNe with higher ejecta masses would produce more 56^{56}Ni. Comparing the t0t_0 and the maximum luminosity, Lmax_{max}\, distribution of a sample of SNe~Ia to predictions from a wide range of explosion models we find an indication that the sub-Chandrasekhar mass models span the range of observed values. However, the bright end of the distribution can be better explained by Chandrasekhar mass delayed detonation models, hinting at multiple progenitor channels to explain the observed bolometric properties of SNe~Ia. iPTF16abc appears to be consistent with the predictions from the Mch_{ch} models.Comment: 13 pages, 8 figures, accepted for publication in MNRA

    A Distributed Greedy Algorithm for Constructing Connected Dominating Sets in Wireless Sensor Networks

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    A Connected Dominating Set (CDS) of the graph representing a Wireless Sensor Network can be used as a virtual backbone for routing in the network. Since sensor nodes are constrained by limited on-board batteries, it is desirable to have a small CDS for the network. However, constructing a minimum size CDS has been shown to be a NP-hard problem. In this paper we present a distributed greedy algorithm for constructing a CDS that we call Greedy Connect. Our algorithm operates in two phases, first constructing a dominating set and then connecting the nodes in this set. We evaluate our algorithm using simulations and compare it to the two-hop K2 algorithm in the literature. Depending on the network topology, our algorithm generally constructs a CDS that is up to 30% smaller in size than K

    A Parallax Distance to the Microquasar GRS 1915+105 and a Revised Estimate of its Black Hole Mass

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    Using the Very Long Baseline Array, we have measured a trigonometric parallax for the micro quasar GRS 1915+105, which contains a black hole and a K-giant companion. This yields a direct distance estimate of 8.6 (+2.0,-1.6) kpc and a revised estimate for the mass of the black hole of 12.4 (+2.0,-1.8) Msun. GRS 1915+105 is at about the same distance as some HII regions and water masers associated with high-mass star formation in the Sagittarius spiral arm of the Galaxy. The absolute proper motion of GRS 1915+105 is -3.19 +/- 0.03 mas/y and -6.24 +/- 0.05 mas/y toward the east and north, respectively, which corresponds to a modest peculiar speed of 22 +/-24 km/s at the parallax distance, suggesting that the binary did not receive a large velocity kick when the black hole formed. On one observational epoch, GRS 1915+105 displayed superluminal motion along the direction of its approaching jet. Considering previous observations of jet motions, the jet in GRS 1915+105 can be modeled with a jet inclination to the line of sight of 60 +/- 5 deg and a variable flow speed between 0.65c and 0.81c, which possibly indicates deceleration of the jet at distances from the black hole >2000 AU. Finally, using our measurements of distance and estimates of black hole mass and inclination, we provisionally confirm our earlier result that the black hole is spinning very rapidly.Comment: 20 pages; 2 tables; 6 figure

    Nebular spectroscopy of SN 2014J: Detection of stable nickel in near infrared spectra

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    We present near infrared (NIR) spectroscopy of the nearby supernova 2014J obtained ∼\sim450 d after explosion. We detect the [Ni II] 1.939 μ\mum line in the spectra indicating the presence of stable 58^{58}Ni in the ejecta. The stable nickel is not centrally concentrated but rather distributed as the iron. The spectra are dominated by forbidden [Fe II] and [Co II] lines. We use lines, in the NIR spectra, arising from the same upper energy levels to place constraints on the extinction from host galaxy dust. We find that that our data are in agreement with the high AVA_V and low RVR_V found in earlier studies from data near maximum light. Using a 56^{56}Ni mass prior from near maximum light γ\gamma-ray observations, we find ∼\sim0.05 M⊙_\odot of stable nickel to be present in the ejecta. We find that the iron group features are redshifted from the host galaxy rest frame by ∼\sim600 km s−1^{-1}.Comment: 6 pages, 4 figures, submitted to A&

    Potential signature of a quadrupolar Hubble expansion in Pantheon+ supernovae

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    The assumption of isotropy -- that the Universe looks the same in all directions on large scales -- is fundamental to the standard cosmological model. This model forms the building blocks of essentially all of our cosmological knowledge to date. It is therefore critical to empirically test in which regimes its core assumptions hold. Anisotropies in the cosmic expansion are expected on small scales due to nonlinear structures in the late Universe, however, the extent to which these anisotropies might impact our low-redshift observations remains to be fully tested. In this paper, we use fully general relativistic simulations to calculate the expected local anisotropic expansion and identify the dominant multipoles in cosmological parameters to be the quadrupole in the Hubble parameter and the dipole in the deceleration parameter. We constrain these multipoles simultaneously in the new Pantheon+ supernova compilation. The fiducial analysis is done in the rest frame of the CMB with peculiar velocity corrections. Under the fiducial range of redshifts in the Hubble flow sample, we find a ∼2σ\sim 2\sigma deviation from isotropy. We constrain the eigenvalues of the quadrupole in the Hubble parameter to be λ1=0.021±0.011\lambda_1 =0.021\pm{ 0.011} and λ2=3.15×10−5±0.012 {\lambda_2= 3.15\times 10^{-5}}\pm 0.012 and place a 1σ1\sigma upper limit on its amplitude of 2.88%2.88\%. We find no significant dipole in the deceleration parameter, finding constraints of qdip=4.5−5.4+1.9q_{\rm dip} = 4.5^{+1.9}_{-5.4}. However, in the rest frame of the CMB without corrections, we find qdip=9.6−6.9+4.0 q_{ \rm dip} = 9.6^{+4.0}_{-6.9}, a >2σ>2\sigma positive amplitude. We also investigate the impact of these anisotropies on the Hubble tension. We find a maximal shift of 0.300.30 km s−1^{-1} Mpc−1^{-1} in the monopole of the Hubble parameter and conclude that local anisotropies are unlikely to fully explain the observed tension.Comment: 12 pages, to be submitted to MNRA
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