/*! 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 53 Determining the Size of the Nucl... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Determining the Size of the Nucless. When radium-226 decays radioactively, it emits an alpha particle (the nucleus of helium), and the end product is radon-222. We can model this decay by thinking of the radium-226 as consisting of an alpha particle emitted from the surface of the spherically symmetric radon-222 nucleus, and we can treat the alpha particle as a point charge. The energy of the alpha particle has been measured in the laboratory and has been found to be 4.79 MeV when the alpha particle is essentially infinitely far from the nucleus. Since radon is much heavier than the alpha particle, we can assume that there is no appreciable recoil of the radon after the decay. The radon nucleus contains 86 protons, while the alpha particle has 2 protons and the radium nucleus has 88 protons. (a) What was the electric potential energy of the alpha-radon combination just before the decay, in MeV and in joules? (b) Use your result from part (a) to calculate the radius of the radon nucleus.

Short Answer

Expert verified
The radius of the radon nucleus is approximately \(7.11 \times 10^{-15}\) meters.

Step by step solution

01

Understand the System

To find the radius of the radon nucleus, we start by visualizing the initial setup. The system consists of an alpha particle and a radon nucleus. The alpha particle can be treated as a point charge moving away from the surface of a spherically symmetric radon-222 nucleus. We know that the radon-222 nucleus has 86 protons, and the alpha particle has 2 protons.
02

Calculate Initial Electric Potential Energy

The potential energy of the alpha particle when it is close to the radon nucleus is given as total kinetic energy at infinite separation. Using the formula for potential energy between two point charges, \(U = \frac{k \cdot q_1 \cdot q_2}{r}\), where \(k=8.99 \times 10^{9} \, \text{N m}^2/\text{C}^2\,\), the charge of a proton \(e = 1.6 \times 10^{-19} \, \text{C}\), and converting MeV to Joules \(1 \, \text{MeV} = 1.6 \times 10^{-13} \, \text{J}\). Alpha's potential energy is thus 4.79 MeV or \(4.79 \times 1.6 \times 10^{-13} \, \text{J} = 7.664 \times 10^{-13} \, \text{J}\).
03

Convert Potential Energy to Joules

Ensure the initial potential energy calculated is precise. Calculate the electric potential energy in joules as previously outlined. The energy is \( U = 7.664 \times 10^{-13} \, \text{J} \).
04

Use Potential Energy to Find Radius

Rearranging the potential energy formula, \( r = \frac{k \cdot q_1 \cdot q_2}{U} \), we substitute the values \( q_1 = 2e \) and \( q_2 = 86e \). Substituting the values, we find \( r = \frac{8.99 \times 10^{9} \times 2 \times 86 \times (1.6 \times 10^{-19})^2}{7.664 \times 10^{-13}} \). When solving, ensure all units cancel properly to leave meters.
05

Solve for Radius

Perform the arithmetic calculations to find the radius: \( r = \frac{8.99 \times 10^{9} \times 2 \times 86 \times (1.6 \times 10^{-19})^2}{7.664 \times 10^{-13}} = 7.11 \times 10^{-15} \, \text{m}\). This result gives us the radius of the radon nucleus.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Alpha Particle
Understanding an alpha particle is key when studying nuclear decay and reactions. An alpha particle is essentially the nucleus of a helium-4 atom. It consists of two protons and two neutrons, leading to a double positive charge. The significance of the alpha particle lies in its role in alpha decay, a process where a radioactive nucleus emits an alpha particle. Not only does this reduce the atomic number of the original nucleus by two, but it also decreases its mass number by four.

This emission is a common form of radioactive decay among heavy elements like uranium and radium. An alpha particle, due to its relatively large mass and its charge, is not as penetrating as other forms of radiation such as beta particles or gamma rays. Instead, it tends to be stopped by just a few centimeters of air or a sheet of paper, making it less of a concern for shielding compared to other radiation types. Understanding the nature of alpha particles helps in exploring nuclear reactions and the changes in elements after radioactive decay.
Electric Potential Energy
Electric potential energy is a form of potential energy associated with the position of charged particles in an electric field. For two point charges, like the alpha particle and the radon nucleus in the decay process, this energy is calculated using the formula:

\[ U = \frac{k \cdot q_1 \cdot q_2}{r} \]

where \( U \) is the electric potential energy, \( k \) is Coulomb's constant \(8.99 \times 10^9 \, \text{N m}^2/\text{C}^2\), \( q_1 \) and \( q_2 \) are the charges involved, and \( r \) is the separation distance.

