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Space representation

In the above discussion of relaxation to equilibrium, the density matrix was implicitly cast in the energy representation. However, the density operator can be cast in a variety of representations other than the energy representation. Two of the most connnonly used are the coordinate representation and the Wigner phase space representation. In addition, there is the diagonal representation of the density operator in this representation, the most general fomi of p takes the fomi... [Pg.234]

We can now proceed to the generation of conformations. First, random values are assigne to all the interatomic distances between the upper and lower bounds to give a trial distam matrix. This distance matrix is now subjected to a process called embedding, in which tl distance space representation of the conformation is converted to a set of atomic Cartesic coordinates by performing a series of matrix operations. We calculate the metric matrix, each of whose elements (i, j) is equal to the scalar product of the vectors from the orig to atoms i and j ... [Pg.485]

If Pmfv) and the plant uncertainty A(.v) are combined to give P(.v), then Figure 9.29 can be simplified as shown in Figure 9.30, also referred to as the two-port state-space representation. [Pg.314]

This converts a transfer function into its state-space representation using tf2ss(num, den) and back again using ss2tf (A,B, C, D, iu) when iu is the itii input u, normaiiy i. [Pg.402]

Example 8.4 transfer function to state space representation... [Pg.402]

The second axiom, which is reminiscent of Mach s principle, also contains the seeds of Leibniz s Monads [reschQl]. All is process. That is to say, there is no thing in the universe. Things, objects, entities, are abstractions of what is relatively constant from a process of movement and transformation. They are like the shapes that children like to see in the clouds. The Einstein-Podolsky-Rosen correlations (see section 12.7.1) remind us that what we empirically accept as fundamental particles - electrons, atoms, molecules, etc. - actually never exist in total isolation. Moreover, recalling von Neumann s uniqueness theorem for canonical commutation relations (which asserts that for locally compact phase spaces all Hilbert-space representations of the canonical commutation relations are physically equivalent), we note that for systems with non-locally-compact phase spaces, the uniqueness theorem fails, and therefore there must be infinitely many physically inequivalent and... [Pg.699]

In terms of the function space representation of Jf mentioned in the last section, orthogonality is expressed by... [Pg.430]

Fock Space Representation of Operators.—Let F be some operator that neither creates nor destroys particles, and is a known function in configuration space for N particles. In symbols such an operator must by definition have the following matrix elements in Fock space ... [Pg.455]

We have carried out tins discussion in occupation number representation or coordinate representation each with a definite number N of particles. Similar results follow for the Fock space representation and the properties of grand ensembles. Averages over grand ensembles are also independent of time when the probabilities > are independent of time, whether the observable commutes with H or not. [Pg.481]

A. Solution Space Representation—Discrete Decision Process.555... [Pg.10]

The way we have stated the domain theory for the state-space representation has enabled us to avoid making explicit reference to the alphabet symbol properties. However, if in other formulations we need to refer to these properties, we would again use a recursive parsing of the list of symbols to enable generalization over the size of the alphabet. [Pg.327]

Ibaraki, T., Branch and bound procedure and state-space representation of combinatorial optimization problems. Inf. Control 36,1-27 (1978). [Pg.330]

Figure 4. (a) Single- and (b) double-space representations of 4 e (solid) and bo (dashed) for a system that does not encircle the Cl. [Pg.8]

Fig. 8 LEED pattern as observed during preparation of a MgCL-film. a Pd(lll), b 1 ML MgCl2(001)/Pd(lll), c multilayer MgCl2(001)/Pd(lll). d Schematic real space representation of b the mesh represents the Cl lattice and spots the underlying Pd lattice... Fig. 8 LEED pattern as observed during preparation of a MgCL-film. a Pd(lll), b 1 ML MgCl2(001)/Pd(lll), c multilayer MgCl2(001)/Pd(lll). d Schematic real space representation of b the mesh represents the Cl lattice and spots the underlying Pd lattice...
Two important facts concerning the set of relations given above are that all the A -representability relations known to us, can be derived from (45) (or (44) in a spin-space representation) by varying the value of N and relation (49) condenses them all. [Pg.71]

We now consider the first order correction to the average potential, i.e. Vn>. In real space representation, substituting Equations (11) and (13) into (10) gives [36]... [Pg.165]

