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Multiplicity of states

Multiplicity of states in hydrogen chemisorption on platinum is a very... [Pg.59]

Triplet states are, however, formed to larger extents and play more important roles than would have been thought to be true twenty or thirty years ago. The classical work of Lewis and Kasha129, whichshowed certain emissions to come from triplet states, opened the way for the rationalization of many phenomena which would otherwise prove to be quite incomprehensible. Perhaps, as Matsen etal.130 have pointed out, an undue emphasis has been placed on electron spin and on the multiplicity of states. The symmetry of the entire wave function is really the important point, and the contributions to it of all states of the molecule must be considered. Viewed in this light the triplet component , to use rather crude language, will depend on the vibrational quantum numbers in the excited state. If other isomers can exist, their contributions to the complete wave function must also be considered. [Pg.56]

Regulations that do pertain to collection of invertebrates fall into several categories where collecting may be done, what may be collected, and how specimens may be transported. The multiplicity of state, federal, and international regulations that may apply in certain instances is beyond the scope of this chapter, but some general guidelines can be given. [Pg.52]

A very interesting series of studies of the influence of end effects in the rotating concentric cylinder problem has been published by Mullin and co-workers T. Mullin, Mutations of steady cellular flows in the Taylor experiment,J. Fluid Mech. 121, 207-18 (1982) T. B. Benjamin and T. Mullin, Notes on the multiplicity of flows in the Taylor experiment, J. Fluid Mech. 121, 219-30 (1982) K. A. Cliff and T. Mullin, A numerical and expwerimental study of anomalous modes in the Taylor experiment, J. Fluid Mech. 153, 243-58 (1985) G. Pfister, H. Schmidt, K. A. Cliffe and T. Mullin, Bifurcation phenomena in Taylor-Couette flow in a very short annulus, J. Fluid Mech. 191, 1-18 (1988) K. A. Cliffe, 1.1. Kobine, and T. Mullin, The role of anomalous modes in Taylor-Couette flow, Proc. R. Soc. London Ser. A 439, 341-57 (1992) T. Mullin, Y. Toya, and S. I. Tavener, Symmetry breaking and multiplicity of states in small aspect ratio Taylor-Couette flow, Phys. Fluids 14, 2778-87 (2002). [Pg.184]

This relation is equivalent to Boltzmann s equation (i.e., S = A lnf2) for the microcanonical ensemble, where all quantum states are equally probable and is the thermodynamic multiplicity of states. The correspondence between S and Z is obtained by invoking the Boltzmann distribution for P, in equation (28-35) using results from (28-31) ... [Pg.763]

The United States has a multiplicity of state and federal regulatory authorities. But no issue is more important than the dividing line between them. Jurisdiction is not shared - it is meticulously divided on the basis of the requirements of the US Constitution. Such a division in regulatory responsibility does not exist within the EU. The Second Directive states ... [Pg.40]

The first selection rule concerns the multiplicity of states Since the components of p are ungerade or odd, the integrand becomes gerade or even only provided the product of the two spin functions is ungerade, i.e., if their multiplicity or the total spin quantum number S does not change, or in other words if AS=0. Thus singlet-triplet transitions are normally forbidden. [Pg.342]

Now a given translational energy corresponds to a multiplicity of states, since each rectangular component of the momentum is itself quantized, and numerous values of and can satisfy... [Pg.291]

A negative aspect of deposit systems is that the per-container cost of managing these systems, as they are currently designed, is higher than the cost of alternative collection systems.A national system rather than the current multiplicity of state systems could reduce some of this cost differential, however. There are also very real sanitary concerns, especially when deposits are expanded to noncarbonated beverages. [Pg.493]

Increasing the energy of a system increases its multiplicity of states. It follows that a tendency toward high multiplicity is a tendency for a system to take up heat from the surroundings. Now why does heat flow from hot objects to cold ones Example 3.4 addresses this question. [Pg.45]

This shows that a principle of maximum multipUcity predicts that heat will flow to equalize energies in this case. Consider the alternative. Suppose A were to lower its energy to 1/ = 1 while B wound up with Ub = 5. Then the multiplicity of states would be... [Pg.45]

