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Additional resources for The MACD Profit Alert
For the modelling of surrounding air in the numerical part of this study, the ideal gas equation of state was used. e. with the fit parameter P ∞ = 0 . e. γ = c p ⁄ c v = Γ + 1 . The quantities c p and c v represent the specific heats at constant pressure and volume, respectively. For some materials, P ∞ can be quite large; examples are water and metals, for which P ∞ is of the order of megabars. 4) Here, we substituted the specific internal energy e from Eq. 2) into Eq. 3). 13 ⋅ 10 Pa . Principal Hugoniot for the Stiffened Gas EOS The locus of possible final states due to the shock compression for a fluid initially at normal density, pressure and zero mass velocity will be referred to as principal Hugoniot.
A water droplet of radius of 100µm collides with an impact velocity of 500 m/s with a flat substrate. Due to the very small time scales ( 10 – 14 – 10 – 11 s , obtained according to CFL condition) and high velocities at which the emerging waves propagate, the first issue that should be addressed is weather the present resolution (up to 4 million grid points) can realistically capture the phenomena. Thus, as a first step, we investigate the grid independence and convergence of the solution. 1 Solution Convergence & Grid Independence The grid independence of the results has been established by both one- and two-dimensional capturing of the accurate shock position and shape.
Mathematical Model & Computational Methodology Fig. 2. Droplet and air density distribution prior to the impact: Emergence and reflection of the bow shock in the air and weak perturbations in the liquid bulk (due to the liquid-air interactions on a droplet surface). Parameters: Impact velocity 500 m/s, motionless air. [numerical result with non-linear colour map (HDF)]. 3 Numerical Modelling The code FronTier, used for the current simulations was developed by a group of researchers at the New York University and the University of Stony Brook -.