A 200 MW fission reactor consumes half its fuel in 3.00 y . How much U235did it contain initially? Assume that all the energy generated arises from the fission of U235 and that this nuclide is consumed only by the fission process.

Short Answer

Expert verified

The mass of the Uranium is 462 kg.

Step by step solution

01

Write the given data from the question:

The power of the reactor, P=200MW

The time, t=3years

The molar number of the uranium, M=235g/mol

02

Determine the formulas to calculate the initially contain mass of the U235 :

The expression to calculate the released energy is given as follows.

E=Pt …… (1)

The expression to calculate the number of fission is given as follows.

n=EQ …… (2)

Here,Qis the energy per fission.

The expression to calculate the number of nuclei is given as follows.

N=2n …… (3)

03

Calculate the initially contain mass of the U235 :

The typical energy released per fission is Q=200MeV

Calculate the released energy.

Substitute 200 MW for P and 3 years into equation (1).

E=200×106×3×365×24×3600=200×106×9.46×107=1.894×1016J=1.183×1029MeV

Calculate the number of the fission.

Substitute 1.183×1029MeV for E and 200 MeV for Q into equation (2).

n=1.183×1029200=0.005913×1029=5.913×1026

calculate the number of the nuclei.

Substitute 5.913×1026 for n into equation (3).

N=2×5.913×1026=11.8375×1026

Calculate the mass of the uranium.

MU=11.8375×1026×235×u=2.15×1026×235×1.661×10-27=4620.59×10-1=462kg

Hence, the mass of the Uranium is 462kg.

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Most popular questions from this chapter

Some uranium samples from the natural reactor site described in Module 43-3 were found to be slightly enrichedin 235U, rather than depleted. Account for this in terms of neutron absorption by the abundant isotope 238Uand the subsequent beta and alpha decay of its products.

Verify that, as reported in Table 43-1, fissioning of theU235 in 1.0 kg ofUO2 (enriched so thatU235 is 3.0% of the total uranium) could keep a 100 W lamp burning for 690 y.

Question: In a particular fission event in which U235is fissioned by slow neutrons, no neutron is emitted and one of the primary fission fragments is Ge83. (a) What is the other fragment? The disintegration energy is Q = 170 MeV. How much of this energy goes to (b) the Ge83fragment and (c) the other fragment? Just after the fission, what is the speed of (d) the Ge83fragment and (e) the other fragment?

(See Problem 21.) Among the many fission products that may be extracted chemically from the spent fuel of a nuclear reactor is Sr90(T1/2=29y). This isotope is produced in typical large reactors at the rate of about 18 kg/y. By its radioactivity, the isotope generates thermal energy at the rate of 0.93 W/g. (a) Calculate the effective disintegration energy Qeffassociated with the decay of a Sr90nucleus. (This energy includes contributions from the decay of the Sr90daughter products in its decay chain but not from neutrinos, which escape totally from the sample.) (b) It is desired to construct a power source generating 150 W (electric power) to use in operating electronic equipment in an underwater acoustic beacon. If the power source is based on the thermal energy generated by 90Sr and if the efficiency of the thermal–electric conversion process is 5.0%, how muchSr90is needed?

Question: Assume that immediately after the fission of U236according to Eq. 43-1, the resulting Xe140andSr94nuclei are just touching at their surfaces. (a) Assuming the nuclei to be spherical, calculate the electric potential energy associated with the repulsion between the two fragments. (Hint: Use Eq. 42-3 to calculate the radii of the fragments.) (b) Compare this energy with the energy released in a typical fission event.

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