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The Earth is constantly being bombarded by cosmic rays, which consist mostly of protons. These protons are incident on the Earth's atmosphere from all directions at a rate of 1245.0 protons per square meter per second. Assuming that the depth of Earth's atmosphere is \(120 \mathrm{~km},\) what is the total charge incident on the atmosphere in \(5.00 \mathrm{~min}\) ? Assume that the radius of the surface of the Earth is \(6378 \mathrm{~km}\).

Short Answer

Expert verified
Answer: The total charge incident on Earth's atmosphere due to cosmic rays in 5.00 minutes is approximately 3.08 × 10^8 C.

Step by step solution

01

Find the Effective Area of Earth's Atmosphere

To find the area of the Earth's atmosphere, we will first assume it is a sphere and calculate the surface area. The given radius of the Earth is \(6378 \mathrm{~km}\), and the depth of the atmosphere is \(120 \mathrm{~km}\). Therefore, the total radius of the atmosphere is \((6378+120) \mathrm{~km}\). We can calculate the surface area of the sphere using the formula \(A=4 \pi r^2\).
02

Calculate the Rate of Incident Charge

Next, we need to calculate the charge incident on the Earth's atmosphere due to cosmic rays. We are given the rate of incident protons as \(1245.0 \mathrm{~protons/m^2/s}\). Since the charge of a proton is \(e = 1.6 \times 10^{-19} \mathrm{C}\), we can find the rate of charge incident per square meter: \(\mathrm{charge\,rate \, density} = (1245.0 \mathrm{~protons/m^2/s}) \times (1.6 \times 10^{-19} \mathrm{C/proton})\).
03

Calculate the Total Charge

Now that we have the rate of charge and the area of the Earth's atmosphere, we can find the total charge incident on the Earth's atmosphere in the given time. First, we need to convert the given time of \(5.00 \mathrm{~min}\) to seconds: \(5.00 \mathrm{~min} \times (60 \mathrm{s/min})\). Then, we can find the total charge by multiplying the charge rate density, the area of the Earth's atmosphere, and the time: \(\mathrm{Total \, Charge} = \mathrm{charge\, rate\, density} \times \mathrm{Area} \times \mathrm{Time}\).
04

Final Calculation and Answer

Let's calculate the final answer by plugging in the values from the previous steps: 1. Calculate the area of the Earth's atmosphere: \(A = 4 \pi ((6378 + 120)\times 10^3 \mathrm{m})^2 = 5.147\times10^{14} \mathrm{m^2}\). 2. Calculate the charge rate density: \(\mathrm{charge\,rate \, density} = (1245.0 \mathrm{~protons/m^2/s}) \times (1.6 \times 10^{-19} \mathrm{C/proton}) = 1.992 \times 10^{-16} \mathrm{C/m^2/s}\). 3. Convert the given time to seconds: \(5.00 \mathrm{~min} \times (60 \mathrm{s/min}) = 300 \mathrm{s}\). 4. Calculate the total charge: \(\mathrm{Total \, Charge} = (1.992 \times 10^{-16} \mathrm{C/m^2/s}) \times (5.147\times10^{14} \mathrm{m^2}) \times (300 \mathrm{s}) \approx 3.08 \times 10^8 \mathrm{C}\). So, the total charge incident on Earth's atmosphere due to cosmic rays in \(5.00 \mathrm{~min}\) is approximately \(3.08 \times 10^8 \mathrm{C}\).

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Key Concepts

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

Earth's atmosphere
Our planet is shrouded in a blanket of gases known as the Earth's atmosphere. This essential layer is composed of multiple levels, each with its own characteristics and roles. The atmosphere is vital for life, as it provides oxygen for breathing, protects us from harmful solar radiation, and helps regulate the Earth's temperature.

When discussing cosmic rays and their interaction with the Earth, it's the outermost layers of the atmosphere that concern us most. Cosmic rays, primarily coming from outside our solar system, are high-energy particles that streak through space at nearly the speed of light. Upon contacting the Earth's atmosphere, these rays collide with atoms, creating a cascade of secondary particles that shower down towards the surface.

