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Commutative property addition

Starting with the quantum-mechanical postulate regarding a one-to-one correspondence between system properties and Hemiitian operators, and the mathematical result that only operators which conmuite have a connnon set of eigenfiinctions, a rather remarkable property of nature can be demonstrated. Suppose that one desires to detennine the values of the two quantities A and B, and that tire corresponding quantum-mechanical operators do not commute. In addition, the properties are to be measured simultaneously so that both reflect the same quantum-mechanical state of the system. If the wavefiinction is neither an eigenfiinction of dnor W, then there is necessarily some uncertainty associated with the measurement. To see this, simply expand the wavefiinction i in temis of the eigenfiinctions of the relevant operators... [Pg.15]

COMMUTATIVE PROPERTY states that when performing a string of addition operations, or a string of multiplication operations, the order does not matter. In other words, a + b = b + a. [Pg.58]

Whereas matrix addition (9.8) and scalar multiplication (9.9) have the usual associative and commutative properties of their scalar analogs, matrix multiplication (9.11), although associative [i.e., A(BC) = (AB)C], is inherently ncommutative [i.e., AB BAJ. This noncommutativity leads to some of the most characteristic and surprising features of matrix algebra, and underlies the still more surprising matrix-algebraic features of quantum theory. [Pg.317]

Commutative Property of Addition. When using addition, the order of the addends does not affect the sum ... [Pg.40]

The commutative property states that, in addition and multiplication, terms may be arbitrarily interchanged. Thus, equation (1.16) applies for addition and equation (1.17) applies for multiplication of complex numbers z and w. The distributive property is demonstrated by equation (1.18), and the associative property is demonstrated by equation (1.19). [Pg.10]

The accumulation of x [ i ] x [ i ] into r in the above example is a critical section (see section 4.1) because r is shared among all threads. The (almost) associative and commutative properties of the addition and other permitted operators allow the reduction operator to provide better performance fhan would be possible by obtaining a mutual exclusion lock for each accumulation into r. [Pg.199]

Additions of cadmium (0.05—1.3%) to copper raise the recrystallization temperature and improve the mechanical properties, especially in cold-worked conditions, with relatively Htde reduction in conductivity. Copper containing 0.07% cadmium is used in automotive cooling fins, heavy-duty radiators, motor commutators, and electric terminals. [Pg.389]

A commutative ring JT is called a field if, in addition to the properties given above, the following two postulates also hold true ... [Pg.36]

Properties and Application. The two independent statistical distributions of the two-phase stacking model are the distributions of amorphous and crystalline thicknesses, h (x) and ii2 x). Both distributions are homologous. The stacking model is commutative and consistent. If the structural entity (i.e., the stack as a whole) is found to show medium or even long-ranging order, the lattice model and its variants should be tested, in addition. As a result the structure and its evolution mechanism may more clearly be discriminated. [Pg.193]

Two properties, the commutative and associative properties, deal with expressions that involve a string of all addition operations, or a string of all multiplication operations. These properties are for addition and multiplication only. [Pg.58]

These commutation relations are taken to be the basic property of all angular momentum operators, including the spin operators which cannot be expressed in terms of the position coordinates xyz. In addition to the components of A/, we must deal with the operator M2 ... [Pg.187]

As discussed in Section 9.3, a higher level of mathematical structure is achieved by defining an additional multiplication (X-Y) operation, that is, a rule that associates a (real) scalar with every pair of objects X, Y in the manifold. For Euclidean-like spaces, the scalar product has distributive, commutative, and positivity properties given by... [Pg.424]

This is as far as we can go with the representation of vector operators without requiring further properties of V in order to obtain the explicit form of the coefficients a and c. The additional properties we shall use are the commutation relations needed to make the six components of J and V into the Lie algebra so(4). [Pg.23]

These rules for adding and subtracting matrices give matrix addition the same properties as ordinary addition and subtraction. It is closed (among matrices of the same size), commutative, and associative. There is an additive identity (the matrix consisting entirely of zeros) and an additive inverse ... [Pg.257]

A system in which an addition and a multiplication are defined and for which the commutative, associative, and distributive properties hold, where there exist identities for addition and multiplication, where every element has an additive inverse, and every non-zero element has a multiplicative inverse, is called a field. Other examples of fields are the set of rational numbers and the set of real numbers. Since the number of elements in our set is finite, we have an example of finite field. [Pg.385]

Figure 6. Concept of applying commutative and additive properties to surface color development of tomatoes stored under two different storage environments. (Reproduced with permission from Ref. 27. Copyright 1987 American Society of Agricultural Engineers.)... Figure 6. Concept of applying commutative and additive properties to surface color development of tomatoes stored under two different storage environments. (Reproduced with permission from Ref. 27. Copyright 1987 American Society of Agricultural Engineers.)...
In addition, they commute with the four-component spin operator —a property... [Pg.287]

The experimental data obtained at finite, but moderate deformations (not more than 30 %) prove that an uncoupling of elastic and plastic properties can be achieved if and only if the l.c.r.c. is used as reference to evaluating the elastic deformation. This is reflected in our model by the definition given to the reversible part of deformation which implies a multiplicative non-commutative decomposition F = EP. We consider that additivity can be obtained for large deformations only if the uncoupling is abandoned. [Pg.247]


See other pages where Commutative property addition is mentioned: [Pg.107]    [Pg.206]    [Pg.55]    [Pg.191]    [Pg.245]    [Pg.50]    [Pg.201]    [Pg.50]    [Pg.225]    [Pg.6]    [Pg.233]    [Pg.389]    [Pg.180]    [Pg.287]    [Pg.100]    [Pg.32]    [Pg.34]    [Pg.46]    [Pg.149]    [Pg.31]    [Pg.556]    [Pg.137]    [Pg.1319]   
See also in sourсe #XX -- [ Pg.178 ]




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Additive properties

Commutability

Commutation

Commutative property

Commutativity

Commutator

Commute

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