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PHYSICS, M8 2023 HSC 26

Consider the following nuclear reaction

\({ }_{\ \ 6}^{12} \text{C} +{ }_1^1 \text{H} \rightarrow{ }_5^9 \text{B} +{ }_2^4 \text{He}\)

The masses of the isotopes in this process are shown in the table.

Isotope Mass (\(u\))
\({ }_{\ \ 6}^{12} \text{C}\) 12.064
\({ }_5^9 \text{B}\) 9.013
\({ }_2^4 \text{He}\) 4.003
\({ }_1^1 \text{H}\) 1.008
Calculate the energy released in this reaction.  (3 marks)

--- 6 WORK AREA LINES (style=lined) ---

Show Answers Only

\(52.164\) \(\text{MeV}\)  or  \(8.357 \times 10^{-12}\) \(\text{J}\)

Show Worked Solution

\(\text{Mass defect}\) \(=m_r-m_p\)  
  \(=(12.064+1.008)-(9.013+4.003)\)  
  \(=0.056\) \(\text{u}\)  

 

\(\text{Energy released}\) \(= 0.056 \times 931.5\) \(\text{MeV}\)  
  \(=52.164\) \(\text{MeV}\)  
  \(=8.357 \times 10^{-12} \) \(\text{J}\)  

Filed Under: Properties of the Nucleus Tagged With: Band 4, smc-3703-20-Conservation of Mass-Energy

PHYSICS, M8 2023 HSC 13 MC

Nucleus \(X\) has a greater binding energy than nucleus \(Y\).

What can be deduced about \(X\) and \(Y\) ?

  1. \(X\) is more stable than \(Y\).
  2. \(Y\) is more stable than \(X\).
  3. \(X\) has a greater mass defect than \(Y\).
  4. \(Y\) has a greater mass defect than \(X\).
Show Answers Only

\(C\)

Show Worked Solution
  • Binding energy is the energy required to split a nucleus into its nucleons. 
  • The mass of the nucleus is less than the sum of the nucleons. The mass equivalent of the binding energy is equal to the mass defect.
  • As nucleus \(X\) has a greater binding energy than nucleus \(Y\), it can be deduced that it also has a greater mass defect.

\(\Rightarrow C\)

♦ Mean mark 43%.

Filed Under: Properties of the Nucleus Tagged With: Band 5, smc-3703-20-Conservation of Mass-Energy

PHYSICS, M8 EQ-Bank 22

Einstein's equation `E = mc^(2)`  is one of the most important equations in the history of physics.

Justify this statement.   (7 marks)

--- 14 WORK AREA LINES (style=lined) ---

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Position Statement

  • Einstein’s equation `E=mc^2` is among physics’ most important equations because it reveals mass-energy equivalence and explains fundamental processes from atomic to cosmic scales.

Nuclear Applications

  • The equation explains energy from nuclear fission and fusion processes. It shows how tiny amounts of matter convert to enormous energy in nuclear reactions.
  • The mass defect in atoms directly relates to binding energy through `E=mc^2` and this principle drives nuclear reactors that power cities and nuclear weapons.
  • These applications are responsible for revolutionising both energy production and global politics.

Cosmic and Particle Physics

  • Stars produce energy by converting mass to energy through fusion reactions. The Sun converts 4 million tonnes of mass to energy every second using this principle
  • Particle accelerators create new particles by converting kinetic energy into mass. This allows scientists to study fundamental matter structure and discover new particles.
  • Furthermore, mass dilation near light speed also follows from this mass-energy relationship.

Reinforcement

  • While other equations like Newton’s gravity law are important, they lack the broad applicability of `E=mc^2`.
  • No other single equation explains phenomena from subatomic particles to stellar processes.
  • The equation unified our understanding of matter and energy as different forms of the same thing.
  • This justifies calling `E=mc^2` one of history’s most important physics equations.
Show Worked Solution

Position Statement

  • Einstein’s equation `E=mc^2` is among physics’ most important equations because it reveals mass-energy equivalence and explains fundamental processes from atomic to cosmic scales.

