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Modern Physics Homework: Conservation of Energy and Momentum in Nuclear Reactions, Assignments of Physics

A modern physics homework problem focusing on the conservation of energy and momentum during nuclear reactions. The problem involves calculating the mass of uranium consumed per year, the energy produced by uranium and coal, and the mass of coal. It also discusses the concept of elastic collisions and the maximization of energy loss in nuclear reactions.

Typology: Assignments

Pre 2010

Uploaded on 02/13/2009

koofers-user-lgy
koofers-user-lgy 🇺🇸

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Download Modern Physics Homework: Conservation of Energy and Momentum in Nuclear Reactions and more Assignments Physics in PDF only on Docsity! Homework 13 Physics 2130 Modern Physics Due: Wednesday December 11, 2002 1. T & Z, #13.50. (a)M(U) = mass of uranium consumed per year. Mass of 235U consumed per year =M(235U) = (0:0072)M(U) because 235U constitutes only 0:72% of all uranium. Energy produced by ssion = (30%)  (number of ssions ) (energy per ssion) = 0:3 0:0072M(U)6:02  1023 particles/mole 235 g/mole ! 200 MeV/ ssion(1:6  1013 J/MeV) = 1:77  108 J/gM(U): Energy per year, power plant = 109 W(3:15  107 s/y) = 3:15  1016 J/y: 1:77  108 J/gM(U) = 3:15  1016 J/y M(U) = 2 108 g = 2 105 kg = 200 tonnes (metric tons) (b) Mass of coal = M(coal). Energy produced by coal = (0:40)M(coal)(33  106 J/kg) = (1:31  107 J/kg)M(coal) = 3:15  1016 J M(coal) = 2:4 106 tonnes (c) M(coal) = 24,000 box car loads  240 trains. (d) M(U) = 2 box car loads < 1 train. 2. T & Z, #13.51. m neutron Initial M p p’ m nucleus P M Final Figure 1: Conservation of momentum P = p p0 (1) Conservation of kinetic energy P 2 2M = p2 2m + p02 2m ! P 2 = p2 p02 (2) Note that kinetic energy is conserved because this is an elastic collision. Dividing equation (2) by (1) and adding the result to equation (1) yields: (1 + )P = p! P = 2p 1 +  (3) The kinetic energy lost by the neutron, K, will be just equal to the kinetic energy of the recoiling nucleus: K = P 2 2M (3) = 4p2 2M(1 + )2 K K = 4p2 2M(1 + )2 2m p2 = 4m M 1 (1 + )2 = 4 (1 + )2 = f() (4) where we have noted that the relative kinetic energy loss of the incident photon is a function of mu and call that function f(). (b) To maximize equation (4) with respect to  we take t he derivative and set it equal to 0: df() d = 4(1 ) (1 + )3 = 0!  = 1; (5) that is, energy loss is maximum when the two masses are equal. (c) Deuterium:  = 1=2 ! K=K = 0:89. Carbon:  = 1=12 ! K=K = 0:28. Note that if K=K = 1, the neutron is brought to a complete halt during the collision. 3. T & Z, #13.55. 1 1H + 12C proton capture! 13N + (6) 13N +-decay! 13C + e+ +  (7) 1 1H + 13C proton capture! 14N + (8) 1 1H + 14N proton capture! 15O + (9) 15O +-decay! 15N + e+ +  (10) 1 1H + 15N -decay! 12C + 4He (11) (b) 4P ! 3 + 2e+ + 2 + 4He. (c) In the CNO cycle, the highest Coulombic barrier is in the last step, reaction (11): UCNO = 7ke2 r1 : In the p p cycle, the highest barrier is for 3He+ 3He! 4He+ 2p: Upp = 4ke2 r2 : If r1 = r2, UCNO=Upp = 7=4. Since the average kinetic energy is proportional to temperature: TCNO Tpp  7 4 : 4. T & Z, #13.56. (3 pts) T & Z #13.56. a = 2ke2 p 2m=h = 2(1:44 MeV fm q 2(4:003)(931:5)=197 MeV fm = 3:97 (MeV)1=2 b = 8 p mke2=h = 8 q 4:003(931:5 MeV)(1:44 MeV fm)=197 MeV fm = 2:98 (fm)1=2
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