Xie-EGM-RPI-2011 - Rensselaer Hartford Campus
... ∇ · J = 0 (Kirchoff’s First Law) J = σ (E + v x B) ...
... ∇ · J = 0 (Kirchoff’s First Law) J = σ (E + v x B) ...
final1-mc-298220-publishable-summary
... Viscoelastic fluids are a class of materials that display characteristics somewhere between those of solids (elasticity) and those of liquids (viscosity). Familiar examples of such fluids include melted cheese, melted plastic, sticky glue, saliva and mucus. The stretchy and stringy properties of the ...
... Viscoelastic fluids are a class of materials that display characteristics somewhere between those of solids (elasticity) and those of liquids (viscosity). Familiar examples of such fluids include melted cheese, melted plastic, sticky glue, saliva and mucus. The stretchy and stringy properties of the ...
Vertical structure of the atmosphere
... we can use pressure as an alternative coordinate. This is a very useful alternative for treating the dynamics of large-scale atmosphere. Since pressure and height has a one-to-one correspondence, we can swap the two by considering z as a function of p, z(p), as our dynamical variable, and p itself a ...
... we can use pressure as an alternative coordinate. This is a very useful alternative for treating the dynamics of large-scale atmosphere. Since pressure and height has a one-to-one correspondence, we can swap the two by considering z as a function of p, z(p), as our dynamical variable, and p itself a ...
Bernoulli`s equation
... so that the total drag force on the sphere, due to the fluid flow around it, is zero! D’Alembert’s paradox: it can be demonstrated that the drag force on any 3-D solid body moving at uniform speed in a potential flow is zero (see, e.g., Paterson, § XI.9, p. 240). This is not true in reality of cours ...
... so that the total drag force on the sphere, due to the fluid flow around it, is zero! D’Alembert’s paradox: it can be demonstrated that the drag force on any 3-D solid body moving at uniform speed in a potential flow is zero (see, e.g., Paterson, § XI.9, p. 240). This is not true in reality of cours ...
Microsoft Word - 12.800 chapter 1,`06
... Stream, coastal upwelling, the polar stratospheric vortex, the Jet Stream can all be approached as fundamental problems in fluid mechanics. It is, as I hope to persuade you in this course, a beautiful subject dealing with compellingly beautiful physical phenomena. Even on the smallest scales accessi ...
... Stream, coastal upwelling, the polar stratospheric vortex, the Jet Stream can all be approached as fundamental problems in fluid mechanics. It is, as I hope to persuade you in this course, a beautiful subject dealing with compellingly beautiful physical phenomena. Even on the smallest scales accessi ...
Fluid thread breakup
Fluid thread breakup is the process by which a single mass of fluid breaks into several smaller fluid masses. The process is characterized by the elongation of the fluid mass forming thin, thread-like regions between larger nodules of fluid. The thread-like regions continue to thin until they break, forming individual droplets of fluid.Thread breakup occurs where two fluids or a fluid in a vacuum form a free surface with surface energy. If more surface area is present than the minimum required to contain the volume of fluid, the system has an excess of surface energy. A system not at the minimum energy state will attempt to rearrange so as to move toward the lower energy state, leading to the breakup of the fluid into smaller masses to minimize the system surface energy by reducing the surface area. The exact outcome of the thread breakup process is dependent on the surface tension, viscosity, density, and diameter of the thread undergoing breakup.