Nuclear Applications

  • The equation explains energy from nuclear fission and fusion processes. It shows how tiny amounts of matter convert to enormous energy in nuclear reactions.
  • The mass defect in atoms directly relates to binding energy through `E=mc^2` and this principle drives nuclear reactors that power cities and nuclear weapons.
  • These applications are responsible for revolutionising both energy production and global politics.

Cosmic and Particle Physics

  • Stars produce energy by converting mass to energy through fusion reactions. The Sun converts 4 million tonnes of mass to energy every second using this principle
  • Particle accelerators create new particles by converting kinetic energy into mass. This allows scientists to study fundamental matter structure and discover new particles.
  • Furthermore, mass dilation near light speed also follows from this mass-energy relationship.

Reinforcement

  • While other equations like Newton’s gravity law are important, they lack the broad applicability of `E=mc^2`.
  • No other single equation explains phenomena from subatomic particles to stellar processes.
  • The equation unified our understanding of matter and energy as different forms of the same thing.
  • This justifies calling `E=mc^2` one of history’s most important physics equations.

Filed Under: Light and Special Relativity, Origins of Elements, Properties of the Nucleus Tagged With: Band 3, Band 4, Band 5, smc-3699-80-E = mc^2, smc-3700-60-Mass-Energy Equivalence, smc-3703-20-Conservation of Mass-Energy

PHYSICS, M8 EQ-Bank 7 MC

The following equation describes the natural decay process of uranium-238.

\({ }_{92}^{238} \text{U} \rightarrow{ }_{90}^{234}\text{Th} +{ }_2^4 \text{He}\)

Which row of the table describes the changes in total mass and total binding energy in the decay of uranium-238?

\begin{align*}
\begin{array}{l}
\rule{0pt}{2.5ex} \ \rule[-1ex]{0pt}{0pt}& \\
\rule{0pt}{2.5ex}\textbf{A.}\rule[-1ex]{0pt}{0pt}\\
\rule{0pt}{2.5ex}\textbf{B.}\rule[-1ex]{0pt}{0pt}\\
\rule{0pt}{2.5ex}\textbf{C.}\rule[-1ex]{0pt}{0pt}\\
\rule{0pt}{2.5ex}\textbf{D.}\rule[-1ex]{0pt}{0pt}\\
\end{array}
\begin{array}{|c|c|}
\hline
\rule{0pt}{2.5ex}\quad \quad \textit{Total mass}\quad  \quad \rule[-1ex]{0pt}{0pt}& \textit{Total binding energy} \\
\hline
\rule{0pt}{2.5ex}\text{Decreases}\rule[-1ex]{0pt}{0pt}&\text{Increases}\\
\hline
\rule{0pt}{2.5ex}\text{Decreases}\rule[-1ex]{0pt}{0pt}& \text{Decreases}\\
\hline
\rule{0pt}{2.5ex}\text{Increases}\rule[-1ex]{0pt}{0pt}& \text{Increases} \\
\hline
\rule{0pt}{2.5ex}\text{Increases}\rule[-1ex]{0pt}{0pt}& \text{Decreases} \\
\hline
\end{array}
\end{align*}

Show Answers Only

\(A\)

Show Worked Solution
  • Mass is converted into energy in this nuclear reaction, so total mass decreases.
  • When elements heavier than iron undergo nuclear fission, the daughter nuclei produced are more stable with a greater binding energy per nucleon. As there are the same number of nucleons before and after the decay, total binding energy increases.

\(\Rightarrow A\)

Filed Under: Properties of the Nucleus Tagged With: Band 4, smc-3703-20-Conservation of Mass-Energy, smc-3703-50-Nuclear Fission

PHYSICS, M8 2019 HSC 36

A radon-198 atom, initially at rest, undergoes alpha decay. The masses of the atoms involved are shown in atomic mass units `(u)`. 
 

The kinetic energy of the polonium atom produced is  `2.55 × 10^(-14)` J.

