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Operator derivative

I EXERCISE 7.19 [ Find the Jacobian for the transformation from Cartesian to cylindrical polar coordinates. [Pg.217]

A triple integral in Cartesian coordinates is transformed into a triple integral in spherical polar coordinates by [Pg.217]

An operator is a symbol for carrying out a mathematical operation (see Chapter 9). There are several vector derivative operators. We first define them in Cartesian coordinates. [Pg.217]

Chapter 7 Calculus With Several Independent Variables [Pg.218]

The gradient of / is sometimes denoted by grad / instead of V/. The direction of the gradient of a scalar function is the direction in which the function is increasing most rapidly, and its magnitude is the rate of change of the function in that direction. [Pg.218]


Using the Heisenberg equation of motion, (AS,2,40). the connnutator in the last expression may be replaced by the time-derivative operator... [Pg.711]

It will be recognized that this generalizes the result proved by Baer in [72]. Though that work did establish the validity of the curl condition for the derivative operator as long as some 25 years ago and the validity is nearly trivial for the second term taken separately, the same result is not self-evident for the combination of the two teiins, due to the nonlinearity of F X). An important special case is when G(R) = R /2. Then... [Pg.155]

The non-adiabatic operator matrix, A can be written as a sum of two terms a matrix of numbers, G, and a derivative operator matrix... [Pg.277]

Finally, making use of the anti-FIermitian properties of the derivative operator,... [Pg.315]

Let us consider an example, that of the derivative operator in the orthonormal basis of Harmonic Oscillator functions. The fact that the solutions of the quantum Harmonic... [Pg.545]

In many applications, derivative operators need to be expressed in spherical coordinates. In converting from cartesian to spherical coordinate derivatives, the chain rule is employed as follows ... [Pg.557]

If we define D, to be the time-derivative operator following the shock path dxjdt = U t), then... [Pg.261]

Here, ej f are the vibration-rotation energies of the initial (anion) and final (neutral) states, and E denotes the kinetic energy carried away by the ejected electron (e.g., the initial state corresponds to an anion and the final state to a neutral molecule plus an ejected electron). The density of translational energy states of the ejected electron is p(E) = 4 nneL (2meE) /h. We have used the short-hand notation involving P P/p to symbolize the multidimensional derivative operators that arise in the non BO couplings as discussed above ... [Pg.289]

The operator Tang contains the cross-terms that give rise to the Coriolis coupling that mixes states with different fl (the projection of the total angular momentum quantum number J onto the intermolecular axis). This term contains first derivative operators in y. On application of Eq. (22), these operators change the matrix elements over ring according to... [Pg.21]

Finally, 3 " (j)[f (x )] is a short symbol expressing the m-th order partial derivative operators, acting first over the function f (x) and then, the resultant function, evaluated at the point x . The differential operators can be defined in the same manner as the terms present in equation (9), but using as second argument the nabla vector ... [Pg.235]

In order to show that the expected-value and derivative operations commute, we begin with the definition of the derivative in terms of a limit 16... [Pg.64]

The expected value on the left-hand side is taken with respect to the entire ensemble of random fields. However, as shown for the velocity derivative starting from (2.82) on p. 45, only two-point information is required to estimate a derivative.14 The first equality then follows from the fact that the expected value and derivative operators commute. In the two integrals after the second equality, only /u,[Pg.264]

In summary, due to the linear nature of the derivative operator, it is possible to express the expected value of a convected derivative of Q in terms of temporal and spatial derivatives of the one-point joint velocity, composition PDF. Two-point information about the random fields U and

expected value and derivative operators commute, and does not appear in the final expression (i.e., (6.9)). [Pg.265]

Substitution of this relation in the vector meson kinetic term (i.e., the replacement of Ffll/(p) by Fpv(v)) gives the following four derivative operator with two time derivatives and two space derivatives [40] ... [Pg.154]

With the help of fractional calculus, Dassas and Duby123 have worked on the problem of diffusion towards the fractal interfaces. They have proposed the following generalized diffusion equation involving a fractional derivative operator ... [Pg.367]

Regarding the electrochemical method, the generalized forms of the Cottrell relation and the Randles-Sevcik relation were theoretically derived from the analytical solutions to the generalized diffusion equation involving a fractional derivative operator under diffusion-controlled constraints and these are useful in to determining the surface fractal dimension. It is noted that ionic diffusion towards self-affine fractal electrode should be described in terms of the apparent self-similar fractal dimension rather than the self-affine fractal dimension. This means the fractal dimension determined by using the diffusion-limited electrochemical method is the self-similar fractal dimension irrespective of the surface scaling property. [Pg.399]


See other pages where Operator derivative is mentioned: [Pg.76]    [Pg.153]    [Pg.155]    [Pg.266]    [Pg.277]    [Pg.280]    [Pg.291]    [Pg.314]    [Pg.314]    [Pg.45]    [Pg.60]    [Pg.88]    [Pg.460]    [Pg.20]    [Pg.20]    [Pg.21]    [Pg.180]    [Pg.257]    [Pg.259]    [Pg.371]    [Pg.382]    [Pg.385]    [Pg.396]    [Pg.419]    [Pg.419]    [Pg.174]    [Pg.445]    [Pg.150]    [Pg.154]    [Pg.394]   
See also in sourсe #XX -- [ Pg.270 ]

See also in sourсe #XX -- [ Pg.270 ]

See also in sourсe #XX -- [ Pg.162 ]




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Derivatives operations

Derived operations

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