Understanding the depth and composition of the atmosphere is integral when calculating the effect of cosmic rays. As seen in the exercise, the atmosphere's depth is taken to be 120 km, which, combined with the radius of the Earth, sets the stage for determining the area this protective shield covers, and in turn, the quantity of cosmic rays it encounters.
Charge of a proton
A proton is one of the building blocks of matter, residing in the nucleus of atoms alongside neutrons. Its significance goes beyond its structural role; the proton carries a fundamental quantity of positive electric charge.

The charge of a proton is approximately equal to the elementary charge, designated as \(e\), which is a constant at \(1.6 \times 10^{-19}\) Coulombs (C). This value is vital for calculations involving electrical phenomena, and it is inversely equal in magnitude to the charge of an electron but of opposite sign, meaning while electrons carry negative charge, protons carry positive charge.

In the context of cosmic rays and our exercise, this elementary charge of protons, when multiplied by the number of protons per unit area and time, yields the charge rate density. This is an essential step towards understanding the total electrical charge that cosmic rays contribute to the Earth's atmosphere over a given period.
Surface area of a sphere
The surface area of a sphere is an essential concept in geometry that extends to various physical applications, including astronomy, physics, and even Earth science. For a sphere with a radius \(r\), the surface area \(A\) is calculated using the formula \(A = 4\pi r^2\).

This calculation is especially relevant when estimating phenomena that cover the Earth, such as satellite coverage areas, weather patterns, or, as in our exercise, cosmic ray exposure. It serves as the base calculation to understand the extent of Earth's atmosphere's exposure to cosmic rays. When using this formula, it's important to keep in mind the units involved; since the radius of the Earth is typically given in kilometers, it should be converted to meters to match the standard scientific units for surface area measurement in square meters (\(m^2\)).

By applying this formula, we can infer that the larger the surface area of a sphere, the greater the potential interaction with external influences such as cosmic rays, which emphasizes the scale of impact these high-energy particles have on our planet.

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Most popular questions from this chapter

A positive charge \(q_{1}=1.00 \mu \mathrm{C}\) is fixed at the origin, and a second charge \(q_{2}=-2.00 \mu \mathrm{C}\) is fixed at \(x=10.0 \mathrm{~cm} .\) Where along the \(x\) -axis should a third charge be positioned so that it experiences no force?

You bring a negatively charged rubber rod close to a grounded conductor without touching it. Then you disconnect the ground. What is the sign of the charge on the conductor after you remove the charged rod? a) negative d) cannot be determined from b) positive the given information c) no charge

A silicon sample is doped with phosphorus at 1 part per \(1.00 \cdot 10^{6} .\) Phosphorus acts as an electron donor, providing one free electron per atom. The density of silicon is \(2.33 \mathrm{~g} / \mathrm{cm}^{3},\) and its atomic mass is \(28.09 \mathrm{~g} / \mathrm{mol}\) a) Calculate the number of free (conduction) electrons per unit volume of the doped silicon. b) Compare the result from part (a) with the number of conduction electrons per unit volume of copper wire (assume each copper atom produces one free (conduction) electron). The density of copper is \(8.96 \mathrm{~g} / \mathrm{cm}^{3},\) and its atomic mass is \(63.54 \mathrm{~g} / \mathrm{mol}\)

Rubbing a balloon causes it to become negatively charged. The balloon then tends to cling to the wall of a room. For this to happen, must the wall be positively charged?

As shown in the figure, charge 1 is \(3.94 \mu \mathrm{C}\) and is located at \(x_{1}=-4.7 \mathrm{~m},\) and charge 2 is \(6.14 \mu \mathrm{C}\) and is at \(x_{2}=\) \(12.2 \mathrm{~m} .\) What is the \(x\) -coordinate of the point at which the net force on a point charge of \(0.300 \mu \mathrm{C}\) is zero?

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