By considering mass defect, calculate the kinetic energy of the alpha particle, and explain why it is significantly greater than that of the polonium atom.   (7 marks)

--- 14 WORK AREA LINES (style=lined) ---

Show Answers Only
`Delta m` `=197.999-(193.988+4.000260)`  
  `=0.0084\ \text{u}`  
  `=0.0084 xx1.661 xx10^(-27)` (Converting to kg)
  `=1.395 xx10^(-29)\ \text{kg}`  

 

`E` `=mc^2`  
  `=1.395 xx10^(-29)xx(3xx10^(8))^(2)`  
  `=1.256 xx10^(-12)\ \text{J}`  

 
Applying the law of conservation of energy:

   `KE_(text{alpha})` `=E_(text{total})-KE_(polonium)`  
  `=1.256 xx10^(-12)-2.44 xx10^(-14)`  
  `=1.23 xx10^(-12)\ \text{J}`  
     
  •  As the radon atom is initially at rest, the initial momentum of this reaction system is zero. So, by applying the principle of conservation of momentum, the decay products must move away from each other with equal and opposite momenta.
  • The alpha particle has a significantly lower mass compared to the polonium atom and therefore has a significantly higher velocity.
  • `KE=(1)/(2)mv^(2)=(1)/(2)mv xx v`  and the momenta, `mv`  are equal for both the alpha particle and polonium atom. The alpha particle therefore has a significantly greater kinetic energy due to its greater velocity.
Show Worked Solution
`Delta m` `=197.999-(193.988+4.000260)`  
  `=0.0084\ \text{u}`  
  `=0.0084 xx1.661 xx10^(-27)` (Converting to kg)
  `=1.395 xx10^(-29)\ \text{kg}`  

 

`E` `=mc^2`  
  `=1.395 xx10^(-29)xx(3xx10^(8))^(2)`  
  `=1.256 xx10^(-12)\ \text{J}`  

 
Applying the law of conservation of energy:

   `KE_(text{alpha})` `=E_(text{total})-KE_(polonium)`  
  `=1.256 xx10^(-12)-2.44 xx10^(-14)`  
  `=1.23 xx10^(-12)\ \text{J}`  
     
  •  As the radon atom is initially at rest, the initial momentum of this reaction system is zero. So, by applying the principle of conservation of momentum, the decay products must move away from each other with equal and opposite momenta.
  • The alpha particle has a significantly lower mass compared to the polonium atom and therefore has a significantly higher velocity.
  • `KE=(1)/(2)mv^(2)=(1)/(2)mv xx v`  and the momenta, `mv`  are equal for both the alpha particle and polonium atom. The alpha particle therefore has a significantly greater kinetic energy due to its greater velocity.

♦♦♦ Mean mark 30%.

Filed Under: Properties of the Nucleus Tagged With: Band 5, Band 6, smc-3703-10-Nuclear Reactions, smc-3703-20-Conservation of Mass-Energy, smc-3703-50-Nuclear Fission

PHYSICS, M8 2019 HSC 34

Use the following information to answer this question.
 

Describe both the production and radiation of energy by the sun. In your answer, include a quantitative analysis of both the power output and the surface temperature of the sun.   (9 marks)

--- 22 WORK AREA LINES (style=lined) ---

Show Answers Only
  • Production of the sun’s energy is predominantly done through the proton-proton chain.
  • Four protons react in the sun’s core to produce one helium atom. The mass of one helium atom is less than the mass of four protons so mass is converted into energy through Einstein’s mass-energy equivalence, `E=mc^2.`
  • The sun acts as a black body and so radiates its energy in the form of black body radiation.
  • It radiates energy as light with a variety of wavelengths, as shown in the black body curve above. It peaks at a specific wavelength which can be used to calculate its temperature:
  •    `lambda_(max)=5.0xx10^-7` m  (see graph above)
  • Using  `lambda_(max)=(b)/(T)`
  •   `T=(2.898xx10^-3)/(5.0xx10^-7)=5796\ \text{K}`
  • Energy radiated from the sun spreads out over a sphere as it travels away from the sun. The intensity of radiated energy decreases at distances further from the sun, consistent with the inverse square law.
  • Using the intensity of the sun’s radiation at earth, its power output can be calculated using  `P=IA`:
  •    `P=Ixx4pi r^2=1360 xx4xx3.142 xx(1.5 xx10^(11))^(2)=3.85 xx10^(26)\ \text{W}`
Show Worked Solution
  • Production of the sun’s energy is predominantly done through the proton-proton chain.
  • Four protons react in the sun’s core to produce one helium atom. The mass of one helium atom is less than the mass of four protons so mass is converted into energy through Einstein’s mass-energy equivalence, `E=mc^2.`
  • The sun acts as a black body and so radiates its energy in the form of black body radiation.
  • It radiates energy as light with a variety of wavelengths, as shown in the black body curve above. It peaks at a specific wavelength which can be used to calculate its temperature:
  •    `lambda_(max)=5.0xx10^-7` m  (see graph above)
  • Using  `lambda_(max)=(b)/(T)`
  •   `T=(2.898xx10^-3)/(5.0xx10^-7)=5796\ \text{K}`
  • Energy radiated from the sun spreads out over a sphere as it travels away from the sun. The intensity of radiated energy decreases at distances further from the sun, consistent with the inverse square law.
  • Using the intensity of the sun’s radiation at earth, its power output can be calculated using  `P=IA`:
  •    `P=Ixx4pi r^2=1360 xx4xx3.142 xx(1.5 xx10^(11))^(2)=3.85 xx10^(26)\ \text{W}`

