Concept explainers
(a)
Energy produced by the fission of
(a)
Answer to Problem 58P
Energy produced by the fission of
Explanation of Solution
Write the equation to find the number of nuclie in the given mass.
Here,
Write the equation to find the total energy produced.
Here,
Conclusion:
Substitute
Substitute
Therefore, the energy produced by the fission of
(b)
Energy produced by the deuterium –tritium fusion reaction.
(b)
Answer to Problem 58P
Energy produced by the deuterium –tritium fusion reaction is
Explanation of Solution
Write the equation to find the Energy produced by the deuterium –tritium fusion reaction.
Here,
Write the equation to find
Here,
Rewrite the expression for
Conclusion:
Substitute
Therefore, the energy produced by the deuterium –tritium fusion reaction is
(c)
Energy produced by the deuterium –tritium fusion reaction for
(c)
Answer to Problem 58P
Energy produced by the deuterium –tritium fusion reaction for
Explanation of Solution
Write the equation to find the energy produced by the deuterium –tritium fusion reaction for given mass of deuterium.
Here,
Write the equation to find the number of nuclie in the given mass.
Here,
Rewrite equation (I) by substituting the above relation for
Conclusion:
Substitute
Therefore, the energy produced by the deuterium –tritium fusion reaction for
(d)
Energy produced by the combustion of
(d)
Answer to Problem 58P
Energy produced by the combustion of
Explanation of Solution
Write the equation to find the energy produced by the deuterium –tritium fusion reaction for given mass of deuterium.
Here,
Write the equation to find the number of nuclie in the given mass.
Here,
Rewrite the equation for
Conclusion:
Substitute
Therefore, the energy produced by the combustion of
(e)
The pros and corns of energy production by fission, fusion, and combustion.
(e)
Explanation of Solution
To produce energy by combustion, coal is used. Coal is abundant form of fossil fuel and it is very cheap. The disadvantage is the high carbon emission and thereby acts as a major contributor in global warming. Energy production by nuclear fission cannot produce carbon and the working of reactor cannot cause any pollution. But the disposal of radioactive waste materials from the reactor is a very big challenge.
Nuclear fusion is better than fission since it does not produce radioactive by-products. But researches on nuclear fusion reactor are in developing stage only and it requires extreme high temperature for its working that cannot be achieved by man at present. Plutonium is a very risky material to handle in fission process.
Therefore, combustion is cheaper, but carbon emission is high, fission cannot cause global warming but produce radioactive bye products, and nuclear fusion cannot produce radioactive pollution but requires very large temperature that cannot be achieved in a laboratory at present.
Want to see more full solutions like this?
Chapter 30 Solutions
Principles of Physics: A Calculus-Based Text
- (a) Calculate the energy released in the neutron- Induced fission reaction n+235U92Kr+142Ba+2n , given m(92Kr) = 91.926269 u and m(142Ba)= 141.916361 u. (b) Confirm that the total number of nucleons and total charge are conserved in this reaction.arrow_forward(a) How many 239Pu nuclei must fission to produce a 20.0kT yield, assuming 200 MeV per fission? (b) What is the mass of this much 239Pu?arrow_forward(a) Calculate the energy released in the neutroninduced fission reaction n+239Pu96Sr+140Ba+4n, given m(96Sr)=95.921750u and m(140Ba)=139.910581u. (b) Confirm that the total number of nucleons and total charge are conserved in this reaction.arrow_forward
- (a) Calculate the energy released in the a decay of 238U . (b) What fraction of the mass of a single 238U is destroyed in the decay? The mass of 234Th is 234.043593 u. (c) Although the fractional mass loss is large for a single nucleus, it is difficult to observe for an entire macroscopic sample of uranium. Why is this?arrow_forwardAssume onefourth of the yield of a typical 320kT strategic bomb comes from fission reactions averaging 200 MeV and the remainder from fusion reactions averaging 20 MeV. (a) Calculate the number of fissions and the approximate mass of uranium and plutonium fissioned, taking the average atomic mass to be 238. (b) Find the number of fusions and calculate the approximate mass of fusion fuel, assuming an average total atomic mass of the two nuclei in each reaction to be 5. (c) Considering the masses found, does it seem reasonable that some missiles could carry 10 warheads? Discuss, noting that the nuclear fuel is only a part of the mass of a warhead.arrow_forward(a) Find the total energy released in MeV in each carbon cycle (elaborated in the above problem) including the annihilation energy. (b) How does this compare with the protonproton cycle output?arrow_forward
- (a) Calculate the energy released in the a decay of 238U. (b) What fraction of the mass at a single 238U is destroyed in the decay? The mass of 234Th is 234.043593 u. (c) Although the fractional mass loss is laws for a single nucleus, it is difficult to observe for an entire macroscopic sample of uranium. Why is this?arrow_forward(a) A cancer patient is exposed to rays from a 5000Ci 60Co transillumination unit for 32.0 s. The rays are collimated in such a manner that only 1.00% of them strike the patient. Of those, 20.0% are absorbed in a tumor having a mass of 1.50 kg. What is the dose in rem to the tumor, it the average energy per decay is 1.25 MeV? None of the s from the decay reach the patient. (b) Is the dose consistent with stated therapeutic doses?arrow_forward(a) Write the complete a decay equation for 249Cf. (b) Find the energy released in the decay.arrow_forward
- Tritium is naturally rare, but can be produced by the reaction n+2H3H+. How much energy in MeV is released in this neutron capture?arrow_forwardSuppose you have a pure radioactive material with a half-life of T1/2. You begin with N0 undecayed nuclei of the material at t = 0. At t=12T1/2, how many of the nuclei have decayed? (a) 14N0 (b) 12N0(C) 34N0 (d) 0.707N0 (e) 0.293N0arrow_forwardis the heaviest stable nuclide, and its BEN is low compared with medium-mass nuclides. Calculate BEN for this nucleus and compare it with the approximate value obtained from the graph in Figure 10.7. fission of nuclei with mass numbers greater than that of Fe. are othermic processes.arrow_forward
- Principles of Physics: A Calculus-Based TextPhysicsISBN:9781133104261Author:Raymond A. Serway, John W. JewettPublisher:Cengage LearningPhysics for Scientists and Engineers with Modern ...PhysicsISBN:9781337553292Author:Raymond A. Serway, John W. JewettPublisher:Cengage LearningModern PhysicsPhysicsISBN:9781111794378Author:Raymond A. Serway, Clement J. Moses, Curt A. MoyerPublisher:Cengage Learning
- College PhysicsPhysicsISBN:9781305952300Author:Raymond A. Serway, Chris VuillePublisher:Cengage LearningCollege PhysicsPhysicsISBN:9781285737027Author:Raymond A. Serway, Chris VuillePublisher:Cengage Learning