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The values of the masses in the reaction \(p+{ }^{19} F \rightarrow \alpha+{ }^{16} O\) have been determined by a mass spectrometer to have the values: $$ \begin{aligned} m(p) &=1.007825 u, \\ m(F) &=18.998405 u, \\ m(\alpha) &=4.002603 u, \\ m(O) &=15.994915 u . \end{aligned} $$ Here \(u\) is the atomic mass unit (Section 1.7). How much energy is released in this reaction? Express your answer in both kilograms and \(\mathrm{MeV}\).

Short Answer

Expert verified
Energy released: 1.4461912 x 10^{-29} kg or 8.121 MeV.

Step by step solution

01

Calculate the initial mass of reactants

The reactants in the reaction are a proton \( m(p) \) and a \( {}^{19}F \) nucleus. Add these masses to get the total initial mass: \[ m_{\text{initial}} = m(p) + m(F) = 1.007825 \text{u} + 18.998405 \text{u} = 20.006230 \text{u} \]
02

Calculate the final mass of products

The products in the reaction are an alpha particle \( m(\alpha) \) and an \( {}^{16}O \) nucleus. Add these masses to get the total final mass: \[ m_{\text{final}} = m(\alpha) + m(O) = 4.002603 \text{u} + 15.994915 \text{u} = 19.997518 \text{u} \]
03

Calculate the mass defect

The mass defect \( \Delta m \) is the difference between the initial mass and the final mass: \[ \Delta m = m_{\text{initial}} - m_{\text{final}} = 20.006230 \text{u} - 19.997518 \text{u} = 0.008712 \text{u} \]
04

Convert the mass defect to kilograms

To convert the mass defect from atomic mass units to kilograms, use the conversion factor \( 1 \text{u} = 1.660539 \times 10^{-27} \text{kg} \): \[ \Delta m = 0.008712 \text{u} \times 1.660539 \times 10^{-27} \text{kg/u} = 1.4461912 \times 10^{-29} \text{kg} \]
05

Calculate the energy released in joules

The energy equivalent (E) of the mass defect can be calculated using Einstein's equation \( E = \Delta m \times c^2 \), where \( c \) is the speed of light \( ( 3 \times 10^8 \text{m/s}) \): \[ E = 1.4461912 \times 10^{-29} \text{kg} \times (3 \times 10^8 \text{m/s})^2 = 1.30157208 \times 10^{-12} \text{J} \]
06

Convert the energy from joules to MeV

To convert the energy from joules to mega-electron volts (MeV), use the conversion factor \( 1 \text{J} = 6.242 \times 10^{12} \text{MeV} \): \[ E = 1.30157208 \times 10^{-12} \text{J} \times 6.242 \times 10^{12} \text{MeV} / \text{J} = 8.121 \text{MeV} \]

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Key Concepts

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

mass defect
When we look at nuclear reactions like the one described in the problem, one of the key concepts to understand is the 'mass defect'. The mass defect refers to the difference between the mass of the reactants and the mass of the products in a nuclear reaction.
During the reaction, some of the mass of the reactants is converted into energy. This 'missing' mass, or mass defect, is crucial for understanding the energy release in nuclear reactions.
In our example reaction, we calculated the initial mass of the reactants (proton and fluorine nucleus) and the final mass of the products (alpha particle and oxygen nucleus). By subtracting the final mass from the initial mass, we discovered the mass defect:
\( \text{mass defect} = 20.006230 \text{u} - 19.997518 \text{u} = 0.008712 \text{u} \)
Understanding this difference in mass is fundamental to finding out how much energy is released during the reaction.
Einstein's equation
The next crucial concept is 'Einstein's equation'. Albert Einstein's famous equation, \( E = mc^2 \), explains the relationship between mass (m) and energy (E), where \( c \) is the speed of light in a vacuum (approximately \( 3 \times 10^8 \text{m/s} \)). This equation tells us that a small amount of mass can be converted into a large amount of energy.
Let's break it down step-by-step:
  • \( E \) is the energy,
  • \( m \) is the mass, and
  • \( c \) is the speed of light.
Using Einstein's equation, we can calculate the energy equivalent of the mass defect identified earlier. The mass defect in our problem was \( 0.008712 \text{u} \).
First, we convert this mass into kilograms to use in the equation.
Then we use Einstein's equation to find the energy \( E = \text{mass} \times (\text{speed of light})^2 \). This gives us the total energy released during the reaction.
mass-energy equivalence
Mass-Energy Equivalence is a principle derived from Einstein's equation. It means that mass and energy are two forms of the same thing; they can be converted into each other. This principle is fundamentally important in nuclear physics and helps us understand how nuclear reactions release such immense amounts of energy.
When a nucleus forms from nucleons, the mass of the nucleus is slightly less than the sum of its parts. The 'lost' mass has been converted into binding energy which holds the nucleus together.
In the example provided, the difference in mass (mass defect) represents the energy released during the fusion process:
With the mass defect \( (\text{mass defect} = 0.008712 \text{u}) \), we used Einstein's equation to show how this small amount of mass converts into a significant energy release, illustrating mass-energy equivalence in action.
atomic mass unit conversion
Understanding 'atomic mass unit conversion' is essential in these kinds of problems. The atomic mass unit (u) is a standard unit used to express atomic and molecular masses. It's defined as one-twelfth of the mass of a carbon-12 atom.
In our calculations, we extensively used this unit. To convert the mass defect from atomic mass units to kilograms, we used the conversion factor:
  • 1 u = 1.660539 \times 10^{-27} kg.
This conversion allows us to use the mass in Einstein's equation, which requires mass in kilograms.
Applying this conversion in our problem:
\( \text{mass defect} = 0.008712 \text{u} \times 1.660539 \times 10^{-27} \text{kg/u} = 1.4461912 \times 10^{-29} \text{kg} \)
Understanding and applying the atomic mass unit conversion correctly is critical to bridging the gap between atomic scale measurements and the macroscopic quantities of energy that we can observe and measure.

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Most popular questions from this chapter

An evacuated tube at rest in the laboratory has a length \(3.00 \mathrm{~m}\) as measured in the laboratory. An electron moves at speed \(v=0.999987 \mathrm{c}\) in the laboratory along the axis of this evacuated tube. What is the length of the tube measured in the rest frame of the electron?

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(a) Two events occur at the same time in the laboratory frame and at the laboratory coordinates \(\left(x_{1}=\right.\) \(\left.10 \mathrm{~km}, y_{1}=4 \mathrm{~km}, z_{1}=6 \mathrm{~km}\right)\) and \(\left(x_{2}=10 \mathrm{~km}, y_{2}=7 \mathrm{~km}, z_{2}=\right.\) \(-10 \mathrm{~km})\). Will these two events be simultaneous in a rocket frame moving with speed \(v^{\text {rel }}=0.8 c\) in the \(x\) direction in the laboratory frame? Explain your answer. (b) Three events occur at the same time in the laboratory frame and at the laboratory coordinates \(\left(x_{0}, y_{1}, z_{1}\right),\left(x_{0}, y_{2}, z_{2}\right)\), and \(\left(x_{0}, y_{3}, z_{3}\right)\), where \(x_{0}\) has the same value for all three events. Will these three events be simultaneous in a rocket frame moving with speed \(v^{\text {rel }}\) in the laboratory \(x\) direction? Explain your answer. (c) Use your results of parts (a) and (b) to make a general statement about simultaneity of events in laboratory and rocket frames.

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