The importance of electric potential energy in nuclear physics is apparent when considering the initial decay scenarios. It dictates how much energy is available to the alpha particle as it moves away from the nucleus. In the given problem, the electric potential energy is initially equivalent to the kinetic energy of the alpha particle when it is infinitely far from the radon nucleus. This equivalence is crucial to understanding not just the energy balance in nuclear reactions but also in calculating further nuclear properties like the radius of the nucleus involved.
Radon Nucleus
The radon nucleus plays a central role in the decay process mentioned in the problem. Radon-222 refers to an isotope of radon produced from the alpha decay of radium-226. This radon nucleus is vital for understanding the decay chain and its implications. Radon, itself, is a heavy noble gas, known to be radioactive and occurs naturally through the decay of other heavier elements.

The presence of 86 protons in its nucleus characterizes radon-222, reflecting its position on the periodic table and its chemical properties. During the decay process, this nucleus loses an alpha particle, leading to a slight change in structure but maintaining its identity as radon-222 because the number of protons remains the key defining feature.
  • Understanding the radon nucleus’s role in radioactive decay helps in grasping the energy transformations involved.
  • It further aids in nuclear calculations - instances like estimating the radius of the nucleus, based on the potential energy of emitted particles.
Knowing how radon behaves after decay provides insights into nuclear stability and the pathways of nuclear transformations.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

In a certain region of space the electric potential is given by \(V=+A x^{2} y-B x y^{2},\) where \(A=5.00 \mathrm{V} / \mathrm{m}^{3}\) and \(B=\) 8.00 \(\mathrm{V} / \mathrm{m}^{3} .\) Calculate the magnitude and direction of the electric field at the point in the region that has coordinates \(x=2.00 \mathrm{m}\) \(y=0.400 \mathrm{m},\) and \(z=0\).

The \(\mathrm{H}_{2}^{+}\) Ion. The \(\mathrm{H}_{2}^{+}\) ion is composed of two protons, each of charge \(+e=1.60 \times 10^{-19} \mathrm{C},\) and an electron of charge \(-e\) and mass \(9.11 \times 10^{-31} \mathrm{kg} .\) The separation between the protons is \(1.07 \times 10^{-10} \mathrm{m} .\) The protons and the electron may be treated as point charges. (a) Suppose the electron is located at the point midway between the two protons. What is the potential energy of the interaction between the electron and the two protons? (Do not include the potential energy due to the interaction between the two protons.) (b) Suppose the electron in part (a) has a velocity of magnitude \(1.50 \times 10^{6} \mathrm{m} / \mathrm{s}\) in a direction along the perpendicular bisector of the line connecting the two protons. How far from the point midway between the two protons can the electron move? Because the masses of the protons are much greater than the electron mass, the motions of the protons are very slow and can be ignored. (Note: A realistic description of the electron motion requires the use of quantum mechanics, not Newtonian mechanics.)

A point charge \(q_{1}=+2.40 \mu \mathrm{C}\) is held stationary at the origin. A second point charge \(q_{2}=-4.30 \mu \mathrm{C}\) moves from the point \(x=0.150 \mathrm{m}, \quad y=0\) to the point \(x=0.250 \mathrm{m},\) \(y=0.250 \mathrm{m} .\) How much work is done by the electric force on \(q_{2} ?\)

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 positive charge \(q\) is fixed at the point \(x=0, y=0\) and a negative charge \(-2 q\) is fixed at the point \(x=a, y=0\). (a) Show the positions of the charges in a diagram. (b) Derive an expression for the potential \(V\) at points on the \(x\) -axis as a function of the coordinate \(x .\) Take \(V\) to be zero at an infinite distance from the charges. (c) At which positions on the \(x\) -axis is \(V=0 ?\) (d) Graph \(V\) at points on the \(x\) -axis as a function of \(x\) in the range from \(x=-2 a\) to \(x=+2 a\) (e) What does the answer to part (b) become when \(x>\) a? Explain why this result is obtained.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.