/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 73 A helium nucleus, also known as ... [FREE SOLUTION] | 91Ó°ÊÓ

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A helium nucleus, also known as an \(\alpha\) (alpha) particle, consists of two protons and two neutrons and has a diameter of \(10^{-15} \mathrm{~m}\) \(=1 \mathrm{fm} .\) The protons, with a charge of te, are subject to a repulsive Coulomb force. since the neutrons have zero charge, there must be an attractive force that counteracts the electric repulsion and keeps the protons from flying apart. This so-called strong force plays a central role in particle physics. (a) As a crude model, assume that an \(\alpha\) particle consists of two pointlike protons attracted by a Hooke's-law spring with spring constant \(k,\) and ignore the neutrons. Assume further that in the absence of other forces, the spring has an equilibrium separation of zero. Write an expression for the potential energy when the protons are separated by distance \(d\). (b) Minimize this potential to find the equilibrium separation \(d_{0}\) in terms of \(e\) and \(k .\) (c) If \(d_{0}=1.00 \mathrm{fm}\), what is the value of \(k ?\) (d) How much energy is stored in this system, in terms of electron volts? (e) A proton has a mass of \(1.67 \times 10^{-27} \mathrm{~kg}\). If the spring were to break, the \(\alpha\) particle would disintegrate and the protons would fly off in opposite directions. What would be their ultimate speed?

Short Answer

Expert verified
The spring constant is \(k = \frac{k_e \cdot e^{2}}{d_{0}^{2}}\). Then potential energy in this system is \(- \frac{k_e \cdot e^{2}}{d_0}\). The protons' speed, once the spring would break, can be calculated from \(\frac{1}{2} m v^{2} = -U\).

Step by step solution

01

Start by modeling the potential energy

Due to the repulsion between the protons, the potential energy of the system between two protons with a spring can be modeled by Hooke's Law and Coulomb's Law. The spring potential energy is \(-\frac{1}{2}k \cdot si^{2}\), the coulomb potential energy is given by \(\frac{k_e \cdot e^{2}}{d}\). Adding the two potential energies, we have total energy \(U = \frac{1}{2}k \cdot d^{2} - \frac{k_e \cdot e^{2}}{d}\)
02

Minimize the potential energy

The equilibrium distance of separation \(d_0\) can be calculated by setting the derivative of potential energy to zero. The derivative is given by \( 0 = k \cdot d - \frac{k_e \cdot e^{2}}{d^{2}} \). Solving this equation gives \(d_0 = \sqrt{\frac{k_e \cdot e^{2}}{k}}\)
03

Calculate the spring constant

Given \(d_{0}=1.00 \mathrm{fm}\), substitute it into the equation from step 2, we obtain the spring constant \(k = \frac{k_e \cdot e^{2}}{d_{0}^{2}}\)
04

Determine the energy

The potential energy stored in the system can be calculated by plugging the equilibrium distance \(d_0\) into the equation of the potential energy. This gives \(U = - \frac{k_e \cdot e^{2}}{d_0}\)
05

Calculate the proton speed

Due to conservation of energy, all the potential energy stored in the system is converted to kinetic energy when the spring breaks. This gives the equation \(K = -U\). Since \(K = \frac{1}{2} m v^{2}\), where \(m\) is the mass and \(v\) the speed of the protons, we can get their ultimate speed by solving for \(v\) in the equation \(\frac{1}{2} m v^{2} = -U\)

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Key Concepts

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

Coulomb's Law
Coulomb's Law is a fundamental principle in electromagnetism describing the force between two point charges. According to this law, the electric force (\( F \)) between two charges (\( q_1 \) and and say, it explains the underlying reasons for the interaction between charged particles like protons in the nucleus of an atom.

For example, in a helium nucleus, the repulsive force keeping two positively charged protons apart is explained by Coulomb's Law, which states that the magnitude of this force is directly proportional to the product of the charges and inversely proportional to the square of the distance between them. Mathematically, it is represented as \( F = k_e \frac{|q_1 \cdot q_2|}{r^2} \) where \( k_e \) is Coulomb's constant, \( q_1 \) and \( q_2 \) are the charges, and \( r \) is the separation distance.

When two protons in a helium nucleus are at a distance \( d \) apart, the potential energy due to the Coulomb force can be derived from this law and is given by \( U = \frac{k_e \cdot e^2}{d} \), where \( e \) is the charge of a proton. This formula plays a crucial role in determining the balance of forces and the potential energy within such nuclear systems.
Hooke's Law
Hooke's Law is a principle of physics that relates to the behavior of springs and other elastic objects. It states that the force needed to extend or compress a spring by some distance is proportional to that distance. This is represented by the equation \( F = -kx \) where \( F \) is the force applied to the spring, \( x \) is the displacement of the spring from its equilibrium position, and \( k \) is the spring constant which measures the stiffness of the spring.

When applying Hooke's Law to the helium nucleus model, it suggests that an invisible 'spring' is what holds together the two protons despite their mutual electric repulsion. The potential energy stored in this 'spring' when the protons are a distance \( d \) apart is \( U = \frac{1}{2}k \cdot d^2 \). Such a model helps to conceptualize the strong nuclear force that acts over short distances within the atomic nucleus to keep it stable and balanced against the electrical repulsion between protons.
Potential Energy Minimization
Potential energy minimization is a concept in physics that states that a system will naturally move towards a state of minimal potential energy. In the context of forces within an atom, this principle allows us to understand the stability of atomic structures.

In the modeling of the helium nucleus, potential energy minimization is crucial for finding the equilibrium separation of protons. By doing so, we are essentially finding the point at which the forces of attraction (modeled by Hooke's Law) and repulsion (described by Coulomb's Law) are balanced. Mathematically, this involves taking the derivative of the total potential energy function and setting it to zero to find the minimum value.