♦♦♦ Mean mark 38%.

Filed Under: Light: Quantum Model, Properties of the Nucleus Tagged With: Band 5, Band 6, smc-3703-10-Nuclear Reactions, smc-3703-20-Conservation of Mass-Energy

PHYSICS M8 2022 HSC 16 MC

The binding energy of helium-4 (He-4) is 28.3 MeV and the binding energy of beryllium-6 (Be-6) is 26.9 MeV.

Which of the following rows in the table is correct?
 

\begin{align*}
\begin{array}{l}
\rule{0pt}{2.5ex}\textbf{A.} & \\
\textbf{}\rule[-1ex]{0pt}{0pt}\\
\rule{0pt}{2.5ex}\textbf{B.}\\
\textbf{}\rule[-1ex]{0pt}{0pt}\\
\rule{0pt}{2.5ex}\textbf{C.}\\
\textbf{}\rule[-1ex]{0pt}{0pt}\\
\rule{0pt}{2.5ex}\textbf{D.}\\
\textbf{}\rule[-1ex]{0pt}{0pt}\\
\end{array}
\begin{array}{|l|l|}
\hline
\rule{0pt}{2.5ex}\text{He-4 requires more energy to separate}\quad & \text{He-4 is less massive than Be-6} \\
\text{into individual protons and neutrons}\rule[-1ex]{0pt}{0pt}&\text{}\\
\hline
\rule{0pt}{2.5ex}\text{He-4 requires less energy to separate}& \text{He-4 is less massive than Be-6}\\
\text{into individual protons and neutrons}\rule[-1ex]{0pt}{0pt}&\text{}\\
\hline
\rule{0pt}{2.5ex}\text{He-4 requires more energy to separate}& \text{He-4 is more massive than Be-6}\\
\text{into individual protons and neutrons}\rule[-1ex]{0pt}{0pt}&\text{}\\
\hline
\rule{0pt}{2.5ex}\text{He-4 requires less energy to separate}& \text{He-4 is more massive than Be-6} \quad \\
\text{into individual protons and neutrons}\rule[-1ex]{0pt}{0pt}&\text{}\\
\hline
\end{array}
\end{align*}

Show Answers Only

\(A\)

Show Worked Solution
  • The binding energy of a nucleus is the energy required to separate it into individual particles.
  • He-4 requires more energy to separate into individual protons and neutrons.
  • He-4 has 4 nucleons while Be-6 has 6 nucleons.
  • He-4 is less massive.

\(\Rightarrow A\)

Filed Under: Properties of the Nucleus Tagged With: Band 4, smc-3703-10-Nuclear Reactions, smc-3703-20-Conservation of Mass-Energy

PHYSICS, M8 2019 HSC 19 MC

Consider the following nuclear reaction.

