from first equation of motion, \(\begin{array}{l}average~ velocity = u ~+~ \frac{v ~-~ u}{2}\end{array} \) \(\begin{array}{l}average~ velocity = \frac{v~+~ u}{2}\end{array} \) where, v = final velocity u = initial velocity similarly, we can define average speed. ...
Equation [2] has been experimentally validated for many metals; an example of data compiled for copper is shown in Figure 1. Perhaps counter-intuitively, the nature of the dislocation distribution does not affect the general relevance of eqn [2]. For example, in some materials dislocations self...
We propose a method for analyzing the scattering of spherical waves by an arbitrarily shaped, perfectly conducting scatterer in relative motion with respect to the source and observation points. To treat this problem more rigorously, we use relativistic notation. Since the scatterer is arbitrarily shap...
In each equation, a different RF parameter can be predicted from the preferred SF, fo (cyc/°). We begin with the scale invariance constraint on RF width $$\sigma _{x,{\mathrm{si}}}(f_{\mathrm{o}}) = 1{\mathrm{/}}\alpha f_{\mathrm{o}}{\mathrm{;}}\,{\mathrm{RF}}\,{\...
Light-sheet fluorescence microscopy (LSFM) has emerged as a powerful method for rapid and optically efficient 3D microscopy. Initial LSFM designs utilized a static sheet of light, termed selective plane illumination microscopy (SPIM), which exhibited sha
13 involved the Brownian motion impact on characteristics of nanoparticles in bioconvective flow. Irfan et al.14 displayed the roles of chemical terms on transient energy equation. Ahmed et al.15 illustrated the carbon nanotubes flow between Riga sheets in existence of viscous dissipation. Kumar et...
Equation (2) is the basis of the leakage–pressure equation proposed by the International Water Association (IWA) water loss task force [8]: 𝑄=𝐶𝑃𝑁.Q=CPN. (2) 𝐶Cis the leakage coefficient;𝑃Pis the pressure inside the pipe; and𝑁Nis the leakage exponent. The relationship ...