More specifically, visual representations can be found for: (a) phenomena that are not observable with the eye (i.e., microscopic or macroscopic); (b) phenomena that do not exist as visual representations but can be translated as such (i.e., sound); and (c) in experimental settings to provide visual data representations (i.e., graphs presenting velocity of moving objects).
On the other hand, using the kinematic approach, we can construct models that incorporate the present velocity and geometry of specific subduction zones to compare the models with observations.
The implication of our present velocity is that we'll have arrived at a figurative 2005 by the time the teams become reacquainted in Australia later this year.
Ohmi and Lees (1995) presented velocity structures of P- and S-waves below the Unzen volcano.
Figure 4b presents velocity space distribution of ions at three locations denoted in Fig. 4a.
In this paper, we present horizontal velocities of spread F structures observed by multipoint continuous Doppler sounding over Tucumán, Northern Argentina (27°S, 65°W, inclination of magnetic field I = 27°), and over Taiwan (24°N, 121°E, inclination of magnetic field I = 35°) and we compare the values with neutral wind velocities obtained from recent experimental model HWM14 (Drob et al. 2015).
Now let's see what we can make of the present position and velocity of the top four browsers in the U.S. Apologies to Opera, but I don't know anyone who uses it, do you?
As an additional illustration of a DN explanation of a particular event, consider a derivation of the position of Mars at some future time from Newton's laws of motion, the Newtonian inverse square law governing gravity, and information about the mass of the sun, the mass of Mars and the present position and velocity of each.
Since the viscosity of the suspending polymer increases as a result of curing process, a new model is presented for settling velocity of particles, combining the Stokes' law and an appropriate rheokinetics model for reactive polymers.
In the present study, laminar burning velocity of lean hydrogen + air flames and its temperature dependence were for the first time studied in stretch-free flat flames on a heat flux burner.
For the present investigation, the drift velocity of oxygen vacancies is considered as a state variable 'w'w
