The target of this ebook is to supply engineers and researchers the instruments useful for modelling, experimenting, and simulating those microflows as a initial step for designing and optimizing fluidic microsystems. a number of the effects of miniaturization at the hydrodynamics of fuel, liquid or two-phase flows, in addition to linked warmth move are analysed. The e-book is illustrated with examples displaying the range and the originality of fluidic microsystems.Content:
Chapter 1 creation to Microflows (pages 1–23): Stephane Colin
Chapter 2 Gaseous Microflows (pages 25–87): Jean?Claude Lengrand and Tatiana T. Elizarova
Chapter three Liquid Microflows: Particularities and Modeling (pages 89–120): Christine Barrot and Jean?Pierre Delplanque
Chapter four Physiological Microflows (pages 121–193): Jacques Dufaux, Marc Durand, Gerard Guiffant and Kristine Jurski
Chapter five Single?Phase warmth move (pages 195–234): Sedat Tardu
Chapter 6 Two?Phase Microflows (pages 235–301): Olivier Lebaigue
Chapter 7 Experimental tools (pages 303–347): Lucien Baldas and Robert Caen
Chapter eight Fluidic Microsystems (pages 349–388): Isabelle Dufour and Olivier Francais
Chapter nine Microsystems in Macroflows lively regulate (pages 389–431): Sedat Tardu
Read or Download Microfluidics PDF
Best solid-state physics books
Assuming an easy wisdom of quantum and statistical physics, this e-book offers a accomplished advisor to imperative actual homes of condensed topic, in addition to the underlying thought worthwhile for a formal knowing in their origins. the subject material covers the critical positive aspects of condensed subject physics, yet with specific accessory at the houses of steel alloys.
Drawing from the huge spectrum of phenomena, defined in additional than 100,000 articles on high-Tc superconductivity, during this e-book, the authors learn these simple homes for which realizing may be completed in the framework of conventional tools of theoretical physics. this can be the case of the overdoped cuprates for which the "Bardeen application" has been discovered: we all know their digital spectrum, we will calculate their simple thermodynamic and electrodynamic homes, and are expecting new phenomena.
Nanotubes and nanosheets are low-dimensional nanomaterials with precise houses that may be exploited for various functions. This booklet deals an entire review in their constitution, houses, improvement, modeling ways, and useful use. It focuses recognition on boron nitride (BN) nanotubes, that have had significant curiosity given their unique high-temperature houses, in addition to graphene nanosheets, BN nanosheets, and steel oxide nanosheets.
- Sputtering by particle bombardment: experiments and computer calculations from threshold to MeV energies
- Physics of Solar Cells - From Principles to New Concepts
- A Primer in Density Functional Theory
- Plasticity of Boronized Layers
- Out of the Crystal Maze: Chapters from The History of Solid State Physics
- Solid State Physics: Advances in Research and Applications, Vol. 40
Additional resources for Microfluidics
Their velocity components and internal energy are prescribed randomly from the distribution functions relative to an equilibrium gas. 33]. All molecules are moved by a quantity c δ t . During this displacement, a molecule can hit a wall. 2). During the collision, its velocity and its energy change. The corresponding exchange of momentum and energy with the wall is recorded. Some molecules exit the computational domain. They are removed from the memory. Molecules are sorted according to the index of the cell in which they are located.
Distribution functions usually depend on time t, on location r in physical space, and on the quantity Q under consideration. 2. Dilute gas The mean volume available for a molecule is 1/n and the mean molecular spacing is δ = 1/n1/3. The molecular diameter, d, characterizes the range of 28 Microfluidics intermolecular forces. If molecules are modeled as hard spheres, d is their diameter. 3] is said to be dilute. The gas itself occupies only a small fraction (typically (d/δ)3) of space. Most of the time, molecules are not submitted to intermolecular forces.
During collision, the relative velocity of molecules deviates by an angle χ that depends on the impact parameter b. The function χ (b ) depends on the function F ( r ) that relates the intermolecular force F to the distance r between molecules. A frontal collision is characterized by χ (0) = π . Realistic functions F ( r ) tend to zero when r tends to infinity. Thus large values of b result in negligibly small deviations of molecules: χ ( b → ∞ ) = 0 . A small limiting angle χ lim can be chosen and by convention all collisions resulting in χ < χlim will be ignored.