Chapter 3: Q3.6P (page 124)
A more elegant proof of the second uniqueness theorem uses Green's
identity (Prob. 1.61c), with . Supply the details.
Short Answer
Answer
It is proved as second uniqueness of theorem by using greens identity.
Chapter 3: Q3.6P (page 124)
A more elegant proof of the second uniqueness theorem uses Green's
identity (Prob. 1.61c), with . Supply the details.
Answer
It is proved as second uniqueness of theorem by using greens identity.
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Get started for freeThe potential at the surface of a sphere (radius ) is given by
,
Where is a constant. Find the potential inside and outside the sphere, as well as the surface charge density on the sphere. (Assume there's no charge inside or outside the sphere.)
A "pure" dipoleis situated at the origin, pointing in thezdirection.
(a) What is the force on a point charge q at (Cartesian coordinates)?
(b) What is the force on q at ?
(c) How much work does it take to move q fromto ?
A cubical box (sides of length a) consists of five metal plates, which are welded together and grounded (Fig. 3.23). The top is made of a separate sheet of metal, insulated from the others, and held at a constant potential. Find the potential inside the box. [What should the potential at the center be ? Check numerically that your formula is consistent with this value.]
(a) Suppose a charge distribution produces a potential , and some othercharge distribution produces a potential . [The two situations mayhave nothing in common, for all I care-perhaps number 1 is a uniformlycharged sphere and number 2 is a parallel-plate capacitor. Please understand that and are not present at the same time;we are talking about two differentproblems,one in which only is present, and another in which only ispresent.] Prove Green's reciprocity theorem:
[Hint:Evaluate two ways, first writing and using integrationby parts to transfer the derivative to , then writing and transferring the derivative to .]
(b) Suppose now that you have two separated conductors (Fig. 3.41). If you chargeup conductor by amount (leaving uncharged), the resulting potential of bis, say,.On the other hand, if you put that same charge on conductor (leaving uncharged), the potential of would be.Use Green's reciprocitytheorem to show that (an astonishing result, since we assumed nothingabout the shapes or placement of the conductors).
A charge is distributed uniformly along the z axis from to. Show that the electric potential at a point r is given by
for .
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