We do not need to carry the algebra further. The points that we want to make are clear. First, even the first vessel has a second order transfer function it arises from the interaction with the second tank. Second, if we expand Eq. (3-46), we should see that the interaction introduces an extra term in the characteristic polynomial, but the poles should remain real and negative.1 That is, the tank responses remain overdamped. Finally, we may be afraid( ) that the algebra might become hopelessly tangled with more complex models. Indeed, we d prefer to use state space representation based on Eqs. (3-41) and (3-42). After Chapters 4 and 9, you can try this problem in Homework Problem 11.39. [Pg.59]

Understand the how a state space representation is related to the transfer function representation. [Pg.64]

Example 4.1 Derive the state space representation of a second order differential equation of a form similar to Eq. (3-16) on page 3-5 ... [Pg.65]

X Example 4.3 Let s try another model with a slightly more complex input. Derive the state space representation of the differential equation... [Pg.66]

Example 4.5 Derive the state space representation of two continuous flow stirred-tank reactors in series (CSTR-in-series). Chemical reaction is first order in both reactors. The reactor volumes are fixed, but the volumetric flow rate and inlet concentration are functions of time. [Pg.68]

We use this example to illustrate how state space representation can handle complex models. First, we make use of the solution to Review Problem 2 in Chapter 3 (p. 3-18) and write the mass balances of reactant A in chemical reactors 1 and 2 ... [Pg.68]

To derive the state space representation, one visual approach is to identify locations in the block diagram where we can assign state variables and write out the individual transfer functions. In this example, we have chosen to use (Fig. E4.6)... [Pg.69]

An important reminder Eq. (E4-23) has zero initial conditions x(0) = 0. This is a direct consequence of deriving the state space representation from transfer functions. Otherwise, Eq. (4-1) is not subjected to this restriction. [Pg.70]

This completes our "feel good" examples. It may not be too obvious, but the hint is that linear system theory can help us analysis complex problems. We should recognize that state space representation can do everything in classical control and more, and feel at ease with the language of... [Pg.76]

The point is that state space representation is general and is not restricted to problems with zero initial conditions. When Eq. (4-1) is homogeneous (/.< ., Bu = 0), the solution is simply... [Pg.77]

While there is no unique state space representation of a system, there are standard ones that control techniques make use of. Given any state equations (and if some conditions are met), it is possible to convert them to these standard forms. We cover in this subsection a couple of important canonical forms. [Pg.78]

A tool that we should be familiar with from introductory linear algebra is similarity transform, which allows us to transform a matrix into another one but which retains the same eigenvalues. If a state x and another x are related via a so-called similarity transformation, the state space representations constmcted with x and x are considered to be equivalent.1... [Pg.78]


See other pages where Space representation is mentioned: [Pg.1528]    [Pg.414]    [Pg.320]    [Pg.4]    [Pg.294]    [Pg.455]    [Pg.457]    [Pg.458]    [Pg.270]    [Pg.277]    [Pg.38]    [Pg.173]    [Pg.139]    [Pg.140]    [Pg.64]    [Pg.64]    [Pg.77]   
See also in sourсe #XX -- [ Pg.71 ]




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Cell-based chemical space representation

Chemical space representation molecular similarity

Chemical space representations

Chemical space representations dimension reduction

Chemical space representations dimensionality

Coordinate-space representation

Data analysis representation of the product space

Design representation space

Dirac momentum-space representation

Hamiltonian operator space representation

Hilbert space Fock representation

Hydrogen momentum-space representation

Induced Representations of Space Groups in q-basis

Linear process model state-space representation

Molecular similarity analysis chemical space representation

Momentum operator space representation

Momentum-Space Representation

Orbital A representation of the space occupied level

Phase-space representations

Phase-space representations atoms

Phase-space representations harmonic oscillator

Pore space schematic representation

Position-space representation

Real-space representation

Representations of Space Groups

Site Symmetry and Induced Representations of Space Groups

Solution Space Representation—Discrete Decision Process

Space group representations

Space group symmetry and its mathematical representation

Space-filling representations

Spinor representations of space groups

State space representation

Target space representations

The Floquet Space Representation

The Fourier Space Representation

The real-space representation

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