Figure 3.9 Energy-level diagrams for the two different systems in Example 3.4 with ten particles each. System /t has total energy (/4 = 2, and B has Ub = 4. System B has the greater multiplicity of states. Figure 3.9 Energy-level diagrams for the two different systems in Example 3.4 with ten particles each. System /t has total energy (/4 = 2, and B has Ub = 4. System B has the greater multiplicity of states.
EXAMPLE 7.4 How does the equality of pressures maxiniize the multiplicity of states Consider a gas contained on two sides of a piston as shown in Figure 7.6. The number Na of particles on the left and the number Nb on the right are each fixed. The total volume is defined by M lattice sites, and the movable piston partitions the volume into Ma sites on the left and Mg sites on the right, with the constraint M = Ma + Mb = constant. [Pg.116]

Coin-flip statistics Equation (1.19) gives the multiplicity of states ... [Pg.222]

Figure 12.2 The entropy S/k of the two-state system as a function of its energy U. At low U, the multiplicity of states W is small because mostly the ground state is populated. Also at high U, W is small because mostly the excited state is populated. More states are populated for intermediate U. The slope of everywhere is l/T, where T is the temperature. T > 0 on the left, T < 0 on the right. Figure 12.2 The entropy S/k of the two-state system as a function of its energy U. At low U, the multiplicity of states W is small because mostly the ground state is populated. Also at high U, W is small because mostly the excited state is populated. More states are populated for intermediate U. The slope of everywhere is l/T, where T is the temperature. T > 0 on the left, T < 0 on the right.
The multiplicity of states is the number of spatial arrangements of the molecules ... [Pg.268]

In the previous chapter we have seen that the stability of the thermodynamic branch is no longer assured when a system is driven far from equilibrium. In section 18.3 we have seen how a necessary condition (18.3.7) for a system to become unstable can be obtained by using the second variation of entropy, 5 5. Beyond this point, we are confronted with a multiplicity of states and unpredictability. To understand the precise conditions for instability and the subsequent behavior of a system, we need to use the specific features of the system, such as the rates of chemical reactions and the hydrodynamic equations. There are, however, some general features of far-from-equilibrium systems that we will summarize in this section. A detailed discussion of dissipative structures will be presented in the following sections. [Pg.428]

An exponential growth of the multiplicities of states is also observed in two-dimensional arrays of pivoted magnets. Extensive experiments with /ix/i, 2fluctuating magnetic fields, and then allowed to settle into locally stable configurations, show that the number of distinct patterns M" N) is of the order of... [Pg.508]

Here the factor gj is the number of energy states with the same energy Ej. In the rotational case the lowest level (J = 0) is a single state ( o = 0 t>ut the higher levels have a (2J + I) multiplicity of states in each level (see Fig. 1.14). Therefore, the Boltzmann distribution function for the number rij of molecules in the J level relative to Wq (those in the J = 0 level) is... [Pg.42]

The possible values for the quantum number wii are -jy..jy and by counting those possibilities, we find there are + 1 of them. This is the multiplicity of states from the ji angular momentum. The total number of states for the whole system is a product of multiplicities, (2/i + 1x2/2 +1). [Pg.225]


See other pages where Multiplicity of states is mentioned: [Pg.54]    [Pg.114]    [Pg.118]    [Pg.18]    [Pg.457]    [Pg.187]    [Pg.114]    [Pg.187]    [Pg.447]    [Pg.99]    [Pg.174]    [Pg.563]    [Pg.208]    [Pg.223]    [Pg.224]    [Pg.225]    [Pg.151]    [Pg.292]    [Pg.511]    [Pg.254]    [Pg.249]    [Pg.3]    [Pg.573]    [Pg.33]    [Pg.340]   
See also in sourсe #XX -- [ Pg.342 , Pg.347 ]

See also in sourсe #XX -- [ Pg.160 , Pg.165 ]




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Existence of multiple states

Multiple Oxidation States of Transition Elements

Multiple states of adsorbed proteins

Multiplicity of Steady States in Catalyst Particles

Multiplicity of electronic state

Multiplicity of stationary states

Multiplicity of steady states

Multiplicity of the Steady-State Regimes

Observation of Multiple Steady States

Simple Examples of Reactions with No Possible Multiple Steady States

Spin Multiplicity of Electronic States

State multiplicity

State of the Art in Theory and Modeling Multiple Scales

Steady-State Multiplicity of CSTR

Steady-State Multiplicity of a Tubular Reactor

Treatment of the Multiple Ionization State Problem

Uniqueness, multiplicity and stability of steady states

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