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Naturally found uranium consists of \(99.274 \%{ }^{238} \mathrm{U},\) \(0.720 \%^{235} \mathrm{U},\) and \(0.006 \%^{233} \mathrm{U}\). As we have seen, \({ }^{235} \mathrm{U}\) is the isotope that can undergo a nuclear chain reaction. Most of the \({ }^{235} \mathrm{U}\) used in the first atomic bomb was obtained by gaseous diffusion of uranium hexafluoride, \(\mathrm{UF}_{6}(g) .(\mathbf{a})\) What is the mass of \(\mathrm{UF}_{6}\) in a 30.0 -L vessel of \(\mathrm{UF}_{6}\) at a pressure of 695 torr at \(350 \mathrm{~K} ?\) (b) What is the mass of \({ }^{235} \mathrm{U}\) in the sample described in part (a)? (c) Now suppose that the UF \(_{6}\) is diffused through a porous barrier and that the change in the ratio of \({ }^{238} \mathrm{U}\) and \({ }^{235} \mathrm{U}\) in the diffused gas can be described by Equation \(10.23 .\) What is the mass of \({ }^{235} \mathrm{U}\) in a sample of

Short Answer

Expert verified
(a) The mass of UF6 in the 30.0-L vessel is 35.2 g. (b) The mass of \({ }^{235}\mathrm{U}\) in the sample is 0.173 g. (c) We cannot solve part (c) without knowing Equation 10.23.

Step by step solution

01

Use the Ideal Gas Law to find the moles of UF6 in the gas

To calculate the moles of UF6 in the gas, we will use the Ideal Gas Law equation: \(PV = nRT\) Where P is the pressure in atm, V is the volume in liters, n is the moles of UF6, R is the gas constant (0.0821 L atm/mol K), and T is the temperature in Kelvin. First, we need to convert the pressure from torr to atm: 695 torr * (1 atm/760 torr) = 0.914 atm Now, plug in the values and solve for n: \( (0.914 \mathrm{atm})(30.0 \mathrm{L}) = n(0.0821\frac{\mathrm{ L\cdot atm}}{\mathrm{mol\cdot K}})(350 \mathrm{K})\)
02

Calculate the moles of UF6

We can now solve for n and find the number of moles: \(n = \frac{(0.914 \mathrm{atm})(30.0 \mathrm{L})}{(0.0821\frac{\mathrm{ L\cdot atm}}{\mathrm{mol\cdot K}})(350 \mathrm{K})} = 0.100 \mathrm{mol}\)
03

Convert moles of UF6 to mass

To convert the moles of UF6 to mass, we need to find the molar mass of UF6, which is: 1 U: 238 g/mol 6 F: 6 * 19 g/mol = 114 g/mol Total: 238 + 114 = 352 g/mol Now we can multiply the moles of UF6 by its molar mass to find the mass: (0.100 mol)(352 g/mol) = 35.2 g
04

Calculate the mass of \({ }^{235}\mathrm{U}\) in the sample

First, calculate the total molar mass of uranium in the sample by multiplying the mass of UF6 by the mass fraction of uranium: (35.2 g) * (238 g/mol) / (352 g/mol) = 24.0 g Next, find the mass of \({ }^{235}\mathrm{U}\) in the sample, knowing that natural uranium contains 0.720% of \({ }^{235}\mathrm{U}\): (24.0 g) * (0.00720) = 0.173 g
05

