CHEM 418 quiz 2 2024
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CHEM 418 Last Name:___________________________ Quiz 2 Assigned: 7-Feb-24 First Name:___________________________ 1
st
Due Date: 13-Feb-24 2
nd
Due Date: 16-Feb-24 Lecture 6: Gamma Decay Lecture 7: Fission Lecture 8: Nuclear Force and Nuclear Structure Lecture 9: Nuclear Reactions Lecture 10: Radiation Interactions Question Lectures 1 Lecture 6 Gamma Decay, Lecture 5 Beta Decay 2 Lecture 7 Fission, Lecture 1 Chart of the Nuclides 3 Lecture 8 Nuclear Force and Nuclear Structure, Lecture 1 Chart of the Nuclides 4 Lecture 9: Nuclear Reactions, Lecture 1 Chart of the Nuclides, Lecture 6 Gamma decay 5 Lecture 10: Radiation interactions 6 Lecture 8: Nuclear Structure 7 Lecture 8: Nuclear Structure, Lecture 2: Nuclear Properties Use lecture notes, textbooks, Chart of the Nuclides, Table of the Isotopes, and web pages. Use the chart of the nuclides as your primary dataset for isotope half-life. Show your work or references on a separate page and save electronically. Please use 3 significant digits for your answers. 1.
(20 Points) Use the decay schemes for the following questions. 1.1.
Provide the following data
1.1.1.
137
Cs half-life (years) 1.1.2.
Half-life of 137m
Ba (minutes)
1.1.3.
Log
ft
value for the most likely beta decay branch of 137
Cs 1.1.4.
Is there another stable isotope of A=137? 1.1.5.
137
Ba spin and parity 1.1.6.
What is the gamma decay energy associated with 137
Cs in keV?
1.1.7.
137
Cs beta decay Q value (keV) 1.1.8.
137
La Electron capture Q value (keV) 1.2.
What are the possible multipole radiations for the gamma decay shown above?
1.3.
What is the actual multipole radiation for the gamma decay shown above?
1.4.
Using the figure above provide the logft values for the ground state to ground decays of 137
Cs and 137
La. 1.4.1.
137
Cs logft 1.4.2.
137
La logft 1.5.
The spin and parity of 137
La is the same as 137
Cs and both decay to 137
Ba. Yet 137
La does not decay to the 11/2- metastable state in the 137
Ba as does 137
Cs. Why? The questions above related to energy provide insight.
2.
(15 Points) Use the chart of the nuclides data below for question 2. Consider the spontaneous fission of 250
Cf
1,2
. 2.1.
Based on the data, what is the spontaneous fission half-life in years for 250
Cf? 2.2.
Based on the spontaneous fission of 250
Cf, provide the data in the figure below. One fission product is provided. For the Coulomb barrier use )
(
8
.
1
44
.
1
V
3
/
1
2
3
/
1
1
2
1
A
A
Z
Z
c
+
=
Reaction # Fission Product 1 Fission Product 2 Vc (MeV) Q value (MeV) 1 88
Kr
___________ ___________ ___________ 2 99
Mo
___________ ___________ ___________ 3 110
Pd
___________ ___________ ___________ 4 134
Te
___________ ___________ ___________ 5 144
Ba
___________ ___________ ___________ 2.3.
From the fissions shown in the table above which fission reaction is most likely? 2.4.
Why did you select the fission product reactions from the question above? 2.5.
What is the difference between spontaneous fission and neutron induced fission?
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3.
(20 Points) Consider the nucleus 99
Mo. This isotope is important for medical applications, as it is the parent of 99m
Tc. These questions will explore why 99m
Tc is the prominent progeny from the decay of 99
Mo rather than the ground state 99
Tc. 3.1.
Provide the spin and parity of 99
Mo from the shell model 3.2.
Provide the spin and parity from chart of the nuclides 3.3.
Based on the actual spin and parity from the chart of the nuclides use the Nilsson diagram on the next page to answer the following questions. 3.3.1.
Is 99
Mo a deformed nucleus? 3.3.2.
Indicate which location on the Nilsson diagram (next page) would be occupied by the unpaired nucleon in 99
Mo. The red circle indicates the possible locations. 3.3.3.
What is the shape of the 99
Mo nucleus?
A B C D E F
4.
(20 Points) The isotope 225
Ac is of interest for medical applications
3
. The reactions of 232
Th with protons shown in the excitation function below is a means to indirectly produce 225
Ac
4
. Use the data to answer the questions below. A comparison of the experimental excitation functions for the 232
Th(p, 3n)
230
Pa reaction (blue diamonds), the 232
Th(p, 4n)
229
Pa reaction (red squares), and the 232
Th(p, 5n)
228
Pa reaction (black circles) with the theoretical PHITS (solid curves) and MCNP6 (dashed curves) excitation functions
4
.
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4.1.
What is the primary gamma decay energy for 225
Ac and its associated gamma yield in %? 4.2.
For the reaction with the highest experimental cross section at 22.5 MeV, provide the following: 4.2.1.
