p8 - F . It is very useful to know that hc = 197MeV fm. (d)...

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Physics 25 Problem Set 8 Harry Nelson due Wednesday, May 28 Please make your work neat, clear, and easy to follow. It is hard to grade sloppy work accurately. Generally, make a clear diagram, and label quantities. Derive symbolic answers, and then plug in numbers after a symbolic answer is available. 1. Let’s consider a Bohr theory for the deuteron. Suppose the force between the neutron and proton is - F 0 for r 0 r r 0 + Δ r , and zero for all other distances r between the neutron and proton. (a) Make a plot of the force F ( r ) and the potential energy derived from it, V ( r ), where V ( r ) 0 as r → ∞ . (b) Suppose the angular momentum between the neutron and proton is exactly ¯ h ; find an ex- pression relating F 0 to distance between the neutron and proton, r 1 . (c) Suppose r 1 = r 0 = 1 × 10 - 13 cm, which is also called 1 fm, where fm stands for fermi or femtometer. Take m n c 2 = m p c 2 = 940 MeV, or million electron volts. Deduce a numerical value for
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Unformatted text preview: F . It is very useful to know that hc = 197MeV fm. (d) Evaluate the speed of the neutron (or proton) in the Bohr orbit, relative to the speed of light. (e) In the rst Bohr orbit it still must be that the total energy (sum of kinetic and potential energy) is negative , to achieve a bound state. This puts a constraint on r ; nd and evaluate that constraint. (f) For the numbers in this problem, numerically evaluate the potential energy near r = 0, and compare your result with page 95 of the text. 2. Consider the photon emitted when a hydrogen atom goes from the n = 100 Bohr orbit to the n = 1 Bohr orbit. Derive an expression for the ratio of the wavelength of the photon to the Bohr radius, and evaluate numerically. 3. Anderson, 2-13 4. Anderson, 2-15 5. Anderson, 2-18 6. Anderson, 2-21...
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This note was uploaded on 08/06/2008 for the course PHYS 25 taught by Professor Nelson during the Spring '08 term at UCSB.

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