Electromagnetic FieldsThis revised edition provides patient guidance in its clear and organized presentation of problems. It is rich in variety, large in number and provides very careful treatment of relativity. One outstanding feature is the inclusion of simple, standard examples demonstrated in different methods that will allow students to enhance and understand their calculating abilities. There are over 145 worked examples; virtually all of the standard problems are included. |
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Page 115
... quadrupole term can be written in terms of the quadrupole moment as 1 Po ( r ) = 1 jk • 3 Απερτ 2 Σ Σ Σ ljlkQjk j = x , y , z k = x , y , z ( 8-30 ) If the point P is very far away and if both the monopole moment Q and the dipole moment ...
... quadrupole term can be written in terms of the quadrupole moment as 1 Po ( r ) = 1 jk • 3 Απερτ 2 Σ Σ Σ ljlkQjk j = x , y , z k = x , y , z ( 8-30 ) If the point P is very far away and if both the monopole moment Q and the dipole moment ...
Page 117
... quadrupole moment at all , it must necessarily have an axis of symmetry that is the direction of its intrinsic angular momentum or “ spin . ” Thus it is essentially the quantity Qa that is found listed in tables of nuclear quadrupole ...
... quadrupole moment at all , it must necessarily have an axis of symmetry that is the direction of its intrinsic angular momentum or “ spin . ” Thus it is essentially the quantity Qa that is found listed in tables of nuclear quadrupole ...
Page 121
... QUADRUPOLE FIELD The general expression for the quadrupole potential as given by ( 8-30 ) can be quite complicated depending on which components Q are different from zero . Conse- quently , we investigate only the special case in which ...
... QUADRUPOLE FIELD The general expression for the quadrupole potential as given by ( 8-30 ) can be quite complicated depending on which components Q are different from zero . Conse- quently , we investigate only the special case in which ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
THE VECTOR POTENTIAL | 16 |
Copyright | |
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Ampère's law angle assume axes axis bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law current density curve cylinder dielectric dipole direction distance divergence theorem E₁ electric field electromagnetic electrostatic energy equipotential evaluate example expression field point free charge function given induction infinitely long integral integrand Laplace's equation line charge line integral located magnetic magnitude Maxwell's equations obtained origin P₁ perpendicular point charge polarized position vector potential difference quadrupole R₁ region result scalar potential Section shown in Figure sphere of radius spherical surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume wave write written xy plane zero Απερ μο дх