The Application of Wave Functions Containing Interelectron Coordinates I the G
The Application of Wave Functions Containing Interelectron Coordinates I the G
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In our eReader you can find the full English version of the book. Read The Application of Wave Functions Containing Interelectron Coordinates I the G Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book The Application of Wave Functions Containing Interelectron Coordinates I the G
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To quickly assess the difficulty of the text, read a short excerpt:
^ v. (0. )g I = dQ.
^" "of«j'«o w is the appropriate weighting function for the angle which appears in the volume element.
The system of Equations (^. 5) must be solved simultaneously, and in practice an iteration procedure is used to solve them. Since the inter- electron coordinates which enter into g do not depend strongly upon the angles, the iteration of Equations (^. 5) converges quite rapidly if a reasonable guess is originally made for the angles.
Writing r. . As the value of r. . At r. ..., 0. , a. We now have for I ijo ij 10 10 10 {k. 6) I^(Z) = g(r^20' ""150' ••■ ' Vl^no^ J ^^^'^1' ^2^ •*• ' ""-^ ^^ n Note the dependence of I upon Z in Equations (^. L) and (4. 6). With large Z the exponential variation of f is so strong that only those regions near the nucleus contribute to I. As long as g is monotonic this means that Equation (4. 1) reduces to (^. 7) 1(00) = g(o, o, o) I .. I f dV .
- 19 This is exactly the form vhich Equation (^. 6) assumes at large Z and that expression is thus exact at Z equal to infinity.
What to read after The Application of Wave Functions Containing Interelectron Coordinates I the G?
You can find similar books in the "Read Also" column, or choose other free books by Peter Walsh to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
^ v. (0. )g I = dQ.
^" "of«j'«o w is the appropriate weighting function for the angle which appears in the volume element.
The system of Equations (^. 5) must be solved simultaneously, and in practice an iteration procedure is used to solve them. Since the inter- electron coordinates which enter into g do not depend strongly upon the angles, the iteration of Equations (^. 5) converges quite rapidly if a reasonable guess is originally made for the angles.
Writing r. . As the value of r. . At r. ..., 0. , a. We now have for I ijo ij 10 10 10 {k. 6) I^(Z) = g(r^20' ""150' ••■ ' Vl^no^ J ^^^'^1' ^2^ •*• ' ""-^ ^^ n Note the dependence of I upon Z in Equations (^. L) and (4. 6). With large Z the exponential variation of f is so strong that only those regions near the nucleus contribute to I. As long as g is monotonic this means that Equation (4. 1) reduces to (^. 7) 1(00) = g(o, o, o) I .. I f dV .
- 19 This is exactly the form vhich Equation (^. 6) assumes at large Z and that expression is thus exact at Z equal to infinity.
What to read after The Application of Wave Functions Containing Interelectron Coordinates I the G?
You can find similar books in the "Read Also" column, or choose other free books by Peter Walsh to read onlineMoreLess
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