10 research outputs found
Profit-oriented disassembly-line balancing
As product and material recovery has gained importance, disassembly volumes have increased, justifying construction of disassembly lines similar to assembly lines. Recent research on disassembly lines has focused on complete disassembly. Unlike assembly, the current industry practice involves partial disassembly with profit-maximization or cost-minimization objectives. Another difference between assembly and disassembly is that disassembly involves additional precedence relations among tasks due to processing alternatives or physical restrictions. In this study, we define and solve the profit-oriented partial disassembly-line balancing problem. We first characterize different types of precedence relations in disassembly and propose a new representation scheme that encompasses all these types. We then develop the first mixed integer programming formulation for the partial disassembly-line balancing problem, which simultaneously determines (1) the parts whose demand is to be fulfilled to generate revenue, (2) the tasks that will release the selected parts under task and station costs, (3) the number of stations that will be opened, (4) the cycle time, and (5) the balance of the disassembly line, i.e. the feasible assignment of selected tasks to stations such that various types of precedence relations are satisfied. We propose a lower and upper-bounding scheme based on linear programming relaxation of the formulation. Computational results show that our approach provides near optimal solutions for small problems and is capable of solving larger problems with up to 320 disassembly tasks in reasonable time
KELT-22Ab: A Massive Hot Jupiter Transiting a Near Solar Twin
We present the discovery of KELT-22Ab, a hot Jupiter from the KELT-South
survey. KELT-22Ab transits the moderately bright () Sun-like G2V
star TYC 7518-468-1. The planet has an orbital period of days, a radius of , and a
relatively large mass of . The star has
, , K,
(cgs), and [m/H] =
, and thus, other than its slightly super-solar
metallicity, appears to be a near solar twin. Surprisingly, KELT-22A exhibits
kinematics and a Galactic orbit that are somewhat atypical for thin disk stars.
Nevertheless, the star is rotating quite rapidly for its estimated age, shows
evidence of chromospheric activity, and is somewhat metal rich. Imaging reveals
a slightly fainter companion to KELT-22A that is likely bound, with a projected
separation of 6\arcsec (1400 AU). In addition to the orbital motion
caused by the transiting planet, we detect a possible linear trend in the
radial velocity of KELT-22A suggesting the presence of another relatively
nearby body that is perhaps non-stellar. KELT-22Ab is highly irradiated (as a
consequence of the small semi-major axis of ), and is
mildly inflated. At such small separations, tidal forces become significant.
The configuration of this system is optimal for measuring the rate of tidal
dissipation within the host star. Our models predict that, due to tidal forces,
the semi-major axis of KELT-22Ab is decreasing rapidly, and is thus predicted
to spiral into the star within the next Gyr
TOI-954 b and K2-329 b: short-period Saturn-mass planets that test whether irradiation leads to inflation
We report the discovery of two short-period Saturn-mass planets, one transiting the G subgiant TOI-954 (TIC 44792534, V = 10.343, T = 9.78) observed in TESS sectors 4 and 5 and one transiting the G dwarf K2-329 (EPIC 246193072, V = 12.70, K = 10.67) observed in K2 campaigns 12 and 19. We confirm and characterize these two planets with a variety of ground-based archival and follow-up observations, including photometry, reconnaissance spectroscopy, precise radial velocity, and high-resolution imaging. Combining all available data, we find that TOI-954 b has a radius of 0.852(-0.062)(+0.053) R-J and a mass of 0.174(-0.017)(+0.018) M-J and is in a 3.68 day orbit, while K2-329 b has a radius of 0.774(-0.024)(+0.026) R-J and a mass if 0.260(-0.022)(+0.020) M-J and is in a 12.46 day orbit. As TOI-954 b is 30 times more irradiated than K2-329 b but more or less the same size, these two planets provide an opportunity to test whether irradiation leads to inflation of Saturn-mass planets and contribute to future comparative studies that explore Saturn-mass planets at contrasting points in their lifetimes
KELT-19Ab: A P ∼ 4.6-day Hot Jupiter Transiting a Likely Am Star with a Distant Stellar Companion
We present the discovery of the giant planet KELT-19Ab, which transits the moderately bright (V ∼ 9.9) A8V star TYC 764-1494-1 with an orbital period of 4.61 days. We confirm the planetary nature of the companion via a combination of radial velocities, which limit the mass to ≳4.1 MJ (3s), and a clear Doppler tomography signal, which indicates a retrograde projected spin-orbit misalignment of λ = -179.7-3.8+3.7degrees. Global modeling indicates that the Teff= 7500 ±110 K host star has M M = 1.62+0.20-0.25and R = 1.83 0.10 R. The planet has a radius of RP = 1.91 0.11 RJ and receives a stellar insolation flux of ∼ 3.2 10 erg s-1cm-2, leading to an inferred equilibrium temperature of Teq ∼ 1935 K assuming zero albedo and complete heat redistribution. With a v I sin 84.8 ±2.0 km s =-1, the host is relatively slowly rotating compared to other stars with similar effective temperatures, and it appears to be enhanced in metallic elements but deficient in calcium, suggesting that it is likely an Am star. KELT-19A would be the first detection of an Am host of a transiting planet of which we are aware. Adaptive optics observations of the system reveal the existence of a companion with late-G9V/early-K1V spectral type at a projected separation of »160 au. Radial velocity measurements indicate that this companion is bound. Most Am stars are known to have stellar companions, which are often invoked to explain the relatively slow rotation of the primary. In this case, the stellar companion is unlikely to have caused the tidal braking of the primary. However, it may have emplaced the transiting planetary companion via the Kozai-Lidov mechanism