Chapter 13: Q11MP (page 663)
The series in Problem 5.12 can be summed (see Problem 2.6). Show that.
Short Answer
The sum of the series in problem 12 is.
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Chapter 13: Q11MP (page 663)
The series in Problem 5.12 can be summed (see Problem 2.6). Show that.
The sum of the series in problem 12 is.
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Find the energy eigenvalues and Eigen functions for the hydrogen atom. The potential energy is in Gaussian units, where is the charge of the electron and r is in spherical coordinates. Since V is a function of r only, you know from Problem 18 that the Eigen functions are R(r) times the spherical harmonics , so you only have to find R(r). Substitute V(r) into the R equation in Problem 18 and make the following simplifications: Let ; show that then
. Let (note that for a bound state, E is negative, so is positive) and , to get the first equation in Problem 22.26 of Chapter 12. Do this problem to find y(x) , and the result that is an integer, say n .[Caution: not the same n as in equation (22.26)]. Hence find the possible values of (these are the radii of the Bohr orbits), and the energy eigenvalues. You should have found proportional to n; let , where ais the value of when n = 1, that is, the radius of the first Bohr orbit. Write the solutions R(r) by substituting back , and , and find from.
Solve Problem 2 if the sides and are insulated.
Show that the gravitational potential satisfies Laplace's equation, that is, show that where.
Show that our results can be extended to find the following solution of (8.22) which satisfies given nonzero boundary conditions:
Where is the Green function (8.28) which is zero on the surface 蟽, and is the normal derivative of G (see Chapter 6, Section 6).
Do the problem in Example 1 for the case of a charge q inside a grounded sphere to obtain the potential V inside the sphere. Sum the series solution and state the image method of solving this problem.
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