The intensity of cosmic ray radiation decreases rapidly with increasing energy, but there are occasionally extremely energetic cosmic rays that create a shower of radiation from all the particles they create by striking a nucleus in the atmosphere. Suppose a cosmic ray particle having an energy of \(10^{10} \mathrm{GeV}\) converts its energy into particles with masses averaging \(200 \mathrm{MeV} / \mathrm{c}^{2}\) (a) How many particles are created? (b) If the particles rain down on a \(1.00-\mathrm{km}^{2}\) area, how many particles are there per square meter?

Short Answer

Expert verified
The initial energy E_initial is \(1.6\times10^1\,\mathrm{J}\) and the average energy E_particle is \(6.4\times10^{-11}\,\mathrm{J}\). To find the number of particles created, we divide the initial energy by the energy per particle, giving \(N=2.5\times10^{14}\) particles. To find the particles per square meter, the given area is \(1.00\,\mathrm{km}^2\), or \(1\times10^6\, \mathrm{m}^2\). Dividing the number of particles by the area, we get \(N_{\mathrm{square\,meter}}=2.5\times10^8\) particles per square meter.

Step by step solution

01

Determine the initial and final energy states

First, we'll convert the given energy units into SI units: Joules (J). 1 GeV = \(1\times10^9\) eV, and 1 eV = \(1.6\times10^{-19}\) J. So, the initial energy of the cosmic ray particle, E_initial, is: \(E_{initial} = 10^{10}\,\mathrm{GeV} \times\frac {1\times10^9\,\mathrm{eV}}{1\,\mathrm{GeV}}\times\frac {1.6\times10^{-19}\,\mathrm{J}}{1\,\mathrm{eV}}\) The average mass of the particles created can also be converted into energy using E=mc^2. Let's convert the mass to energy: \(E_{particle} = (200\,\frac{\mathrm{MeV}}{\mathrm{c}^2})\times\frac {1\times10^6\,\mathrm{eV}}{1\,\mathrm{MeV}}\times\frac {1.6\times10^{-19}\,\mathrm{J}}{1\,\mathrm{eV}}\times\frac {c}{c^2}\) Where c is the speed of light \(3\times10^8\) m/s.
02

Calculate the number of particles created

To find the number of particles created, divide the initial energy by the energy per particle: \(N = \frac{E_{initial}}{E_{particle}}\)
03

Calculate the particles per square meter

The given area is 1.00 km^2, and we are asked to determine the particles per square meter: Area = \(1.00 \,\mathrm{km}^2 \times\frac{1\times10^6\,\mathrm{m}^2}{1\,\mathrm{km}^2}\) Now, we can calculate the number of particles per square meter: \(N_{\mathrm{square\,meter}} = \frac{N}{\mathrm{Area}}\)

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 Vaia!

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 supernovae, neutrinos are produced in huge amounts. They were detected from the 1987 A supernova in the Magellanic Cloud, which is about 120,000 lightyears away from Earth (relatively close to our Milky Way Galaxy). If neutrinos have a mass, they cannot travel at the speed of light, but if their mass is small, their velocity would be almost that of light. (a) Suppose a neutrino with a \(7-\mathrm{eV} / c^{2}\) mass has a kinetic energy of \(700 \mathrm{keV}\). Find the relativistic quantity \(\gamma=\frac{1}{\sqrt{1-v^{2} / c^{2}}}\) for it. (b) If the neutrino leaves the 1987 A supernova at the same time as a photon and both travel to Earth, how much sooner does the photon arrive? This is not a large time difference, given that it is impossible to know which neutrino left with which photon and the poor efficiency of the neutrino detectors. Thus, the fact that neutrinos were observed within hours of the brightening of the supernova only places an upper limit on the neutrino's mass. (Hint: You may need to use a series expansion to find \(v\) for the neutrino, since its \(\gamma\) is so large.)

Each of the following strong nuclear reactions is forbidden. Identify a conservation law that is violated for each one. (a) \(\mathrm{p}+\overline{\mathrm{p}} \rightarrow \mathrm{p}+\mathrm{n}+\overline{\mathrm{p}}\) (b) \(\mathrm{p}+\mathrm{n} \rightarrow \mathrm{p}+\overrightarrow{\mathrm{p}}+\mathrm{n}+\pi^{+}\) (c) \(\pi^{-}+\mathrm{p} \rightarrow \Sigma^{+}+\mathrm{K}^{-}\) (d) \(\mathrm{K}^{-}+\mathrm{p} \rightarrow \Lambda^{0}+\mathrm{n}\)

(a) Calculate the approximate age of the universe from the average value of the Hubble constant, \(H_{0}=20 \mathrm{km} / \mathrm{s} \cdot \mathrm{Mly} .\) To do this, calculate the time it would take to travel \(0.307 \mathrm{Mpc}\) at a constant expansion rate of \(20 \mathrm{km} / \mathrm{s} .\) (b) If somehow acceleration occurs, would the actual age of the universe be greater or less than that found here? Explain.

If a theory is developed that unifies all four forces, will it still be correct to say that the orbit of the Moon is determined by the gravitational force? Explain why.

What is the wavelength of a \(50-\mathrm{GeV}\) electron, which is produced at SLAC? This provides an idea of the limit to the detail it can probe.

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.

Sign-up for free