\(\text{W} + \text{X} \rightarrow \text{Y} + \text{Z}\)

Information about W, X and Y is given in the table.

\begin{array}{|c|c|}
\hline
\rule{0pt}{2.5ex}\textit{Species} & \textit{Mass defect} & \textit{Total binding energy} & \textit{Binding energy per nucleon}\\
\textit{} & \textit{(u)} \rule[-1ex]{0pt}{0pt}& \text{(MeV)} & \text{(MeV)}\\
\hline \rule{0pt}{2.5ex}\text{W} \rule[-1ex]{0pt}{0pt}& 0.00238817 & 2.224566 & 1.112283 \\
\hline \rule{0pt}{2.5ex}\text{X} \rule[-1ex]{0pt}{0pt}& 0.00910558 & 8.481798 & 2.827266 \\
\hline \rule{0pt}{2.5ex}\text{Y }\rule[-1ex]{0pt}{0pt}& 0.03037664 & 28.29566 & 7.073915 \\
\hline
\end{array}

Which of the following is a correct statement about energy in this reaction?

  1. The reaction gives out energy because the mass defect of \(\text{Y}\) is greater than that of either \(\text{W}\) or \(\text{X}\).
  2. It cannot be deduced whether the reaction releases energy because the properties of \(\text{Z}\) are not known.
  3. The reaction requires an input of energy because the mass defect of the products is greater than the sum of the mass defects of the reactants.
  4. Energy is released by the reaction because the binding energy of the products is greater than the sum of the binding energies of the reactants.
Show Answers Only

\(D\)

Show Worked Solution
  • Energy required to break \(\text{W}\) and \(\text{X}\) into their constituent nucleons:
  •    \(2.22+8.48=10.70 \ \text{MeV}\)
  • Energy released in the formation of the products is given by the sum of binding energies of \(\text{Y}\) and \(\text{Z}\):
  •    \(28.30\  \text{MeV} +\) binding energy of \(\text{Z}\)
  • As this is greater than the sum of binding energies of the reactants regardless of the binding energy of \(\text{Z}\), there is a net release of energy in the reaction.

\(\Rightarrow D\)


♦ Mean mark 31%.

Filed Under: Properties of the Nucleus Tagged With: Band 5, smc-3703-10-Nuclear Reactions, smc-3703-20-Conservation of Mass-Energy

PHYSICS, M8 2021 HSC 35

A spacecraft is powered by a radioisotope generator. Pu-238 in the generator undergoes alpha decay, releasing energy. The decay is shown with the mass of each species in atomic mass units, `u`

\begin{array} {ccccc}
\ce{^{238}Pu} & \rightarrow & \ce{^{234}U} & + & \alpha \\
238.0495\ u &  & 234.0409\ u &  & 4.0026\ u \end{array}

  1. Show that the energy released by one decay is  `9.0 × 10^(-13)` J.   (3 marks)

    --- 6 WORK AREA LINES (style=lined) ---

  1. At launch, the generator contains  `9.0 × 10^24`  atoms of Pu-238. The half-life of Pu-238 is 87.7 years.
  2. Calculate the total energy produced by the generator during the first ten years after launch.  (3 marks)

    --- 6 WORK AREA LINES (style=lined) ---

Show Answers Only
  1. `9.0xx10^(-13)\ \text{J}`
  2. `6.2xx10^(11)\ \text{J}`
Show Worked Solution

a.   `text{Find Energy released:}`

`Delta m` `=(234.0409+4.0026)-238.0495=-0.006\ u`  
`Delta m` `=0.006 xx1.661 xx10^(-27)=9.966 xx10^(-30)\ \text{kg}`  

  
`\text{Using}\ \ E=mc^2:`

`E_text{released}=9.966 xx10^(-30)xx(3xx10^(8))^(2)=9.0 xx10^(-13)\ \text{J}`

   

b.   `\text{Find total energy:}`

`lambda=(ln 2)/(t_((1)/(2)))=(ln 2)/(87.7)=0.0079\ text{year}^(-1)`

`N=N_(0)e^(-lambda t)=9xx10^(24)xxe^(-0.0079 xx10)=8.316 xx10^(24)`

`Delta N=9xx10^(24)-8.316 xx10^(24)=6.84 xx10^(23)`

`E=6.84 xx10^(23)xx9.0 xx10^(-13)=6.2 xx10^(11)\ \text{J}`


♦ Mean mark part (b) 51%.

Filed Under: Properties of the Nucleus Tagged With: Band 4, Band 5, smc-3703-20-Conservation of Mass-Energy, smc-3703-40-Radioactive Decay

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