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Polar to Cartesian coordinates

Transformation from polar to Cartesian coordinates clarifies the 2px designation, noting that the new wave function becomes... [Pg.217]

As an example of transformation cf polar to Cartesian coordinates, we ll graph the wave function for the dx2-y2 orbital in the x, y plane. The angular component of the wave fimction in the x, y plane is... [Pg.190]

Figure 9-23. Converting from polar to Cartesian coordinates... Figure 9-23. Converting from polar to Cartesian coordinates...
Matrix.xls illustrates the tools available for matrix mathematics, with examples. Polar.xls illustrates how to convert from polar to Cartesian coordinates. [Pg.465]

The classical potential energy term is just a sum of the Coulomb interaction terms (Equation 2.1) that depend on the various inter-particle distances. The potential energy term in the quantum mechanical operator is exactly the same as in classical mechanics. The operator Hop has now been obtained in terms of second derivatives with respect to Cartesian coordinates and inter-particle distances. If one desires to use other coordinates (e.g., spherical polar coordinates, elliptical coordinates, etc.), a transformation presents no difficulties in principle. The solution of a differential equation, known as the Schrodinger equation, gives the energy levels Emoi of the molecular system... [Pg.39]

Figure 9e. A projection of the Cremer-Pople sphere see Fig. 9A) onto a plane perpendicular to the polar axis. 8 and values for experiment and models were converted to cartesian coordinates, with the model points connected by solid lines. The central (0,0) point corresponds to a perfect chair, and the dashed line follows the 60 -240 meridian. Figure 9e. A projection of the Cremer-Pople sphere see Fig. 9A) onto a plane perpendicular to the polar axis. 8 and values for experiment and models were converted to cartesian coordinates, with the model points connected by solid lines. The central (0,0) point corresponds to a perfect chair, and the dashed line follows the 60 -240 meridian.
Cartesian coordinates is a product of N — 1 Jacobians for the local transformations from polar to Cartesian components for each bond vector Q for j < — 1, times the Jacobian det[A ]p = 1 for the transformation of Q... [Pg.80]

Spherical polar coordinates. The spherical polar coordinates r, 9,

radius vector r from the origin to point (x,y,z) 0 is the angle between r and the positive z axis r is the distance of (x,y,z) from the origin

relation between spherical polar and Cartesian coordinates is... [Pg.265]

Figure 8.1 Diagram showing the relation of polar coordinates, r, 0, (j>, to Cartesian coordinates for the point P. Figure 8.1 Diagram showing the relation of polar coordinates, r, 0, (j>, to Cartesian coordinates for the point P.
The variation of iff with the angles 9 and 0 is exactly the same as illustrated in Fig 3.14 in Section 3.4. The angular dependence of atomic orbitals is often represented in another way, using the relation between spherical polar and cartesian coordinates. For example, the cosd function appropriate to l = 1 and m = 0 can be expressed as... [Pg.64]

This method reduces the number of associations to be considered with the a.o.s of the central atom, because some of them correspond to zero overlap. The metal a.o.s are, for the first transition series, the 4s orbital, the three 4p orbitals and the five 3d orbitals. The latter are expressed below in polar coordinates (see page 46), together with the appropriate connection to cartesian coordinates. These expressions are real linear combinations of the complex forms of the d functions which correspond to each of the possible values of the magnetic quantum number m. The corresponding angular parts are depicted in Fig. 11.2. [Pg.250]

Cylindrical polar coordinates p, Cartesian coordinates by the equations of transformation... [Pg.105]

Changing from plane polar coordinates to Cartesian coordinates is an example of transformation of coordinates, and can be done by using the equations... [Pg.33]

In atoms the Coulomb forces refer to a centre and thus we speak about the central field. In this important case the introduction of polar coordinates (r, ft, Cartesian coordinates through formulae... [Pg.44]

Fig. 3. Spherical polar coordinates in relationship to Cartesian coordinates. Fig. 3. Spherical polar coordinates in relationship to Cartesian coordinates.
Figure 8.12 Polar and cartesian coordinate systems used to describe stress field around a crack. Figure 8.12 Polar and cartesian coordinate systems used to describe stress field around a crack.
Fig. 7.2. Polar and Cartesian coordinate systems used to describe the position of an electron in the hydrogen molecule ion. The stippled lines indicate a plane containing the z-axis and the electron. Fig. 7.2. Polar and Cartesian coordinate systems used to describe the position of an electron in the hydrogen molecule ion. The stippled lines indicate a plane containing the z-axis and the electron.
The use of redundant coordinates requires extensive modification of the lattice dynamical procedure. It is, however, often worth the additional complication to use redundancies if this facilitates the formulation of symmetry coordinates. When the Wigner projection operator (Wigner, 1931) is used to build such symmetry coordinates, it is necessary to first understand the results of the application of all symmetry operations of the applicable group to the displacement coordinates chosen. This is indeed relatively straightforward for the direction cosine displacement coordinates and therein lies their principal value. These coordinates transform like axial vectors in contrast to cartesian coordinates, which transform like polar vectors. [Pg.228]

Fig. 4.4 The average value of cos d can be obtained by integrating over the surface of a sphere. The arrow represents a vector with length r parallel to the transition dipole of a particular molecule the z axis is the polarization axis of the light. The area of a small elcanent on the surface of the sphere is r sin0dipd0. The polar coordinates used here can be converted to Cartesian coordinates by the transformation z = rcos( ), x = rsin(0)cos(( ), y = rsin(0)sin( )... Fig. 4.4 The average value of cos d can be obtained by integrating over the surface of a sphere. The arrow represents a vector with length r parallel to the transition dipole of a particular molecule the z axis is the polarization axis of the light. The area of a small elcanent on the surface of the sphere is r sin0dipd0. The polar coordinates used here can be converted to Cartesian coordinates by the transformation z = rcos( ), x = rsin(0)cos(( ), y = rsin(0)sin( )...
A, of an n-dimensional Euclidean space X is generated as follows. Each point x of a set A, is represented by suitable hyperpolar coordinates of one radial coordinate and n — I angle coordinates, where n is the dimension of the underlying space X and the origin is attached to a specified point c of set A In three dimensions, the usual polar coordinates r, 0, and 0 can be used, with respect to the center c of each set A, and with reference to Cartesian coordinate axes defined parallel to axes of a coordinate system of the laboratory frame. [Pg.2899]


See other pages where Polar to Cartesian coordinates is mentioned: [Pg.80]    [Pg.422]    [Pg.423]    [Pg.190]    [Pg.190]    [Pg.228]    [Pg.190]    [Pg.190]    [Pg.530]    [Pg.80]    [Pg.422]    [Pg.423]    [Pg.190]    [Pg.190]    [Pg.228]    [Pg.190]    [Pg.190]    [Pg.530]    [Pg.434]    [Pg.227]    [Pg.290]    [Pg.261]    [Pg.438]    [Pg.192]    [Pg.383]    [Pg.211]    [Pg.1271]   
See also in sourсe #XX -- [ Pg.189 ]




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