The equilibrium distance \( d_0 \) is the separation at which the potential energy of the system reaches its minimal value. According to the step-by-step solution, \( d_0 \) is given by \( d_0 = \sqrt{\frac{k_e \cdot e^2}{k}} \), where \( k_e \) is Coulomb's constant, \( e \) is the charge of the proton, and \( k \) is the spring constant. At this separation, the forces are in perfect balance, thus explaining the relative stability of the helium nucleus.

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Most popular questions from this chapter

A very long insulating cylinder of charge of radius \(2.50 \mathrm{~cm}\) carries a uniform linear density of \(15.0 \mathrm{nC} / \mathrm{m}\). If you put one probe of a voltmeter at the surface, how far from the surface must the other probe be placed so that the voltmeter reads \(175 \mathrm{~V} ?\)

A particle with charge \(+7.60 \mathrm{nC}\) is in a uniform electric field directed to the left. Another force, in addition to the electric force, acts on the particle so that when it is released from rest, it moves to the right. After it has moved \(8.00 \mathrm{~cm}\), the additional force has done \(6.50 \times 10^{-5} \mathrm{~J}\) of work and the particle has \(4.35 \times 10^{-5} \mathrm{~J}\) of kinetic energy. (a) What work was done by the electric force? (b) What is the potential of the starting point with respect to the end point? (c) What is the magnitude of the electric field?

A very large plastic sheet carries a uniform charge density of \(-6.00 \mathrm{nC} / \mathrm{m}^{2}\) on one face. (a) As you move away from the sheet along a line perpendicular to it, does the potential increase or decrease? How do you know, without doing any calculations? Does your answer depend on where you choose the reference point for potential? (b) Find the spacing between equipotential surfaces that differ from each other by \(1.00 \mathrm{~V}\). What type of surfaces are these?

The Millikan Oil-Drop Experiment. The charge of an electron was first measured by the American physicist Robert Millikan during \(1909-1913 .\) In his experiment, oil was sprayed in very fine drops (about \(10^{-4} \mathrm{~mm}\) in diameter) into the space between two parallel horizontal plates separated by a distance \(d\). A potential difference \(V_{A B}\) was maintained between the plates, causing a downward electric field between them. Some of the oil drops acquired a negative charge because of frictional effects or because of ionization of the surrounding air by x rays or radioactivity. The drops were observed through a microscope. (a) Show that an oil drop of radius \(r\) at rest between the plates remained at rest if the magnitude of its charge was \(q=\frac{4 \pi}{3} \frac{\rho r^{3} g d}{V_{A B}}\) where \(\rho\) is oil's density. (Ignore the buoyant force of the air.) By adjusting \(V_{A B}\) to keep a given drop at rest, Millikan determined the charge on that drop. provided its radius \(r\) was known. (b) Millikan's oil drops were much too small to measure their radii directly. Instead, Millikan determincd \(r\) by cutting off the electric field and measuring the terminal speed \(u_{\mathrm{i}}\) of the drop as it fell. (We discussed terminal speed in Section \(\left.5.3 .\right)\) The viscous force \(F\) on a sphere of radius \(r\) moving at speed \(v\) through a fluid with viscosity \(\eta\) is given by Stokes's law: \(F=6 \pi \eta r v .\) When a drop fell at \(v_{1}\), the viscous force just balanced the drop's weight \(w=m g\). Show that the magnitude of the charge on the drop was \(q=18 \pi \frac{d}{V_{A B}} \sqrt{\frac{\eta^{3} v_{1}^{3}}{2 \rho g}}\) (c) You repeat the Millikan oil-drop experiment. Four of your measured values of \(V_{A B}\) and \(v_{1}\) are listed in the table: $$ \begin{array}{lcccc} \text { Drop } & 1 & 2 & 3 & 4 \\ \hline V_{A B}(\mathrm{~V}) & 9.16 & 4.57 & 12.32 & 6.28 \\ v_{1}\left(10^{-5} \mathrm{~m} / \mathrm{s}\right) & 2.54 & 0.767 & 4.39 & 1.52 \end{array} $$ In your apparatus, the separation \(d\) between the horizontal plates is \(1.00 \mathrm{~mm}\). The density of the oil you use is \(824 \mathrm{~kg} / \mathrm{m}^{3}\). For the viscosity \(\eta\) of air, use the value \(1.81 \times 10^{-5} \mathrm{~N} \cdot \mathrm{s} / \mathrm{m}^{2}\). Assume that \(g=9.80 \mathrm{~m} / \mathrm{s}^{2}\). Calculate the charge \(q\) of each drop. (d) If electric charge is quantized (that is, exists in multiples of the magnitude of the charge of an electron), then the charge on each drop is -ne, where \(n\) is the number of excess electrons on each drop. (All four drops in your table have negative charge.) Drop 2 has the smallest magnitude of charge observed in the experiment, for all 300 drops on which measurements were made, so assume that its charge is due to an excess charge of one electron. Determine the number of excess electrons \(n\) for each of the other three drops. (e) Use \(q=-n e\) to calculate \(e\) from the data for each of the four drops, and average these four values to get your best experimental value of \(e .\)

Two stationary point charges \(+3.00 \mathrm{nC}\) and \(+2.00 \mathrm{nC}\) are separated by a distance of \(50.0 \mathrm{~cm}\). An electron is released from rest at a point midway between the two charges and moves along the line connecting the two charges. What is the speed of the electron when it is \(10.0 \mathrm{~cm}\) from the \(+3.00 \mathrm{nC}\) charge?

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