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Waves nodes

Under total external reflection condition, for 0 — 0, a standing-wave node lies at the mirror surface with the first antinode infinitely far above the surface. As the incident angle 9 is increased through the reflection, the first antinode moves inward until it coincides with the mirror surface for 9 = 9c. Above 9c, the first antinode remains at the mirror surface while the amplitude of the standing wave decreases very rapidly because of the drastic reduction in intensity of the specularly reflected plane wave. [Pg.165]

Targets and spirals have been observed in the CIMA/CDIMA system [13] and also in dilute flames (i.e. flames close to their lean flammability limits) in situations of enlianced heat loss [33]. In such systems, substantial fiiel is left unbumt. Spiral waves have also been implicated in the onset of cardiac arrhytlnnia [32] the nomial contractive events occurring across the atria in the mannnalian heart are, in some sense, equivalent to a wave pulse initiated from the sino-atrial node, which acts as a pacemaker. If this pulse becomes fragmented, perhaps by passing over a region of heart muscle tissue of lower excitability, then spiral structures (in 3D, these are scroll waves) or re-entrant waves may develop. These have the incorrect... [Pg.1107]

Dilfusion and Green s function QMC calculations are often done using a fixed-node approximation. Within this scheme, the nodal surfaces used define the state that is obtained as well as ensuring an antisymmetric wave function. [Pg.219]

Nodal surface (Section 1 1) A plane drawn through an orbital where the algebraic sign of a wave function changes The probability of finding an electron at a node is zero... [Pg.1289]

A UHF wave function may also be a necessary description when the effects of spin polarization are required. As discussed in Differences Between INDO and UNDO, a Restricted Hartree-Fock description will not properly describe a situation such as the methyl radical. The unpaired electron in this molecule occupies a p-orbital with a node in the plane of the molecule. When an RHF description is used (all the s orbitals have paired electrons), then no spin density exists anywhere in the s system. With a UHF description, however, the spin-up electron in the p-orbital interacts differently with spin-up and spin-down electrons in the s system and the s-orbitals become spatially separate for spin-up and spin-down electrons with resultant spin density in the s system. [Pg.232]

The solutions describe the vibrational modes of the system. As waves, the solutions are characterized by integers p which essentially count the number of nodes along the chain in a particular mode of vibration. The upper limit of p corresponds to the number of subchains in the molecule N, . [Pg.187]

The Cardiac Cycle. The heart (Eig. lb) performs its function as a pump as a result of a rhythmical spread of a wave of excitation (depolarization) that excites the atrial and ventricular muscle masses to contract sequentially. Maximum pump efficiency occurs when the atrial or ventricular muscle masses contract synchronously (see Eig. 1). The wave of excitation begins with the generation of electrical impulses within the SA node and spreads through the atria. The SA node is referred to as the pacemaker of the heart and exhibits automaticity, ie, it depolarizes and repolarizes spontaneously. The wave then excites sequentially the AV node the bundle of His, ie, the penetrating portion of the AV node the bundle branches, ie, the branching portions of the AV node the terminal Purkinje fibers and finally the ventricular myocardium. After the wave of excitation depolarizes these various stmetures of the heart, repolarization occurs so that each of the stmetures is ready for the next wave of excitation. Until repolarization occurs the stmetures are said to be refractory to excitation. During repolarization of the atria and ventricles, the muscles relax, allowing the chambers of the heart to fill with blood that is to be expelled with the next wave of excitation and resultant contraction. This process repeats itself 60—100 times or beats per minute... [Pg.111]

Slmn. iml/nr long wave raJutton on vLufjce node (wjII gam WG)... [Pg.1071]

Introduction of negative energy (positron) states. The coupling between the electronic and positronic states introduce a small component in the eleetronic wave funetion. The result is that the shape of the orbitals change, relativistic orbitals, for example, do not have nodes. [Pg.214]

Figure 1.5 Shapes of the 2p orbitals. Each of the three mutually perpendicular, dumbbell-shaped orbitals has two lobes separated by a node. The two lobes have different algebraic signs in the corresponding wave function, as indicated by the different colors. Figure 1.5 Shapes of the 2p orbitals. Each of the three mutually perpendicular, dumbbell-shaped orbitals has two lobes separated by a node. The two lobes have different algebraic signs in the corresponding wave function, as indicated by the different colors.

See other pages where Waves nodes is mentioned: [Pg.386]    [Pg.214]    [Pg.70]    [Pg.214]    [Pg.15]    [Pg.236]    [Pg.50]    [Pg.648]    [Pg.2657]    [Pg.408]    [Pg.1598]    [Pg.220]    [Pg.253]    [Pg.126]    [Pg.166]    [Pg.1587]    [Pg.158]    [Pg.386]    [Pg.214]    [Pg.70]    [Pg.214]    [Pg.15]    [Pg.236]    [Pg.50]    [Pg.648]    [Pg.2657]    [Pg.408]    [Pg.1598]    [Pg.220]    [Pg.253]    [Pg.126]    [Pg.166]    [Pg.1587]    [Pg.158]    [Pg.281]    [Pg.1364]    [Pg.2277]    [Pg.344]    [Pg.232]    [Pg.174]    [Pg.171]    [Pg.195]    [Pg.413]    [Pg.279]    [Pg.181]    [Pg.112]    [Pg.2437]    [Pg.151]    [Pg.33]    [Pg.58]    [Pg.413]    [Pg.332]    [Pg.15]    [Pg.171]    [Pg.5]   
See also in sourсe #XX -- [ Pg.343 ]

See also in sourсe #XX -- [ Pg.343 ]




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