Reaction notation 4.2.2.
Reaction Q-values (MeV) 4.2.3.
Threshold Reaction Energy (MeV) 4.2.4.
Coulomb Barrier in MeV using the equation )
(
8
.
1
44
.
1
V
3
/
1
2
3
/
1
1
2
1
A
A
Z
Z
c
+
=
4.3.
Consider the calculations for the Q-value, Threshold Reaction Energy, and Coulomb Barrier. Provide the laboratory reaction energy necessary for producing the reaction. 4.4.
Which is the reaction that will indirectly produce the medical isotope 225
Ac? 4.5.
Describe how the 225
Ac is eventually produced from this reaction. 4.6.
Which proton energies would eventually produce an isotope with an alpha decay energy at 5.6855 MeV? 4.7.
A foil of 232
Th is irradiated with protons. Immediately after the end of bombardment the sample is measured in a gamma detector. The following gamma activity is found:
Gamma Energy (keV) 911.2 463.02 Activity (counts per second) 1025 1500 Select the proton energy in MeV used in the reaction. 4.8.
What is the activity for the gamma energies in counts per second 24 hours after the end of bombardment? 4.9.
An irradiation is performed with a 30 MeV proton. The sample is measured 21 days after the end of bombardment. Select the Pa isotope(s) present in the sample. 4.10.
To maximize the production of 225
Ac, what proton energy on target in MeV should be used?
5.
(20 Points) The generation of the medical isotope 225
Ac can use 229
Th as a parent. There is 229
Th available which has a significant amount of 228
Th. An isotope from the decay of 228
Th produces a gamma ray with an energy of 2.6 MeV. A generator with this 228
Th requires shielding to limit dose. The mass attenuation coefficient (
µ/ρ
) of a 2.6 MeV photon in Pb is 4.38E-2 cm
2
g
-1
5
. The attenuation of the photon is found through: I
f
=I
o
e-
((
µ/ρ
)x
ρ
)
where the density of Pb (
ρ)
is 11.35 g mL
-1
. The thickness of Pb is cm is x. 5.1.
What is the half-thickness of Pb for a 2.6 MeV gamma ray? 5.2.
How thick of a Pb layer is needed to reduce the dose from the 2.6 MeV gamma ray to 5 % of the initial dose? 5.3.
At the edge of a glovebox containing a 225
Ac generator with 229
Th and 228
Th, the measured dose is 40 mrem/hr. You wish to have a dose of 5 mrem/hr at the edge of the glovebox. What thickness of Pb shielding in cm should be used? 5.4.
What is the isotope from the 228
Th decay chain that is the source of the 2.6 MeV photon? 5.5.
Why not separate the 228
Th from the 229
Th to remove the source of the dose? 5.6.
The figure below shows the cross sections for the different photon interaction with Pb. Which is the primary interaction for the photon of concern for the progeny of 228
Th discussed above.?
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6.
(5 Points). Discuss the relationship between fission and criticality
.
7.
(5 Points) A recent article postulates an extremely dense asteroid may contain superheavy elements
6
. An estimated density of an element with Z=162 is between 36.0 4 g cm
-3
and 68.4 g cm
-3
. For this element to be reasonable to exist, say with a long half-life, estimate its atomic mass A. 8.
(Bonus 5 Points) What name would you give this element? References (1) Flynn, K. F.; Gindler, J. E.; Glendenin, L. E. Mass Distributions for the Spontaneous Fission of 248Cm and 250Cf. Journal of Inorganic and Nuclear Chemistry
1977
, 39
(5), 759–762. https://doi.org/10.1016/0022-1902(77)80149-8.
(2) Hoffman, D. C.; Ford, G. P.; Balagna, J. P. Kinetic Energy Distributions in the Spontaneous Fission of Cm250 and Cf250. Phys Rev C
1973
, 7
(1), 276–279. https://doi.org/10.1103/PhysRevC.7.276. (3) Thiele, N. A.; Wilson, J. J. Actinium-
225 for Targeted α Therapy: Coordination Chemistry and Current Chelation Approaches. Cancer Biother Radiopharm
2018
, 33
(8), 336–348. https://doi.org/10.1089/cbr.2018.2494. (4) Griswold, J. R.; Jost, C. U.; Stracener, D. W.; Bruffey, S. H.; Denton, D.; Garland, M.; Heilbronn, L.; Mirzadeh, S. Production of 229Th for Medical Applications: Excitation Functions of Low-Energy Protons on 232Th Targets. Phys Rev C
2018
, 98
(4), 044607. https://doi.org/10.1103/PhysRevC.98.044607. (5) X-Ray Mass Attenuation Coefficients
. https://physics.nist.gov/PhysRefData/XrayMassCoef/chap2.html (accessed 2024-02-06). (6) LaForge, E.; Price, W.; Rafelski, J. Superheavy Elements and Ultradense Matter. Eur Phys J Plus
2023
, 138
(9). https://doi.org/10.1140/epjp/s13360-023-04454-8.
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