Fundamentals of Physics, Binder Ready Version
Fundamentals of Physics, Binder Ready Version
10th Edition
ISBN: 9781118230640
Author: Halliday, David; Resnick, Robert; Walker, Jearl
Publisher: WILEY
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Chapter 39, Problem 15Q
To determine

To find:

The states that are not possible to exist, from the given five options, for a hydrogen atom.

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Form factor of atomic hydrogen. For the hydrogen atom in its ground state, the number density is n(r) = (7a) exp(-2r/a,), where a, is the Bohr radius. Show that the form factor is fc = 16/(4 + Gʻa)*. %3D %3D
The electron in a hydrogen atom occupies the orbital state |2, -1> and the spin state |1/2, -1/2>. what are the possible states? a. None O b. [5/2,-1/2> and 13/2,-3/2> O c. [5/2,-1/2> and |3/2,-1/2> O d. [5/2,-3/2> and |3/2,-1/2> e. [5/2,-3/2> and |3/2,-3/2>
3. Consider a monatomic linear with equilibrium separation a. Suppose the outer electrons (of mass m) in a given atom move with a displacement different from that of the corresponding ion core (of mass M). Let the displacement of the ion core s be: Us = uei(Ksa-wt) and the displacement of the center of mass of the outer electrons associated with ion s be: V = vei(Ksa-wt) Each ion core is assumed to interact only with its own outer electrons with a force proportional to the displacement of the electron distribution from the nucleus, and the force constant is C₂. However, neighboring electron distributions interact with a force constant C₁. a) Show that -w² Mus = C₂ (vs - Us) -w²mvs = C₂ (us - Vs) + C₁ (Vs+1 + Vs-1-2vs) b) Substitute for the displacements, and solve the resulting simultaneous equations. Find an expression for w². c) Take the limit as m → 0 (the mass of electrons is much smaller than that of the ion core), and show that the dispersion relation for the acoustic mode is…

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Fundamentals of Physics, Binder Ready Version

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