Calculate the mass of \({ }^{235}\mathrm{U}\) in the sample of diffused gas

We are not given a direct method for finding the mass of \({ }^{235}\mathrm{U}\) after diffusion has occurred. We are however told the change in the ratio can be described by Equation 10.23. Without knowing this equation, we cannot solve part (c).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Uranium Isotopes
Uranium isotopes are naturally occurring variants of the element uranium, distinguished by the number of neutrons within their nuclear core. The most common isotopes are
  • \(^{238}\mathrm{U}\): This is the most abundant isotope of uranium, making up approximately 99.274% of natural uranium. It has 146 neutrons.
  • \(^{235}\mathrm{U}\): This isotope constitutes about 0.720% of uranium and is notable for being fissile, meaning it can sustain a chain reaction when bombarded by neutrons, making it crucial for nuclear reactors and weapons.
  • \(^{233}\mathrm{U}\): Although present in negligible amounts of 0.006%, it's used in certain nuclear applications such as thorium fuel cycles.
Understanding these isotopes is key, especially since the nuclear reactions of \(^{235}\mathrm{U}\) provide a powerful energy source. The unique properties and reactivities of these isotopes highlight the complexity and the potential of nuclear chemistry. Each isotope has its own set of properties, uses, and implications for both energy generation and weaponry.
Molar Mass Calculation
Molar mass is a fundamental concept in chemistry, representing the mass of one mole of a given substance. It is calculated by summing the atomic masses of each element in a compound, adjusted for the number of each type of atom present.
For example, for uranium hexafluoride (\( \mathrm{UF}_6 \)), we calculate its molar mass as follows:
  • Determine the atomic mass of uranium (U), which is approximately 238 g/mol.
  • Each fluorine atom (F) has an atomic mass of roughly 19 g/mol. As there are six fluorine atoms in \( \mathrm{UF}_6 \), their combined mass is \(6 \times 19 = 114 \text{ g/mol} \).
  • Adding these, the molar mass of \( \mathrm{UF}_6 \) becomes \(238 + 114 = 352 \text{ g/mol} \).
Knowing the molar mass allows us to convert between the moles and grams, which is crucial in stoichiometric calculations as seen in the context of uranium isotope separation and use in nuclear processes.
Gaseous Diffusion
Gaseous diffusion is a method used to separate isotopes of uranium, particularly to increase the concentration of \(^{235}\mathrm{U}\) in uranium hexafluoride (\(\mathrm{UF}_6\)).
This separation technique exploits the small differences in the molecular weights of the isotopes:
  • \(\mathrm{UF}_6\) containing \(^{235}\mathrm{U}\) is slightly lighter than that with \(^{238}\mathrm{U}\).
  • By passing the gas through a barrier with tiny pores, the lighter \(^{235}\mathrm{U}F_6\) molecules diffuse more readily than their heavier \(^{238}\mathrm{U}F_6\) counterparts.
This process gradually collects a sample with a higher proportion of \(^{235}\mathrm{U}\). While effective, it's energy-intensive, requiring several diffusion stages to achieve significant enrichment levels.
Understanding gaseous diffusion is fundamentally important for nuclear fuel preparation, influencing everything from power generation to international policies on nuclear material handling and non-proliferation.
Stoichiometry in Chemistry
Stoichiometry in chemistry involves the calculation of reactants and products in chemical reactions. It is essential for predicting the results of reactions and for scaling them for various applications.
Key aspects of stoichiometry include:
  • Molar Ratios: These are derived from the balanced chemical equation and indicate the proportion of reactants and products involved.
  • Mole to Mass Conversions: By using molar masses, chemists convert between the mass of a substance and the number of moles.
  • Limiting Reactant: This component determines the maximum extent of the reaction, as it's completely consumed. Understanding this allows for optimization of reactant quantities to maximize yield and efficiency.
In the context of uranium processing for nuclear reactions, stoichiometry helps determine the precise amounts of \(^{235}\mathrm{U}\) required and the byproducts expected in reactions, ensuring both safety and efficiency in the handling of nuclear materials.

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Most popular questions from this chapter

The Sun radiates energy into space at the rate of \(3.9 \times 10^{26} \mathrm{~J} / \mathrm{s} .\) (a) Calculate the rate of mass loss from the Sun in kg/s. (b) How does this mass loss arise? (c) It is estimated that the Sun contains \(9 \times 10^{56}\) free protons. How many protons per second are consumed in nuclear reactions in the Sun?

In 2002 , a team of scientists from Russia and the United States reported the creation of the first atom of element 118 , which is named oganesson, and whose symbol is Og. The synthesis involved the collision of californium- 249 atoms with accelerated ions of an atom which we will denote X. In the synthesis, an oganesson-294 is formed together with three neutrons. $$ { }_{98}^{249} \mathrm{Cf}+\mathrm{X} \longrightarrow{ }_{118}^{294} \mathrm{Og}+3{ }_{0}^{1} \mathrm{n} $$ (a) What are the identities of isotopes X? (b) Isotope \(X\) is unusual in that it is very long-lived (its half-life is on the order of \(10^{19} \mathrm{yr}\) ) in spite of having an unfavorable neutron-to-proton ratio (Figure 21.1). Can you propose a reason for its unusual stability? (c) Oganesson-294 decays into livermorium-290 by alpha decay. Write a balanced equation for this.

It takes 180 minutes for a 200 -mg sample of an unknown radioactive substance to decay to \(112 \mathrm{mg}\). What is the halflife of this substance?

Decay of which nucleus will lead to the following products: (a) uranium-235 by alpha decay; (b) aluminium-26 by positron emission; \((\mathbf{c})\) deuterium by alpha decay; (d) yttrium-90 by beta decay?

Cobalt-60 is a strong gamma emitter that has a half-life of \(5.26 \mathrm{yr}\). The cobalt- 60 in a radiotherapy unit must be replaced when its radioactivity falls to \(75 \%\) of the original sample. If an original sample was purchased in June \(2016,\) when will it be necessary to replace the cobalt- \(60 ?\)

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